This document describes the room temperature synthesis of copper sulfide (Cu9S5), copper selenide (CuSe), lead sulfide (PbS), and lead selenide (PbSe) by reacting the elemental powders in 2-mercaptoethanol solvent for 24 hours. Characterization by powder X-ray diffraction and Raman spectroscopy showed the products were highly crystalline. Reactions in ethylene glycol also yielded copper sulfide and lead sulfide but reactions in dimercaptoethane did not yield metal chalcogenides. This solvent-mediated room temperature synthesis provides a simple method for producing these metal chalcogenide materials.
Study the effect of Mn2+ ions on the ac electrical properties of some iron do...IJRES Journal
Oxide glasses doped with transition metal ions are of high interest because of their variant applications in both science and technology fields. However, the normal melt quench method have used to prepared some iron doped phosphate glasses according the following molecular formula: (65-x) mol% P2O5 - 20 mol% Na2O - 15 mol% Fe2O3 - x mol% MnO, Where x= 0, 5,10, 20, 25. The room temperature Mössbauer Effect ME Spectra used to characterized the glassy state homogeneity of these glasses. ME spectra show, for all glasses, no magnetic field participate which mean good glassy state formation. The ac electrical transport properties were also measured, as function of temperature up to 500k. It was found that the ac conductivity increased with the gradual increase of Mn2+ cations, while the electrical activation energy decreased.
Vacancy and Copper-doping Effect on Superconductivity for Clathrate MaterialsYang Li
We present a joint experimental and theoretical study of the superconductivity and electronic structures in type-I Cu-doped silicon clathrates and germanium clathrates. The superconducting critical temperature in Ba8Si46–xCux is shown to decrease strongly with copper content increasing. These results are corroborated by CASTEP approach, first-principles simulations calculated from the density-functional theory with plane waves and pseudopotentials. The simulations show that Cu-doping results in a large decrease of electronic density of states in Fermi level, which can explain the superconducting critical temperature decrease with Cu-doping in the BCS theoretical frame. Further, comparison of Ba8Ge46 and Ba8Si46 within the CASTEP approach shows that the superconductivity is an intrinsic property of the sp3 silicon and germanium clathrates without vacancy in the cage framework. By analysis of the density of states (DOS) and reported experimental results of the Zintl-like Ba8Ge43, a new mechanism of vacancy defect is suggested to explain the absence of superconductivity in Ge clathrates, which is of benefit to eliminating the divarication between theoretical prediction and the experimental observation for superconductivity in Ge clathrates. Keeping an entire Si and Ge cage structure without vacancy is the prerequisite for occurrence of superconductivity in clathrates.
Superconductivity in Gallium-substituted Ba8Si46 ClathratesYang Li
We report a joint experimental and theoretical investigation of superconductivity in Ga-substituted type-I silicon clathrates. We prepared samples of the general formula Ba8Si46−xGax, with different values of x. We show that Ba8Si40Ga6 is a bulk superconductor, with an onset at TC=3.3 K. For x=10 and higher, no superconductivity was observed down to T=1.8 K. This represents a strong suppression of superconductivity with increasing Ga content, compared to Ba8Si46 with TC=8 K. Suppression of superconductivity can be attributed primarily to a decrease in the density of states at the Fermi level, caused by a reduced integrity of the sp3-hybridized networks as well as the lowering of carrier concentration. These results are corroborated by first-principles calculations, which show that Ga substitution results in a large decrease of the electronic density of states at the Fermi level, which explains the decreased superconducting critical temperature within the BCS framework. To further characterize the superconducting state, we carried out magnetic measurements showing Ba8Si40Ga6 to be a type-II superconductor. The critical magnetic fields were measured to be Hc1=35 Oe and Hc2=8.5 kOe.We deduce the London penetration depth 3700 Å and the coherence length 200 Å. Our estimate of the electron-phonon coupling reveals that Ba8Si40Ga6 is a moderate phonon-mediated BCS superconductor.
