Nickel nanoparticle-decorated phosphorous-doped graphitic carbon nitride (Ni@g-PC3N4)
was synthesized and used as an efficient photoactive catalyst for the reduction of various
nitrobenzenes under visible light irradiation. Hydrazine monohydrate was used as the source
of protons and electrons for the intended reaction. The developed photocatalyst was found to be
highly active and afforded excellent product yields under mild experimental conditions. In addition,
the photocatalyst could easily be recovered and reused for several runs without any detectable
leaching during the reaction.
Metal-organic hybrid: Photoreduction of CO2 using graphitic carbon nitride su...Pawan Kumar
A novel heteroleptic iridium complex supported on graphitic carbon nitride was synthesized and used
for photoreduction of carbon dioxide under visible light irradiation. The methanol yield obtained after
24 h irradiation was 9934 mmol g1cat (TON 1241 with respect to Ir) by using triethylamine (TEA) as a
sacrificial donor, which was significantly higher as compared to the semiconductor carbon nitride
145 mmol g1cat under identical conditions. The presence of triethylamine was found to be vital for the
higher methanol yield. After the reaction, the photocatalyst could easily be recovered and reused for
subsequent six runs without significant loss in photo activity.
Metal-organic hybrid: Photoreduction of CO2 using graphitic carbon nitride su...Pawan Kumar
A novel heteroleptic iridium complex supported on graphitic carbon nitride was synthesized and used
for photoreduction of carbon dioxide under visible light irradiation. The methanol yield obtained after
24 h irradiation was 9934 mmol g1cat (TON 1241 with respect to Ir) by using triethylamine (TEA) as a
sacrificial donor, which was significantly higher as compared to the semiconductor carbon nitride
145 mmol g1cat under identical conditions. The presence of triethylamine was found to be vital for the
higher methanol yield. After the reaction, the photocatalyst could easily be recovered and reused for
subsequent six runs without significant loss in photo activity.
Metal-organic hybrid: Photoreduction of CO2 using graphitic carbon nitride su...Pawan Kumar
A novel heteroleptic iridium complex supported on graphitic carbon nitride was synthesized and used for photoreduction of carbon dioxide under visible light irradiation. The methanol yield obtained after 24 h irradiation was 9934 μmol g−1cat (TON 1241 with respect to Ir) by using triethylamine (TEA) as a sacrificial donor, which was significantly higher as compared to the semiconductor carbon nitride 145 μmol g−1cat under identical conditions. The presence of triethylamine was found to be vital for the higher methanol yield. After the reaction, the photocatalyst could easily be recovered and reused for subsequent six runs without significant loss in photo activity.
A highly efficient, recyclable and magnetically separable core-shell structured CuZnO@Fe3O4 microsphere
wrapped with reduced graphene oxide (rGO@CuZnO@Fe3O4) photocatalyst has been developed and used
for the photoreduction of carbon dioxide with water to produce methanol under visible light irradiation.
Owing to the synergistic effect of the components and to the presence of a thin Fe2O3 layer on Fe3O4,
rGO@CuZnO@Fe3O4 4 exhibited higher catalytic activity as compared to the other possible combinations
such as CuZnO@Fe3O4 2 and GO@CuZnO@Fe3O4 3 microspheres. The yield of methanol in case of using
2 and 3 as photocatalyst was found to be 858 and 1749 mol g−1 cat, respectively. However, the yield
was increased to 2656 mol g−1 cat when rGO@CuZnO@Fe3O4 4 was used as photocatalyst under similar
experimental conditions. This superior photocatalytic activity of 4 was assumed to be due to the
restoration of the sp2 hybridized aromatic system in rGO, which facilitated the movement of electrons
and resulted in better charge separation. The synthesized heterogeneous photocatalyst could readily be
recovered by external magnet and successfully reused for six subsequent cycles without significant loss
in the product yield
Water-splitting photoelectrodes consisting of heterojunctions of carbon nitri...Pawan Kumar
Quinary and senary non-stoichiometric double perovskites such as Ba2Ca0.66Nb1.34-xFexO6-δ (BCNF) have been utilized for gas sensing, solid oxide fuel cells and thermochemical CO2 reduction. Herein, we examined their potential as narrow bandgap semiconductors for use in solar energy harvesting. A cobalt co-doped BCNF, Ba2Ca0.66Nb0.68Fe0.33Co0.33O6-δ (BCNFCo), exhibited an optical absorption edge at ~ 800 nm, p-type conduction and a distinct photoresponse upto 640 nm while demonstrating high thermochemical stability. A nanocomposite of BCNFCo and g-C3N4 (CN) was prepared via a facile solvent assisted exfoliation/blending approach using dichlorobenzene and glycerol at a moderate temperature. The exfoliation of g-C3N4 followed by wrapping on perovskite established an effective heterojunction between the materials for charge separation. The conjugated 2D sheets of CN enabled better charge migration resulting in increased photoelectrochemical performance. A blend composed of 40 wt% perovskite and CN performed optimally, whilst achieving a photocurrent density as high as 1.5 mA cm-2 for sunlight-driven water-splitting with a Faradaic efficiency as high as ~ 88%.
Optical Control of Selectivity of High Rate CO2 Photoreduction Via Interband-...Pawan Kumar
Photonic crystals consisting of TiO2 nanotube arrays (PMTiNTs) with periodically modulated diameters were fabricated using a precise charge-controlled pulsed anodization technique. The PMTiNTs were decorated with gold nanoparticles (Au NPs) to form plasmonic photonic crystal photocatalysts (Au-PMTiNTs). A systematic study of CO2 photoreduction performance on as-prepared samples was conducted using different wavelengths and illumination sequences. A remarkable selectivity of the mechanism of CO2 photoreduction could be engineered by merely varying the spectral composition of the illumination sequence. Under AM1.5 G simulated sunlight (pathway#1), the Au-PMTiNTs produced methane (302 µmol h-1) from CO2 with high selectivity (89.3%). When also illuminated by a UV-poor white lamp (pathway#2), the Au-PMTiNTs produced formaldehyde (420 µmol h-1) and carbon monoxide (323 µmol h-1) with almost no methane evolved. We confirmed the photoreduction results by 13C isotope labeling experiments using GC-MS. These results point to optical control of the selectivity of high-rate CO2 photoreduction through selection of one of two different mechanistic pathways. Pathway#1 implicates electron-hole pairs generated through interband transitions in TiO2 and Au as the primary active species responsible for reducing CO2 to methane. Pathway#2 involves excitation of both TiO2 and surface plasmons in Au. Hot electrons produced by plasmon damping and photogenerated holes in TiO2 proceed to reduce CO2 to HCHO and CO through a plasmonic Z-scheme.
Reduced graphene oxide–CuO nanocomposites for photocatalyticconversion of CO2...Pawan Kumar
tReduced graphene oxide (rGO)–copper oxide nanocomposites are prepared by covalent grafting of CuOnanorods on the rGO skeleton. Chemical and structural features of rGO–CuO nanocomposites are probedby FTIR, XPS, XRD and HRTEM analyses. Photocatalytic potential of rGO–CuO nanocomposites is exploredfor reduction of CO2into the methanol under the visible light irradiation. The breadth of CuO nanorods andthe oxidation state of Cu in the rGO–CuO/Cu2O nanocomposites are systematically varied to investigatetheir photocatalytic activities. The pristine CuO nanorods exhibited very low photocatalytic activity owingto fast recombination of charge carriers and yielded 175 mol g−1methanol, whereas rGO–Cu2O andrGO–CuO exhibited significantly improved photocatalytic activities and yielded five (862 mol g−1) andseven (1228 mol g−1) folds methanol, respectively. The superior photocatalytic activity of CuO in therGO–CuO nanocomposites was attributed to slow recombination of charge carriers and efficient transferof photo-generated electrons through the rGO skeleton. This study further excludes the use of scavengingdonor.
Metal-organic hybrid: Photoreduction of CO2 using graphitic carbon nitride su...Pawan Kumar
A novel heteroleptic iridium complex supported on graphitic carbon nitride was synthesized and used
for photoreduction of carbon dioxide under visible light irradiation. The methanol yield obtained after
24 h irradiation was 9934 mmol g1cat (TON 1241 with respect to Ir) by using triethylamine (TEA) as a
sacrificial donor, which was significantly higher as compared to the semiconductor carbon nitride
145 mmol g1cat under identical conditions. The presence of triethylamine was found to be vital for the
higher methanol yield. After the reaction, the photocatalyst could easily be recovered and reused for
subsequent six runs without significant loss in photo activity.
Metal-organic hybrid: Photoreduction of CO2 using graphitic carbon nitride su...Pawan Kumar
A novel heteroleptic iridium complex supported on graphitic carbon nitride was synthesized and used
for photoreduction of carbon dioxide under visible light irradiation. The methanol yield obtained after
24 h irradiation was 9934 mmol g1cat (TON 1241 with respect to Ir) by using triethylamine (TEA) as a
sacrificial donor, which was significantly higher as compared to the semiconductor carbon nitride
145 mmol g1cat under identical conditions. The presence of triethylamine was found to be vital for the
higher methanol yield. After the reaction, the photocatalyst could easily be recovered and reused for
subsequent six runs without significant loss in photo activity.
Metal-organic hybrid: Photoreduction of CO2 using graphitic carbon nitride su...Pawan Kumar
A novel heteroleptic iridium complex supported on graphitic carbon nitride was synthesized and used for photoreduction of carbon dioxide under visible light irradiation. The methanol yield obtained after 24 h irradiation was 9934 μmol g−1cat (TON 1241 with respect to Ir) by using triethylamine (TEA) as a sacrificial donor, which was significantly higher as compared to the semiconductor carbon nitride 145 μmol g−1cat under identical conditions. The presence of triethylamine was found to be vital for the higher methanol yield. After the reaction, the photocatalyst could easily be recovered and reused for subsequent six runs without significant loss in photo activity.
A highly efficient, recyclable and magnetically separable core-shell structured CuZnO@Fe3O4 microsphere
wrapped with reduced graphene oxide (rGO@CuZnO@Fe3O4) photocatalyst has been developed and used
for the photoreduction of carbon dioxide with water to produce methanol under visible light irradiation.
Owing to the synergistic effect of the components and to the presence of a thin Fe2O3 layer on Fe3O4,
rGO@CuZnO@Fe3O4 4 exhibited higher catalytic activity as compared to the other possible combinations
such as CuZnO@Fe3O4 2 and GO@CuZnO@Fe3O4 3 microspheres. The yield of methanol in case of using
2 and 3 as photocatalyst was found to be 858 and 1749 mol g−1 cat, respectively. However, the yield
was increased to 2656 mol g−1 cat when rGO@CuZnO@Fe3O4 4 was used as photocatalyst under similar
experimental conditions. This superior photocatalytic activity of 4 was assumed to be due to the
restoration of the sp2 hybridized aromatic system in rGO, which facilitated the movement of electrons
and resulted in better charge separation. The synthesized heterogeneous photocatalyst could readily be
recovered by external magnet and successfully reused for six subsequent cycles without significant loss
in the product yield
Water-splitting photoelectrodes consisting of heterojunctions of carbon nitri...Pawan Kumar
Quinary and senary non-stoichiometric double perovskites such as Ba2Ca0.66Nb1.34-xFexO6-δ (BCNF) have been utilized for gas sensing, solid oxide fuel cells and thermochemical CO2 reduction. Herein, we examined their potential as narrow bandgap semiconductors for use in solar energy harvesting. A cobalt co-doped BCNF, Ba2Ca0.66Nb0.68Fe0.33Co0.33O6-δ (BCNFCo), exhibited an optical absorption edge at ~ 800 nm, p-type conduction and a distinct photoresponse upto 640 nm while demonstrating high thermochemical stability. A nanocomposite of BCNFCo and g-C3N4 (CN) was prepared via a facile solvent assisted exfoliation/blending approach using dichlorobenzene and glycerol at a moderate temperature. The exfoliation of g-C3N4 followed by wrapping on perovskite established an effective heterojunction between the materials for charge separation. The conjugated 2D sheets of CN enabled better charge migration resulting in increased photoelectrochemical performance. A blend composed of 40 wt% perovskite and CN performed optimally, whilst achieving a photocurrent density as high as 1.5 mA cm-2 for sunlight-driven water-splitting with a Faradaic efficiency as high as ~ 88%.
Optical Control of Selectivity of High Rate CO2 Photoreduction Via Interband-...Pawan Kumar
Photonic crystals consisting of TiO2 nanotube arrays (PMTiNTs) with periodically modulated diameters were fabricated using a precise charge-controlled pulsed anodization technique. The PMTiNTs were decorated with gold nanoparticles (Au NPs) to form plasmonic photonic crystal photocatalysts (Au-PMTiNTs). A systematic study of CO2 photoreduction performance on as-prepared samples was conducted using different wavelengths and illumination sequences. A remarkable selectivity of the mechanism of CO2 photoreduction could be engineered by merely varying the spectral composition of the illumination sequence. Under AM1.5 G simulated sunlight (pathway#1), the Au-PMTiNTs produced methane (302 µmol h-1) from CO2 with high selectivity (89.3%). When also illuminated by a UV-poor white lamp (pathway#2), the Au-PMTiNTs produced formaldehyde (420 µmol h-1) and carbon monoxide (323 µmol h-1) with almost no methane evolved. We confirmed the photoreduction results by 13C isotope labeling experiments using GC-MS. These results point to optical control of the selectivity of high-rate CO2 photoreduction through selection of one of two different mechanistic pathways. Pathway#1 implicates electron-hole pairs generated through interband transitions in TiO2 and Au as the primary active species responsible for reducing CO2 to methane. Pathway#2 involves excitation of both TiO2 and surface plasmons in Au. Hot electrons produced by plasmon damping and photogenerated holes in TiO2 proceed to reduce CO2 to HCHO and CO through a plasmonic Z-scheme.
Reduced graphene oxide–CuO nanocomposites for photocatalyticconversion of CO2...Pawan Kumar
tReduced graphene oxide (rGO)–copper oxide nanocomposites are prepared by covalent grafting of CuOnanorods on the rGO skeleton. Chemical and structural features of rGO–CuO nanocomposites are probedby FTIR, XPS, XRD and HRTEM analyses. Photocatalytic potential of rGO–CuO nanocomposites is exploredfor reduction of CO2into the methanol under the visible light irradiation. The breadth of CuO nanorods andthe oxidation state of Cu in the rGO–CuO/Cu2O nanocomposites are systematically varied to investigatetheir photocatalytic activities. The pristine CuO nanorods exhibited very low photocatalytic activity owingto fast recombination of charge carriers and yielded 175 mol g−1methanol, whereas rGO–Cu2O andrGO–CuO exhibited significantly improved photocatalytic activities and yielded five (862 mol g−1) andseven (1228 mol g−1) folds methanol, respectively. The superior photocatalytic activity of CuO in therGO–CuO nanocomposites was attributed to slow recombination of charge carriers and efficient transferof photo-generated electrons through the rGO skeleton. This study further excludes the use of scavengingdonor.
tA highly efficient, recyclable and magnetically separable core-shell structured CuZnO@Fe3O4microspherewrapped with reduced graphene oxide (rGO@CuZnO@Fe3O4) photocatalyst has been developed and usedfor the photoreduction of carbon dioxide with water to produce methanol under visible light irradiation.Owing to the synergistic effect of the components and to the presence of a thin Fe2O3layer on Fe3O4,rGO@CuZnO@Fe3O44 exhibited higher catalytic activity as compared to the other possible combinationssuch as CuZnO@Fe3O42 and GO@CuZnO@Fe3O43 microspheres. The yield of methanol in case of using2 and 3 as photocatalyst was found to be 858 and 1749 mol g−1cat, respectively. However, the yieldwas increased to 2656 mol g−1cat when rGO@CuZnO@Fe3O44 was used as photocatalyst under sim-ilar experimental conditions. This superior photocatalytic activity of 4 was assumed to be due to therestoration of the sp2hybridized aromatic system in rGO, which facilitated the movement of electronsand resulted in better charge separation. The synthesized heterogeneous photocatalyst could readily berecovered by external magnet and successfully reused for six subsequent cycles without significant loss in the product yield.
A bridged ruthenium dimer (Ru–Ru) for photoreduction of CO2 under visible li...Pawan Kumar
A bridged binuclear complex consisting of two ruthenium units (Ru–Ru) connected through a bridging ligand was synthesized, in which one unit serves as a photosensitizer, while another unit works as a catalyst. The synthesized Ru–Ru photocatalyst was tested for photoreduction of CO2 to give CO and HCOOH under visible light irradiation in the presence of triethanolamine as a sacrificial donor. The yield of CO and HCOOH was found to be 54 ppm and 28 ppm respectively after 12 h of irradiation. Due to the binding of photosensitizer and catalyst units in a single molecule via bridging ligand provides faster and efficient electron transfer from sensitizer to catalyst unit which resulted in the higher activity and better product yields.
Nitrogen-doped graphene-supported copper complex: a novel photocatalyst for C...Pawan Kumar
A copper(II) complex grafted to nitrogen-doped graphene (GrN700–CuC) was synthesized and then
demonstrated as an efficient photocatalyst for CO2 reduction into methanol under visible light irradiation
using a DMF/water mixture. The chemical and microstructural features of GrN700–CuC nanosheets were
studied by FTIR, XPS, XRD and HRTEM analyses. Owing to its truly heterogeneous nature, GrN700–CuC
could be easily recovered after the photocatalytic reaction and showed efficient recyclability for
subsequent runs.
A bridged ruthenium dimer (ru–ru) for photoreduction of co2 under visible lig...Pawan Kumar
A bridged binuclear complex consisting of two ruthenium units (Ru–Ru) connected through a bridging
ligand was synthesized, in which one unit serves as a photosensitizer, while another unit works as a
catalyst. The synthesized Ru–Ru photocatalyst was tested for photoreduction of CO2 to give CO and
HCOOH under visible light irradiation in the presence of triethanolamine as a sacrificial donor. The yield
of CO and HCOOH was found to be 54 ppm and 28 ppm respectively after 12 h of irradiation. Due to the
binding of photosensitizer and catalyst units in a single molecule via bridging ligand provides faster and
efficient electron transfer from sensitizer to catalyst unit which resulted in the higher activity and better
product yields
Bicrystalline Titania Photocatalyst for Reduction of CO2 to Solar FuelsA'Lester Allen
Degussa P25, a mixture of anatase and rutile crystal structures, is the most commonly used precursor to form the photoactive layer in solar cells; however, the photocatalytic activity of rutile is inferior to brookite. This presentation discusses the enhancement in photocatalytic activity of an antase brookite mixture.
Photo-induced reduction of CO2 using a magnetically separable Ru-CoPc@TiO2@Si...Pawan Kumar
An efficient photo-induced reduction of CO2 using magnetically separable Ru-CoPc@TiO2@SiO2@Fe3O4
as a heterogeneous catalyst in which CoPc and Ru(bpy)2phene complexes were attached to a solid
support via covalent attachment under visible light is described. The as-synthesized catalyst was characterized
by a series of techniques including FTIR, UV-Vis, XRD, SEM, TEM, etc. and subsequently tested for
the photocatalytic reduction of carbon dioxide using triethylamine as a sacrificial donor and water as a
reaction medium. The developed photocatalyst exhibited a significantly higher catalytic activity to give a
methanol yield of 2570.78 μmol per g cat after 48 h.
