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ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108
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Synthesis of 2-aminocyclopent-1-ene-1-carbodithioic acid (ACA)
Capped Silver nanoparticles, Characterisation and Fluorescence
application
M. Padma1*
, Ch.Madhu1
, R. Sarada2
, B. Venkateswara Rao1
*
1
*Department of Engineering Chemistry, College of Engineering, Andhra University, Visakhapatnam, India-
530003.
2
Department of Chemistry, ANITS College of Engineering, Sanghivalasa, Visakhapatnam, India-531162
ABSTRACT
The present work deals with the formation, morphology and photophysical activity of the 2-aminocyclopent-1-
ene-1-carbodithioic acid (ACA) Capped Silver nanoparticles via chemical reduction method. The method
utilizes a simple chemical reaction of silver idodide and sodium borohydride. The advantages of this method are
ease of preparation, convenience in use and especially, that the obtained silver nano particles are uniform in
their shapes and sizes. This is important for fluorescence & bio-evolution measurements. Furthermore, UV-
visible (UV-vis) spectroscopy is employed to monitor the formation process of the nano particles and to
determine the optimum conditions for the preparation of stable and highly fluorescence-active silver colloids.
Specifically, we observed changes in the shapes of the silver nano particles during the formation. This may be
helpful in understanding the growth of the nano particles and creates a new dimension in controlling the shapes
of the nano particles.SEM, TEM and XRD studies are carried out. The suitability of ACA capped Ag-NPs as
Biomarkers is also Tested by Fluorescence study.
Key words – Biomarkers, Capped Silver Nanoparticles, Chemical Reduction, Fluorescence.
I. INTRODUCTION
Recently, fluorescent nanoparticles, have
attracted much attention for a variety of purposes and
applications in biology and medicine, for example, in
immuno-labeling,1
as cell markers,2
in cell motility
assays,3
in biological assembly,4
and especially in
optical imaging agents,5
due to their photostability
and other excellent optical properties. Due to the
urgent need of environmentally-friendly fluorescent
nanoparticles, the emerging carbon dots (CDs) appear
to be a promising alternative to semiconductor QDs
in many applications such as bioimaging, disease
detection, and drug delivery 6
because of their
superiority in chemical inertness, biocompatibility,
low toxicity, cheaper cost and promising
upconversion property.7
However, the fluorescent intensity of Carbon
Dots is relatively low in most reports,8
but metal
(such as gold or silver) has an enhanced effect on the
fluorophore, as known as metal-enhanced
fluorescence (MEF).9
It is well established that the
interactions of fluorophores with silver nano particles
results in an increased photostability, fluorescence
enhancement, and a decreased lifetime due to
increased rates of system radioactive decay.10
The
fluorescence enhancement noted in these studies can
stem from a mechanism of surface Plasmon
resonance.11
Excellent overlap of the CDs
absorption/emission spectrum with the scattering
spectrum of the silver surface is required for effective
surface plasmon resonance, while CDs show a broad
absorption and emission spectrum, which provides a
good overlap with the silver scattering spectrum.12
The spontaneous emission of light by molecules
and atoms at nano structured metallic surfaces is
remarkably modified due to a complex interplay of
enhancing and quenching physicochemical processes.
Fluorescence enhancement can be promoted by
surface plasmons excited in metal and by a modified
density of photon states in a nano structured
surface,13
while quenching processes include
chemical bonding and non radiative energy transfer
from the luminescent species to the metal.
Importantly, the degree of metal-fluorophore
interactions strongly depends on the distance between
the fluorophore and the metal surface.
In the present study, ACA Capped Ag-NPs are
prepared by a simple, direct chemical Reduction
Method and is Tested for its suitability as Biomarker
by studying Florescence Emission Spectra of the
prepared Ag-NPs.
II. Materials & Methods
2.1 Chemicals & Instruments Used
All the reagents used were of AR grade. Silver
nitrate was obtained from National Refinery Pvt. Ltd,
and a 0.1 M aqueous solution was used as stock
solution. Sodium borohydroxide was obtained from
RESEARCH ARTICLE OPEN ACCESS
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ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108
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Merck, India. Organic-free water was used
throughout the experiment.
2-aminocyclopent-1-ene-1-carbodithioic acid
(ACA)
The UV-visible spectra were recorded on a
Schimadzu UV-vis spectrophotometer, and the
solutions were taken in a 1 cm well-stopper quartz
cuvette. Fourier transform infrared (FTIR) spectral
characteristics of the samples were collected on a
Schimadzu FTIR spectrometer with the samples as
KBr pellets. The FTIR spectrum was recorded over
45 scans of each sample, and the background
spectrum was automatically subtracted. The
formation of single-phase compound was checked by
X-ray diffraction (XRD) technique. The XRD pattern
was taken with X-ray diffractometer (XPERT-PRO)
at room temperature, using CuKα radiation λ=1.5406
A˚ over a wide range of Bragg angles (300
≤ 2θ ≤
850
). SEM micrograph of ACA capped Ag-NP was
obtained at 20 K data was obtained on a F20 Tecnai
High Resolution microscope (Philips, Netherlands).
For SEM analysis, the specimen was suspended in
distilled water, dispersed ultrasonically to separate
individual particles, and one or two drop of the
suspension deposited onto holey-carbon coated
copper grids and dried under Infrared lamp.
Fluorescence spectra were measured on a Schimadzu
spectrofluorometer. The optical path was 1 cm and
spectra were collected at a resolution of five data
points per nanometer. When recording fluorescence
spectra the total absorption in no case exceeded 0.06,
making the necessary correction for the inner filter
effect small.