Microstructural and Dielectric Characterization of Sr doped Ba(Fe0.5Ta0.5)O3 ...theijes
Solid state reaction method was used to synthesize Ba1-xSrx(Fe0.5Ta0.5)O3 ceramic(x=0, 0.1, 0.2, 0.3, 0.4 and 0.5). The raw materials of making Sr doped Ba(Fe0.5Ta0.5)O3 were BaCO3, SrCO3, Fe2O3, Ta2O5 (purity better than 99%). Pellet and ring shaped samples prepared from each composition were sintered at 1400 and 1450ºC for 5 hour. The phase formation of Ba1-xSrx(Fe0.5Ta0.5)O3 was checked using X-ray diffraction (XRD) technique and observed a cubic perovskite crystal structure in space group Pm3m (221). Microstructure of the individual compound was examined by the field emission scanning electron micrograph (FESEM). Grain size was found to be varied with Sr content. The lattice parameter decreased with increasing Sr content. Dielectric spectroscopy was applied to investigate the electrical properties of BSFT at room temperature and in a frequency range of 100Hz–100 MHz. An analysis of the dielectric constant εʹ and loss tangent tan with frequency was performed assuming a distribution of relaxation times. The low frequency dielectric dispersion corresponds to the DC electrical conductivity.
Computational Study on the Effect of Axial Ligation Upon the Electronic Struc...Roxana Kincses
Computational Study on the Effect of Axial Ligation Upon the
Electronic Structure of Copper (II) Porphyrinate
(CuTPPs = [5,10,15,20-tetrakis(N-methylpyridyl-4)porhinato]copper(II)tetratosylate))
- Electronic Structure with Different Axial Ligands
Surface Activation of C-sp3 in Boron-Doped Diamond ElectrodeAlejandro Medel
Abstract C-sp2 (graphite) impurities are undesirable in synthetic diamond electrodes (C-sp3), because they can affect the electrochemical response. In this work, we demonstrate that Csp3 surfaces can be activated successfully by applying an anodic current density corresponding to sufficiently high potential where the hydroxyl radicals (●OH) are generated. The
effectiveness of this activation process was verified by Raman spectroscopy, X-ray diffraction, scanning electron microscopy, and cyclic voltammetry.
Thermal and spectroscopy studies of Ag2SO4 and LiAgSO4IOSR Journals
A comparative study is conducted on the structure, electronic and spectroscopic properties of Ag2SO4 and LiAgSO4. Both the sulphates crystallise in an orthorhombic structure with the same space group of Fddd (70). A red shift in Raman modes indicates the stiffness of the crystal Ag2SO4 over LiAgSO4. From ESR, it is observed that these sulphates has Mn2+ impurities leading to the gav= 2.1040 at a field of 3255 G. This indicates that the Mn2+ ions have an environment close to octahedral symmetry. The g value corresponding to Ag2SO4 is 2.3005. The endothermic peaks in LiAgSO4 at 388.8 and 4200C are due to the formation of BCC structure of LiAgSO4. The peak at 420.90C in Ag2SO4 may be due to the phase transition of β-Ag2SO4 particles to α-Ag2SO4 on heating.
Oxygen Vacancy Conduction in Double PerovskitesMegha Patel
Fuel cells and solar panels provide more environmentally friendly alternatives to burning fossil fuels. Fuel cells currently need better oxygen vacancy conducting cathode materials while solar materials need ways of tuning the band gap. Understanding of oxygen vacancy structure and conduction in perovskites and double perovskites is critical in solving these two challenges. A neutron pair distribution analysis study of the double perovskite Sr2MSbO5.5 (M=Ca, Sr, Ba) found that multiple structures where oxygen vacancies significantly altered the local geometry of the system could explain the same neutron scattering measurements. Our goal is to find all the energetically favored structures in these systems and their impact to oxygen vacancy conduction in these double perovskites. Density functional theory (DFT) with the PBE functional and a generalized gradient approximation (GGA) implementation in the Vienna ab-initio simulation package (VASP) was used to find energies. The conjugate gradient method was used to find minimum energy configurations of the Sr2MSbO6 double perovskites from all 23 possible Glazer octahedral distortions. Oxygen vacancies were introduced without distortions, with trigonal bipyramidal distortions, and with pentagonal distortions. All structures were optimized. The minima featured distorted SbO5 square pyramids and trigonal bipyramids in most systems and sometimes MO7-x pentagonal bipyramidal structures with that structure becoming more favored with increasing ionic size for the M ion. Both of these distortions were suggested by experiment to lead to the neutron scattering measurements. A detailed energetic analysis of these options is presented. Further, implications of these distortions on oxygen vacancy conduction in double perovskite systems are discussed.