Synthesis of flower-like magnetite nanoassembly: Application in the efficient...Pawan Kumar
A facile approach for the synthesis of magnetite microspheres with flower-like morphology is reported
that proceeds via the reduction of iron(III) oxide under a hydrogen atmosphere. The ensuing magnetic
catalyst is well characterized by XRD, FE-SEM, TEM, N2 adsorption-desorption isotherm, and
Mössbauer spectroscopy and explored for a simple yet efficient transfer hydrogenation reduction of a
variety of nitroarenes to respective anilines in good to excellent yields (up to 98%) employing hydrazine
hydrate. The catalyst could be easily separated at the end of a reaction using an external magnet and
can be recycled up to 10 times without any loss in catalytic activity.
Metal-organic hybrid: Photoreduction of CO2 using graphitic carbon nitride su...Pawan Kumar
A novel heteroleptic iridium complex supported on graphitic carbon nitride was synthesized and used
for photoreduction of carbon dioxide under visible light irradiation. The methanol yield obtained after
24 h irradiation was 9934 mmol g1cat (TON 1241 with respect to Ir) by using triethylamine (TEA) as a
sacrificial donor, which was significantly higher as compared to the semiconductor carbon nitride
145 mmol g1cat under identical conditions. The presence of triethylamine was found to be vital for the
higher methanol yield. After the reaction, the photocatalyst could easily be recovered and reused for subsequent six runs without significant loss in photo activity
Visible light assisted reduction of nitrobenzenes using Fe(bpy)3+2/rGOnanocom...Pawan Kumar
Visible-light-induced photocatalytic reduction of aromatic nitrobenzenes to the corresponding anilinesat room temperature using reduced graphene oxide (rGO) immobilized iron(II) bipyridine complex asphotocatalyst is described. The rGO-immobilized iron catalyst exhibited superior catalytic activity thanhomogeneous iron(II) bipyridine complex and much higher than metal free rGO photocatalysts. Theheterogeneous photocatalyst was found to be robust and could easily be recovered and reused for severalruns without any significant loss in photocatalytic activity.
Visible light assisted reduction of nitrobenzenes using Fe(bpy)3+2/rGOnanocom...Pawan Kumar
Visible-light-induced photocatalytic reduction of aromatic nitrobenzenes to the corresponding anilinesat room temperature using reduced graphene oxide (rGO) immobilized iron(II) bipyridine complex asphotocatalyst is described. The rGO-immobilized iron catalyst exhibited superior catalytic activity thanhomogeneous iron(II) bipyridine complex and much higher than metal free rGO photocatalysts. Theheterogeneous photocatalyst was found to be robust and could easily be recovered and reused for severalruns without any significant loss in photocatalytic activity.
Carbon Nitride Grafted Cobalt Complex (Co@npg-C3N4) for Visible LightAssiste...Pawan Kumar
Azide containing bipyridine complex of cobalt was grafted to
the propargylated nanoporous graphitic carbon nitride (npg-C3
N4) via click reaction to obtain heterogenized photocatalyst
which could efficiently provide direct esterification of aldehydes
under visible light irradiation at room temperature. The use of
click reaction as grafting strategy provided covalent attachment
of the cobalt complex to support which not only provided
higher loading but also precluded the leaching. Furthermore,
the presence of carbon nitride support exhibited synergistic
effect to enhance the reaction rate. In addition, the milder basic
nature of nitrogen containing graphitic support provided
efficient ester synthesis without the need for an external base.
The synthesized photocatalyst was found to be quite robust
which could easily be recovered and reused several times
without significantly losing activity.
A Prussian blue/carbon dot nanocomposite as an efficient visible light active...Pawan Kumar
A Prussian blue/carbon dot (PB/CD) nanocomposite was synthesised and used as a visible-light active
photocatalyst for the oxidative cyanation of tertiary amines to α-aminonitriles by using NaCN/acetic acid
as a cyanide source and H2O2 as an oxidant. The developed photocatalyst afforded high yields of products
after 8 h of visible light irradiation at room temperature. The catalyst was recycled and reused several
times without any significant loss in its activity
Visible light assisted hydrogen generation from complete decomposition of hyd...Pawan Kumar
Hydrogen is considered to be an ideal energy carrier, which produces only water when combined with
oxygen and thus has no detrimental effect on the environment. While the catalytic decomposition of
hydrous hydrazine for the production of hydrogen is well explored, little is known about its photocatalytic
decomposition. The present paper describes a highly efficient photochemical methodology for the production
of hydrogen through the decomposition of aqueous hydrazine using titanium dioxide nanoparticles
modified with a Rh(I) coordinated catechol phosphane ligand (TiO2–Rh) as a photocatalyst under visible
light irradiation. After 12 h of visible light irradiation, the hydrogen yield was 413 μmol g−1 cat with a hydrogen
evolution rate of 34.4 μmol g−1 cat h−1. Unmodified TiO2 nanoparticles offered a hydrogen yield of
83 μmol g−1 cat and a hydrogen evolution rate of only 6.9 μmol g−1 cat h−1. The developed photocatalyst
was robust under the experimental conditions and could be efficiently reused for five subsequent runs
without any significant change in its activity. The higher stability of the photocatalyst is attributed to the
covalent attachment of the Rh complex, whereas the higher activity is believed to be due to the synergistic
mechanism that resulted in better electron transfer from the Rh complex to the conduction band of TiO2
Heterojunctions of halogen-doped carbon nitride nanosheets and BiOI for sunli...Pawan Kumar
A fluorine-doped, chlorine-intercalated carbon nitride (CNF-Cl) photocatalyst has been synthesized for simultaneous improvements in light harvesting capability along with suppression
of charge recombination in bulk g-C3N4. The formation of heterojunctions of these CNF-Cl nanosheets with low bandgap, earth abundant bismuth oxyiodide (BiOI) was achieved, and the
synthesized heterojunctions were tested as active photoanodes in photoelectrochemical water splitting experiments. BiOI/CNF-Cl heterojunctions exhibited extended light harvesting with a
band-edge of 680 nm and generated photocurrent densities approaching 1.3 mA cm−2 under AM1.5 G one sun illumination. Scanning Kelvin probe force microscopy under optical bias
showed a surface potential of 207 mV for the 50% BiOI/CNF-Cl nanocomposite, while pristine CNF-Cl and BiOI had surface photopotential values of 83 mV and 98 mV, respectively, which in turn, provided direct evidence of superior charge separation in the heterojunction blends. Enhanced charge carrier separation and improved light harvesting capability in BiOI/CNF-Cl hybrids were found to be the dominant factors in increased photocurrent, compared to the pristine constituent materials.
Nitrogen-doped graphene-supported copper complex: a novel photocatalyst for C...Pawan Kumar
A copper(II) complex grafted to nitrogen-doped graphene (GrN700–CuC) was synthesized and then
demonstrated as an efficient photocatalyst for CO2 reduction into methanol under visible light irradiation
using a DMF/water mixture. The chemical and microstructural features of GrN700–CuC nanosheets were
studied by FTIR, XPS, XRD and HRTEM analyses. Owing to its truly heterogeneous nature, GrN700–CuC
could be easily recovered after the photocatalytic reaction and showed efficient recyclability for
subsequent runs.
Visible light assisted photocatalytic reduction of CO2 using a graphene oxide...Pawan Kumar
A new heteroleptic ruthenium complex containing 2-thiophenyl benzimidazole ligands was synthesized
using a microwave technique and was immobilized to graphene oxide via covalent attachment. The synthesized
catalyst was used for the photoreduction of carbon dioxide under visible light irradiation without
using a sacrificial agent, which gave 2050 μmol g−1 cat methanol after 24 h of irradiation
Visible light assisted photocatalytic reduction of CO2 using a graphene oxide...Pawan Kumar
A new heteroleptic ruthenium complex containing 2-thiophenyl benzimidazole ligands was synthesized
using a microwave technique and was immobilized to graphene oxide via covalent attachment. The synthesized
catalyst was used for the photoreduction of carbon dioxide under visible light irradiation without
using a sacrificial agent, which gave 2050 μmol g−1 cat methanol after 24 h of irradiation
A [Fe(bpy)3]2+ grafted graphitic carbon nitride hybrid for visible light assi...Pawan Kumar
The present paper describes the use of a readily synthesized, environmentally benign, reusable and nontoxic
iron based nanocomposite i.e iron(II) bipyridine grafted to graphitic carbon nitride (Fe(bpy)3/npg-
C3N4) as a photocatalyst, molecular oxygen as an oxidant and a household white LED as a light emitting
source for the oxidative coupling of benzylamines under mild reaction conditions. The developed heterogenized
homogeneous photocatalyst showed excellent activity with the added benefits of facile recovery
and efficient recycling ability without any significant loss in catalytic activity.
A [Fe(bpy)3]2+ grafted graphitic carbon nitride hybrid for visible light assi...Pawan Kumar
The present paper describes the use of a readily synthesized, environmentally benign, reusable and nontoxic
iron based nanocomposite i.e iron(II) bipyridine grafted to graphitic carbon nitride (Fe(bpy)3/npg-
C3N4) as a photocatalyst, molecular oxygen as an oxidant and a household white LED as a light emitting
source for the oxidative coupling of benzylamines under mild reaction conditions. The developed heterogenized
homogeneous photocatalyst showed excellent activity with the added benefits of facile recovery
and efficient recycling ability without any significant loss in catalytic activity.
C3N5: A Low Bandgap Semiconductor Containing an Azo-Linked Carbon Nitride Fra...Pawan Kumar
Modification of carbon nitride based polymeric 2D materials for tailoring their optical, electronic and chemical properties for various applications has gained significant interest. The present report demonstrates the synthesis of a novel modified carbon nitride framework with a remarkable 3:5 C:N stoichiometry (C3N5) and an electronic bandgap of 1.76 eV, by thermal deammoniation of the melem hydrazine precursor. Characterization revealed that in the C3N5 polymer, two s-heptazine units are bridged together with azo linkage, which constitutes an entirely new and different bonding fashion from g-C3N4 where three heptazine units are linked together with tertiary nitrogen. Extended conjugation due to overlap of azo nitrogens and increased electron density on heptazine nucleus due to the aromatic π network of heptazine units lead to an upward shift of the valence band maximum resulting in bandgap reduction
C3N5: A Low Bandgap Semiconductor Containing an Azo-Linked Carbon Nitride Fra...Pawan Kumar
Modification of carbon nitride based polymeric
2D materials for tailoring their optical, electronic and
chemical properties for various applications has gained
significant interest. The present report demonstrates the
synthesis of a novel modified carbon nitride framework with a
remarkable 3:5 C:N stoichiometry (C3N5) and an electronic
bandgap of 1.76 eV, by thermal deammoniation of the melem
hydrazine precursor. Characterization revealed that in the
C3N5 polymer, two s-heptazine units are bridged together with
azo linkage, which constitutes an entirely new and different
bonding fashion from g-C3N4 where three heptazine units are
linked together with tertiary nitrogen. Extended conjugation
due to overlap of azo nitrogens and increased electron density
on heptazine nucleus due to the aromatic π network of heptazine units lead to an upward shift of the valence band maximum
resulting in bandgap reduction down to 1.76 eV. XRD, He-ion imaging, HR-TEM, EELS, PL, fluorescence lifetime imaging,
Raman, FTIR, TGA, KPFM, XPS, NMR and EPR clearly show that the properties of C3N5 are distinct from pristine carbon
nitride (g-C3N4). When used as an electron transport layer (ETL) in MAPbBr3 based halide perovskite solar cells, C3N5
outperformed g-C3N4, in particular generating an open circuit photovoltage as high as 1.3 V, while C3N5 blended with
MAxFA1−xPb(I0.85Br0.15)3 perovskite active layer achieved a photoconversion efficiency (PCE) up to 16.7%. C3N5 was also
shown to be an effective visible light sensitizer for TiO2 photoanodes in photoelectrochemical water splitting. Because of its
electron-rich character, the C3N5 material displayed instantaneous adsorption of methylene blue from aqueous solution reaching
complete equilibrium within 10 min, which is significantly faster than pristine g-C3N4 and other carbon based materials. C3N5
coupled with plasmonic silver nanocubes promotes plasmon-exciton coinduced surface catalytic reactions reaching completion
at much low laser intensity (1.0 mW) than g-C3N4, which showed sluggish performance even at high laser power (10.0 mW).
The relatively narrow bandgap and 2D structure of C3N5 make it an interesting air-stable and temperature-resistant
semiconductor for optoelectronic applications while its electron-rich character and intrasheet cavity make it an attractive
supramolecular adsorbent for environmental applications.
tA highly efficient, recyclable and magnetically separable core-shell structured CuZnO@Fe3O4microspherewrapped with reduced graphene oxide (rGO@CuZnO@Fe3O4) photocatalyst has been developed and usedfor the photoreduction of carbon dioxide with water to produce methanol under visible light irradiation.Owing to the synergistic effect of the components and to the presence of a thin Fe2O3layer on Fe3O4,rGO@CuZnO@Fe3O44 exhibited higher catalytic activity as compared to the other possible combinationssuch as CuZnO@Fe3O42 and GO@CuZnO@Fe3O43 microspheres. The yield of methanol in case of using2 and 3 as photocatalyst was found to be 858 and 1749 mol g−1cat, respectively. However, the yieldwas increased to 2656 mol g−1cat when rGO@CuZnO@Fe3O44 was used as photocatalyst under sim-ilar experimental conditions. This superior photocatalytic activity of 4 was assumed to be due to therestoration of the sp2hybridized aromatic system in rGO, which facilitated the movement of electronsand resulted in better charge separation. The synthesized heterogeneous photocatalyst could readily berecovered by external magnet and successfully reused for six subsequent cycles without significant loss in the product yield.
A bridged ruthenium dimer (Ru–Ru) for photoreduction of CO2 under visible li...Pawan Kumar
A bridged binuclear complex consisting of two ruthenium units (Ru–Ru) connected through a bridging ligand was synthesized, in which one unit serves as a photosensitizer, while another unit works as a catalyst. The synthesized Ru–Ru photocatalyst was tested for photoreduction of CO2 to give CO and HCOOH under visible light irradiation in the presence of triethanolamine as a sacrificial donor. The yield of CO and HCOOH was found to be 54 ppm and 28 ppm respectively after 12 h of irradiation. Due to the binding of photosensitizer and catalyst units in a single molecule via bridging ligand provides faster and efficient electron transfer from sensitizer to catalyst unit which resulted in the higher activity and better product yields.
Nitrogen-doped graphene-supported copper complex: a novel photocatalyst for C...Pawan Kumar
A copper(II) complex grafted to nitrogen-doped graphene (GrN700–CuC) was synthesized and then
demonstrated as an efficient photocatalyst for CO2 reduction into methanol under visible light irradiation
using a DMF/water mixture. The chemical and microstructural features of GrN700–CuC nanosheets were
studied by FTIR, XPS, XRD and HRTEM analyses. Owing to its truly heterogeneous nature, GrN700–CuC
could be easily recovered after the photocatalytic reaction and showed efficient recyclability for
subsequent runs.
A bridged ruthenium dimer (ru–ru) for photoreduction of co2 under visible lig...Pawan Kumar
A bridged binuclear complex consisting of two ruthenium units (Ru–Ru) connected through a bridging
ligand was synthesized, in which one unit serves as a photosensitizer, while another unit works as a
catalyst. The synthesized Ru–Ru photocatalyst was tested for photoreduction of CO2 to give CO and
HCOOH under visible light irradiation in the presence of triethanolamine as a sacrificial donor. The yield
of CO and HCOOH was found to be 54 ppm and 28 ppm respectively after 12 h of irradiation. Due to the
binding of photosensitizer and catalyst units in a single molecule via bridging ligand provides faster and
efficient electron transfer from sensitizer to catalyst unit which resulted in the higher activity and better
product yields
Bicrystalline Titania Photocatalyst for Reduction of CO2 to Solar FuelsA'Lester Allen
Degussa P25, a mixture of anatase and rutile crystal structures, is the most commonly used precursor to form the photoactive layer in solar cells; however, the photocatalytic activity of rutile is inferior to brookite. This presentation discusses the enhancement in photocatalytic activity of an antase brookite mixture.
Photo-induced reduction of CO2 using a magnetically separable Ru-CoPc@TiO2@Si...Pawan Kumar
An efficient photo-induced reduction of CO2 using magnetically separable Ru-CoPc@TiO2@SiO2@Fe3O4
as a heterogeneous catalyst in which CoPc and Ru(bpy)2phene complexes were attached to a solid
support via covalent attachment under visible light is described. The as-synthesized catalyst was characterized
by a series of techniques including FTIR, UV-Vis, XRD, SEM, TEM, etc. and subsequently tested for
the photocatalytic reduction of carbon dioxide using triethylamine as a sacrificial donor and water as a
reaction medium. The developed photocatalyst exhibited a significantly higher catalytic activity to give a
methanol yield of 2570.78 μmol per g cat after 48 h.
Synthesis of flower-like magnetite nanoassembly: Application in the efficient...Pawan Kumar
A facile approach for the synthesis of magnetite microspheres with flower-like morphology is reported
that proceeds via the reduction of iron(III) oxide under a hydrogen atmosphere. The ensuing magnetic
catalyst is well characterized by XRD, FE-SEM, TEM, N2 adsorption-desorption isotherm, and
Mössbauer spectroscopy and explored for a simple yet efficient transfer hydrogenation reduction of a
variety of nitroarenes to respective anilines in good to excellent yields (up to 98%) employing hydrazine
hydrate. The catalyst could be easily separated at the end of a reaction using an external magnet and
can be recycled up to 10 times without any loss in catalytic activity.
Metal-organic hybrid: Photoreduction of CO2 using graphitic carbon nitride su...Pawan Kumar
A novel heteroleptic iridium complex supported on graphitic carbon nitride was synthesized and used
for photoreduction of carbon dioxide under visible light irradiation. The methanol yield obtained after
24 h irradiation was 9934 mmol g1cat (TON 1241 with respect to Ir) by using triethylamine (TEA) as a
sacrificial donor, which was significantly higher as compared to the semiconductor carbon nitride
145 mmol g1cat under identical conditions. The presence of triethylamine was found to be vital for the
higher methanol yield. After the reaction, the photocatalyst could easily be recovered and reused for subsequent six runs without significant loss in photo activity
Visible light assisted reduction of nitrobenzenes using Fe(bpy)3+2/rGOnanocom...Pawan Kumar
Visible-light-induced photocatalytic reduction of aromatic nitrobenzenes to the corresponding anilinesat room temperature using reduced graphene oxide (rGO) immobilized iron(II) bipyridine complex asphotocatalyst is described. The rGO-immobilized iron catalyst exhibited superior catalytic activity thanhomogeneous iron(II) bipyridine complex and much higher than metal free rGO photocatalysts. Theheterogeneous photocatalyst was found to be robust and could easily be recovered and reused for severalruns without any significant loss in photocatalytic activity.
Visible light assisted reduction of nitrobenzenes using Fe(bpy)3+2/rGOnanocom...Pawan Kumar
Visible-light-induced photocatalytic reduction of aromatic nitrobenzenes to the corresponding anilinesat room temperature using reduced graphene oxide (rGO) immobilized iron(II) bipyridine complex asphotocatalyst is described. The rGO-immobilized iron catalyst exhibited superior catalytic activity thanhomogeneous iron(II) bipyridine complex and much higher than metal free rGO photocatalysts. Theheterogeneous photocatalyst was found to be robust and could easily be recovered and reused for severalruns without any significant loss in photocatalytic activity.