2.2 Synthesis of 2-aminocyclopent-1-ene-1-
carbodithioic acid (ACA):
Cyclopentanone (25.02g) was mixed with 27.5
ml carbon disulfide in 100 ml concentrated
ammonium hydroxide (28% solution) in a 250-ml
flask. The mixture was stirred at 00
C in an ice bath
for 6 h (scheme-1). A yellow precipitate gradually
falls out of the solution. The crude product was
recrystalized from ethanol. That was ammonium salt
from the dithio acid and was fairly unstable. Thus,
the salt was collected by suction filtration and was
immediately dissolved in about 200 ml of water.
Then, with vigorous stirring, 2M HCl was added until
the pH reached 4-5. A yellow precipitate would be
formed. That was the free dithioacid. The free acid
was collected by suction filtration and was washed
several times with water and was dried. This
procedure was done according to the earlier
recommended report 14
. The crystals were
recrystalized from ethanol. The IR spectra showed
(KBr disk method) 3450, 1618, 1605, 1470, 1450,
1425.The NMR spectra showed (in DMSO) δ
10.7(m, NH), 9.0(s, SH), 3.40(t, C-1 H), 2.95(t, C-5
H2), 2.72 (t, C-3 H2), 1.85(m, C-4 H2) which are in
agreement with the earlier reported procedure.
2.3 Synthesis of ACA Capped Silver Nano
particle Assembly:
A total of 2.5 mL of 10-2
M AgNO3 was added to
75 mL of triply distilled organic-free water. A total of
5 mL of 10-2
M 2-aminocyclopent-1-ene-1-
carbodithioic acid (dissolved in hot water) was added
as stabilizer to the solution with stirring. After 10 min
of mixing, 2.5 mL of 10-2
M Sodium Iodide (NaI)
was dropped into the solution slowly, yielding a
green yellow AgI colloid. A total of 20 mg of NaBH4
was added to the AgI colloidal solution, and the
reaction mixture was continually stirred for about 20
min. The silver colloid was finally obtained. During
the whole reaction, the color of the colloidal solution
changed from yellow to brown at the beginning, then
finally to black.
2.4 Results and discussion
Evolution and Characterization of Silver Nano
particle Aggregates:
UV–vis spectroscopy Study:
The aggregates of silver nano particles have been
synthesized using silver nitrate as the precursor salt
and ACA as the capping agent. The successive
changes of the absorption spectra of synthesized
silver nano particles aggregates are shown in Figure
1. After the addition of AgNO3 to the sodium iodide
solution, the color of the solution changes from
colorless to light yellow indicates the nucleation of
the silver particles at their infancy. The UV
absorption measurements of the synthesized nano
particles were further studied by dissolving in solvent
DMSO.
“Fig” 1 shows the UV-vis spectra of silver
colloids obtained. The surface Plasmon resonance
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(SPR) band is broad indicating poly-dispersed nano
particles. A smooth and narrow absorption, a band at
421 nm is observed in DMSO solvent of ACA
capped Ag-NP by above procedure, whereas 390 nm
is observed for ACA in DMSO which clearly
indicates the formation of silver colloids. UV-visible
spectroscopy is one of the most widely used
techniques for structural characterization of silver
nano particles. The optical absorption spectra of
metal nano particles are dominated by surface
plasmon resonances (SPR), which shift to longer
wavelengths with increasing particle size. The
position and shape of plasmon absorption of silver
nano clusters are strongly dependent on the particle
size, dielectric medium, and surface-adsorbed
species. The surface plasmon absorption of silver
nano particles have the short wavelength band in the
visible region around 409 nm is due to the transverse
electronic oscillation.
Fig. 1. UV–vis absorbance spectra of 2-
aminocyclopent-1-ene-1-carbodithioic acid capped
AgNP in DMSO.
2.5 Scanning electron microscopy study:
The SEM images obtained for colloid is shown
in “Fig.” 2. It is clear from the SEM images in Fig. 2,
that the particles are nearly crystalline spherical
particles respectively.
The Scherrer rings, characteristic of fcc silver is
clearly observed, showing that the structure seen in
the SEM image are nano crystalline in nature. It is
observed that the silver nano particles are scattered
over the surface and no aggregates are noticed under
SEM. The difference in size is possibly due to the
fact that the nano particles are being formed at
different times.
The TEM images obtained for colloid is shown
in Fig.3. It is clear from the TEM images that the
particle size, nearly spherical particles of average size
6.5 nm is obtained. The typical high resolution TEM
image (Fig.3a) confirms the particles are spherical in
shape.
The Scherrer rings, characteristic of fcc silver is
clearly observed, showing that the structure seen in
the TEM image are nano crystalline in nature. It is
observed that the silver nanoparticles are scattered
over the surface and no aggregates are noticed under
TEM. The difference in size is possibly due to the
fact that the nanoparticles are being formed at
different times.
Fig 2: SEM images of 2-aminocyclopent-1-ene-1-carbodithioic acid onto a surface of silver Nanoparticles
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Figure 3: Transmission electron micrographs of the silver nanoparticles used in this work. (a) The bar marker
represents 20 nm, (b) 5 nm
2.6. X-ray diffraction study:
The XRD spectrum confirms the tendency of
nano particles to form the organized structures, as
seen from the peaks in the small angle XRD spectrum
in “Fig.”4. The peaks are broadened because of the
nano crystalline nature of silver nanoparticles. By
comparing with standard database values, all the
peaks can be indexed to face-centered cubic (fcc)
silver crystal structure. Three peaks at 2y values of
37.99, 62.843 and 75.462, correspond to the (1 1 1),
(2 0 0) and (2 2 0) planes of silver nanoparticle,
respectively.