Critical magnetic fields of superconducting aluminum-substituted Ba8Si42Al4 c...Yang Li
In recent years, efforts have been made to explore the superconductivity of clathrates containing crystalline frameworks of group-IV elements. The superconducting silicon clathrate is unusual in that the structure is dominated by strong sp3 covalent bonds between silicon atoms, rather than the metallic bonding that is more typical of traditional superconductors. This paper reports on critical magnetic fields of superconducting Al-substituted silicon clathrates, which were investigated by transport, ac susceptibility, and dc magnetization measurements in magnetic fields up to 90 kOe. For the sample Ba8Si42Al4, the critical magnetic fields were measured to be HC1=40.2 Oe and HC2=66.4 kOe. The London penetration depth of 4360A ° and the coherence length 70A ° were obtained, whereas the estimated Ginzburg–Landau parameter 62 revealed that Ba8Si42Al4 is a strong type-II superconductor.
Study the effect of Mn2+ ions on the ac electrical properties of some iron do...IJRES Journal
Oxide glasses doped with transition metal ions are of high interest because of their variant applications in both science and technology fields. However, the normal melt quench method have used to prepared some iron doped phosphate glasses according the following molecular formula: (65-x) mol% P2O5 - 20 mol% Na2O - 15 mol% Fe2O3 - x mol% MnO, Where x= 0, 5,10, 20, 25. The room temperature Mössbauer Effect ME Spectra used to characterized the glassy state homogeneity of these glasses. ME spectra show, for all glasses, no magnetic field participate which mean good glassy state formation. The ac electrical transport properties were also measured, as function of temperature up to 500k. It was found that the ac conductivity increased with the gradual increase of Mn2+ cations, while the electrical activation energy decreased.
Vacancy and Copper-doping Effect on Superconductivity for Clathrate MaterialsYang Li
We present a joint experimental and theoretical study of the superconductivity and electronic structures in type-I Cu-doped silicon clathrates and germanium clathrates. The superconducting critical temperature in Ba8Si46–xCux is shown to decrease strongly with copper content increasing. These results are corroborated by CASTEP approach, first-principles simulations calculated from the density-functional theory with plane waves and pseudopotentials. The simulations show that Cu-doping results in a large decrease of electronic density of states in Fermi level, which can explain the superconducting critical temperature decrease with Cu-doping in the BCS theoretical frame. Further, comparison of Ba8Ge46 and Ba8Si46 within the CASTEP approach shows that the superconductivity is an intrinsic property of the sp3 silicon and germanium clathrates without vacancy in the cage framework. By analysis of the density of states (DOS) and reported experimental results of the Zintl-like Ba8Ge43, a new mechanism of vacancy defect is suggested to explain the absence of superconductivity in Ge clathrates, which is of benefit to eliminating the divarication between theoretical prediction and the experimental observation for superconductivity in Ge clathrates. Keeping an entire Si and Ge cage structure without vacancy is the prerequisite for occurrence of superconductivity in clathrates.
Superconductivity in Gallium-substituted Ba8Si46 ClathratesYang Li
We report a joint experimental and theoretical investigation of superconductivity in Ga-substituted type-I silicon clathrates. We prepared samples of the general formula Ba8Si46−xGax, with different values of x. We show that Ba8Si40Ga6 is a bulk superconductor, with an onset at TC=3.3 K. For x=10 and higher, no superconductivity was observed down to T=1.8 K. This represents a strong suppression of superconductivity with increasing Ga content, compared to Ba8Si46 with TC=8 K. Suppression of superconductivity can be attributed primarily to a decrease in the density of states at the Fermi level, caused by a reduced integrity of the sp3-hybridized networks as well as the lowering of carrier concentration. These results are corroborated by first-principles calculations, which show that Ga substitution results in a large decrease of the electronic density of states at the Fermi level, which explains the decreased superconducting critical temperature within the BCS framework. To further characterize the superconducting state, we carried out magnetic measurements showing Ba8Si40Ga6 to be a type-II superconductor. The critical magnetic fields were measured to be Hc1=35 Oe and Hc2=8.5 kOe.We deduce the London penetration depth 3700 Å and the coherence length 200 Å. Our estimate of the electron-phonon coupling reveals that Ba8Si40Ga6 is a moderate phonon-mediated BCS superconductor.