Carbon Nitride Grafted Cobalt Complex (Co@npg-C3N4) for Visible LightAssiste...Pawan Kumar
Azide containing bipyridine complex of cobalt was grafted to
the propargylated nanoporous graphitic carbon nitride (npg-C3
N4) via click reaction to obtain heterogenized photocatalyst
which could efficiently provide direct esterification of aldehydes
under visible light irradiation at room temperature. The use of
click reaction as grafting strategy provided covalent attachment
of the cobalt complex to support which not only provided
higher loading but also precluded the leaching. Furthermore,
the presence of carbon nitride support exhibited synergistic
effect to enhance the reaction rate. In addition, the milder basic
nature of nitrogen containing graphitic support provided
efficient ester synthesis without the need for an external base.
The synthesized photocatalyst was found to be quite robust
which could easily be recovered and reused several times
without significantly losing activity.
A Prussian blue/carbon dot nanocomposite as an efficient visible light active...Pawan Kumar
A Prussian blue/carbon dot (PB/CD) nanocomposite was synthesised and used as a visible-light active
photocatalyst for the oxidative cyanation of tertiary amines to α-aminonitriles by using NaCN/acetic acid
as a cyanide source and H2O2 as an oxidant. The developed photocatalyst afforded high yields of products
after 8 h of visible light irradiation at room temperature. The catalyst was recycled and reused several
times without any significant loss in its activity
Visible light assisted hydrogen generation from complete decomposition of hyd...Pawan Kumar
Hydrogen is considered to be an ideal energy carrier, which produces only water when combined with
oxygen and thus has no detrimental effect on the environment. While the catalytic decomposition of
hydrous hydrazine for the production of hydrogen is well explored, little is known about its photocatalytic
decomposition. The present paper describes a highly efficient photochemical methodology for the production
of hydrogen through the decomposition of aqueous hydrazine using titanium dioxide nanoparticles
modified with a Rh(I) coordinated catechol phosphane ligand (TiO2–Rh) as a photocatalyst under visible
light irradiation. After 12 h of visible light irradiation, the hydrogen yield was 413 μmol g−1 cat with a hydrogen
evolution rate of 34.4 μmol g−1 cat h−1. Unmodified TiO2 nanoparticles offered a hydrogen yield of
83 μmol g−1 cat and a hydrogen evolution rate of only 6.9 μmol g−1 cat h−1. The developed photocatalyst
was robust under the experimental conditions and could be efficiently reused for five subsequent runs
without any significant change in its activity. The higher stability of the photocatalyst is attributed to the
covalent attachment of the Rh complex, whereas the higher activity is believed to be due to the synergistic
mechanism that resulted in better electron transfer from the Rh complex to the conduction band of TiO2
Heterojunctions of halogen-doped carbon nitride nanosheets and BiOI for sunli...Pawan Kumar
A fluorine-doped, chlorine-intercalated carbon nitride (CNF-Cl) photocatalyst has been synthesized for simultaneous improvements in light harvesting capability along with suppression
of charge recombination in bulk g-C3N4. The formation of heterojunctions of these CNF-Cl nanosheets with low bandgap, earth abundant bismuth oxyiodide (BiOI) was achieved, and the
synthesized heterojunctions were tested as active photoanodes in photoelectrochemical water splitting experiments. BiOI/CNF-Cl heterojunctions exhibited extended light harvesting with a
band-edge of 680 nm and generated photocurrent densities approaching 1.3 mA cm−2 under AM1.5 G one sun illumination. Scanning Kelvin probe force microscopy under optical bias
showed a surface potential of 207 mV for the 50% BiOI/CNF-Cl nanocomposite, while pristine CNF-Cl and BiOI had surface photopotential values of 83 mV and 98 mV, respectively, which in turn, provided direct evidence of superior charge separation in the heterojunction blends. Enhanced charge carrier separation and improved light harvesting capability in BiOI/CNF-Cl hybrids were found to be the dominant factors in increased photocurrent, compared to the pristine constituent materials.
Nitrogen-doped graphene-supported copper complex: a novel photocatalyst for C...Pawan Kumar
A copper(II) complex grafted to nitrogen-doped graphene (GrN700–CuC) was synthesized and then
demonstrated as an efficient photocatalyst for CO2 reduction into methanol under visible light irradiation
using a DMF/water mixture. The chemical and microstructural features of GrN700–CuC nanosheets were
studied by FTIR, XPS, XRD and HRTEM analyses. Owing to its truly heterogeneous nature, GrN700–CuC
could be easily recovered after the photocatalytic reaction and showed efficient recyclability for
subsequent runs.
Visible light assisted photocatalytic reduction of CO2 using a graphene oxide...Pawan Kumar
A new heteroleptic ruthenium complex containing 2-thiophenyl benzimidazole ligands was synthesized
using a microwave technique and was immobilized to graphene oxide via covalent attachment. The synthesized
catalyst was used for the photoreduction of carbon dioxide under visible light irradiation without
using a sacrificial agent, which gave 2050 μmol g−1 cat methanol after 24 h of irradiation
Visible light assisted photocatalytic reduction of CO2 using a graphene oxide...Pawan Kumar
A new heteroleptic ruthenium complex containing 2-thiophenyl benzimidazole ligands was synthesized
using a microwave technique and was immobilized to graphene oxide via covalent attachment. The synthesized
catalyst was used for the photoreduction of carbon dioxide under visible light irradiation without
using a sacrificial agent, which gave 2050 μmol g−1 cat methanol after 24 h of irradiation
A [Fe(bpy)3]2+ grafted graphitic carbon nitride hybrid for visible light assi...Pawan Kumar
The present paper describes the use of a readily synthesized, environmentally benign, reusable and nontoxic
iron based nanocomposite i.e iron(II) bipyridine grafted to graphitic carbon nitride (Fe(bpy)3/npg-
C3N4) as a photocatalyst, molecular oxygen as an oxidant and a household white LED as a light emitting
source for the oxidative coupling of benzylamines under mild reaction conditions. The developed heterogenized
homogeneous photocatalyst showed excellent activity with the added benefits of facile recovery
and efficient recycling ability without any significant loss in catalytic activity.
A [Fe(bpy)3]2+ grafted graphitic carbon nitride hybrid for visible light assi...Pawan Kumar
The present paper describes the use of a readily synthesized, environmentally benign, reusable and nontoxic
iron based nanocomposite i.e iron(II) bipyridine grafted to graphitic carbon nitride (Fe(bpy)3/npg-
C3N4) as a photocatalyst, molecular oxygen as an oxidant and a household white LED as a light emitting
source for the oxidative coupling of benzylamines under mild reaction conditions. The developed heterogenized
homogeneous photocatalyst showed excellent activity with the added benefits of facile recovery
and efficient recycling ability without any significant loss in catalytic activity.
C3N5: A Low Bandgap Semiconductor Containing an Azo-Linked Carbon Nitride Fra...Pawan Kumar
Modification of carbon nitride based polymeric 2D materials for tailoring their optical, electronic and chemical properties for various applications has gained significant interest. The present report demonstrates the synthesis of a novel modified carbon nitride framework with a remarkable 3:5 C:N stoichiometry (C3N5) and an electronic bandgap of 1.76 eV, by thermal deammoniation of the melem hydrazine precursor. Characterization revealed that in the C3N5 polymer, two s-heptazine units are bridged together with azo linkage, which constitutes an entirely new and different bonding fashion from g-C3N4 where three heptazine units are linked together with tertiary nitrogen. Extended conjugation due to overlap of azo nitrogens and increased electron density on heptazine nucleus due to the aromatic π network of heptazine units lead to an upward shift of the valence band maximum resulting in bandgap reduction
C3N5: A Low Bandgap Semiconductor Containing an Azo-Linked Carbon Nitride Fra...Pawan Kumar
Modification of carbon nitride based polymeric
2D materials for tailoring their optical, electronic and
chemical properties for various applications has gained
significant interest. The present report demonstrates the
synthesis of a novel modified carbon nitride framework with a
remarkable 3:5 C:N stoichiometry (C3N5) and an electronic
bandgap of 1.76 eV, by thermal deammoniation of the melem
hydrazine precursor. Characterization revealed that in the
C3N5 polymer, two s-heptazine units are bridged together with
azo linkage, which constitutes an entirely new and different
bonding fashion from g-C3N4 where three heptazine units are
linked together with tertiary nitrogen. Extended conjugation
due to overlap of azo nitrogens and increased electron density
on heptazine nucleus due to the aromatic π network of heptazine units lead to an upward shift of the valence band maximum
resulting in bandgap reduction down to 1.76 eV. XRD, He-ion imaging, HR-TEM, EELS, PL, fluorescence lifetime imaging,
Raman, FTIR, TGA, KPFM, XPS, NMR and EPR clearly show that the properties of C3N5 are distinct from pristine carbon
nitride (g-C3N4). When used as an electron transport layer (ETL) in MAPbBr3 based halide perovskite solar cells, C3N5
outperformed g-C3N4, in particular generating an open circuit photovoltage as high as 1.3 V, while C3N5 blended with
MAxFA1−xPb(I0.85Br0.15)3 perovskite active layer achieved a photoconversion efficiency (PCE) up to 16.7%. C3N5 was also
shown to be an effective visible light sensitizer for TiO2 photoanodes in photoelectrochemical water splitting. Because of its
electron-rich character, the C3N5 material displayed instantaneous adsorption of methylene blue from aqueous solution reaching
complete equilibrium within 10 min, which is significantly faster than pristine g-C3N4 and other carbon based materials. C3N5
coupled with plasmonic silver nanocubes promotes plasmon-exciton coinduced surface catalytic reactions reaching completion
at much low laser intensity (1.0 mW) than g-C3N4, which showed sluggish performance even at high laser power (10.0 mW).
The relatively narrow bandgap and 2D structure of C3N5 make it an interesting air-stable and temperature-resistant
semiconductor for optoelectronic applications while its electron-rich character and intrasheet cavity make it an attractive
supramolecular adsorbent for environmental applications.
Water-splitting photoelectrodes consisting of heterojunctions of carbon nitri...Devika Laishram
Quinary and senary non-stoichiometric double perovskites such as Ba2Ca0.66Nb1.34−xFexO6−δ
(BCNF) have been utilized for gas sensing, solid oxide fuel cells and thermochemical CO2
reduction. Herein, we examined their potential as narrow bandgap semiconductors for use in solar
energy harvesting. A cobalt co-doped BCNF, Ba2Ca0.66Nb0.68Fe0.33Co0.33O6−δ (BCNFCo),
exhibited an optical absorption edge at ∼800 nm, p-type conduction and a distinct photoresponse
up to 640 nm while demonstrating high thermochemical stability. A nanocomposite of BCNFCo
and g-C3N4 (CN) was prepared via a facile solvent-assisted exfoliation/blending approach using
dichlorobenzene and glycerol at a moderate temperature. The exfoliation of g-C3N4 followed by
wrapping on perovskite established an effective heterojunction between the materials for charge
separation. The conjugated 2D sheets of CN enabled better charge migration resulting in increased
photoelectrochemical performance. A blend composed of 40 wt% perovskites and CN performed
optimally, whilst achieving a photocurrent density as high as 1.5 mA cm−2 for sunlight-driven
water-splitting with a Faradaic efficiency as high as ∼88%.
Water-splitting photoelectrodes consisting of heterojunctions of carbon nitri...Pawan Kumar
Quinary and senary non-stoichiometric double perovskites such as Ba2Ca0.66Nb1.34−xFexO6−δ (BCNF) have been utilized for gas sensing, solid oxide fuel cells and thermochemical CO2 reduction. Herein, we examined their potential as narrow bandgap semiconductors for use in solar energy harvesting. A cobalt co-doped BCNF, Ba2Ca0.66Nb0.68Fe0.33Co0.33O6−δ (BCNFCo), exhibited an optical absorption edge at ∼800 nm, p-type conduction and a distinct photoresponse up to 640 nm while demonstrating high thermochemical stability. A nanocomposite of BCNFCo and g-C3N4 (CN) was prepared via a facile solvent-assisted exfoliation/blending approach using dichlorobenzene and glycerol at a moderate temperature. The exfoliation of g-C3N4 followed by wrapping on perovskite established an effective heterojunction between the materials for charge separation. The conjugated 2D sheets of CN enabled better charge migration resulting in increased photoelectrochemical performance. A blend composed of 40 wt% perovskites and CN performed optimally, whilst achieving a photocurrent density as high as 1.5 mA cm−2 for sunlight-driven water-splitting with a Faradaic efficiency as high as ∼88%.
Reduced graphene oxide–CuO nanocomposites for photocatalyticconversion of CO2...Pawan Kumar
Reduced graphene oxide (rGO)–copper oxide nanocomposites are prepared by covalent grafting of CuOnanorods on the rGO skeleton. Chemical and structural features of rGO–CuO nanocomposites are probedby FTIR, XPS, XRD and HRTEM analyses. Photocatalytic potential of rGO–CuO nanocomposites is exploredfor reduction of CO2into the methanol under the visible light irradiation. The breadth of CuO nanorods andthe oxidation state of Cu in the rGO–CuO/Cu2O nanocomposites are systematically varied to investigatetheir photocatalytic activities. The pristine CuO nanorods exhibited very low photocatalytic activity owingto fast recombination of charge carriers and yielded 175 mol g−1methanol, whereas rGO–Cu2O andrGO–CuO exhibited significantly improved photocatalytic activities and yielded five (862 mol g−1) andseven (1228 mol g−1) folds methanol, respectively. The superior photocatalytic activity of CuO in therGO–CuO nanocomposites was attributed to slow recombination of charge carriers and efficient transferof photo-generated electrons through the rGO skeleton. This study further excludes the use of scavengingdonor.
Photocatalytic reduction of carbon dioxide to methanol using a ruthenium trin...Pawan Kumar
A ruthenium trinuclear polyazine complex was synthesized and subsequently immobilized through
complexation to a graphene oxide support containing phenanthroline ligands (GO-phen). The developed
photocatalyst was used for the photocatalytic reduction of CO2 to methanol, using a 20 watt white cold
LED flood light, in a dimethyl formamide–water mixture containing triethylamine as a reductive
quencher. After 48 h illumination, the yield of methanol was found to be 3977.57 5.60 mmol gcat
1.
The developed photocatalyst exhibited a higher photocatalytic activity than graphene oxide, which
provided a yield of 2201.40 8.76 mmol gcat
1. After the reaction, the catalyst was easily recovered and
reused for four subsequent runs without a significant loss of catalytic activity and no leaching of the
metal/ligand was detected during the reaction
Vapor Deposition of Semiconducting Phosphorus Allotropes into TiO2 Nanotube A...Pawan Kumar
Recent evidence of exponential environmental degradation will demand a drastic shift in research and development toward exploiting alternative energy resources such as solar energy. Here, we report the successful low-cost and easily accessible synthesis of hybrid semiconductor@TiO2 nanotube photocatalysts. In order to realize its maximum potential in harvesting photons in the visible-light range, TiO2 nanotubes have been loaded with earth-abundant, low-band-gap fibrous red and black phosphorus (P). Scanning electron microscopy– and scanning transmission electron microscopy–energy-dispersive X-ray spectroscopy, X-ray diffraction, Raman spectroscopy, X-ray photoelectron microscopy, and UV–vis measurements have been performed, substantiating the deposition of fibrous red and black P on top and inside the cavities of 100-μm-long electrochemically fabricated nanotubes. The nanotubular …
BaAl1.4Si0.6O3.4N0.6:Eu 2+ green phosphors’ application for improving lumin...IJECEIAES
The molten salt synthesis (MSS) method was used to effectively prepare green phosphors BaAl1.4Si0.6O3.4N0.6:Eu 2+ (or BSON:Eu 2+ ) via one homogeneous sphere-like morphology utilizing NaNO3 in the form of the reacting agent. The phosphors produced one wide stimulation spectrum between 250 and 460 nm, as well as a significant green emission has a maximum point at 510 nm owing to the 4f 6 1 5d 7 -4f 8 ( S7/2) shifts for Eu 2+ ions. With illumination under 365 as well as 450 nm, the ideal discharge strengths for the specimen prepared utilizing melted salt would receive a boost of 17% and 13%, surpassing the specimen prepared utilizing the traditional solid-state reaction (SSR) approach. The abatement of concentration for the ions of Eu 2+ from BSON:Eu 2+ is 5 mol%. In addition, the interactivity of dipole-dipole would be the cause of said abatement. Heat abatement would be studied utilizing the formation coordinate method with abatement temperature reaching ∼200 C. Elemental mapping as well as power-dispersing X-ray spectroscopy (EDS) spectra demonstrated that the expected BaAl1.4Si0.6O3.4N0.6:Eu 2+ materials were formed.
Photo-induced reduction of CO2 using a magnetically separable Ru-CoPc@TiO2@Si...Pawan Kumar
An efficient photo-induced reduction of CO2 using magnetically separable Ru-CoPc@TiO2@SiO2@Fe3O4
as a heterogeneous catalyst in which CoPc and Ru(bpy)2phene complexes were attached to a solid
support via covalent attachment under visible light is described. The as-synthesized catalyst was characterized
by a series of techniques including FTIR, UV-Vis, XRD, SEM, TEM, etc. and subsequently tested for
the photocatalytic reduction of carbon dioxide using triethylamine as a sacrificial donor and water as a
reaction medium. The developed photocatalyst exhibited a significantly higher catalytic activity to give a
methanol yield of 2570.78 μmol per g cat after 48 h.
Vapor Deposition of Semiconducting Phosphorus Allotropes into TiO2 Nanotube A...Pawan Kumar
Recent evidence of exponential environmental degradation will demand a drastic shift in research and development toward
exploiting alternative energy resources such as solar energy. Here, we
report the successful low-cost and easily accessible synthesis of hybrid
semiconductor@TiO2 nanotube photocatalysts. In order to realize its
maximum potential in harvesting photons in the visible-light range, TiO2
nanotubes have been loaded with earth-abundant, low-band-gap fibrous
red and black phosphorus (P). Scanning electron microscopy− and
scanning transmission electron microscopy−energy-dispersive X-ray
spectroscopy, X-ray diffraction, Raman spectroscopy, X-ray photoelectron microscopy, and UV−vis measurements have been performed,
substantiating the deposition of fibrous red and black P on top and
inside the cavities of 100-μm-long electrochemically fabricated nanotubes. The nanotubular morphology of titania and a vapor-transport technique are utilized to form heterojunctions of P and
TiO2. Compared to pristine anatase 3.2 eV TiO2 nanotubes, the creation of heterojunctions in the hybrid material resulted in
1.5−2.1 eV photoelectrocatalysts. An enhanced photoelectrochemical water-splitting performance under visible light compared
with the individual components resulted for the P@TiO2 hybrids. This feature is due to synergistically improved charge
separation in the heterojunction and more effective visible-light absorption. The electronic band structure and charge-carrier
dynamics are investigated in detail using ultraviolet photoelectron spectroscopy and Kelvin probe force microscopy to elucidate
the charge-separation mechanism. A Fermi-level alignment in P@TiO2 heterojunctions leads to a more reductive flat-band
potential and a deeper valence band compared to pristine P and thus facilitates a better water-splitting performance. Our results
demonstrate effective conversion efficiencies for the nanostructured hybrids, which may enable future applications in
optoelectronic applications such as photodetectors, photovoltaics, photoelectrochemical catalysts, and sensors.