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The XRD of different particle sizes of Ag-NPs
capped with 2-aminocyclopent-1-ene-1-carbodithioic
acid prepared in water as solvent. From this figure, it
can be noticed that the particles appeared basically
amorphous and abroad. Size-dependent and structure-
specific features in diffraction patterns can be quite
striking in nano meter-sized particles. Small particles
have fairly distinct diffraction patterns, both as a
function of size and as a function of structure type. In
general, regardless of structure, there is a steady
evolution in the aspect of diffraction profiles: as
particles become larger, abrupt changes do not occur,
features grow continuously from the diffraction
profile and more details are resolved. These
observations form the basis for a direct technique of
diffraction pattern analysis that can be used to obtain
structural information from experimental diffraction
data. The Ag-NPs are almost crystallized with the
appearance of diffraction peaks at the scattering
angles (2y) at 37-39, which could be indexed to the
scattering from the planes (111), (200), (220) and
(311), respectively, which is in agreement with the
results of Leff et al. 15
. It is well known that with
diminishing crystallite size the measured XRD
pattern exhibits broadening, and very often
overlapping reflections. The broadening of the
reflections is inversely proportional to the crystallite
size (i.e. size of coherently diffracting domains). The
relation is known as Scherrer‟s equation where “y” is
the diffraction angle of a particular reflection. The
total diffracted intensity for a given Bragg reflection
from a crystallite is the sum of independently
diffracted intensities by each of the unit-cell columns
making-up the crystallite. It means that the calculated
size distribution is in fact a distribution of diffraction
column lengths in a given crystallographic direction
perpendicular to the diffraction planes and not of
crystallite (coherently diffracting domains) sizes.
Theoretical considerations show that the interference
function of a polycrystalline or nano crystalline solid
is identical to that of an arrangement of isolated
particles with the same size or size distribution as
those of the polycrystalline or nano crystalline solid
16,17
. Thus the values of Scherrer‟s formula are solely
an estimate of a volume-weighed average column
length. This explains the difference between the
experimental and theoretical values, and the values
from the Scherrer‟s formula is termed „„apparent
crystallite size‟‟ 18
.
“Fig.” 4: XRD patterns 2-aminocyclopent-1-ene-1-carbodithioic acid capped silver nanoparticles.
2.7 FT-IR analysis:
The IR spectra of the free 2-aminocyclopent-1-
ene-1-carbodithioic acid and the particles capped by
2-aminocyclopent-1-ene-1-carbodithioic acid are
given in Fig. 5. The IR spectra of the nano particles
and the free 2-aminocyclopent-1-ene-1-carbodithioic
acid molecule are similar to one another, indicating
that the organic molecules have indeed become a part
of the nano particles. However, are markable
difference in the peak intensity is found between the
peaks of IR spectra of free 2-aminocyclopent-1-ene-
1-carbodithioic acid and 2-aminocyclopent-1-ene-1-
carbodithioic acid capped Ag-NP in “Fig.”5. The
reason for the intensity difference between the
spectra is believed to be the thiolate molecules on the
nano particle forming a relatively closely packed
thiol layer and molecular motion being constrained 19
.
Thus, this steric constraining effect on the
transverse mode (rocking mode, wagging mode, etc.)
is stronger than that on the longitudinal mode
(stretching mode, etc). Therefore, the change of the
peak intensity of the longitudinal modes is smaller
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than that of the transverse mode. The C–S stretching
mode is due to the position of the C–S bond nearest
to the surface of the silver particle, and a chemical
bond can form between S and Ag atoms.
The FTIR spectrum of the nano crystals provides
additional information about the local molecular
environment of 2-aminocyclopent-1-ene-1-
carbodithioic acid. The FTIR spectra of the free 2-
aminocyclopent-1-ene-1-carbodithioic acid and Ag
nanoparticle capped by 2-aminocyclopent-1-ene-1-
carbodithioic acid thiol are represented in Fig. 4.
From the spectrum of free 2-aminocyclopent-1-ene-
1-carbodithioic acid thiol, it can be noticed that the
azo group appeared at 1580 – 1650 cm-1
,
respectively. The weak band appeared at 2360 cm-1
is
attributed to the S–H stretching vibration
mode7
. The two bands appeared between 1380 and
1240 cm-1
are assigned to the stretching vibration of
C-N group. The band appeared at 1627 - 1690 cm_1
is
attributed to the N-H primary stretching group. The
band appeared at 756 cm-1
is assigned to C–S
stretching mode 20
. Generally, the vibrational
spectrum of Ag-NPs capped with 2-aminocyclopent-
1-ene-1-carbodithioic acid thiol molecule is similar to
the spectrum of 2-aminocyclopent-1-ene-1-
carbodithioic acid thiol indicating that, the organic
molecules have indeed become a part of the
nanoparticles.
However, there is a remarkable difference in the
peak intensity found between the peaks of the
transverse mode (rocking mode, bending mode, etc.)
in 2-aminocyclopent-1-ene-1-carbodithioic acid and
Ag nanoparticles capped by 2-aminocyclopent-1-ene-
1-carbodithioic acid. The reason for the intensity
difference between the spectras is believed to be that
the thiolate molecules on the nanoparticle form are
relatively close packed thiol layer and molecular
motion is constrained 21
. Thus, this steric constraining
effect on the transverse mode is stronger than that on
the longitudinal mode. Therefore, the change of the
peak intensity of the longitudinal modes is smaller
than that of the transverse mode. The small peak at
2360 cm-1
which corresponds to the S–H stretching
vibration mode, disappears when the 2-
aminocyclopent-1-ene-1-carbodithioic acid
molecules adsorb on the silver particle surface
(comparing spectra of free 2-aminocyclopent-1-ene-
1-carbodithioic acid (4a) and Ag-NP capped by 2-
aminocyclopent-1-ene-1-carbodithioic acid (4b),
giving strong evidence that 2-aminocyclopent-1-ene-
1-carbodithioic acid anchors on the silver surface
through the sulfur atom in the mercapto group 22
.