Microstructural and Dielectric Characterization of Sr doped Ba(Fe0.5Ta0.5)O3 ...theijes
Solid state reaction method was used to synthesize Ba1-xSrx(Fe0.5Ta0.5)O3 ceramic(x=0, 0.1, 0.2, 0.3, 0.4 and 0.5). The raw materials of making Sr doped Ba(Fe0.5Ta0.5)O3 were BaCO3, SrCO3, Fe2O3, Ta2O5 (purity better than 99%). Pellet and ring shaped samples prepared from each composition were sintered at 1400 and 1450ºC for 5 hour. The phase formation of Ba1-xSrx(Fe0.5Ta0.5)O3 was checked using X-ray diffraction (XRD) technique and observed a cubic perovskite crystal structure in space group Pm3m (221). Microstructure of the individual compound was examined by the field emission scanning electron micrograph (FESEM). Grain size was found to be varied with Sr content. The lattice parameter decreased with increasing Sr content. Dielectric spectroscopy was applied to investigate the electrical properties of BSFT at room temperature and in a frequency range of 100Hz–100 MHz. An analysis of the dielectric constant εʹ and loss tangent tan with frequency was performed assuming a distribution of relaxation times. The low frequency dielectric dispersion corresponds to the DC electrical conductivity.
Computational Study on the Effect of Axial Ligation Upon the Electronic Struc...Roxana Kincses
Computational Study on the Effect of Axial Ligation Upon the
Electronic Structure of Copper (II) Porphyrinate
(CuTPPs = [5,10,15,20-tetrakis(N-methylpyridyl-4)porhinato]copper(II)tetratosylate))
- Electronic Structure with Different Axial Ligands
Surface Activation of C-sp3 in Boron-Doped Diamond ElectrodeAlejandro Medel
Abstract C-sp2 (graphite) impurities are undesirable in synthetic diamond electrodes (C-sp3), because they can affect the electrochemical response. In this work, we demonstrate that Csp3 surfaces can be activated successfully by applying an anodic current density corresponding to sufficiently high potential where the hydroxyl radicals (●OH) are generated. The
effectiveness of this activation process was verified by Raman spectroscopy, X-ray diffraction, scanning electron microscopy, and cyclic voltammetry.
Thermal and spectroscopy studies of Ag2SO4 and LiAgSO4IOSR Journals
A comparative study is conducted on the structure, electronic and spectroscopic properties of Ag2SO4 and LiAgSO4. Both the sulphates crystallise in an orthorhombic structure with the same space group of Fddd (70). A red shift in Raman modes indicates the stiffness of the crystal Ag2SO4 over LiAgSO4. From ESR, it is observed that these sulphates has Mn2+ impurities leading to the gav= 2.1040 at a field of 3255 G. This indicates that the Mn2+ ions have an environment close to octahedral symmetry. The g value corresponding to Ag2SO4 is 2.3005. The endothermic peaks in LiAgSO4 at 388.8 and 4200C are due to the formation of BCC structure of LiAgSO4. The peak at 420.90C in Ag2SO4 may be due to the phase transition of β-Ag2SO4 particles to α-Ag2SO4 on heating.
Oxygen Vacancy Conduction in Double PerovskitesMegha Patel
Fuel cells and solar panels provide more environmentally friendly alternatives to burning fossil fuels. Fuel cells currently need better oxygen vacancy conducting cathode materials while solar materials need ways of tuning the band gap. Understanding of oxygen vacancy structure and conduction in perovskites and double perovskites is critical in solving these two challenges. A neutron pair distribution analysis study of the double perovskite Sr2MSbO5.5 (M=Ca, Sr, Ba) found that multiple structures where oxygen vacancies significantly altered the local geometry of the system could explain the same neutron scattering measurements. Our goal is to find all the energetically favored structures in these systems and their impact to oxygen vacancy conduction in these double perovskites. Density functional theory (DFT) with the PBE functional and a generalized gradient approximation (GGA) implementation in the Vienna ab-initio simulation package (VASP) was used to find energies. The conjugate gradient method was used to find minimum energy configurations of the Sr2MSbO6 double perovskites from all 23 possible Glazer octahedral distortions. Oxygen vacancies were introduced without distortions, with trigonal bipyramidal distortions, and with pentagonal distortions. All structures were optimized. The minima featured distorted SbO5 square pyramids and trigonal bipyramids in most systems and sometimes MO7-x pentagonal bipyramidal structures with that structure becoming more favored with increasing ionic size for the M ion. Both of these distortions were suggested by experiment to lead to the neutron scattering measurements. A detailed energetic analysis of these options is presented. Further, implications of these distortions on oxygen vacancy conduction in double perovskite systems are discussed.