Arrays of TiO2 nanorods embedded with fluorine doped carbon nitride quantum d...Pawan Kumar
Graphenic semiconductors such as carbon nitride are attracting increasing attention as photocatalysts due to their chemical stability, visible light absorption and excellent electronic properties. The photocatalytic activity of nanostructured TiO2 catalysts is constrained by the wide bandgap and concomitant low visible light responsivity of TiO2. In this context we present the formation of new fluorine doped carbon nitride quantum dots (CNFQDs) by solid state reaction and the subsequent examination of their heterojunctions with TiO2 for photoelectrochemical water splitting. Arrays of rutile phase TiO2 nanorods embedded with CNFQDs were synthesized by a simple in situ hydrothermal approach and the resulting nanomaterials were found to exhibit strong visible light absorption. The energetics at the heterojunction were favorable for efficient electron transfer from CNFQDs to TiO2 under visible light irradiation and …
Arrays of TiO2 nanorods embedded with fluorine doped carbon nitride quantum d...Pawan Kumar
Graphenic semiconductors such as carbon nitride are attracting increasing attention as photocatalysts due to their chemical stability, visible light absorption and excellent electronic properties. The photocatalytic activity of nanostructured TiO2 catalysts is constrained by the wide bandgap and concomitant low visible light responsivity of TiO2. In this context we present the formation of new fluorine doped carbon nitride quantum dots (CNFQDs) by solid state reaction and the subsequent examination of their heterojunctions with TiO2 for photoelectrochemical water splitting. Arrays of rutile phase TiO2 nanorods embedded with CNFQDs were synthesized by a simple in situ hydrothermal approach and the resulting nanomaterials were found to exhibit strong visible light absorption. The energetics at the heterojunction were favorable for efficient electron transfer from CNFQDs to TiO2 under visible light irradiation and transfer of holes to the aqueous electrolyte. CNFQD-sensitized TiO2 nanorods exhibited a strong photoelectrochemical response up to 500 nm. Reuse experiments confirmed robustness and long term stability of the sample without exhausting the catalytic performance. The present work demonstrates a new pathway to sensitize TiO2 to visible photons by the in situ formation of embedded heterojunctions with fluorine doped carbon nitride quantum dots
A photoactive bimetallic complex comprising a photosensitizer
ruthenium unit and a catalytic Mn(I) unit connected via a
bipyrimidine (bpm) bridging ligand is prepared and used for the first
time for developing a light induced copper catalyzed [3 + 2] azide−
alkyne “click” (CuAAC) reaction for the formation of 1,2,3-triazoles
under visible light irradiation. The developed bimetallic complex
exhibited enhanced activity as both the photosensitizer ruthenium unit
as well as manganese catalyst unit are attached in a single molecule,
providing efficient electron transfer for the photochemical reduction of
Cu(II) to Cu(I) in situ which subsequently was used for the
cycloaddition of azides with terminal alkynes to give 1,4-disubstituted
1,2,3-triazoles in the presence of triethylamine as a sacrificial donor.
Visible light assisted reduction of nitrobenzenes using Fe(bpy)3+2/rGOnanocom...Pawan Kumar
Visible-light-induced photocatalytic reduction of aromatic nitrobenzenes to the corresponding anilinesat room temperature using reduced graphene oxide (rGO) immobilized iron(II) bipyridine complex asphotocatalyst is described. The rGO-immobilized iron catalyst exhibited superior catalytic activity thanhomogeneous iron(II) bipyridine complex and much higher than metal free rGO photocatalysts. Theheterogeneous photocatalyst was found to be robust and could easily be recovered and reused for severalruns without any significant loss in photocatalytic activity
Heterojunctions of halogen-doped carbon nitride nanosheets and BiOI for sunli...Pawan Kumar
A fluorine-doped, chlorine-intercalated carbon nitride (CNF-Cl) photocatalyst has been synthesized for simultaneous improvements in light harvesting capability along with suppression of charge recombination in bulk gC 3 N 4. The formation of heterojunctions of these CNF-Cl nanosheets with low bandgap, earth abundant bismuth oxyiodide (BiOI) was achieved, and the synthesized heterojunctions were tested as active photoanodes in photoelectrochemical water splitting experiments. BiOI/CNF-Cl heterojunctions exhibited extended light harvesting with a band-edge of 680 nm and generated photocurrent densities approaching 1.3 mA cm− 2 under AM1. 5 G one sun illumination. Scanning Kelvin probe force microscopy under optical bias showed a surface potential of 207 mV for the 50% BiOI/CNF-Cl nanocomposite, while pristine CNF-Cl and BiOI had surface photopotential values of 83 mV and 98 mV …
Visible light driven photocatalytic oxidation of thiols to disulfides using i...Pawan Kumar
The present paper describes the synthesis of graphene oxide immobilized iron phthalocyanine (FePc) for
the photocatalytic oxidation of thiols to disulfides under alkaline free conditions. Iron phthalocyanine
tetrasulfonamide was immobilized on carboxylated graphene oxide supports via covalent attachment.
The loading of FePc on GO nanosheets was confirmed by FTIR, Raman, ICP-AES, UV-Vis and elemental
analyses. The synthesized catalyst was found to be highly efficient for the photo-oxidation of thiols to
disulfides in aqueous medium using molecular oxygen as oxidant under visible light irradiation. The
identification of photo-oxidation products and their quantitative determination was done using GC-MS.
After completion of the reaction, the catalyst was easily recovered by filtration and reused for several
runs without loss in activity and no leaching was observed during the reaction
Similar to Nickel Decorated on Phosphorous-Doped Carbon Nitride as an Efficient Photocatalyst for Reduction of Nitrobenzenes (20)
Isolated Iridium Sites on Potassium-Doped Carbon-nitride wrapped Tellurium Na...Pawan Kumar
Many industrial processes such transesterification of fatty acid for biodiesel production, soap manufacturing and biosynthesis of ethanol generate glycerol as a major by-product that can be used to produce commodity chemicals. Photocatalytic transformation of glycerol is an enticing approach that can exclude the need of harsh oxidants and extraneous thermal energy. However, the product yield and selectivity remain poor due to low absorption and unsymmetrical site distribution on the catalyst surface. Herein, tellurium (Te) nanorods/nanosheets (TeNRs/NSs) wrapped potassium-doped carbon nitride (KCN) van der Waal (vdW) heterojunction (TeKCN) is designed to enhance charge separation and visible-NIR absorption. The iridium (Ir) single atom sites decoration on the TeKCN core-shell structure (TeKCNIr) promotes selective oxidation of glycerol to glyceraldehyde with a conversion of 45.6% and selectivity of 61.6% under AM1.5G irradiation. The catalytic selectivity can reach up to 88% under 450 nm monochromatic light. X-ray absorption spectroscopy (XAS) demonstrates the presence of undercoordinated IrN2O2 sites which improved catalytic selectivity for glycol oxidation. Band energies and computational calculations reveal faile charge transfer in the TeKCNIr heterostructure. EPR and scavenger tests discern that superoxide (O2•−) and hydroxyl (•OH) radicals are prime components driving glycerol oxidation.
Isolated Iridium Sites on Potassium-Doped Carbon-nitride wrapped Tellurium Na...Pawan Kumar
Many industrial processes such transesterification of fatty acid for biodiesel production, soap manufacturing and biosynthesis of ethanol generate glycerol as a major by-product that can be used to produce commodity chemicals. Photocatalytic transformation of glycerol is an enticing approach that can exclude the need of harsh oxidants and extraneous thermal energy. However, the product yield and selectivity remain poor due to low absorption and unsymmetrical site distribution on the catalyst surface. Herein, tellurium (Te) nanorods/nanosheets (TeNRs/NSs) wrapped potassium-doped carbon nitride (KCN) van der Waal (vdW) heterojunction (TeKCN) is designed to enhance charge separation and visible-NIR absorption. The iridium (Ir) single atom sites decoration on the TeKCN core-shell structure (TeKCNIr) promotes selective oxidation of glycerol to glyceraldehyde with a conversion of 45.6% and selectivity of 61.6% under AM1.5G irradiation. The catalytic selectivity can reach up to 88% under 450 nm monochromatic light. X-ray absorption spectroscopy (XAS) demonstrates the presence of undercoordinated IrN2O2 sites which improved catalytic selectivity for glycol oxidation. Band energies and computational calculations reveal faile charge transfer in the TeKCNIr heterostructure. EPR and scavenger tests discern that superoxide (O2•−) and hydroxyl (•OH) radicals are prime components driving glycerol oxidation.
Isolated Iridium Sites on Potassium-Doped Carbon-nitride wrapped Tellurium Na...Pawan Kumar
Many industrial processes such transesterification of fatty acid for biodiesel production, soap manufacturing and biosynthesis of ethanol generate glycerol as a major by-product that can be used to produce commodity chemicals. Photocatalytic transformation of glycerol is an enticing approach that can exclude the need of harsh oxidants and extraneous thermal energy. However, the product yield and selectivity remain poor due to low absorption and unsymmetrical site distribution on the catalyst surface. Herein, tellurium (Te) nanorods/nanosheets (TeNRs/NSs) wrapped potassium-doped carbon nitride (KCN) van der Waal (vdW) heterojunction (TeKCN) is designed to enhance charge separation and visible-NIR absorption. The iridium (Ir) single atom sites decoration on the TeKCN core-shell structure (TeKCNIr) promotes selective oxidation of glycerol to glyceraldehyde with a conversion of 45.6% and selectivity of 61.6% under AM1.5G irradiation. The catalytic selectivity can reach up to 88% under 450 nm monochromatic light. X-ray absorption spectroscopy (XAS) demonstrates the presence of undercoordinated IrN2O2 sites which improved catalytic selectivity for glycol oxidation. Band energies and computational calculations reveal faile charge transfer in the TeKCNIr heterostructure. EPR and scavenger tests discern that superoxide (O2•−) and hydroxyl (•OH) radicals are prime components driving glycerol oxidation.
Solar-Driven Cellulose Photorefining into Arabinose over Oxygen-Doped Carbon ...Pawan Kumar
Biomass photorefining is a promising strategy to address the energy crisis and transition toward carbon carbon-neutral society. Here, we demonstrate the feasibility of direct cellulose photorefining into arabinose by a rationally designed oxygen-doped polymeric carbon nitride, which generates favorable oxidative species (e.g., O2–, •OH) for selective oxidative reactions at neutral conditions. In addition, we also illustrate the mechanism of the photocatalytic cellulose to arabinose conversion by density functional theory calculations. The oxygen insertion derived from oxidative radicals at the C1 position of glucose within cellulose leads to oxidative cleavage of β-1,4 glycosidic linkages, resulting in the subsequent gluconic acid formation. The following decarboxylation process of gluconic acid via C1–C2 α-scissions, triggered by surface oxygen-doped active sites, generates arabinose and formic acid, respectively. This work not only offers a mechanistic understanding of cellulose photorefining to arabinose but also sets up an example for illuminating the path toward direct cellulose photorefining into value-added bioproducts under mild conditions.
Solar-Driven Cellulose Photorefining into Arabinose over Oxygen-Doped Carbon ...Pawan Kumar
Biomass photorefining is a promising strategy to address the energy crisis and transition toward carbon carbon-neutral society. Here, we demonstrate the feasibility of direct cellulose photorefining into arabinose by a rationally designed oxygen-doped polymeric carbon nitride, which generates favorable oxidative species (e.g., O2–, •OH) for selective oxidative reactions at neutral conditions. In addition, we also illustrate the mechanism of the photocatalytic cellulose to arabinose conversion by density functional theory calculations. The oxygen insertion derived from oxidative radicals at the C1 position of glucose within cellulose leads to oxidative cleavage of β-1,4 glycosidic linkages, resulting in the subsequent gluconic acid formation. The following decarboxylation process of gluconic acid via C1–C2 α-scissions, triggered by surface oxygen-doped active sites, generates arabinose and formic acid, respectively. This work not only offers a mechanistic understanding of cellulose photorefining to arabinose but also sets up an example for illuminating the path toward direct cellulose photorefining into value-added bioproducts under mild conditions.
Solar-Driven Cellulose Photorefining into Arabinose over Oxygen-Doped Carbon ...Pawan Kumar
Biomass photorefining is a promising strategy to address the energy crisis and transition toward carbon carbon-neutral society. Here, we demonstrate the feasibility of direct cellulose photorefining into arabinose by a rationally designed oxygen-doped polymeric carbon nitride, which generates favorable oxidative species (e.g., O2–, •OH) for selective oxidative reactions at neutral conditions. In addition, we also illustrate the mechanism of the photocatalytic cellulose to arabinose conversion by density functional theory calculations. The oxygen insertion derived from oxidative radicals at the C1 position of glucose within cellulose leads to oxidative cleavage of β-1,4 glycosidic linkages, resulting in the subsequent gluconic acid formation. The following decarboxylation process of gluconic acid via C1–C2 α-scissions, triggered by surface oxygen-doped active sites, generates arabinose and formic acid, respectively. This work not only offers a mechanistic understanding of cellulose photorefining to arabinose but also sets up an example for illuminating the path toward direct cellulose photorefining into value-added bioproducts under mild conditions.
Partial Thermal Condensation Mediated Synthesis of High-Density Nickel Single...Pawan Kumar
Direct selective transformation of greenhouse methane (CH4) to liquid oxygenates (methanol) can substitute energy-intensive two-step (reforming/Fischer–Tropsch) synthesis while creating environmental benefits. The development of inexpensive, selective, and robust catalysts that enable room temperature conversion will decide the future of this technology. Single-atom catalysts (SACs) with isolated active centers embedded in support have displayed significant promises in catalysis to drive challenging reactions. Herein, high-density Ni single atoms are developed and stabilized on carbon nitride (NiCN) via thermal condensation of preorganized Ni-coordinated melem units. The physicochemical characterization of NiCN with various analytical techniques including HAADF-STEM and X-ray absorption fine structure (XAFS) validate the successful formation of Ni single atoms coordinated to the heptazine-constituted CN network. The presence of uniform catalytic sites improved visible absorption and carrier separation in densely populated NiCN SAC resulting in 100% selective photoconversion of (CH4) to methanol using H2O2 as an oxidant. The superior catalytic activity can be attributed to the generation of high oxidation (NiIII═O) sites and selective C─H bond cleavage to generate •CH3 radicals on Ni centers, which can combine with •OH radicals to generate CH3OH.
Partial Thermal Condensation Mediated Synthesis of High-Density Nickel Single...Pawan Kumar
Direct selective transformation of greenhouse methane (CH4) to liquid oxygenates (methanol) can substitute energy-intensive two-step (reforming/Fischer–Tropsch) synthesis while creating environmental benefits. The development of inexpensive, selective, and robust catalysts that enable room temperature conversion will decide the future of this technology. Single-atom catalysts (SACs) with isolated active centers embedded in support have displayed significant promises in catalysis to drive challenging reactions. Herein, high-density Ni single atoms are developed and stabilized on carbon nitride (NiCN) via thermal condensation of preorganized Ni-coordinated melem units. The physicochemical characterization of NiCN with various analytical techniques including HAADF-STEM and X-ray absorption fine structure (XAFS) validate the successful formation of Ni single atoms coordinated to the heptazine-constituted CN network. The presence of uniform catalytic sites improved visible absorption and carrier separation in densely populated NiCN SAC resulting in 100% selective photoconversion of (CH4) to methanol using H2O2 as an oxidant. The superior catalytic activity can be attributed to the generation of high oxidation (NiIII═O) sites and selective C─H bond cleavage to generate •CH3 radicals on Ni centers, which can combine with •OH radicals to generate CH3OH.
Selective Cellobiose Photoreforming for Simultaneous Gluconic Acid and Syngas...Pawan Kumar
Here, we demonstrate the selective cellobiose (building block of cellulose) photoreforming for gluconic acid and syngas co-production in acidic conditions by rationally designing a bifunctional polymeric carbon nitride (CN) with potassium/sulfur co-dopant. This heteroatomic doped CN photocatalyst possesses enhanced visible light absorption, higher charge separation efficiency than pristine CN. Under acidic conditions, cellobiose is not only more efficiently hydrolyzed into glucose but also promotes the syngas and gluconic acid production. Density functional theory (DFT) calculations reveal the favorable generation of •O2− during the photocatalytic reaction, which is essential for gluconic acid production. Consequently, the fine-designed photocatalyst presents excellent cellobiose conversion (>80%) and gluconic acid selectivity (>70%) together with the co-production of syngas (~56 μmol g-1 h-1) under light illumination. The current work demonstrates the feasibility of biomass photoreforming with value-added chemicals and syngas co-production under mild condition.
Selective Cellobiose Photoreforming for Simultaneous Gluconic Acid and Syngas...Pawan Kumar
Here, we demonstrate the selective cellobiose (building block of cellulose) photoreforming for gluconic acid and syngas co-production in acidic conditions by rationally designing a bifunctional polymeric carbon nitride (CN) with potassium/sulfur co-dopant. This heteroatomic doped CN photocatalyst possesses enhanced visible light absorption, higher charge separation efficiency than pristine CN. Under acidic conditions, cellobiose is not only more efficiently hydrolyzed into glucose but also promotes the syngas and gluconic acid production. Density functional theory (DFT) calculations reveal the favorable generation of •O2− during the photocatalytic reaction, which is essential for gluconic acid production. Consequently, the fine-designed photocatalyst presents excellent cellobiose conversion (>80%) and gluconic acid selectivity (>70%) together with the co-production of syngas (~56 μmol g-1 h-1) under light illumination. The current work demonstrates the feasibility of biomass photoreforming with value-added chemicals and syngas co-production under mild condition.
Selective Cellobiose Photoreforming for Simultaneous Gluconic Acid and Syngas...Pawan Kumar
Here, we demonstrate the selective cellobiose (building block of cellulose) photoreforming for gluconic acid and syngas co-production in acidic conditions by rationally designing a bifunctional polymeric carbon nitride (CN) with potassium/sulfur co-dopant. This heteroatomic doped CN photocatalyst possesses enhanced visible light absorption, higher charge separation efficiency than pristine CN. Under acidic conditions, cellobiose is not only more efficiently hydrolyzed into glucose but also promotes the syngas and gluconic acid production. Density functional theory (DFT) calculations reveal the favorable generation of •O2− during the photocatalytic reaction, which is essential for gluconic acid production. Consequently, the fine-designed photocatalyst presents excellent cellobiose conversion (>80%) and gluconic acid selectivity (>70%) together with the co-production of syngas (~56 μmol g-1 h-1) under light illumination. The current work demonstrates the feasibility of biomass photoreforming with value-added chemicals and syngas co-production under mild condition.
Partial Thermal Condensation Mediated Synthesis of High-Density Nickel Single...Pawan Kumar
Direct selective transformation of greenhouse methane (CH4) to liquid oxygenates (methanol) can substitute energy-intensive two-step (reforming/Fischer–Tropsch) synthesis while creating environmental benefits. The development of inexpensive, selective, and robust catalysts that enable room temperature conversion will decide the future of this technology. Single-atom catalysts (SACs) with isolated active centers embedded in support have displayed significant promises in catalysis to drive challenging reactions. Herein, high-density Ni single atoms are developed and stabilized on carbon nitride (NiCN) via thermal condensation of preorganized Ni-coordinated melem units. The physicochemical characterization of NiCN with various analytical techniques including HAADF-STEM and X-ray absorption fine structure (XAFS) validate the successful formation of Ni single atoms coordinated to the heptazine-constituted CN network. The presence of uniform catalytic sites improved visible absorption and carrier separation in densely populated NiCN SAC resulting in 100% selective photoconversion of (CH4) to methanol using H2O2 as an oxidant. The superior catalytic activity can be attributed to the generation of high oxidation (NiIII═O) sites and selective C─H bond cleavage to generate •CH3 radicals on Ni centers, which can combine with •OH radicals to generate CH3OH.