“Fig.” 5. FT-IR spectra of (a) 2-aminocyclopent-1-ene-1-carbodithioic acid; (b) 2-aminocyclopent-1-ene-1-
carbodithioic acid capped AgNP;
III. Photophysical properties of the new
ACA capped AgNPs:
3.1 Fluorescence emission spectra measurement:
The above synthesized 2-aminocyclopent-1-ene-
1-carbodithioic acid capped Ag-NP (0.1mmoles) is
dissolved in solvent DMSO to study their
photoluminescence activity. “Fig” 6 shows the
luminescence of 2-aminocyclopent-1-ene-1-
carbodithioic acid (Left) & Ag-NP (Right) in DMSO
at (a) daylight and (b) UV-lamp of 254 nm
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excitations respectively. Basing on this reference the
fluorescence studies were carried to our synthesized
silver nanomaterials. “Fig.” 7 and 8 shows the
fluorescence emission spectra for synthesized silver
nanoparticles. The emission spectra were recorded
for these systems, in which fluorescence excitation
wavelength was fixed.
Silver nanoparticles in DMSO showed
fluorescence emissions at 522 nm. Whereas 2-
aminocyclopent-1-ene-1-carbodithioic acid in DMSO
showed 479 nm emission which is little bit lesser
than the synthesized nanoparticles. From absorption
and emission spectra‟s the stokes shifts observed as
58nm. The detailed description with Stokes shifts
were presented in table-4.
“Fig.” 6. Emission colors of fluorescent 2-aminocyclopent-1-ene-1-carbodithioic acid capped Ag-NP
nanoclusters excited with a UV lamp (Left - In day light; Right – In UV lamp@254 nm) in DMSO solvent.
Fig. 7 & 8: Fluorescence spectra‟s exhibited by 2-aminocyclopent-1-ene-1-carbodithioic acid & synthesized
Ag-NP‟s in DMSO solvent.
Table 5.5: Photophysical Data of 2-
aminocyclopent-1-ene-1-carbodithioic acid (ACA)
Capped AgNP’s:
IV. CONCLUSION
ACA capped Ag-Nps are prepared by a simple,
direct method. The progress of the reaction is
observed through UV- Visible Spectrophotometric
Studies. The Size & shape of nanoparticles are
studied through SEM, TEM and XRD. From the
study of Fluorescence spectra exhibited by 2-
aminocyclopent-1-ene-1-carbodithioic acid &
synthesized Ag-NP‟s in DMSO solvent, it is clearly
evident that these ACA Capped Ag-NPs are suitable
biomarkers.
Sl.
no
Sample Excitation
wavelengt
h
(nm)
Emission
wavelengt
h (nm)
Stocks
shift (nm)
1 ACA 421 479 58
2 ACA-Ag-
NP
452 522 70
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V. Acknowledgements
Authors are grateful to Andhra University,
Visakhapatnam, India for support in Advanced
Analytical Laboratories, a National facility, Andhra
University for providing XRD & SEM.
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Synthesis of 2-aminocyclopent-1-ene-1-carbodithioic acid (ACA) Capped Silver nanoparticles, Characterisation and Fluorescence application

  • 1. M. Padma et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108 www.ijera.com 100 | P a g e Synthesis of 2-aminocyclopent-1-ene-1-carbodithioic acid (ACA) Capped Silver nanoparticles, Characterisation and Fluorescence application M. Padma1* , Ch.Madhu1 , R. Sarada2 , B. Venkateswara Rao1 * 1 *Department of Engineering Chemistry, College of Engineering, Andhra University, Visakhapatnam, India- 530003. 2 Department of Chemistry, ANITS College of Engineering, Sanghivalasa, Visakhapatnam, India-531162 ABSTRACT The present work deals with the formation, morphology and photophysical activity of the 2-aminocyclopent-1- ene-1-carbodithioic acid (ACA) Capped Silver nanoparticles via chemical reduction method. The method utilizes a simple chemical reaction of silver idodide and sodium borohydride. The advantages of this method are ease of preparation, convenience in use and especially, that the obtained silver nano particles are uniform in their shapes and sizes. This is important for fluorescence & bio-evolution measurements. Furthermore, UV- visible (UV-vis) spectroscopy is employed to monitor the formation process of the nano particles and to determine the optimum conditions for the preparation of stable and highly fluorescence-active silver colloids. Specifically, we observed changes in the shapes of the silver nano particles during the formation. This may be helpful in understanding the growth of the nano particles and creates a new dimension in controlling the shapes of the nano particles.SEM, TEM and XRD studies are carried out. The suitability of ACA capped Ag-NPs as Biomarkers is also Tested by Fluorescence study. Key words – Biomarkers, Capped Silver Nanoparticles, Chemical Reduction, Fluorescence. I. INTRODUCTION Recently, fluorescent nanoparticles, have attracted much attention for a variety of purposes and applications in biology and medicine, for example, in immuno-labeling,1 as cell markers,2 in cell motility assays,3 in biological assembly,4 and especially in optical imaging agents,5 due to their photostability and other excellent optical properties. Due to the urgent need of environmentally-friendly fluorescent nanoparticles, the emerging carbon dots (CDs) appear to be a promising alternative to semiconductor QDs in many applications such as bioimaging, disease detection, and drug delivery 6 because of their superiority in chemical inertness, biocompatibility, low toxicity, cheaper cost and promising upconversion property.7 However, the fluorescent intensity of Carbon Dots is relatively low in most reports,8 but metal (such as gold or silver) has an enhanced effect on the fluorophore, as known as metal-enhanced fluorescence (MEF).9 It is well established that the interactions of fluorophores with silver nano particles results in an increased photostability, fluorescence enhancement, and a decreased