Critical magnetic fields of superconducting aluminum-substituted Ba8Si42Al4 c...Yang Li
In recent years, efforts have been made to explore the superconductivity of clathrates containing crystalline frameworks of group-IV elements. The superconducting silicon clathrate is unusual in that the structure is dominated by strong sp3 covalent bonds between silicon atoms, rather than the metallic bonding that is more typical of traditional superconductors. This paper reports on critical magnetic fields of superconducting Al-substituted silicon clathrates, which were investigated by transport, ac susceptibility, and dc magnetization measurements in magnetic fields up to 90 kOe. For the sample Ba8Si42Al4, the critical magnetic fields were measured to be HC1=40.2 Oe and HC2=66.4 kOe. The London penetration depth of 4360A ° and the coherence length 70A ° were obtained, whereas the estimated Ginzburg–Landau parameter 62 revealed that Ba8Si42Al4 is a strong type-II superconductor.
Analysis and Design of Lead Salt PbSe/PbSrSe Single Quantum Well In the Infra...IJASCSE
There is a considerable interest in studying the energy spectrum changes due to the non parabolic energy band structure in nano structures and nano material semiconductors. Most material systems have parabolic band structures at the band edge, however away from the band edge the bands are strongly non parabolic. Other material systems are strongly parabolic at the band edge such as IV-VI lead salt semiconductors. A theoretical model was developed to conduct this study on PbSe/Pb 0.934 Sr0.066 Se nanostructure system in the infrared region. Moreover, we studied the effects of four temperatures on the analysis and design of this system. It will be shown that the total losses for the system are higher than the modal gain values for lasing to occur and multiple quantum well structures are a better design choice.
Spectral studies of 5-({4-amino-2-[(Z)-(2-hydroxybenzylidene) amino] pyrimidi...IOSR Journals
Some transition metal ions Complexes with 5-({4-amino-2-[(Z)-(2-hydroxybenzylidene) amino]
pyrimidin-5-yl} methyl)-2,3,4-trimethoxybenzene were prepared and characterized by elemental analyses,
Infrared , magnetic moment, electronic spectra , mass spectra, X-ray powder diffraction, molar conductance
and thermal analysis (TGA). The complexes have general formulae [ML2.2H2O] {where M = Mn (II), Co (II), Ni
(II), Cu (II), Zn (II), Pd (II) and Pt (II). The coordination behavior of the metal ions towards to the investigated
Schiff base takes place through –C=N,-NH2 and –OH groups. The obtained C, H and N elemental analysis data
showed the Metal: Ligand ratio is 1:2 [M: L] ratio. The molar conductance data reveal that all the metal
complexes are non-electrolytic in nature. From the magnetic moments the complexes are paramagnetic except
Zn metal ion complexes have octahedral geometry with coordination number eight. The thermal behavior of
these complexes shows that, the hydrated complexes have loses two water molecules and immediately followed
by decomposition of the anions and ligand molecules in the second and third stage. The Schiff bases and metal
complexes show good activity against some bacteria. The antimicrobial results indicate that, the metal
complexes have better antimicrobial activity as compared to the prepared Schiff base.
A Review: Synthesis and characterization of metals complexes with paracetamol...TaghreedHAlnoor
In this review, previous studies on the synthesis and characterization of the metal Complexes with
paracetamol by elemental analysis, thermal analysis, (IR, NMR and UV-Vis (spectroscopy and conductivity.