Recent advancements in tuning the electronic structures of transitional metal...Pawan Kumar
The smooth transition from finite non-renewables to renewable energy conversion technologies will require efficient electrocatalysts which can harness intermittent energies to store in the form of chemical bonds. The oxygen evolution reaction (OER) impedes the widespread usage of water electrolyzers to convert H2O into H2 and persists as a bottleneck, including other energy conversion devices with sluggish four H+/e− kinetics. In this context, designing highly active and stable catalysts capable of driving a lower overpotential in the OER to produce continuous hydrogen (H2) is a primary demanded. This chapter discussed the mechanism of the OER in conventional adsorbate oxygen and lattice oxygen participation in transition metal oxides (TMOs). Further, the influences of surface engineering, doping, and defects in the TMOs and understanding the electronic structure to screen electrodes towards the structure–activity relationship are highlighted. Specifically, the adsorption strength of O 2p is understood in detail as its binding ability over the surface of TMOs can be correlated directly to the OER activity. The iterative development of TMOs in terms of understanding electronic structural attributes is essential for the commercial deployment of energy conversion technologies. The comprehensive outlook of this chapter investigates thoroughly how TMOs can be used as significant materials for the OER in the near future.
Hole transport materials (HTMs) have a significant impact on the effectiveness of organic electronic devices; therefore, we present a molecular architecture of pyrazino[2,3-g]quinoxaline (PQ10)-based room-temperature organic liquid crystalline semiconductor (OLCS) as an alternative HTM. The PQ10 compound exhibits three different rectangular columnar (Colr) phases offering an impressive hole mobility of 8.8 × 10−3 cm2V−1s−1 which is found to be dexterous than most of existing polymeric hole transport materials. The charge transport mechanism is governed by the hole polarons hopping through H-aggregates of the PQ10 molecules and the hole mobility remains nearly constant throughout the mesophase range, but it decreases with increasing applied electric field. The current-voltage characteristics of the PQ10 have also been investigated in all three Colr phases and explained via the Poole-Frenkel conduction mechanism. The dielectric spectroscopy has been eventually carried out to understand the nature of dielectric permittivity and conductivity as a function of temperature and a correlation is established between the molecular architecture of the Colr phases and aforementioned physical properties. Solar cell simulation has been additionally performed to demonstrate that the PQ10 material can be a better choice as HTM for organic electronics and photovoltaic applications.
Multifunctional carbon nitride nanoarchitectures for catalysisPawan Kumar
Catalysis is at the heart of modern-day chemical and pharmaceutical industries, and there is an urgent demand to develop metal-free, high surface area, and efficient catalysts in a scalable, reproducible and economic manner. Amongst the ever-expanding two-dimensional materials family, carbon nitride (CN) has emerged as the most researched material for catalytic applications due to its unique molecular structure with tunable visible range band gap, surface defects, basic sites, and nitrogen functionalities. These properties also endow it with anchoring capability with a large number of catalytically active sites and provide opportunities for doping, hybridization, sensitization, etc. To make considerable progress in the use of CN as a highly effective catalyst for various applications, it is critical to have an in-depth understanding of its synthesis, structure and surface sites. The present review provides an overview of the recent advances in synthetic approaches of CN, its physicochemical properties, and band gap engineering, with a focus on its exclusive usage in a variety of catalytic reactions, including hydrogen evolution reactions, overall water splitting, water oxidation, CO2 reduction, nitrogen reduction reactions, pollutant degradation, and organocatalysis. While the structural design and band gap engineering of catalysts are elaborated, the surface chemistry is dealt with in detail to demonstrate efficient catalytic performances. Burning challenges in catalytic design and future outlook are elucidated.
Production of Renewable Fuels by the Photocatalytic Reduction of CO2 using Ma...Pawan Kumar
The photo-reductive performance of natural ilmenite was boosted and the production of renewable fuels from the reduction of CO2 was enhanced by doping the natural mineral with magnesium. The doping was achieved by high energy ball milling in the presence of MgO and Mg(NO3)2. The photo-reduction of CO2 in aqueous solution led to the evolution of H2, CH4, C2H4, and C2H6, and the insertion of Mg in the structure of ilmenite enabled increases of up to 1245% in the fuel production yield, reaching total production of 210.9 µmol h-1 gcat-1. Displacements of the conduction band to more negative potentials were evidenced for the samples doped with magnesium. Indirect effects such as increases in the valence band maximum, and the introduction of intermediate energy levels were also evidenced through the measurement of the crystallite size and the determination of the band structure of the materials. Mott-Schottky analyses of the samples showed the n-type nature of the semiconductor materials and enabled the estimation of the density of charge carriers, which strongly influenced the photocatalytic performance. The strong potential of the application of natural ilmenite in gas phase artificial photosynthesis was proved by the evaluation of CO2 reduction in gas conditions, which allowed the enhancement in the selectivity and significantly increased the production of CH4 as compared to aqueous solution, reaching an important yield of CH4 of 16.1 µmol h-1 gcat-1.
Nanoengineered Au-Carbon Nitride Interfaces Enhance PhotoCatalytic Pure Water...Pawan Kumar
Photocatalytic pure water splitting using solar energy is one of the promising routes to produce sustainable green hydrogen (H2). Tuning the interfacial active site density at catalytic heterojunctions and better light management are imperative to steer the structure-activity correlations to enhance the photo-efficiency of nanocomposite photocatalysts. Herein, we report the decoration of nitrogen defects-rich carbon nitride CN(T) with metallic Au nanostructures of different morphologies and sizes to investigate their influence on the photocatalytic hydrogen evolution reactions (HER). The CN(T)-7-NP nano-heterostructure comprises Au nanoparticles (NPs) of ~7 nm and thiourea-derived defective CN exhibits an excellent H2 production rate of 76.8 µmol g–1 h–1 from pure water under simulated AM 1.5 solar irradiation. In contrast to large-size Au nanorods, the high activity of CN(T)-7-NP was attributed to their strong localized surface plasmon resonance (LSPR) mediated visible absorption and interfacial charge separation. The surface ligands used to control Au nanostructures morphology were found to play a major role in the stabilization of NPs and improve interfacial charge transport between Au NPs and CN(T). First-principles calculations revealed that defects in CN and Au-CN interfacial sites in these nanocomposites facilitate the separation of e-/h+ pairs after light excitation and provide lower energy barrier pathways for H2 production by photocatalytic water splitting.
Nanoengineered Au-Carbon Nitride Interfaces Enhance Photo-Catalytic Pure Wate...Pawan Kumar
Photocatalytic pure water splitting using solar energy is one of the promising routes to produce sustainable green hydrogen (H2). Tuning the interfacial active site density at catalytic heterojunctions and better light management are imperative to steer the structure-activity correlations to enhance the photo-efficiency of nanocomposite photocatalysts. Herein, we report the decoration of nitrogen defects-rich carbon nitride CN(T) with metallic Au nanostructures of different morphologies and sizes to investigate their influence on the photocatalytic hydrogen evolution reactions (HER). The CN(T)-7-NP nano-heterostructure comprises Au nanoparticles (NPs) of ~7 nm and thiourea-derived defective CN exhibits an excellent H2 production rate of 76.8 µmol g–1 h–1 from pure water under simulated AM 1.5 solar irradiation. In contrast to large-size Au nanorods, the high activity of CN(T)-7-NP was attributed to their strong localized surface plasmon resonance (LSPR) mediated visible absorption and interfacial charge separation. The surface ligands used to control Au nanostructures morphology were found to play a major role in the stabilization of NPs and improve interfacial charge transport between Au NPs and CN(T). First-principles calculations revealed that defects in CN and Au-CN interfacial sites in these nanocomposites facilitate the separation of e-/h+ pairs after light excitation and provide lower energy barrier pathways for H2 production by photocatalytic water splitting.
Cooperative Copper Single Atom Catalyst in Two-dimensional Carbon Nitride for...Pawan Kumar
Renewable electricity powered carbon dioxide (CO2) reduction (eCO2R) to high-value fuels like methane (CH4) holds the potential to close the carbon cycle at meaningful scales. However, this kinetically staggered 8-electron multistep reduction still suffers from inadequate catalytic efficiency and current density. Atomic Cu-structures can boost eCO2R-to-CH4 selectivity due to enhanced intermediate binding energies (BEs) resulting from favorably shifted d-band centers. Herein, we exploit two-dimensional carbon nitride (CN) matrices, viz. Na-polyheptazine (PHI) and Li-polytriazine imides (PTI), to host Cu-N2 type single atom sites with high density (∼1.5 at%), via a facile metal ion exchange process. Optimized Cu loading in nanocrystalline Cu-PTI maximizes eCO2R-to-CH4 performance with Faradaic efficiency (FECH4) of ≈68% and a high partial current density of 348 mA cm−2 at a low potential of -0.84 V versus RHE, surpassing the state-of-the-art catalysts. Multi-Cu substituted N-appended nanopores in the CN frameworks yield thermodynamically stable quasi-dual/triple sites with large interatomic distances dictated by the pore dimensions. First-principles calculations elucidate the relative Cu-CN cooperative effects between the two matrices and how the Cu-Cu distance and local environment dictate the adsorbate BEs, density of states, and CO2-to-CH4 energy profile landscape. The 9N pores in Cu-PTI yield cooperative Cu-Cu sites that synergistically enhance the kinetics of the rate-limiting steps in the eCO2R-to-CH4 pathway.
Bioinspired multimetal electrocatalyst for selective methane oxidationPawan Kumar
Selective partial electrooxidation of methane (CH4) to liquid oxygenates has been a long-sought goal. However, the high activation energy of C–H bonds and competing oxygen evolution reaction limit product selectivity and reaction rates. Inspired by iron (IV)-oxo containing metalloenzymes’ functionality to activate the C–H bond, here we report on the design of a copper-iron-nickel catalyst for selective oxidation of CH4 to formate via a peroxide-assisted pathway. Each catalyst serves a specific role which is confirmed via electrochemical, in situ, and theoretical studies. A combination of electrochemical and in situ spectroelectrochemical studies revealed that H2O2 oxidation on nickel led to the formation of active oxygen species which trigger the formation of iron (IV) at low voltages. Density functional theory analysis helped reveal the role of iron (IV)-oxo species in reducing the activation energy barrier for CH4 deprotonation and the critical role of copper to suppress overoxidation. Our multimetal catalyst exhibits a formate faradaic efficiency of 42% at an applied potential of 0.9 V versus a reversible hydrogen electrode.
Observation of Io’s Resurfacing via Plume Deposition Using Ground-based Adapt...Sérgio Sacani
Since volcanic activity was first discovered on Io from Voyager images in 1979, changes
on Io’s surface have been monitored from both spacecraft and ground-based telescopes.
Here, we present the highest spatial resolution images of Io ever obtained from a groundbased telescope. These images, acquired by the SHARK-VIS instrument on the Large
Binocular Telescope, show evidence of a major resurfacing event on Io’s trailing hemisphere. When compared to the most recent spacecraft images, the SHARK-VIS images
show that a plume deposit from a powerful eruption at Pillan Patera has covered part
of the long-lived Pele plume deposit. Although this type of resurfacing event may be common on Io, few have been detected due to the rarity of spacecraft visits and the previously low spatial resolution available from Earth-based telescopes. The SHARK-VIS instrument ushers in a new era of high resolution imaging of Io’s surface using adaptive
optics at visible wavelengths.
DERIVATION OF MODIFIED BERNOULLI EQUATION WITH VISCOUS EFFECTS AND TERMINAL V...Wasswaderrick3
In this book, we use conservation of energy techniques on a fluid element to derive the Modified Bernoulli equation of flow with viscous or friction effects. We derive the general equation of flow/ velocity and then from this we derive the Pouiselle flow equation, the transition flow equation and the turbulent flow equation. In the situations where there are no viscous effects , the equation reduces to the Bernoulli equation. From experimental results, we are able to include other terms in the Bernoulli equation. We also look at cases where pressure gradients exist. We use the Modified Bernoulli equation to derive equations of flow rate for pipes of different cross sectional areas connected together. We also extend our techniques of energy conservation to a sphere falling in a viscous medium under the effect of gravity. We demonstrate Stokes equation of terminal velocity and turbulent flow equation. We look at a way of calculating the time taken for a body to fall in a viscous medium. We also look at the general equation of terminal velocity.
Richard's aventures in two entangled wonderlandsRichard Gill
Since the loophole-free Bell experiments of 2020 and the Nobel prizes in physics of 2022, critics of Bell's work have retreated to the fortress of super-determinism. Now, super-determinism is a derogatory word - it just means "determinism". Palmer, Hance and Hossenfelder argue that quantum mechanics and determinism are not incompatible, using a sophisticated mathematical construction based on a subtle thinning of allowed states and measurements in quantum mechanics, such that what is left appears to make Bell's argument fail, without altering the empirical predictions of quantum mechanics. I think however that it is a smoke screen, and the slogan "lost in math" comes to my mind. I will discuss some other recent disproofs of Bell's theorem using the language of causality based on causal graphs. Causal thinking is also central to law and justice. I will mention surprising connections to my work on serial killer nurse cases, in particular the Dutch case of Lucia de Berk and the current UK case of Lucy Letby.
Toxic effects of heavy metals : Lead and Arsenicsanjana502982
Heavy metals are naturally occuring metallic chemical elements that have relatively high density, and are toxic at even low concentrations. All toxic metals are termed as heavy metals irrespective of their atomic mass and density, eg. arsenic, lead, mercury, cadmium, thallium, chromium, etc.
Phenomics assisted breeding in crop improvementIshaGoswami9
As the population is increasing and will reach about 9 billion upto 2050. Also due to climate change, it is difficult to meet the food requirement of such a large population. Facing the challenges presented by resource shortages, climate
change, and increasing global population, crop yield and quality need to be improved in a sustainable way over the coming decades. Genetic improvement by breeding is the best way to increase crop productivity. With the rapid progression of functional
genomics, an increasing number of crop genomes have been sequenced and dozens of genes influencing key agronomic traits have been identified. However, current genome sequence information has not been adequately exploited for understanding
the complex characteristics of multiple gene, owing to a lack of crop phenotypic data. Efficient, automatic, and accurate technologies and platforms that can capture phenotypic data that can
be linked to genomics information for crop improvement at all growth stages have become as important as genotyping. Thus,
high-throughput phenotyping has become the major bottleneck restricting crop breeding. Plant phenomics has been defined as the high-throughput, accurate acquisition and analysis of multi-dimensional phenotypes
during crop growing stages at the organism level, including the cell, tissue, organ, individual plant, plot, and field levels. With the rapid development of novel sensors, imaging technology,
and analysis methods, numerous infrastructure platforms have been developed for phenotyping.
Comparing Evolved Extractive Text Summary Scores of Bidirectional Encoder Rep...University of Maribor
Slides from:
11th International Conference on Electrical, Electronics and Computer Engineering (IcETRAN), Niš, 3-6 June 2024
Track: Artificial Intelligence
https://www.etran.rs/2024/en/home-english/
Deep Behavioral Phenotyping in Systems Neuroscience for Functional Atlasing a...Ana Luísa Pinho
Functional Magnetic Resonance Imaging (fMRI) provides means to characterize brain activations in response to behavior. However, cognitive neuroscience has been limited to group-level effects referring to the performance of specific tasks. To obtain the functional profile of elementary cognitive mechanisms, the combination of brain responses to many tasks is required. Yet, to date, both structural atlases and parcellation-based activations do not fully account for cognitive function and still present several limitations. Further, they do not adapt overall to individual characteristics. In this talk, I will give an account of deep-behavioral phenotyping strategies, namely data-driven methods in large task-fMRI datasets, to optimize functional brain-data collection and improve inference of effects-of-interest related to mental processes. Key to this approach is the employment of fast multi-functional paradigms rich on features that can be well parametrized and, consequently, facilitate the creation of psycho-physiological constructs to be modelled with imaging data. Particular emphasis will be given to music stimuli when studying high-order cognitive mechanisms, due to their ecological nature and quality to enable complex behavior compounded by discrete entities. I will also discuss how deep-behavioral phenotyping and individualized models applied to neuroimaging data can better account for the subject-specific organization of domain-general cognitive systems in the human brain. Finally, the accumulation of functional brain signatures brings the possibility to clarify relationships among tasks and create a univocal link between brain systems and mental functions through: (1) the development of ontologies proposing an organization of cognitive processes; and (2) brain-network taxonomies describing functional specialization. To this end, tools to improve commensurability in cognitive science are necessary, such as public repositories, ontology-based platforms and automated meta-analysis tools. I will thus discuss some brain-atlasing resources currently under development, and their applicability in cognitive as well as clinical neuroscience.
Remote Sensing and Computational, Evolutionary, Supercomputing, and Intellige...University of Maribor
Slides from talk:
Aleš Zamuda: Remote Sensing and Computational, Evolutionary, Supercomputing, and Intelligent Systems.
11th International Conference on Electrical, Electronics and Computer Engineering (IcETRAN), Niš, 3-6 June 2024
Inter-Society Networking Panel GRSS/MTT-S/CIS Panel Session: Promoting Connection and Cooperation
https://www.etran.rs/2024/en/home-english/
The ability to recreate computational results with minimal effort and actionable metrics provides a solid foundation for scientific research and software development. When people can replicate an analysis at the touch of a button using open-source software, open data, and methods to assess and compare proposals, it significantly eases verification of results, engagement with a diverse range of contributors, and progress. However, we have yet to fully achieve this; there are still many sociotechnical frictions.
Inspired by David Donoho's vision, this talk aims to revisit the three crucial pillars of frictionless reproducibility (data sharing, code sharing, and competitive challenges) with the perspective of deep software variability.
Our observation is that multiple layers — hardware, operating systems, third-party libraries, software versions, input data, compile-time options, and parameters — are subject to variability that exacerbates frictions but is also essential for achieving robust, generalizable results and fostering innovation. I will first review the literature, providing evidence of how the complex variability interactions across these layers affect qualitative and quantitative software properties, thereby complicating the reproduction and replication of scientific studies in various fields.
I will then present some software engineering and AI techniques that can support the strategic exploration of variability spaces. These include the use of abstractions and models (e.g., feature models), sampling strategies (e.g., uniform, random), cost-effective measurements (e.g., incremental build of software configurations), and dimensionality reduction methods (e.g., transfer learning, feature selection, software debloating).
I will finally argue that deep variability is both the problem and solution of frictionless reproducibility, calling the software science community to develop new methods and tools to manage variability and foster reproducibility in software systems.
Exposé invité Journées Nationales du GDR GPL 2024
Deep Software Variability and Frictionless Reproducibility
Nickel Decorated on Phosphorous-Doped Carbon Nitride as an Efficient Photocatalyst for Reduction of Nitrobenzenes
1. nanomaterials
Article
Nickel Decorated on Phosphorous-Doped Carbon
Nitride as an Efficient Photocatalyst for Reduction
of Nitrobenzenes
Anurag Kumar 1,2, Pawan Kumar 1,2,†, Chetan Joshi 1,†, Manvi Manchanda 1,
Rabah Boukherroub 3,* and Suman L. Jain 1,*
1 CSIR Indian Institute of Petroleum, Haridwar road Mohkampur, Dehradun 248005, India;
anuragmnbd@gmail.com (A.K.); choudhary.2486pawan@yahoo.in (P.K.); chetanjoshi019@gmail.com (C.J.);
manvimanchanda@gmail.com (M.M.)