lifetime due to increased rates of system radioactive decay.10 The fluorescence enhancement noted in these studies can stem from a mechanism of surface Plasmon resonance.11 Excellent overlap of the CDs absorption/emission spectrum with the scattering spectrum of the silver surface is required for effective surface plasmon resonance, while CDs show a broad absorption and emission spectrum, which provides a good overlap with the silver scattering spectrum.12 The spontaneous emission of light by molecules and atoms at nano structured metallic surfaces is remarkably modified due to a complex interplay of enhancing and quenching physicochemical processes. Fluorescence enhancement can be promoted by surface plasmons excited in metal and by a modified density of photon states in a nano structured surface,13 while quenching processes include chemical bonding and non radiative energy transfer from the luminescent species to the metal. Importantly, the degree of metal-fluorophore interactions strongly depends on the distance between the fluorophore and the metal surface. In the present study, ACA Capped Ag-NPs are prepared by a simple, direct chemical Reduction Method and is Tested for its suitability as Biomarker by studying Florescence Emission Spectra of the prepared Ag-NPs. II. Materials & Methods 2.1 Chemicals & Instruments Used All the reagents used were of AR grade. Silver nitrate was obtained from National Refinery Pvt. Ltd, and a 0.1 M aqueous solution was used as stock solution. Sodium borohydroxide was obtained from RESEARCH ARTICLE OPEN ACCESS
  • 2. M. Padma et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108 www.ijera.com 101 | P a g e Merck, India. Organic-free water was used throughout the experiment. 2-aminocyclopent-1-ene-1-carbodithioic acid (ACA) The UV-visible spectra were recorded on a Schimadzu UV-vis spectrophotometer, and the solutions were taken in a 1 cm well-stopper quartz cuvette. Fourier transform infrared (FTIR) spectral characteristics of the samples were collected on a Schimadzu FTIR spectrometer with the samples as KBr pellets. The FTIR spectrum was recorded over 45 scans of each sample, and the background spectrum was automatically subtracted. The formation of single-phase compound was checked by X-ray diffraction (XRD) technique. The XRD pattern was taken with X-ray diffractometer (XPERT-PRO) at room temperature, using CuKα radiation λ=1.5406 A˚ over a wide range of Bragg angles (300 ≤ 2θ ≤ 850 ). SEM micrograph of ACA capped Ag-NP was obtained at 20 K data was obtained on a F20 Tecnai High Resolution microscope (Philips, Netherlands). For SEM analysis, the specimen was suspended in distilled water, dispersed ultrasonically to separate individual particles, and one or two drop of the suspension deposited onto holey-carbon coated copper grids and dried under Infrared lamp. Fluorescence spectra were measured on a Schimadzu spectrofluorometer. The optical path was 1 cm and spectra were collected at a resolution of five data points per nanometer. When recording fluorescence spectra the total absorption in no case exceeded 0.06, making the necessary correction for the inner filter effect small. 2.2 Synthesis of 2-aminocyclopent-1-ene-1- carbodithioic acid (ACA): Cyclopentanone (25.02g) was mixed with 27.5 ml carbon disulfide in 100 ml concentrated ammonium hydroxide (28% solution) in a 250-ml flask. The mixture was stirred at 00 C in an ice bath for 6 h (scheme-1). A yellow precipitate gradually falls out of the solution. The crude product was recrystalized from ethanol. That was ammonium salt from the dithio acid and was fairly unstable. Thus, the salt was collected by suction filtration and was immediately dissolved in about 200 ml of water. Then, with vigorous stirring, 2M HCl was added until the pH reached 4-5. A yellow precipitate would be formed. That was the free dithioacid. The free acid was collected by suction filtration and was washed several times with water and was dried. This procedure was done according to the earlier recommended report 14 . The crystals were recrystalized from ethanol. The IR spectra showed (KBr disk method) 3450, 1618, 1605, 1470, 1450, 1425.The NMR spectra showed (in DMSO) δ 10.7(m, NH), 9.0(s, SH), 3.40(t, C-1 H), 2.95(t, C-5 H2), 2.72 (t, C-3 H2), 1.85(m, C-4 H2) which are in agreement with the earlier reported procedure. 2.3 Synthesis of ACA Capped Silver Nano particle Assembly: A total of 2.5 mL of 10-2 M AgNO3 was added to 75 mL of triply distilled organic-free water. A total of 5 mL of 10-2 M 2-aminocyclopent-1-ene-1- carbodithioic acid (dissolved in hot water) was added as stabilizer to the solution with stirring. After 10 min of mixing, 2.5 mL of 10-2 M Sodium Iodide (NaI) was dropped into the solution slowly, yielding a green yellow AgI colloid. A total of 20 mg of NaBH4 was added to the AgI colloidal solution, and the reaction mixture was continually stirred for about 20 min. The silver colloid was finally obtained. During the whole reaction, the color of the colloidal solution changed from yellow to brown at the beginning, then finally to black. 2.4 Results and discussion Evolution and Characterization of Silver Nano particle Aggregates: UV–vis spectroscopy Study: The aggregates of silver nano particles have been synthesized using silver nitrate as the precursor salt and ACA as the capping agent. The successive changes of the absorption spectra of synthesized silver nano particles aggregates are shown in Figure 1. After the addition of AgNO3 to the sodium iodide solution, the color of the solution changes from colorless to light yellow indicates the nucleation of the silver particles at their infancy. The UV absorption measurements of the synthesized nano particles were further studied by dissolving in solvent DMSO. “Fig” 1 shows the UV-vis spectra of silver colloids obtained. The surface Plasmon resonance