In reviewing these studies, the authors found that paracetamol can be coordinated through the pair of electrons
on the hydroxyl O-atom, carbonyl O-atom, and N-atom of the amide group. If the paracetamol was a
monodentate ligand, it will be coordinated by one of the following atoms O-hydroxyl, O-carbonyl or N-amide.
But if the paracetamol was bidentate, it is coordinated by atoms (O-carbonyl and N-amide), (O-hydroxyl and
N-amide) or (O-carbonyl and O-hydroxyl). The authors also found that free paracetamol and its complexes
have antimicrobial activity.
Heterostructured nanocomposite tin phthalocyanine@mesoporous ceria (SnPc@CeO2...Pawan Kumar
Heterostructured tin phthalocyanine supported to mesoporous ceria was synthesized and used a
photocatalyst for CO2 reduction under visible light. The photoreduction CO2 activities of the
heterostructures were investigated in the presence of triethylamine as sacrificial agent. The developed
photocatalyst exhibited high catalytic activity for photoreduction of CO2 and after 24 hours of visible
light irradiation 2342 mmol g1 cat of methanol (fMeOH ¼ 0.0223 or 2.23%) and 840 mmol g1 cat of CO
(fCO ¼ 0.0026 or 0.26%) were obtained as the major reaction products. The methanol formation rate
(RMeOH) and CO formation rate (RCO) was found to be 97.5 mmol h1 g1 cat and 35.0 mmol h1 g1 cat
respectively. While under the identical experimental conditions mesoporous ceria (meso-CeO2) gave
only 316 mmol g1 cat of methanol (fMeOH ¼ 0.003 or 0.30%) and 126 mmol g1 cat CO (fCO ¼ 0.0004
or 0.04%) with product formation rate RMeOH ¼ 13.2 mmol h1 g1 cat and RCO ¼ 5.3 mmol h1 g1 cat.
Furthermore, the recovered catalyst showed consistent catalytic activity for at least five runs without any
significant loss in product yields
Selective Oxidation of Cyclohexene, Toluene and Ethyl Benzene Catalyzed by Bi...Iranian Chemical Society
Bis-(L-tyrosinato)copper(II) was reacted with 3-(chloropropyl)-trimethoxysilane functionalized silica that has infused magnetite to yield a magnetically separable catalyst in which the copper carboxylate is covalently linked to the silica matrix through the silane linkage. The immobilized catalyst has been characterized by spectroscopic studies (such as FT-IR, EPR, Magnetic Measurement, SEM) and chemical analyses. The immobilized catalytic system functions as an efficient heterogeneous catalyst for oxidation of cyclohexene, toluene and ethyl benzene in the presence of hydrogen peroxide (as an oxidant) and sodium bicarbonate (a co-catalyst). The reaction conditions have been optimized for solvent, temperature and amount of oxidant and catalyst. Comparison of the encapsulated catalyst with the corresponding homogeneous catalyst showed that the heterogeneous catalyst had higher activity and selectivity than the homogeneous catalyst. The immobilized catalyst could be readily recovered from the reaction mixture by using a simple magnet, and reused up to five times without any loss of activity.
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
Graphene oxide immobilized copper phthalocyanine tetrasulphonamide: the first...Pawan Kumar
The first successful synthesis of DMC directly from methanol and carbon dioxide using a heterogenized
homogeneous graphene oxide immobilized copper phthalocyanine tetrasulphonamide catalyst in the
presence of N,N0-dicyclohexylcarbodiimide (DCC) as a dehydrating agent is described. The presence of a
dehydrating agent was found to be vital and in its absence the yield of DMC was found to be decreased
significantly. Under the optimized reaction conditions, the maximum yield of DMC reaches up to 13.3%.
Although the homogeneous copper phthalocyanine tetrasulphonamide catalyst provided a little higher
yield of DMC (14.2%), the facile recovery and recycling ability of the heterogeneous catalyst make the
developed method more attractive from environmental and economical viewpoints.
synthesis and characterization of hydrazone ligand and their metal complexesMUBASHIRA M
This slide mainly contain the synthesis, characterization of a few hydrazine based heterocyclic ligand such as hydralazone and phenyl hydralazone and also their metal complexes. so in this work, my aim is to synthesise the ligands; 2-thiophenecarboxylaldehydehydralazone and 2,3-butanedionephenylhydrazone. also to characterized the synthesised hydrazones by different physiochemical techniques.