2 Academy of Scientific and Industrial Research (AcSIR), New Delhi 110001, India
3 Institut d’Electronique, de Microélectronique et de Nanotechnologie (IEMN), UMR CNRS 8520,
Université Lille1, Avenue Poincaré-BP 60069, 59652 Villeneuve d’Ascq, France
* Correspondence: rabah.boukherroub@iemn.univ-lille1.fr (R.B.); suman@iip.res.in (S.L.J.);
Tel.: +91-135-2525-788 (S.L.J.); +33-0-3-62-53-17-24 (R.B.);
Fax: +91-135-2660-098 (S.L.J.); +33-0-3-62-53-17-01 (R.B.)
† These authors contributed equally to this work.
Academic Editors: Hermenegildo García and Sergio Navalón
Received: 3 February 2016; Accepted: 21 March 2016; Published: 1 April 2016
Abstract: Nickel nanoparticle-decorated phosphorous-doped graphitic carbon nitride (Ni@g-PC3N4)
was synthesized and used as an efficient photoactive catalyst for the reduction of various
nitrobenzenes under visible light irradiation. Hydrazine monohydrate was used as the source
of protons and electrons for the intended reaction. The developed photocatalyst was found to be
highly active and afforded excellent product yields under mild experimental conditions. In addition,
the photocatalyst could easily be recovered and reused for several runs without any detectable
leaching during the reaction.
Keywords: carbon nitride; nickel nanoparticles; photocatalysis; visible light; nitrobenzene reduction
1. Introduction
Solar energy is abundant, inexpensive and has great potential for use as a clean and economical
energy source for organic transformations [1–4]. Thus, the efficient conversion of solar energy to
chemical energy, i.e., visible light-driven chemical conversion (photocatalysis) is an area of tremendous
importance and has been rapidly growing worldwide during the last two decades. The reduction of
nitrobenzenes to the corresponding amines is an important transformation both in organic synthesis
as well as in the chemical industry [5–7]. The conventional methods for this reaction mainly
require harsh reaction conditions, expensive reagents, multi-step synthetic procedures and mostly
generate hazardous waste [8,9]. Owing to the current need to develop greener and sustainable
synthesis, the visible light-assisted reduction of nitrobenzenes to the corresponding amines is highly
desired, as these reactions occur under mild and ambient conditions [10]. So far, semiconducting
materials, mainly TiO2-based heterogeneous photocatalysts, have been widely used for the reduction
of nitrobenzenes [11]. However, these photocatalysts work only under ultraviolet (UV) irradiation,
which is a small part of the solar spectrum and also needs special reaction vessels. In order to improve
their efficiency in the visible region, surface modification of the TiO2 photocatalyst by doping metal or
metal oxides, oxide halides (i.e., PbPnO2X (Pn = Bi, Sb; X = Br, Cl) and sensitization with dyes has also
been demonstrated [12–14]. However, the tedious synthetic procedures and poor product yields limit
the synthetic utility of these methods.
Nanomaterials 2016, 6, 59; doi:10.3390/nano6040059 www.mdpi.com/journal/nanomaterials
2. Nanomaterials 2016, 6, 59 2 of 14
Another semiconducting material, i.e., carbon nitride, has gained significant attention in recent
years due to its low band gap (2.7 eV) and easy synthesis method [15–17]. The graphitic carbon nitride
(g-C3N4) is a two dimensional (2D) polymer consisting of interconnected tri-s-triazine units via tertiary
amines. The low band gap and the appropriate position of the conduction (´1.1 eV) and valence
(+1.6 eV) bands enable it to initiate any redox reaction [18]. Despite of several advantages, it also suffers
from certain drawbacks such as only being able to absorb blue light up to the 450 nm wavelength, so
the red region of visible light cannot be harvested. In order to widen the absorption profile in the whole
visible region, the doping of elements such as phosphorus (P), boron (B), fluorine (F), etc is important
because these atoms form bonds with nitrogen and contribute their electrons to the π-conjugated
system more efficiently. Recently, Zhang et al. synthesized P-doped g-C3N4 with an improved
photocurrent response by using 1-butyl-3-methylimidazolium hexafluorophosphate (BmimPF6) as
a source of phosphorous [19]. Hong and coworkers synthesized sulfur-doped mesoporous carbon
nitride (mpgCNS) using an in situ doping method, which showed increased photocatalytic performance
for the solar hydrogen production [20]. Wang et al. synthesized fluorine-doped carbon nitride by
using ammonium fluoride as a cheap source of fluorine for the enhanced visible light-driven hydrogen
evolution reaction [21]. Very recently, our group reported an iron(II) bipyridine complex grafted
nanoporous carbon nitride (Fe(bpy)3/npg-C3N4) photocatalyst for the visible light-mediated oxidative
coupling of benzylamines to imines [22].
In continuation of our ongoing research on the development of novel photocatalysts [23–25],
herein we report for the first time on nickel nanoparticles grafted on P-doped g-C3N4 (Ni@g-PC3N4)
as a high-performance photocatalyst for the reduction of nitrobenzenes to the corresponding amines at
ambient temperature under visible light irradiation (Scheme 1). Due to better visible light absorption,
P-doped carbon nitride can generate electron-hole pairs under visible light irradiation, while nickel
nanoparticles, due to their lower Fermi level than conduction band of P-C3N4, can work as electron
capturing agents to slow down the process of electron-hole recombination and enhance the catalytic
activity and reaction rate.
Nanomaterials 2016, 6, 59 2 of 15
also been demonstrated [12–14]. However, the tedious synthetic procedures and poor product yields
limit the synthetic utility of these methods.
Another semiconducting material, i.e., carbon nitride, has gained significant attention in recent
years due to its low band gap (2.7 eV) and easy synthesis method [15–17]. The graphitic carbon nitride
(g-C3N4) is a two dimensional (2D) polymer consisting of interconnected tri-s-triazine units via
tertiary amines. The low band gap and the appropriate position of the conduction (−1.1 eV) and
valence (+1.6 eV) bands enable it to initiate any redox reaction [18]. Despite of several advantages, it
also suffers from certain drawbacks such as only being able to absorb blue light up to the 450 nm
wavelength, so the red region of visible light cannot be harvested. In order to widen the absorption
profile in the whole visible region, the doping of elements such as phosphorus (P), boron (B), fluorine
(F), etc is important because these atoms form bonds with nitrogen and contribute their electrons to
the π-conjugated system more efficiently. Recently, Zhang et al. synthesized P-doped g-C3N4 with an
improved photocurrent response by using 1-butyl-3-methylimidazolium hexafluorophosphate
(BmimPF6) as a source of phosphorous [19]. Hong and coworkers synthesized sulfur-doped
mesoporous carbon nitride (mpgCNS) using an in situ doping method, which showed increased
photocatalytic performance for the solar hydrogen production [20]. Wang et al. synthesized fluorine-
doped carbon nitride by using ammonium fluoride as a cheap source of fluorine for the enhanced
visible light-driven hydrogen evolution reaction [21]. Very recently, our group reported an iron(II)
bipyridine complex grafted nanoporous carbon nitride (Fe(bpy)3/npg-C3N4) photocatalyst for the
visible light-mediated oxidative coupling of benzylamines to imines [22].
In continuation of our ongoing research on the development of novel photocatalysts [23–25],
herein we report for the first time on nickel nanoparticles grafted on P-doped g-C3N4 (Ni@g-PC3N4)
as a high-performance photocatalyst for the reduction of nitrobenzenes to the corresponding amines
at ambient temperature under visible light irradiation (Scheme 1). Due to better visible light
absorption, P-doped carbon nitride can generate electron-hole pairs under visible light irradiation,
while nickel nanoparticles, due to their lower Fermi level than conduction band of P-C3N4, can work
as electron capturing agents to slow down the process of electron-hole recombination and enhance
the catalytic activity and reaction rate.
Scheme 1. Reduction of nitrobenzenes on Ni@g-PC3N4 (nickel nanoparticles grafted on P-doped g-
C3N4) catalyst.
Scheme 1. Reduction of nitrobenzenes on Ni@g-PC3N4 (nickel nanoparticles grafted on P-doped
g-C3N4) catalyst.
2. Results and Discussion
2.1. Synthesis and Characterization of the Photocatalyst
At first, nickel nanoparticles were synthesized by reducing nickel chloride hexahydrate by sodium
borohydride in the presence of cetyltrimethylammonium bromide (CTAB) as a template by following
the literature procedure in [26]. Next, the synthesis of phosphorous-doped graphitic carbon nitride
(g-PC3N4) was performed by using ionic liquid 1-butyl-3-methylimidazolium hexafluorophosphate
3. Nanomaterials 2016, 6, 59 3 of 14
[BmimPF6] as a source of phosphorous and dicyandiamide as a precursor for the graphitic
carbon nitride skeleton [17,27]. Nickel nanoparticle-decorated phosphorous-doped carbon nitride
(Ni@g-PC3N4) with variable nickel content (2–7.5 wt %) was synthesized by the addition of nickel
nanoparticles, BmimPF6 and dicyandiamide into water with continuous stirring. The resulting
suspension was heated at 100 ˝C until all the water was evaporated. Then, the obtained solid was
heated at a programmed temperature in a similar manner to the one used for P-doped carbon nitride
(Scheme 2). Bare graphitic carbon nitride (g-C3N4) was synthesized for comparison by heating
dicyandiamide under identical programmed temperature. Among the various nanocomposites
synthesized, 5% nickel nanoparticles grafted on P-doped g-C3N4 (5%Ni@PC3N4) exhibited the best
performance for the photocatalytic reduction of nitrobenzene; thus, we have used this photocatalyst
for detailed characterization and further studies.
2.1. Synthesis and Characterization of the Photocatalyst
At first, nickel nanoparticles were synthesized by reducing nickel chloride hexahydrate by
sodium borohydride in the presence of cetyltrimethylammonium bromide (CTAB) as a template by
following the literature procedure in [26]. Next, the synthesis of phosphorous-doped graphitic carbon
nitride (g-PC3N4) was performed by using ionic liquid 1-butyl-3-methylimidazolium
hexafluorophosphate [BmimPF6] as a source of phosphorous and dicyandiamide as a precursor for
the graphitic carbon nitride skeleton [17,27]. Nickel nanoparticle-decorated phosphorous-doped
carbon nitride (Ni@g-PC3N4) with variable nickel content (2–7.5 wt %) was synthesized by the
addition of nickel nanoparticles, BmimPF6 and dicyandiamide into water with continuous stirring.
The resulting suspension was heated at 100 °C until all the water was evaporated. Then, the obtained
solid was heated at a programmed temperature in a similar manner to the one used for P-doped carbon
nitride (Scheme 2). Bare graphitic carbon nitride (g-C3N4) was synthesized for comparison by heating
dicyandiamide under identical programmed temperature. Among the various nanocomposites
synthesized, 5% nickel nanoparticles grafted on P-doped g-C3N4 (5%Ni@PC3N4) exhibited the best
performance for the photocatalytic reduction of nitrobenzene; thus, we have used this photocatalyst
for detailed characterization and further studies.
Scheme 2. Synthetic illustration of Ni@g-PC3N4 catalyst. NiNPs: nickel nanoparticles; BmimPF6: 1-
butyl-3-methylimidazolium hexafluorophosphate.
The surface morphology of the synthesized materials was determined by field emission
scanning electron microscopy (FE-SEM). The graphitic carbon nitride (g-C3N4) showed many
enfolded and crumpled sheet-like structures (Figure 1a). The framework of C3N4 contains nitrogen as
a substituted heteroatom forming similarly to the π-conjugated system, as in graphitic planes, due to
sp2 hybridization between carbon and nitrogen atoms. The phosphorous-doped carbon nitride (g-
PC3N4) exhibits similar morphological characteristics (Figure 1b). In the case of nickel nanoparticle-
grafted g-PC3N4 (5%Ni@g-PC3N4), a similar sheet-like morphology was observed that may be due to
the incorporation of nickel nanoparticles between the graphitic carbon nitride sheets (Figure 1c). The
energy dispersive X-ray spectroscopy (EDX) pattern of g-PC3N4 clearly showed the presence of
phosphorous (Figure 1e) and, in 5%Ni@g-PC3N4, the peak due to nickel can clearly be seen, which
confirmed the presence of both components in the synthesized photocatalyst (Figure 1f).
Scheme 2. Synthetic illustration of Ni@g-PC3N4 catalyst. NiNPs: nickel nanoparticles; BmimPF6:
1-butyl-3-methylimidazolium hexafluorophosphate.
The surface morphology of the synthesized materials was determined by field emission scanning
electron microscopy (FE-SEM). The graphitic carbon nitride (g-C3N4) showed many enfolded
and crumpled sheet-like structures (Figure 1a). The framework of C3N4 contains nitrogen as
a substituted heteroatom forming similarly to the π-conjugated system, as in graphitic planes,
due to sp2 hybridization between carbon and nitrogen atoms. The phosphorous-doped carbon
nitride (g-PC3N4) exhibits similar morphological characteristics (Figure 1b). In the case of nickel
nanoparticle-grafted g-PC3N4 (5%Ni@g-PC3N4), a similar sheet-like morphology was observed that
may be due to the incorporation of nickel nanoparticles between the graphitic carbon nitride sheets
(Figure 1c). The energy dispersive X-ray spectroscopy (EDX) pattern of g-PC3N4 clearly showed the
presence of phosphorous (Figure 1e) and, in 5%Ni@g-PC3N4, the peak due to nickel can clearly be
seen, which confirmed the presence of both components in the synthesized photocatalyst (Figure 1f).
The fine morphological features of the synthesized materials were determined with the help of
high-resolution transmission electron microscopy (HRTEM). The transmission electron microscopy
(TEM) image of g-C3N4 at 100 nm resolution displayed enfolded sheets of carbon nitride (Figure 2a).
For g-PC3N4, similar folded sheet-like structures were observed, indicating that phosphorus doping
did not change the structural features of the material (Figure 2b). In the TEM image of 5%Ni@g-PC3N4,
several small dark spots were observed, suggesting the presence of nickel nanoparticles between the
scaffolds of graphitic structure of phosphorous-doped carbon nitride (Figure 2c). The presence of
several rings and bright spots in the selected area electron diffraction (SAED) pattern of 5%Ni@g-PC3N4
confirmed the presence of nickel nanoparticles in the composite structure (Figure 2d). Further EDX
patterns of 5%Ni@g-PC3N4 revealed the presence of all the expected elements in the photocatalyst
(Figure 2e).
4. Nanomaterials 2016, 6, 59 4 of 14
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Figure 1. Field emission scanning electron microscopy (FE-SEM) image of: (a) graphitic carbon nitride
(g-C3N4); (b) phosphorous-doped graphitic carbon nitride (g-PC3N4); (c) nickel nanoparticle-grafted
g-PC3N4 (Ni@g-PC3N4); energy dispersive X-ray spectroscopy (EDX) pattern of: (d) g-C3N4; (e) g-
PC3N4; (f) 5%Ni@g-PC3N4.
The fine morphological features of the synthesized materials were determined with the help of
high-resolution transmission electron microscopy (HRTEM). The transmission electron microscopy
(TEM) image of g-C3N4 at 100 nm resolution displayed enfolded sheets of carbon nitride (Figure 2a).
For g-PC3N4, similar folded sheet-like structures were observed, indicating that phosphorus doping
did not change the structural features of the material (Figure 2b). In the TEM image of 5%Ni@g-PC3N4,
several small dark spots were observed, suggesting the presence of nickel nanoparticles between the
scaffolds of graphitic structure of phosphorous-doped carbon nitride (Figure 2c). The presence of
several rings and bright spots in the selected area electron diffraction (SAED) pattern of 5%Ni@g-
PC3N4 confirmed the presence of nickel nanoparticles in the composite structure (Figure 2d). Further
EDX patterns of 5%Ni@g-PC3N4 revealed the presence of all the expected elements in the
photocatalyst (Figure 2e).
Figure 1. Field emission scanning electron microscopy (FE-SEM) image of: (a) graphitic carbon nitride
(g-C3N4); (b) phosphorous-doped graphitic carbon nitride (g-PC3N4); (c) nickel nanoparticle-grafted
g-PC3N4 (Ni@g-PC3N4); energy dispersive X-ray spectroscopy (EDX) pattern of: (d) g-C3N4;
(e) g-PC3N4; (f) 5%Ni@g-PC3N4.
Nanomaterials 2016, 6, 59 5 of 15
Figure 2. Transmission electron microscopy (TEM) images of: (a) g-C3N4; (b) g-PC3N4; (c) Ni@g-PC3N4;
(d) selected area electron diffraction (SAED) pattern of Ni@g-PC3N4; (e) EDX pattern of Ni@g-PC3N4.
The vibrational spectra of the synthesized materials are depicted in Figure 3. The Fourier
transform infrared (FTIR) spectrum of as-synthesized nickel nanoparticles by using cetyl
trimethylammonium chloride as a template was found to be well in agreement with the known
literature and gave peaks at 676 cm−1 due to the Ni–O stretch of oxidized nickel [28]. Some additional
peaks were also identified that may be due to the residual template molecules in the particles. The
FTIR spectrum of carbon nitride (g-C3N4) showed a characteristic peak at 815 cm−1 related to C–N
Figure 2. Transmission electron microscopy (TEM) images of: (a) g-C3N4; (b) g-PC3N4; (c) Ni@g-PC3N4;
(d) selected area electron diffraction (SAED) pattern of Ni@g-PC3N4; (e) EDX pattern of Ni@g-PC3N4.
5. Nanomaterials 2016, 6, 59 5 of 14
The vibrational spectra of the synthesized materials are depicted in Figure 3. The Fourier transform
infrared (FTIR) spectrum of as-synthesized nickel nanoparticles by using cetyl trimethylammonium
chloride as a template was found to be well in agreement with the known literature and gave peaks at
676 cm´1 due to the Ni–O stretch of oxidized nickel [28]. Some additional peaks were also identified
that may be due to the residual template molecules in the particles. The FTIR spectrum of carbon
nitride (g-C3N4) showed a characteristic peak at 815 cm´1 related to C–N heterocycles due to the
triazine ring mode. Another peak in the range of 1200–1600 cm´1, attributed to the specific aromatic
skeleton vibration of carbon nitride, was observed [29]. A broad band was evident in the range of
3000–3700 cm´1 corresponding to adsorbed moisture, i.e., the presence of water molecules, or due
to the stretching mode of –NH2, which are uncondensed amine groups, or to N–H group vibrations
present at the surface of carbon nitride (Figure 3a). For the P-doped carbon nitride (g-PC3N4), peaks
related to C–N at 1520, 1440 and 1310 cm´1 were found to be diminished, which is mainly due to the
displacement of some carbon atoms in the ring skeleton by the phosphorous atoms to give P–N bonds.
Furthermore, a new peak at 980 cm´1 due to the vibration of the C–P heterocycle was clearly observed
(Figure 3c). For the 5%Ni@g-PC3N4, the appearance of some peaks due to nickel nanoparticles with
g-PC3N4 confirmed the successful synthesis of nickel-grafted P-doped g-C3N4 (Figure 3d).
Nanomaterials 2016, 6, 59 6 of 15
nanoparticles with g-PC3N4 confirmed the successful synthesis of nickel-grafted P-doped g-C3N4
(Figure 3d).