  • 3. M. Padma et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108 www.ijera.com 102 | P a g e (SPR) band is broad indicating poly-dispersed nano particles. A smooth and narrow absorption, a band at 421 nm is observed in DMSO solvent of ACA capped Ag-NP by above procedure, whereas 390 nm is observed for ACA in DMSO which clearly indicates the formation of silver colloids. UV-visible spectroscopy is one of the most widely used techniques for structural characterization of silver nano particles. The optical absorption spectra of metal nano particles are dominated by surface plasmon resonances (SPR), which shift to longer wavelengths with increasing particle size. The position and shape of plasmon absorption of silver nano clusters are strongly dependent on the particle size, dielectric medium, and surface-adsorbed species. The surface plasmon absorption of silver nano particles have the short wavelength band in the visible region around 409 nm is due to the transverse electronic oscillation. Fig. 1. UV–vis absorbance spectra of 2- aminocyclopent-1-ene-1-carbodithioic acid capped AgNP in DMSO. 2.5 Scanning electron microscopy study: The SEM images obtained for colloid is shown in “Fig.” 2. It is clear from the SEM images in Fig. 2, that the particles are nearly crystalline spherical particles respectively. The Scherrer rings, characteristic of fcc silver is clearly observed, showing that the structure seen in the SEM image are nano crystalline in nature. It is observed that the silver nano particles are scattered over the surface and no aggregates are noticed under SEM. The difference in size is possibly due to the fact that the nano particles are being formed at different times. The TEM images obtained for colloid is shown in Fig.3. It is clear from the TEM images that the particle size, nearly spherical particles of average size 6.5 nm is obtained. The typical high resolution TEM image (Fig.3a) confirms the particles are spherical in shape. The Scherrer rings, characteristic of fcc silver is clearly observed, showing that the structure seen in the TEM image are nano crystalline in nature. It is observed that the silver nanoparticles are scattered over the surface and no aggregates are noticed under TEM. The difference in size is possibly due to the fact that the nanoparticles are being formed at different times. Fig 2: SEM images of 2-aminocyclopent-1-ene-1-carbodithioic acid onto a surface of silver Nanoparticles
  • 4. M. Padma et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108 www.ijera.com 103 | P a g e Figure 3: Transmission electron micrographs of the silver nanoparticles used in this work. (a) The bar marker represents 20 nm, (b) 5 nm 2.6. X-ray diffraction study: The XRD spectrum confirms the tendency of nano particles to form the organized structures, as seen from the peaks in the small angle XRD spectrum in “Fig.”4. The peaks are broadened because of the nano crystalline nature of silver nanoparticles. By comparing with standard database values, all the peaks can be indexed to face-centered cubic (fcc) silver crystal structure. Three peaks at 2y values of 37.99, 62.843 and 75.462, correspond to the (1 1 1), (2 0 0) and (2 2 0) planes of silver nanoparticle, respectively.
  • 5. M. Padma et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108 www.ijera.com 104 | P a g e The XRD of different particle sizes of Ag-NPs capped with 2-aminocyclopent-1-ene-1-carbodithioic acid prepared in water as solvent. From this figure, it can be noticed that the particles appeared basically amorphous and abroad. Size-dependent and structure- specific features in diffraction patterns can be quite striking in nano meter-sized particles. Small particles have fairly distinct diffraction patterns, both as a function of size and as a function of structure type. In general, regardless of structure, there is a steady evolution in the aspect of diffraction profiles: as particles become larger, abrupt changes do not occur, features grow continuously from the diffraction profile and more details are resolved. These observations form the basis for a direct technique of diffraction pattern analysis that can be used to obtain structural information from experimental diffraction data. The Ag-NPs are almost crystallized with the appearance of diffraction peaks at the scattering angles (2y) at 37-39, which could be indexed to the scattering from the planes (111), (200), (220) and (311), respectively, which is in agreement with the results of Leff et al. 15 . It is well known that with diminishing crystallite size the measured XRD pattern exhibits broadening, and very often overlapping reflections. The broadening of the reflections is inversely proportional to the crystallite size (i.e. size of coherently diffracting domains). The relation is known as Scherrer‟s equation where “y” is the diffraction angle of a particular reflection. The total diffracted intensity for a given Bragg reflection from a crystallite is the sum of independently diffracted intensities by each of the unit-cell columns making-up the crystallite. It means that the calculated size distribution is in fact a distribution of diffraction column lengths in a given crystallographic direction perpendicular to the diffraction planes and not of crystallite (coherently diffracting domains) sizes. Theoretical considerations show that the interference function of a polycrystalline or nano crystalline solid is identical to that of an arrangement of isolated particles with the same size or size distribution as those of the polycrystalline or nano crystalline solid 16,17 . Thus the values of Scherrer‟s formula are solely an estimate of a volume-weighed average column length. This explains the difference between the experimental and theoretical values, and the values from the Scherrer‟s formula is termed „„apparent crystallite size‟‟ 18 . “Fig.” 4: XRD patterns 2-aminocyclopent-1-ene-1-carbodithioic acid capped silver nanoparticles. 