The synthesis and characterization of three new metal chalcogenide aerogels, Chalcogels,
AFe3Zn3S17 (A= Na, K, or Rb) is described. Alkali metal polychalcogenides (Na2S5, K2S5, or Rb2S5)
reactwith metal acetate like Fe(OAc)2 and Zn(OAc)2in formamide solutionforming extended polymeric
frameworks by gelation. Chalcogels obtained aftersupercritical drying have BET surface areas of
430, 444, and 435 m
2
/g for NaFe3Zn3S17, KFe3Zn3S17, and RbFe3Zn3S17, respectively. The effect of the
counter ions (K, Na, and Rb) wasstudied by examined the adsorption capacities of the resulting
chalcogels toward different gases and volatile organic compounds. The measurements showed that
CO2 and toluene adsorption capacities increase with the polarizability of the surface atoms in the
following order: Rb chalcogel> K chalcogel> Na chalcogel.This finding reveals a trend based on
cation size and acid–base surface properties that might have a significant impact on altering
adsorptive properties of chalcogels by using more polarizable counter ions.
2. Cu9S5(Cu1.8S) (JCPDS file no. 47-1748). The peaks can very
well be indexed in rhombohedral symmetry with a = 3.951 Å
and c = 48.13 Å. The presence of the S−S stretching mode at
470 cm−1
(Figure 1b) in the Raman spectrum strongly
suggested the product to be Cu9S5(Cu1.8S).12,15
The room
temperature diamagnetic character also supported the product
to be copper sulfide, in which the copper existed in the 1+
oxidation state (Figure 1c).12b,16
Hexagonal CuSe resulted from
the reaction of copper and selenium powders (in a 1:1 mole
ratio), as endorsed by the peak positions and intensities in its
PXRD pattern (JCPDS file no. 34-0171; Figure 1d). The peaks
were indexable, taking a = 3.939 Å and c = 17.25 Å as the lattice
constants. A natural question arises as to whether sulfur would
also be present in the lattice with selenium when a sulfur-
containing solvent is used for the synthesis of metal selenides.
This is particularly applicable to copper metal because a
continuous solid solution, CuS1−xSex has been reported.17
Ishii et al.18
employed Raman spectroscopy as the pivotal
tool to study the solid solution CuS1−xSex in which the
progressive disappearance of the S−S stretching mode at
around 460 cm−1
with the emergence of the Se−Se stretching
mode positioned at around 270 cm−1
was reported to occur as
the selenium content increased. The absence of the S−S
stretching mode (at 470 cm−1
), together with the presence of a
band at 258 cm−1
(due to Se−Se stretching), confirmed the
formation of CuSe without sulfur in the lattice (Figure 1e).
Energy-dispersive X-ray (EDX) analysis [of its scanning
electron microscopy (SEM) image] also confirmed the ratio
of copper to selenium to be very close to unity (Figure S2 in
the SI). The characteristic paramagnetic behavior of CuSe16
was observed at room temperature with χg of 4.02 × 10−6
emu/
g (Figure 1f). The use of 2-mercaptoethanol for the room
temperature elemental combination reactions was extended to
lead, a nontransition metal. The PXRD pattern of the product
from the reaction of lead and sulfur powders (in a 1:1 mole
ratio) clearly indicated the formation of highly crystalline cubic
PbS (JCPDS file no. 78-1901), with the observed reflections
being indexable with a = 5.931 Å (Figure 2a). The cubic
symmetry of PbS was also supported by the presence of the
fundamental Raman band at 135 cm−1
and the first overtone at
270 cm−1
(Figure 2b).15
An increased cubic unit cell of a =
6.105 Å was observed for PbSe from its PXRD pattern (Figure
2c), matching closely with JCPDS file no. 78-1902.
To verify whether a simple mechanochemical reaction (due
to the vigorous stirring) might be promoting the copper sulfide
formation (in which the solvent remains as a mute spectator),
copper and sulfur powders (in a 1:1 mole ratio) were
suspended in 2-mercaptoethanol at room temperature without
stirring. Black colored product indicated the formation of
copper sulfide as revealed in its PXRD pattern (Figure S3 in the
SI). The broadness of the observed reflections in the PXRD
pattern suggested nanosized crystallites (with average size of 6
nm as estimated by Schreer analysis). SEM analysis showed
agglomeration of nano crystallites (Figure S3 in the SI). This
observation provided evidence that the metal chalcogenides are
indeed formed from the concerted chemical reaction between
the metal and chalcogen in 2-mercaptoethanol, whose
crystallinity is further improved by the mechanical stirring.