Figure 3. Fourier transform infrared (FTIR) spectra of: (a) nickel nanoparticles (NiNPs); (b) g-C3N4; (c)
g-PC3N4; (d) 5%Ni@g-PC3N4.
The crystallinity and phase structure of the nanocomposites were determined by X-ray
diffraction (XRD) (Figure 4). The XRD diffraction pattern of graphitic carbon nitride (g-C3N4) revealed
an intense broad peak at the 2θ value of 27.4°, indexed to (002) planes with 0.32 nm interlayer distance
due to the stacking of graphite-like conjugated triazine aromatic sheets, which matches well with
Joint committee on powder diffraction standards (JCPDS) 87–1526 for g-C3N4 (Figure 4a) [30]. The g-
PC3N4 also exhibited an identical diffraction pattern; however, the intensity of the peak at 27.4°was
found to be reduced due to the replacement of carbon atoms by phosphorous atoms (Figure 4b).The
diffraction pattern of the 5%Ni@g-PC3N4 did not show any peak of nickel nanoparticles. This is most
likely due to the amorphous nature of the material (Figure 4c). Furthermore, the peak at 27.4° was
absent in 5%Ni@g-PC3N4, which was most probably due to the intercalation of nickel nanoparticles
between the sheets. Therefore, the interlayer distance between sheets increased and the diffraction
due to stacked sheets disappeared.
Figure 3. Fourier transform infrared (FTIR) spectra of: (a) nickel nanoparticles (NiNPs); (b) g-C3N4;
(c) g-PC3N4; (d) 5%Ni@g-PC3N4.
The crystallinity and phase structure of the nanocomposites were determined by X-ray diffraction
(XRD) (Figure 4). The XRD diffraction pattern of graphitic carbon nitride (g-C3N4) revealed an intense
broad peak at the 2θ value of 27.4˝, indexed to (002) planes with 0.32 nm interlayer distance due
to the stacking of graphite-like conjugated triazine aromatic sheets, which matches well with Joint
committee on powder diffraction standards (JCPDS) 87–1526 for g-C3N4 (Figure 4a) [30]. The g-PC3N4
also exhibited an identical diffraction pattern; however, the intensity of the peak at 27.4˝ was found to
be reduced due to the replacement of carbon atoms by phosphorous atoms (Figure 4b). The diffraction
pattern of the 5%Ni@g-PC3N4 did not show any peak of nickel nanoparticles. This is most likely due
to the amorphous nature of the material (Figure 4c). Furthermore, the peak at 27.4˝ was absent in
5%Ni@g-PC3N4, which was most probably due to the intercalation of nickel nanoparticles between the
6. Nanomaterials 2016, 6, 59 6 of 14
sheets. Therefore, the interlayer distance between sheets increased and the diffraction due to stacked
sheets disappeared.Nanomaterials 2016, 6, 59 7 of 15
Figure 4. X-ray diffraction (XRD) patterns of: (a) g-C3N4; (b) g-PC3N4; (c) 5%Ni@g-PC3N4. a.u.:
arbitrary units.
To determine the surface properties of the synthesized materials, N2 adsorption-desorption
isotherms were determined by using multilayer Brunauer–Emmett–Teller (BET) adsorption-
desorption theory. As seen in Figure 5, the adsorption-desorption isotherms were of type IV,
suggesting the mesoporous nature of the materials [31]. The BET surface area (SBET), total pore volume
(Vp) and mean pore diameter (rp) of g-C3N4 were found to be 14.67 m2·g−1, 0.15 cm3·g−1 and 4.21 nm,
while for g-PC3N4 these values were determined to be 24.59 m2·g−1, 0.14 cm3·g−1 and 3.83 nm,
respectively. For the 5%Ni@g-PC3N4 surface area (SBET), the total pore volume (Vp) and mean pore
diameter (rp) were 48.62 m2·g−1, 0.17 cm3·g−1 and 2.64 nm, respectively. The change in the surface
properties clearly indicated the grafting of nickel nanoparticles between the sheets of carbon nitride
(Figure 5). The higher surface area provides more sites for reaction to proceed on the surface of the
Ni@g-PC3N4 catalyst.
Figure 5. N2 adsorption-desorption isotherm and pore size distribution of: (a) g-C3N4; (b) g-PC3N4; (c)
5%Ni@g-PC3N4.
Figure 4. X-ray diffraction (XRD) patterns of: (a) g-C3N4; (b) g-PC3N4; (c) 5%Ni@g-PC3N4. a.u.:
arbitrary units.
To determine the surface properties of the synthesized materials, N2 adsorption-desorption
isotherms were determined by using multilayer Brunauer–Emmett–Teller (BET) adsorption-desorption
theory. As seen in Figure 5, the adsorption-desorption isotherms were of type IV, suggesting the
mesoporous nature of the materials [31]. The BET surface area (SBET), total pore volume (Vp) and
mean pore diameter (rp) of g-C3N4 were found to be 14.67 m2¨ g´1, 0.15 cm3¨ g´1 and 4.21 nm, while
for g-PC3N4 these values were determined to be 24.59 m2¨ g´1, 0.14 cm3¨ g´1 and 3.83 nm, respectively.
For the 5%Ni@g-PC3N4 surface area (SBET), the total pore volume (Vp) and mean pore diameter (rp)
were 48.62 m2¨ g´1, 0.17 cm3¨ g´1 and 2.64 nm, respectively. The change in the surface properties clearly
indicated the grafting of nickel nanoparticles between the sheets of carbon nitride (Figure 5). The higher
surface area provides more sites for reaction to proceed on the surface of the Ni@g-PC3N4 catalyst.
Nanomaterials 2016, 6, 59 7 of 15
Figure 4. X-ray diffraction (XRD) patterns of: (a) g-C3N4; (b) g-PC3N4; (c) 5%Ni@g-PC3N4. a.u.:
arbitrary units.
To determine the surface properties of the synthesized materials, N2 adsorption-desorption
isotherms were determined by using multilayer Brunauer–Emmett–Teller (BET) adsorption-
desorption theory. As seen in Figure 5, the adsorption-desorption isotherms were of type IV,
suggesting the mesoporous nature of the materials [31]. The BET surface area (SBET), total pore volume
(Vp) and mean pore diameter (rp) of g-C3N4 were found to be 14.67 m2·g−1, 0.15 cm3·g−1 and 4.21 nm,
while for g-PC3N4 these values were determined to be 24.59 m2·g−1, 0.14 cm3·g−1 and 3.83 nm,
respectively. For the 5%Ni@g-PC3N4 surface area (SBET), the total pore volume (Vp) and mean pore
diameter (rp) were 48.62 m2·g−1, 0.17 cm3·g−1 and 2.64 nm, respectively. The change in the surface
properties clearly indicated the grafting of nickel nanoparticles between the sheets of carbon nitride
(Figure 5). The higher surface area provides more sites for reaction to proceed on the surface of the
Ni@g-PC3N4 catalyst.
Figure 5. N2 adsorption-desorption isotherm and pore size distribution of: (a) g-C3N4; (b) g-PC3N4; (c)
5%Ni@g-PC3N4.
Figure 5. N2 adsorption-desorption isotherm and pore size distribution of: (a) g-C3N4; (b) g-PC3N4;
(c) 5%Ni@g-PC3N4.
7. Nanomaterials 2016, 6, 59 7 of 14
Electronic and optical properties are of fundamental importance to determine the photo activity
of a catalyst. The absorption properties of synthesized materials were determined by UV-visible
(UV-Vis) spectroscopy. The UV-visible spectrum of pure g-C3N4 shows an absorption spectrum similar
to a typical semiconductor absorption spectrum between 200–450 nm, originating from the charge
transfer from a populated valence band of nitrogen atom (2p orbitals) to a conduction band of carbon
atom (2p orbitals) of carbon nitride [32]. An additional sharp peak at 256 nm, attributed to the aromatic
ring’s π Ñ π* transition, was observed. Another intense peak at 384 nm, due to the n Ñ π* transitions
caused by the electron transfer from a nitrogen nonbonding orbital to an aromatic anti-bonding orbital,
was also present in the UV-Vis spectrum. The band tailing from 410 to 500 nm suggests a slight
visible light absorption capacity of carbon nitride (Figure 6a). After doping with phosphorous atoms,
the absorption band due to the nitrogen nonbonding to aromatic antibonding (n Ñ π*) transition
was diminished due to the replacement of carbon atoms with phosphorous, whereas the absorption
pattern was found to be redshifted due to the better charge contribution by loosely bound electrons
of phosphorous in the aromatic conjugated system (Figure 6b) [33]. After incorporation of nickel
nanoparticles (5%Ni@g-PC3N4), the material exhibited lower absorbance in the visible region as the
nickel nanoparticles have lower absorbance in the visible region, and therefore reduce the absorption
profile in the visible region (Figure 6c).
Nanomaterials 2016, 6, 59 8 of 15
Electronic and optical properties are of fundamental importance to determine the photo activity
of a catalyst. The absorption properties of synthesized materials were determined by UV-visible (UV-
Vis) spectroscopy. The UV-visible spectrum of pure g-C3N4 shows an absorption spectrum similar to
a typical semiconductor absorption spectrum between 200–450 nm, originating from the charge
transfer from a populated valence band of nitrogen atom (2p orbitals) to a conduction band of carbon
atom (2p orbitals) of carbon nitride [32]. An additional sharp peak at 256 nm, attributed to the
aromatic ring’s π π* transition, was observed. Another intense peak at 384 nm, due to the n π*
transitions caused by the electron transfer from a nitrogen nonbonding orbital to an aromatic anti-
bonding orbital, was also present in the UV-Vis spectrum. The band tailing from 410 to 500 nm
suggests a slight visible light absorption capacity of carbon nitride (Figure 6a). After doping with
phosphorous atoms, the absorption band due to the nitrogen nonbonding to aromatic antibonding
(n π*) transition was diminished due to the replacement of carbon atoms with phosphorous,
whereas the absorption pattern was found to be redshifted due to the better charge contribution by
loosely bound electrons of phosphorous in the aromatic conjugated system (Figure 6b) [33]. After
incorporation of nickel nanoparticles (5%Ni@g-PC3N4), the material exhibited lower absorbance in
the visible region as the nickel nanoparticles have lower absorbance in the visible region, and
therefore reduce the absorption profile in the visible region (Figure 6c).
Figure 6. Ultraviolet--visible (UV-Vis) absorption spectra of: (a) g-C3N4; (b) g-PC3N4; (c) 5%Ni@g-
PC3N4.
In order to confirm the visible light absorption of the synthesized photocatalysts, a Tauc plot
was obtained as shown in Figure 7. From the Tauc plot, the band gap value for the g-C3N4 was
determined to be 2.69 eV due to the uneven synthesis of sheets, and was well in concordance with
the existing literature [18]. After doping with phosphorous atoms (g-PC3N4), the value of the band
gap decreased to 1.45 eV, which may be due to the displacement of carbon atoms by the phosphorous
atoms in the triazine ring skeletons of carbon nitride. For the 5%Ni@g-PC3N4, a band gap value of
1.52 eV was calculated, which is nearly similar to that of g-PC3N4.
The thermal stability of the synthesized materials was examined by thermogravimetric analysis
(Figure 8). A thermogravimetric analysis (TGA) pattern of pristine nickel nanoparticles showed
steady weight loss (approx. 15%) from 100 to 500 °C, which may be due to loss of the residual organic
template (CTAB) and loss of other oxygen-carrying functionalities during the crystallization step
(Figure 8a). The thermogram of g-C3N4 exhibited a sharp weight loss in the range of 560 to 720 °C
(Figure 8b). The P-doped g-C3N4 displayed a similar weight loss pattern as g-C3N4 (Figure 8c). For
the 5%Ni@g-PC3N4, a small weight loss at around 100 °C was observed due to the loss of moisture,
followed by steady weight loss up to 700 °C due to the loss of template in nickel and the slow
degradation of the phosphorous-doped sheets. At 770 °C, a sharp weight loss was observed due to the
complete degradation of P-doped carbon nitride sheets (Figure 8d).
Figure 6. Ultraviolet–visible (UV-Vis) absorption spectra of: (a) g-C3N4; (b) g-PC3N4;
(c) 5%Ni@g-PC3N4.
In order to confirm the visible light absorption of the synthesized photocatalysts, a Tauc plot was
obtained as shown in Figure 7. From the Tauc plot, the band gap value for the g-C3N4 was determined
to be 2.69 eV due to the uneven synthesis of sheets, and was well in concordance with the existing
literature [18]. After doping with phosphorous atoms (g-PC3N4), the value of the band gap decreased
to 1.45 eV, which may be due to the displacement of carbon atoms by the phosphorous atoms in the
triazine ring skeletons of carbon nitride. For the 5%Ni@g-PC3N4, a band gap value of 1.52 eV was
calculated, which is nearly similar to that of g-PC3N4.
The thermal stability of the synthesized materials was examined by thermogravimetric analysis
(Figure 8). A thermogravimetric analysis (TGA) pattern of pristine nickel nanoparticles showed steady
weight loss (approx. 15%) from 100 to 500 ˝C, which may be due to loss of the residual organic
template (CTAB) and loss of other oxygen-carrying functionalities during the crystallization step
(Figure 8a). The thermogram of g-C3N4 exhibited a sharp weight loss in the range of 560 to 720 ˝C
(Figure 8b). The P-doped g-C3N4 displayed a similar weight loss pattern as g-C3N4 (Figure 8c). For the
5%Ni@g-PC3N4, a small weight loss at around 100 ˝C was observed due to the loss of moisture,
followed by steady weight loss up to 700 ˝C due to the loss of template in nickel and the slow
degradation of the phosphorous-doped sheets. At 770 ˝C, a sharp weight loss was observed due to the
complete degradation of P-doped carbon nitride sheets (Figure 8d).
8. Nanomaterials 2016, 6, 59 8 of 14
Nanomaterials 2016, 6, 59 9 of 15
Figure 7. Tauc plots of (a) g-C3N4; (b) g-PC3N4; (c) Ni@g-PC3N4. α: absoption coefficient; hν: energy of
incident photon.
Figure 8. Thermogravimetric analysis (TGA) spectra of: (a) NiNPs; (b) g-C3N4; (c) g-PC3N4; (d)
5%Ni@g-PC3N4.
2.2 Photocatalytic Reduction Reaction
The photocatalytic activity of the synthesized NiNPs, g-C3N4, g-PC3N4 and 2–7.5%Ni@g-PC3N4
catalysts was tested for the reduction of nitrobenzene as a model substrate using hydrazine
monohydrate as a proton source under visible light irradiation. The results of these optimization
experiments are summarized in Table 1. There was no conversion obtained with pristine nickel
nanoparticles (NiNPs) (Table 1, entry 1). However, the yield of product was found to be 24.6 % when
g-C3N4 was used as a photocatalyst (Table 1, entry 2). In case of P-doped g-PC3N4, the yield of aniline
increased up to 54.2%, which clearly indicated the promoting effect of P-doping due to the better
visible light absorption (Table 1, entry 3). Furthermore, the yield of aniline increased to manifold by
using Ni@g-PC3N4 and, after 8 h of visible light irradiation, the yield reached 96.5% (Table 1, entries
4–6). This increase in the reaction rate and product yield can be explained because the nickel
nanoparticles work as electron sinks, and the photogenerated electrons flow from conduction band
of g-PC3N4 to nickel nanoparticles. This makes the electron unavailable for the recombination and
therefore increases the activity of the catalyst. We also determined the optimum nickel content in the
photocatalyst. It was found that among all the synthesized Ni@g-PC3N4 nanocomposites having
Figure 7. Tauc plots of (a) g-C3N4; (b) g-PC3N4; (c) Ni@g-PC3N4. α: absoption coefficient; hν: energy
of incident photon.
Nanomaterials 2016, 6, 59 9 of 15
Figure 7. Tauc plots of (a) g-C3N4; (b) g-PC3N4; (c) Ni@g-PC3N4. α: absoption coefficient; hν: energy of
incident photon.
Figure 8. Thermogravimetric analysis (TGA) spectra of: (a) NiNPs; (b) g-C3N4; (c) g-PC3N4; (d)
5%Ni@g-PC3N4.
2.2 Photocatalytic Reduction Reaction
The photocatalytic activity of the synthesized NiNPs, g-C3N4, g-PC3N4 and 2–7.5%Ni@g-PC3N4
catalysts was tested for the reduction of nitrobenzene as a model substrate using hydrazine
monohydrate as a proton source under visible light irradiation. The results of these optimization
experiments are summarized in Table 1. There was no conversion obtained with pristine nickel
nanoparticles (NiNPs) (Table 1, entry 1). However, the yield of product was found to be 24.6 % when
g-C3N4 was used as a photocatalyst (Table 1, entry 2). In case of P-doped g-PC3N4, the yield of aniline
increased up to 54.2%, which clearly indicated the promoting effect of P-doping due to the better
visible light absorption (Table 1, entry 3). Furthermore, the yield of aniline increased to manifold by
using Ni@g-PC3N4 and, after 8 h of visible light irradiation, the yield reached 96.5% (Table 1, entries
4–6). This increase in the reaction rate and product yield can be explained because the nickel
nanoparticles work as electron sinks, and the photogenerated electrons flow from conduction band
of g-PC3N4 to nickel nanoparticles. This makes the electron unavailable for the recombination and
therefore increases the activity of the catalyst. We also determined the optimum nickel content in the
photocatalyst. It was found that among all the synthesized Ni@g-PC3N4 nanocomposites having
Figure 8. Thermogravimetric analysis (TGA) spectra of: (a) NiNPs; (b) g-C3N4; (c) g-PC3N4;
(d) 5%Ni@g-PC3N4.
2.2. Photocatalytic Reduction Reaction
The photocatalytic activity of the synthesized NiNPs, g-C3N4, g-PC3N4 and 2–7.5%Ni@g-PC3N4
catalysts was tested for the reduction of nitrobenzene as a model substrate using hydrazine
monohydrate as a proton source under visible light irradiation. The results of these optimization
experiments are summarized in Table 1. There was no conversion obtained with pristine nickel
nanoparticles (NiNPs) (Table 1, entry 1). However, the yield of product was found to be 24.6 % when
g-C3N4 was used as a photocatalyst (Table 1, entry 2). In case of P-doped g-PC3N4, the yield of aniline
increased up to 54.2%, which clearly indicated the promoting effect of P-doping due to the better
visible light absorption (Table 1, entry 3). Furthermore, the yield of aniline increased to manifold
by using Ni@g-PC3N4 and, after 8 h of visible light irradiation, the yield reached 96.5% (Table 1,
entries 4–6). This increase in the reaction rate and product yield can be explained because the nickel
nanoparticles work as electron sinks, and the photogenerated electrons flow from conduction band
of g-PC3N4 to nickel nanoparticles. This makes the electron unavailable for the recombination and
therefore increases the activity of the catalyst. We also determined the optimum nickel content in
the photocatalyst. It was found that among all the synthesized Ni@g-PC3N4 nanocomposites having
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the
yield of product was lower, whereas no significant enhancement was observed with increasing the
9. Nanomaterials 2016, 6, 59 9 of 14
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence of
hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4: graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h´1)
1 NiNPs
Dark 24 - -
Visible light - - -
2 g-C3N4
Dark 24 - -
Visible light 12 24.6 2.0
3 g-P-C3N4
Dark 24 - -
Visible light 12 54.2 4.5
4 2%Ni@g-PC3N4
Dark 24 - -
Visible light 8 82.0 10.2
5 5%Ni@g-PC3N4
Dark 24 Trace -
Visible light 8 96.5 12.1
Visible light 24 c - c - c
6 7.5%Ni@g-PC3N4
Dark 24 10 0.4
Visible light 8 97.0 12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol; Irradiation,
White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2; b Isolated yield;
c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and the
results are summarized in Table 2. It can be seen that the substituent effect did not play much of a role
and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b Yield (%) c TOF (h´1)
1
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
8.0 98.0 96.5 12.1
2
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
8.0 95.5 94.2 11.7
3
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
8.0 96.4 95.4 11.9
4
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
8.0 94.8 93.0 11.6
5
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
8.0 95.6 94.2 11.7
6
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
8.0 96.0 94.6 11.8
7
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
8.5 90.5 89.4 10.5
8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
8.5 92.4 91.0 10.7
9
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.8
Nanomaterials 2016, 6, 59 10 of 15
variable nickel contents (2–7.5 wt % Ni), the nanocomposite having 5 wt % nickel nanoparticles was
the most active and afforded maximum product yield (Table 1, entry 5). In the case of 2%Ni, the yield
of product was lower, whereas no significant enhancement was observed with increasing the
concentration of Ni beyond 5% (Table 1, entry 6). Furthermore, the reaction did not take place in dark
conditions at ambient temperature by using g-C3N4, g-PC3N4 and Ni@g-PC3N4 photocatalysts, which
clearly revealed that the reaction was visible light promoted (Table 1). The use of hydrazine hydrate
was found to be essential as it provided required protons and no product was formed in the absence
of hydrazine hydrate (Table 1, entry 5).