2.7 FT-IR analysis: The IR spectra of the free 2-aminocyclopent-1- ene-1-carbodithioic acid and the particles capped by 2-aminocyclopent-1-ene-1-carbodithioic acid are given in Fig. 5. The IR spectra of the nano particles and the free 2-aminocyclopent-1-ene-1-carbodithioic acid molecule are similar to one another, indicating that the organic molecules have indeed become a part of the nano particles. However, are markable difference in the peak intensity is found between the peaks of IR spectra of free 2-aminocyclopent-1-ene- 1-carbodithioic acid and 2-aminocyclopent-1-ene-1- carbodithioic acid capped Ag-NP in “Fig.”5. The reason for the intensity difference between the spectra is believed to be the thiolate molecules on the nano particle forming a relatively closely packed thiol layer and molecular motion being constrained 19 . Thus, this steric constraining effect on the transverse mode (rocking mode, wagging mode, etc.) is stronger than that on the longitudinal mode (stretching mode, etc). Therefore, the change of the peak intensity of the longitudinal modes is smaller
  • 6. M. Padma et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108 www.ijera.com 105 | P a g e than that of the transverse mode. The C–S stretching mode is due to the position of the C–S bond nearest to the surface of the silver particle, and a chemical bond can form between S and Ag atoms. The FTIR spectrum of the nano crystals provides additional information about the local molecular environment of 2-aminocyclopent-1-ene-1- carbodithioic acid. The FTIR spectra of the free 2- aminocyclopent-1-ene-1-carbodithioic acid and Ag nanoparticle capped by 2-aminocyclopent-1-ene-1- carbodithioic acid thiol are represented in Fig. 4. From the spectrum of free 2-aminocyclopent-1-ene- 1-carbodithioic acid thiol, it can be noticed that the azo group appeared at 1580 – 1650 cm-1 , respectively. The weak band appeared at 2360 cm-1 is attributed to the S–H stretching vibration mode7 . The two bands appeared between 1380 and 1240 cm-1 are assigned to the stretching vibration of C-N group. The band appeared at 1627 - 1690 cm_1 is attributed to the N-H primary stretching group. The band appeared at 756 cm-1 is assigned to C–S stretching mode 20 . Generally, the vibrational spectrum of Ag-NPs capped with 2-aminocyclopent- 1-ene-1-carbodithioic acid thiol molecule is similar to the spectrum of 2-aminocyclopent-1-ene-1- carbodithioic acid thiol indicating that, the organic molecules have indeed become a part of the nanoparticles. However, there is a remarkable difference in the peak intensity found between the peaks of the transverse mode (rocking mode, bending mode, etc.) in 2-aminocyclopent-1-ene-1-carbodithioic acid and Ag nanoparticles capped by 2-aminocyclopent-1-ene- 1-carbodithioic acid. The reason for the intensity difference between the spectras is believed to be that the thiolate molecules on the nanoparticle form are relatively close packed thiol layer and molecular motion is constrained 21 . Thus, this steric constraining effect on the transverse mode is stronger than that on the longitudinal mode. Therefore, the change of the peak intensity of the longitudinal modes is smaller than that of the transverse mode. The small peak at 2360 cm-1 which corresponds to the S–H stretching vibration mode, disappears when the 2- aminocyclopent-1-ene-1-carbodithioic acid molecules adsorb on the silver particle surface (comparing spectra of free 2-aminocyclopent-1-ene- 1-carbodithioic acid (4a) and Ag-NP capped by 2- aminocyclopent-1-ene-1-carbodithioic acid (4b), giving strong evidence that 2-aminocyclopent-1-ene- 1-carbodithioic acid anchors on the silver surface through the sulfur atom in the mercapto group 22 . “Fig.” 5. FT-IR spectra of (a) 2-aminocyclopent-1-ene-1-carbodithioic acid; (b) 2-aminocyclopent-1-ene-1- carbodithioic acid capped AgNP; III. Photophysical properties of the new ACA capped AgNPs: 3.1 Fluorescence emission spectra measurement: The above synthesized 2-aminocyclopent-1-ene- 1-carbodithioic acid capped Ag-NP (0.1mmoles) is dissolved in solvent DMSO to study their photoluminescence activity. “Fig” 6 shows the luminescence of 2-aminocyclopent-1-ene-1- carbodithioic acid (Left) & Ag-NP (Right) in DMSO at (a) daylight and (b) UV-lamp of 254 nm