Varying the copper-to-sulfur ratio (2:1 or 1:2) yielded
Cu9S5(Cu1.8S) as the sole crystalline product, suggesting that
the final product stoichiometry was not governed by the ratio of
the reactants.
Additionally, dimercaptoethane and ethylene glycol were also
examined as solvents for these reactions. While CuS could be
Figure 1. (a) PXRD pattern, (b) Raman spectra, and (c) M−H plot of
the product from the reaction of copper and sulfur powders in 2-
mercaptoethanol at room temperature for 24 h. (d) PXRD pattern, (e)
Raman spectra, and (f) M−H plot of the product from the reaction of
copper and selenium powders in 2-mercaptoethanol at room
temperature for 24 h. JCPDS patterns are provided for reference.
Figure 2. PXRD pattern and Raman spectra (a and b) of the product
from the reaction of lead and sulfur powders in 2-mercaptoethanol at
room temperature for 24 h. PXRD pattern and Raman spectra (c and
d) of the product from the reaction of lead and selenium powders in 2-
mercaptoethanol at room temperature for 24 h. (The * in parts a and c
denote reflections due to unreacted sulfur and selenium, respectively. #
denotes reflections due to lead.) JCPDS patterns are provided for
reference.
Inorganic Chemistry Communication
dx.doi.org/10.1021/ic301422x | Inorg. Chem. 2012, 51, 7945−79477946
3. identified as the product after 24 h of reaction in ethylene
glycol, copper sulfide formation was not observed in
dimercaptoethane (Figure S4 in the SI). The reaction of lead
powder with sulfur powder in ethylene glycol also yielded PbS
(with unreacted lead and sulfur) as deduced from its PXRD
pattern (Figure S4 in the SI). The reaction of selenium powder
with copper powder in ethylene glycol indicated few reflections
due to CuSe in its PXRD pattern (Figure S5 in the SI).
Copper (in powder form), having the native oxide layer, is
known to chemisorb multilayers of thiols.19
The preparation of
copper thiolates (containing aliphatic groups) has been
reported to be unsuccessful in most cases, and those prepared
in situ had very short lifetimes in solution.20,21
The fact that the
reactions in dimercaptoethane did not yield copper sulfide and
the reactions in 2-mercaptoethanol and ethylene glycol
produced crystalline copper and lead sulfides at room
temperature reinforces the existence of intriguing chemistry
involved in these reactions. Further investigations, such as the
detection of the real driving force for this redox reaction,
isolating the intermediates (generated if any) are required to
ascertain the plausible mechanism behind the formation of
metal chalcogenides using these solvents. Efforts in this
direction are in progress.
Scope of the Reaction. This work has provided a new
direction for synthetic chemists and elucidating the mechanism
of these reactions will be of fundamental importance.
Caution! Because thiols are toxic having stench, the reactions
must be conducted in the fume hood and in sealed flasks.
■ ASSOCIATED CONTENT
*S Supporting Information
Digital photograph of the progress of the reaction between
copper and sulfur in 2-mercaptoethanol at room temperature,
SEM-EDX analysis of CuSe, PXRD pattern of the product from
the unstirred reaction of copper and sulfur powders in 2-
mercaptoethanol and its SEM image, and PXRD patterns of the
product from the reaction of copper with sulfur, lead with
sulfur, and copper with selenium in ethylene glycol. This
material is available free of charge via the Internet at http://
pubs.acs.org.
■ AUTHOR INFORMATION
Corresponding Author
*E-mail: rnagarajan@chemistry.du.ac.in.
Notes
The authors declare no competing financial interest.
■ ACKNOWLEDGMENTS
The authors thank the University of Delhi for funding the
research. P.K. and M.G. thanks DST and CSIR, New Delhi,
India, for scholarship support. Constant academic support from
Dr. S. Uma is gratefully acknowledged.
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