Table 1. Results of optimization experiments a. NiNPs: nickel nanoparticles; g-C3N4:graphitic carbon
nitride; g-PC3N4: phosphorous doped g-C3N4; Ni@g-PC3N4: nickel nanoparticles grafted on P-doped
g-C3N4; TOF: turn over frequency.
Entry Catalyst Conditions Time (h) AnilineYield (%) b TOF (h−1)
1 NiNPs
Dark
Visible light
24
-
-
-
-
-
2 g-C3N4
Dark
Visible light
24
12
-
24.6
-
2.0
3 g-P-C3N4
Dark
Visible light
24
12
-
54.2
-
4.5
4 2%Ni@g-PC3N4
Dark
Visible light
24
8
-
82.0
-
10.2
5 5%Ni@g-PC3N4
Dark
Visible light
Visible light
24
8
24 c
Trace
96.5
- c
-
12.1
- c
6 7.5%Ni@g-PC3N4
Dark
Visible light
24
8
10
97.0
0.4
12.1
a Reaction conditions: nitrobenzene, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W light emitting diode (LED) λ > 400 nm, Power at reaction vessel 70 W/m2;
b Isolated yield; c without hydrazine monohydrate.
Based on these optimization experiments, 5%Ni@g-PC3N4 was selected as the optimum catalyst
for further studies. The reaction was further generalized for various substituted nitrobenzenes and
the results are summarized in Table 2. It can be seen that the substituent effect did not play much of
a role and excellent product yields were obtained in all cases within 8 to 10.5 h.
Table 2. 5%Ni@g-PC3N4 catalyzed photoreduction of nitrobenzenes a.
Entry Reactant Product Time/h Conversion (%) b
Yield
(%) c
TOF (h−1)
1 NO2 NH2 8.0 98.0 96.5 12.1
2 HO NO2 HO NH2 8.0 95.5 94.2 11.7
3 H3C NO2 H3C NH2 8.0 96.4 95.4 11.9
4 NO2 NH2 8.0 94.8 93.0 11.6
5 NO2H3CO NH2H3CO 8.0 95.6 94.2 11.7
6 C2H5O NO2 C2H5O NH2 8.0 96.0 94.6 11.8
7 Cl NO2 Cl NH2 8.5 90.5 89.4 10.5
8 Br NO2 Br NH2 8.5 92.4 91.0 10.7
9 NO2I NH2I 10.5 93.6 92.8 8.810.5 93.6 92.8 8.8
10
Nanomaterials 2016, 6, 59 11 of 15
10 NO2F3C NH2F3C 10.5 90.4 89.6 8.5
a Reaction conditions: nitro compound, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W LED λ > 400 nm, Power at reaction vessel 70 W/m2; b Conversion (Conv.)
was determined with gas chromatography (GC); c Isolated yield.
The experiments were performed to probe the heterogeneous nature and reusability of the
photocatalyst. After the completion of the reaction, the photocatalyst was recovered by centrifugation,
washed with methanol and dried at 50 °C. The recovered photocatalyst was reused for five
subsequent runs under described experimental conditions. No significant loss was observed in the
Nanomaterials 2016, 6, 59 11 of 15
10 NO2F3C NH2F3C 10.5 90.4 89.6 8.5
a Reaction conditions: nitro compound, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W LED λ > 400 nm, Power at reaction vessel 70 W/m2; b Conversion (Conv.)
was determined with gas chromatography (GC); c Isolated yield.
The experiments were performed to probe the heterogeneous nature and reusability of the
photocatalyst. After the completion of the reaction, the photocatalyst was recovered by centrifugation,
washed with methanol and dried at 50 °C. The recovered photocatalyst was reused for five
subsequent runs under described experimental conditions. No significant loss was observed in the
10.5 90.4 89.6 8.5
a Reaction conditions: nitro compound, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol; Irradiation,
White cold 20 W LED λ > 400 nm, Power at reaction vessel 70 W/m2; b Conversion (Conv.) was determined
with gas chromatography (GC); c Isolated yield.
10. Nanomaterials 2016, 6, 59 10 of 14
The experiments were performed to probe the heterogeneous nature and reusability of the
photocatalyst. After the completion of the reaction, the photocatalyst was recovered by centrifugation,
washed with methanol and dried at 50 ˝C. The recovered photocatalyst was reused for five
subsequent runs under described experimental conditions. No significant loss was observed in
the activity of the recycled catalyst, and the product yield remained almost unchanged even after five
recycling experiments, which confirmed the true heterogeneous nature of the developed photocatalyst.
Furthermore, an inductively coupled plasma-atomic emission spectrometry (ICP-AES) analysis of the
photocatalyst after five recycling experiments showed a nickel content of 4.92 wt %, which is nearly
similar to that of a fresh catalyst (4.98 wt %). These results confirmed that the developed photocatalyst
was truly heterogeneous in nature and had not shown any detectable leaching during the reaction
(Figure 9).
Nanomaterials 2016, 6, 59 11 of 15
10 NO2F3C NH2F3C 10.5 90.4 89.6 8.5
a Reaction conditions: nitro compound, 0.1 mmol; catalyst, 25 mg; hydrazine monohydrate, 1 mmol;
Irradiation, White cold 20 W LED λ > 400 nm, Power at reaction vessel 70 W/m2; b Conversion (Conv.)
was determined with gas chromatography (GC); c Isolated yield.
The experiments were performed to probe the heterogeneous nature and reusability of the
photocatalyst. After the completion of the reaction, the photocatalyst was recovered by centrifugation,
washed with methanol and dried at 50 °C. The recovered photocatalyst was reused for five
subsequent runs under described experimental conditions. No significant loss was observed in the
activity of the recycled catalyst, and the product yield remained almost unchanged even after five
recycling experiments, which confirmed the true heterogeneous nature of the developed
photocatalyst. Furthermore, an inductively coupled plasma-atomic emission spectrometry (ICP-AES)
analysis of the photocatalyst after five recycling experiments showed a nickel content of 4.92 wt %,
which is nearly similar to that of a fresh catalyst (4.98 wt %). These results confirmed that the
developed photocatalyst was truly heterogeneous in nature and had not shown any detectable
leaching during the reaction (Figure 9).
Figure 9. Results of recycling experiments.
Although the exact mechanism of the reaction is not clear at this stage, we assume that the
generation of electron-hole pairs after the absorption of visible light is the first step to initiate the
reaction [34]. Since the optical band gap of P-doped g-PC3N4 is 1.52 eV, it can generate electrons and
holes in its conduction and valence band, respectively. Electrons from the conduction band of P-
doped carbon nitride get transferred to nickel nanoparticles due to lower Fermi level, which therefore
work as electron sinks and capture the photogenerated electrons and prevent back charge
recombination [35]. The electrons from NiNPs are transferred to nitrobenzene, which initiate a one
electron reduction step [36]. The holes in the valence band of g-PC3N4 oxidize hydrazine hydrate and
generate electrons and protons along with nitrogen gas. The protons were used for the hydrogenation
of activated molecules of nitrobenzene. As for the reduction of nitrobenezene to aniline, six protons
and six electrons are required, so 3/2 NH2NH2·H2O mole were consumed per mole of reactant
(Scheme 3).
Figure 9. Results of recycling experiments.
Although the exact mechanism of the reaction is not clear at this stage, we assume that the
generation of electron-hole pairs after the absorption of visible light is the first step to initiate the
reaction [34]. Since the optical band gap of P-doped g-PC3N4 is 1.52 eV, it can generate electrons and
holes in its conduction and valence band, respectively. Electrons from the conduction band of P-doped
carbon nitride get transferred to nickel nanoparticles due to lower Fermi level, which therefore work as
electron sinks and capture the photogenerated electrons and prevent back charge recombination [35].
The electrons from NiNPs are transferred to nitrobenzene, which initiate a one electron reduction
step [36]. The holes in the valence band of g-PC3N4 oxidize hydrazine hydrate and generate electrons
and protons along with nitrogen gas. The protons were used for the hydrogenation of activated
molecules of nitrobenzene. As for the reduction of nitrobenezene to aniline, six protons and six
electrons are required, so 3/2 NH2NH2¨ H2O mole were consumed per mole of reactant (Scheme 3).
11. Nanomaterials 2016, 6, 59 11 of 14
Nanomaterials 2016, 6, 59 12 of 15
Scheme 3. Plausible mechanism on the basis of the band gap structure for the visible light reduction
of nitrobenzenes by Ni@g-PC3N4 photocatalyst. CB: conduction band; VB: valence band.
3. Experimental Section
3.1. Materials
Dicyandiamide (99%), 1-butyl-3-methylimidazolium hexafluorophosphate [BmimPF6] (≥98.5%),
nickel chloride hexahydrate (≥98%), cetyltrimethylammonium bromide (≥98%) and sodium
borohydride (≥98.0%) were purchased from Aldrich (St. Louis, MO, USA) and used as received. All
substrates and solvents were purchased from Merck India Ltd (Mumbai, Maharashtra, India) and
used without further purification.
3.2. Characterizations
The rough morphological surface properties of materials were determined with the help of
scanning electron microscopy (SEM) using FE-SEM (Jeol Model JSM-6340F (Tokyo, Japan). For
elaborating the fine structure of the catalysts, high-resolution transmission electron microscopy
(HRTEM) was used and HRTEM images were collected on FEI-TecnaiG2 Twin TEM (Hillsboro, OR,
USA) operating at an acceleration voltage of 200 kV. For sample preparation, a very dilute suspension
of material was deposited on a carbon coated TEM grid. TEM images were processed on GATAN
micrograph software (Munchen, Germany). The vibration spectra (FT-IR) of samples were recorded
on a Perkin–Elmer spectrum RX-1 IR spectrophotometer (Waltham, MA, USA) using a potassium
bromide window. X-ray diffraction patterns for determining the phase structure and crystalline
properties of the materials were obtained on a Bruker D8 Advance diffractometer (Billerica, MA, USA)
working at 40 kV and 40 mA with Cu Kα radiation (λ = 0.15418 nm). Nitrogen adsorption-desorption
isotherms for calculating surface properties like Brunauer-Emmet-Teller surface area (SBET), Barret-
Joiner-Halenda (BJH) porosity, pore volume, etc., were acquired on a VP. Micromeritics ASAP2010
(Norcross, GA, USA) at 77 K. UV-Vis absorption spectra of solid samples were collected on a Perkin
Elmer lambda-19 UV-VIS-NIR spectrophotometer (Waltham, MA, USA) by making 1 mm thick
pellets using BaSO4 as reference. To check the thermal stability of materials, thermogravimetric
analysis (TGA) was performed by using a TA-SDT Q-600 thermal analyser (Champaign, IL, USA) in
the temperature range of 45 to 800 °C under nitrogen flow with a heating rate of 10 °C/min. To
determine the nickel content in the synthesized composites, ICP-AES analysis was performed by
using inductively coupled plasma atomic emission spectrometer (ICP-AES, DRE, PS-3000UV,
Leeman Labs Inc., Hudson, NH, USA). Samples for ICP-AES were made by digesting a calculated
amount of samples with nitric acid followed by filtration and making volume up to 10 mL by adding
deionized water.
3.3. Synthesis of Nickel Nanoparticles [26]
Scheme 3. Plausible mechanism on the basis of the band gap structure for the visible light reduction of
nitrobenzenes by Ni@g-PC3N4 photocatalyst. CB: conduction band; VB: valence band.
3. Experimental Section
3.1. Materials
Dicyandiamide (99%), 1-butyl-3-methylimidazolium hexafluorophosphate [BmimPF6] (ě98.5%),
nickel chloride hexahydrate (ě98%), cetyltrimethylammonium bromide (ě98%) and sodium
borohydride (ě98.0%) were purchased from Aldrich (St. Louis, MO, USA) and used as received.
All substrates and solvents were purchased from Merck India Ltd (Mumbai, Maharashtra, India) and
used without further purification.
3.2. Characterizations
The rough morphological surface properties of materials were determined with the help
of scanning electron microscopy (SEM) using FE-SEM (Jeol Model JSM-6340F (Tokyo, Japan).
For elaborating the fine structure of the catalysts, high-resolution transmission electron microscopy
(HRTEM) was used and HRTEM images were collected on FEI-TecnaiG2 Twin TEM (Hillsboro, OR,
USA) operating at an acceleration voltage of 200 kV. For sample preparation, a very dilute suspension
of material was deposited on a carbon coated TEM grid. TEM images were processed on GATAN
micrograph software (Munchen, Germany). The vibration spectra (FT-IR) of samples were recorded on
a Perkin–Elmer spectrum RX-1 IR spectrophotometer (Waltham, MA, USA) using a potassium bromide
window. X-ray diffraction patterns for determining the phase structure and crystalline properties of the
materials were obtained on a Bruker D8 Advance diffractometer (Billerica, MA, USA) working at 40 kV
and 40 mA with Cu Kα radiation (λ = 0.15418 nm). Nitrogen adsorption-desorption isotherms for
calculating surface properties like Brunauer-Emmet-Teller surface area (SBET), Barret-Joiner-Halenda
(BJH) porosity, pore volume, etc., were acquired on a VP. Micromeritics ASAP2010 (Norcross, GA,
USA) at 77 K. UV-Vis absorption spectra of solid samples were collected on a Perkin Elmer lambda-19
UV-VIS-NIR spectrophotometer (Waltham, MA, USA) by making 1 mm thick pellets using BaSO4 as
reference. To check the thermal stability of materials, thermogravimetric analysis (TGA) was performed
by using a TA-SDT Q-600 thermal analyser (Champaign, IL, USA) in the temperature range of 45 to
800 ˝C under nitrogen flow with a heating rate of 10 ˝C/min. To determine the nickel content in the
synthesized composites, ICP-AES analysis was performed by using inductively coupled plasma atomic
emission spectrometer (ICP-AES, DRE, PS-3000UV, Leeman Labs Inc., Hudson, NH, USA). Samples
for ICP-AES were made by digesting a calculated amount of samples with nitric acid followed by
filtration and making volume up to 10 mL by adding deionized water.
12. Nanomaterials 2016, 6, 59 12 of 14
3.3. Synthesis of Nickel Nanoparticles [26]
Nickel nanoparticles were synthesized by following a literature procedure. In brief, to an aqueous
suspension of nickel chloride hexahydrate (0.152 mmol, 0.019 g) and cetyltrimethyl ammonium
bromide, CTAB (0.288 mmol, 0.105 g), an aqueous solution (1.5 mL) of NaBH4 (0.020 g, 0.526 mmol)
was added dropwise. The mixture was vigorously stirred to obtain a black suspension. The particles
were separated by centrifugation and washed with water several times.
3.4. Synthesis of Phosphorous-Doped Graphitic Carbon Nitride (g-PC3N4) [19,27]
Phosphorous-doped graphitic carbon nitride was synthesized by using BmimPF4 as a source of
phosphorous. The phosphorous containing ionic liquid, BmimPF4 (0.5 g) was dissolved in water (6 mL)
and stirred for 5 min. After that, dicyandiamide (1 g) was added to this solution and the mixture was
heated at 100 ˝C until all the water had completely evaporated, which resulted in the formation of
a white solid. The obtained solid was subjected to heating at a programmed temperature. Firstly the
sample was heated up to 350 ˝C within 2 h, then the temperature was maintained at a constant for the
next 4 h. The temperature was then raised to 550 ˝C in 1 h and then this temperature was maintained
at a constant for the next 4 h. The sample was collected at room temperature.
3.5. Synthesis of Nickel Nanoparticles Decorated on Phosphorous-Doped Graphitic Carbon Nitride (Ni@g-PC3N4)
For the synthesis of nickel nanoparticle-decorated carbon nitride, nickel particles were added
along with BmimPF4 and dicyandiamide during the synthesis step. Then the sample was heated at
a programmed temperature as in the synthesis of P-doped carbon nitride.
3.6. Photocatalytic Reduction Experiment
To check the activity of the catalyst for the visible light mediated reduction, a 20 watt LED (Model
No. HP-FL-20W-F-Hope LED Opto-Electric Co., Ltd (Shenzhen, China), λ > 400 nm) was used as
a source of visible light. A round bottom flask was charged with 25 mg of 5%Ni@g-PC3N4 catalyst,
0.1 mmol of nitrobenzene and 1.0 mmol of hydrazine monohydrate in 10 mL solvent mixture of
acetonitrile/DCM/methanol. After sonication for 10 min, the resulting mixture was irradiated under
visible light. To monitor the progress of the reaction, the sample was withdrawn at a certain period of
time and analyzed by gas chromatography-flame ionization detector (GC-FID). After the completion of
the reaction, the solvent was removed by rotary evaporation and the product was isolated using column
chromatography. The identification of product was done by gas chromatography-mass spectrometry
(GC-MS) and 1H-nuclear magnetic resonance (1H-NMR).
4. Conclusions
We have synthesized a novel, highly efficient and visible light-active nickel nanoparticles-
decorated P-doped carbon nitride for the selective hydrogenation of nitro compounds to the
corresponding amines in the presence of hydrazine monohydrate as a proton donor. Due to P-doping,
the developed photocatalyst absorbs the maximum part of the visible region and nickel nanoparticles
work as an electron trap. The developed photocatalyst was found to be highly effective and afforded
excellent product yields within 8–10.5 h at ambient temperature under visible light irradiation. Due to
the heterogeneous nature of photocatalyst, it can be easily recovered and reused for further reactions
without any significant decrease in its activity. The enhanced performance of the catalyst in the visible
region can be explained on the basis of reduced band gap, which generates electron-hole pairs through
the absorption of visible light. Photogenerated electrons are efficiently captured by nickel nanoparticles
on the sheets and subsequently transferred to substrate molecule, while holes are used to oxidize
hydrazine hydrate and extract required protons and electrons for the reaction.
Acknowledgments: Authors are thankful to Director IIP for granting permission to publish these results.
Anurag Kumar and Pawan Kumar are thankful to Council of Scientific and Industrial Research (CSIR) New Delhi