  • 7. M. Padma et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108 www.ijera.com 106 | P a g e excitations respectively. Basing on this reference the fluorescence studies were carried to our synthesized silver nanomaterials. “Fig.” 7 and 8 shows the fluorescence emission spectra for synthesized silver nanoparticles. The emission spectra were recorded for these systems, in which fluorescence excitation wavelength was fixed. Silver nanoparticles in DMSO showed fluorescence emissions at 522 nm. Whereas 2- aminocyclopent-1-ene-1-carbodithioic acid in DMSO showed 479 nm emission which is little bit lesser than the synthesized nanoparticles. From absorption and emission spectra‟s the stokes shifts observed as 58nm. The detailed description with Stokes shifts were presented in table-4. “Fig.” 6. Emission colors of fluorescent 2-aminocyclopent-1-ene-1-carbodithioic acid capped Ag-NP nanoclusters excited with a UV lamp (Left - In day light; Right – In UV lamp@254 nm) in DMSO solvent. Fig. 7 & 8: Fluorescence spectra‟s exhibited by 2-aminocyclopent-1-ene-1-carbodithioic acid & synthesized Ag-NP‟s in DMSO solvent. Table 5.5: Photophysical Data of 2- aminocyclopent-1-ene-1-carbodithioic acid (ACA) Capped AgNP’s: IV. CONCLUSION ACA capped Ag-Nps are prepared by a simple, direct method. The progress of the reaction is observed through UV- Visible Spectrophotometric Studies. The Size & shape of nanoparticles are studied through SEM, TEM and XRD. From the study of Fluorescence spectra exhibited by 2- aminocyclopent-1-ene-1-carbodithioic acid & synthesized Ag-NP‟s in DMSO solvent, it is clearly evident that these ACA Capped Ag-NPs are suitable biomarkers. Sl. no Sample Excitation wavelengt h (nm) Emission wavelengt h (nm) Stocks shift (nm) 1 ACA 421 479 58 2 ACA-Ag- NP 452 522 70
  • 8. M. Padma et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 2, ( Part -5) February 2015, pp.100-108 www.ijera.com 107 | P a g e V. Acknowledgements Authors are grateful to Andhra University, Visakhapatnam, India for support in Advanced Analytical Laboratories, a National facility, Andhra University for providing XRD & SEM. References: [1] F. Osaki, T. Kanamori, S. Sando, T. Sera, Y. A. Aoyagi, J. Am. Chem. Soc., 2004, 126, 6520. [2] H.Y. Xie,C. Zuo, Y. Liu,Z. L. Zhang, D.W. Pang,X.L.Li, J. P.Gong, C. Dickinson W. Zhou, Small, 2005, 1, 506. [3] W. J. Park, R. Boudreau, M. Le Gros, D. Gerion, D. Zanchet, C. M. Micheel, S. C. Williams, A. P. Alivisatos, C. Larabell, Adv. Mater., 2002, 14, 882. [4] Y. Wang, Z. Tang, S. Tan, N. A. Kotov, Nano Lett., 2005, 5, 243. [5] M. De, P. S. Ghosh, V. M. Rotello, Adv. Mater., 2008, 20, 4225. [6] L. Cao, X.Wang,M. J. Meziani, F. S. Lu, H. F.Wang, P. G. Luo, Y. Lin, B. A. Harruff, L. M. Veca, D. Murray, S. Y. Xie, Y. P. Sun, J. Am. Chem. Soc., 2007, 129, 11318. [7] (a). H. Zhu, X. Wang, Y. Li, Z. Wang, F. Yang, X. Yang, Chem. Commun., 2009, 5118. (b). S. -T. Yang, X. Wang, H. F. Wang, F. S. Lu, P. J.G. Luo, L. Cao, M. J. Meziani, J. -H. Liu, Y. F. Liu, M. Chen, Y. P. Huang and Y. -P. Sun, J. Phys. Chem. C, 2009, 113, 18110. (c). F. Zhang, G. B. Braun, Y. F. Shi, Y. C. Zhang, X. H. Sun, N. O. Reich, D. Y. Zhao, G. Stucky, J. Am. Chem. Soc., 2010, 132, 2850. [8] (a). A. B. Bourlinos, A. Stassinopoulos, D. Anglos, R. Zboril, M. Karakassides, E. P. Giannelis, Small, 2008, 4, 455. b. L. Tian, D. Ghosh, W. Chen, S. Pradhan, X. Chang, S. Chen, Chem. Mater., 2009, 21, 2803. [9] J.Yang, F. Zhang, Y. Chen, S.Qian, P. Hu,W. Li, Y. Deng,Y. Fang, L. Han, M. Luqman, D. Zhao, Chem. Commun., 2011, 47, 11618. [10] (a). K. Aslan, J. Huang, G. M. Wilson, C. D. Geddes, J. Am. Chem. Soc., 2006, 128, 4206. (b) K. Aslan, P. Holley, C.D.Geddes, J. Mater. Chem., 2006, 16, 2846. [11] C. D. Geddes, J. R. Lakowicz, J. Fluoresc., 2002, 12, 121. [12] [12].Y. Zhang, H. Goncalves, J. C. G. Esteves da Silva, C. D. Geddes, Chem. Commun., 2011, 47, 5313. [13] A. Vaseashta, D. Dimova-Malinovska, Sci. Technol. Adv. Mater, 2005, 6, 312. [14] Y. L. N. Murthy, B. Govindh, B. S. Diwakar,K. Nagalakshmi, E.R.singh, International Journal of Chem Tech Research, Coden( USA): IJCRGG ISSN: 0974-4290, 2011, 3, No.3, pp 1285-1291,. [15] D.V. Leff, Journal of Physical Chemistry, 1995, 99, 7036. [16] J.L¨ offler, J. Weissm¨ uller, Physical Review B,1995, 52, 7076. [17] L. Kundakovic, M.F. Stephanopoulos, Applied Catalysis A, 1999, 183, 35. [18] P. Knauth, J. Schoonman, Nanostructured Materials Selected Synthesis Methods, Properties and Applications, Kluwer Academic Publishers, Boston, 2002. [19] H. Shengtai, Y. Jiannian, J. Peng, S. Dongxia, Z. Haoxu, G.H. Jun, Langmuir, 2001, 17, 1571. [20] J.B. Lambert, H.F. Shurvell, D.A. Lightner, R.G. Cooks, Organic Structural Spectroscopy, Prentice Hall, New Jersey, 1998. [21] A. Miller, D.W. Mayo, R.W. Hannah, Course Notes on the Interpretation of Infrared and Raman Spectra: Deducing Structures of Complex Molecules, Wiley- IEEE, 2004. [22] B.A. Korgel, S. Fullam, S. Connolly, D. Fitzmaurice, Journal of Physical Chemistry B, 1998, 102, 8379. [23] F. Osaki, T. Kanamori, S. Sando, T. Sera, Y. A. Aoyagi, J. Am. Chem. Soc., 2004, 126, 6520. [24] H.Y. Xie,C. Zuo, Y. Liu,Z. L. Zhang, D.W. Pang,X.L.Li, J. P.Gong, C. Dickinson W. Zhou, Small, 2005, 1, 506. [25] W. J. Park, R. Boudreau, M. Le Gros, D. Gerion, D. Zanchet, C. M. Micheel, S. C. Williams, P. Alivisatos, C. Larabell, Adv. Mater., 2002, 14, 882. [26] Y. Wang, Z. Tang, S. Tan, N. A. Kotov, Nano Lett., 2005, 5, 243. [27] M. De, P. S. Ghosh, V. M. Rotello, Adv. Mater., 2008, 20, 4225. [28] L. Cao, X.Wang,M. J. Meziani, F. S. Lu, H. F.Wang, P. G. Luo, Y. Lin, B. A. Harruff, L. M. Veca, D. Murray, S. Y. Xie, Y. P. Sun, J. Am. Chem. Soc., 2007, 129, 11318. [29] (a) H. Zhu, X. Wang, Y. Li, Z. Wang, F. Yang, X. Yang, Chem. Commun., 2009, 5118. (b) S. -T. Yang, X. Wang, H. F. Wang, F. S. Lu, P. J.G. Luo, L. Cao, M. J. Meziani, J. -H. Liu, Y. F. Liu, M. Chen, Y. P. Huang and Y. -P. Sun, J. Phys. Chem. C, 2009, 113, 18110. (c) F. Zhang, G. B. Braun, Y. F. Shi, Y. C. Zhang, X. H. Sun, N. O. Reich, D. Y. Zhao, G. Stucky, J. Am. Chem. Soc., 2010, 132, 2850. [30] (a) A. B. Bourlinos, A. Stassinopoulos, D. Anglos, R. Zboril, M. Karakassides, E. P. Giannelis, Small, 2008, 4, 455. (b) L. Tian,
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