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BARC/2013/E/016 BARC/2013/E/016 2013 GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION by G.R. Dey Radiation & Photochemistry Division

GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION

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Page 1: GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION

BARC/2013/E/016BA

RC/2013/E/016

2013

GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION

by

G.R. DeyRadiation & Photochemistry Division

Page 2: GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION

BIBLIOGRAPHIC DESCRIPTION SHEET FOR TECHNICAL REPORT(as per IS : 9400 - 1980)

01 Security classification : Unclassified

02 Distribution : External

03 Report status : New

04 Series : BARC External

05 Report type : Technical Report

06 Report No. : BARC/2013/E/016

07 Part No. or Volume No. :

08 Contract No. :

10 Title and subtitle : Gold nanoparticles: generation and characterization

11 Collation : 26 p., 10 figs., 1 tab.

13 Project No. :

20 Personal author(s) : G..R. Dey

21 Affiliation of author(s) : Radiation and Photochemistry Division, Bhabha Atomic Research Centre, Mumbai

22 Corporate author(s) : Bhabha Atomic Research Centre, Mumbai - 400 085

23 Originating unit : Radiation and Photochemistry Division, BARC, Mumbai

24 Sponsor(s) Name : Department of Atomic Energy

Type : Government

Contd...

BARC/2013/E/016

Page 3: GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION

BARC/2013/E/016

30 Date of submission : June 2013

31 Publication/Issue date : July 2013

40 Publisher/Distributor : Head, Scientific Information Resource Division, Bhabha Atomic Research Centre, Mumbai

42 Form of distribution : Hard copy

50 Language of text : English

51 Language of summary : English, Hindi

52 No. of references : 35 refs.

53 Gives data on :

60

70 Keywords/Descriptors : NANOSTRUCTURES; GOLD; CITRIC ACID; RADIOLYSIS; PHVALUE; RADICALS; COBALT 60; STRONTIUM 90; PULSE TECHNIQUES

71 INIS Subject Category : S38

99 Supplementary elements :

Abstract : In this presentation we report the reduction of Au3+ through chemical and free radical (esolv

-)

reactions both in non-aqueous and aqueous media. In chemical reduction, the spectral nature in ascorbicacid (AA) and citric acid (CA) systems was different. The band intensity of gold nanoparticles was lower

in AA system. While in free radical reaction, the yield of nanoparticles was pure i.e. free from excessreactants. Under the study 60-200 nm size nanoparticles were generated, which are inert to oxygen. Using

pulse radiolysis technique, the initial rate for esolv

- reaction with Au3+ was determined to be 7.6 x 109 M-1

s-1.

Page 4: GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION

BARC/2013/E/016BA

RC/2

013/

E/01

6

GOVERNMENT OF INDIAATOMIC ENERGY COMMISSION

BHABHA ATOMIC RESEARCH CENTREMUMBAI, INDIA

2013

GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION

by

G.R. DeyRadiation & Photochemistry Division

Page 5: GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION

1

svaNa^ saUxmakNa kI ]%pi<a evaM vaOSaoiYakta

saaraMSa

[sa p`itpadna mao svaNa^ Aayana ka jalaIya tqaa inaja^laIya maaGyama maMo rsaayainak evaM f`I roizkola p`itik`yaa Wara

nyaUnaIkrNa ka ivavarNa ikyaa gayaa ho . rsaayainak irD@sana maoM eskaoribak eisaz tqaa saa[iT`k eisaz p`Naailayaao ka

vaNa^k`ma saMbaMQaI svaBaava ivaiBanna qaa. eskaoribak eisaz p`NaalaI maoM svaNa^ saUxmakNa ka baOMD tIv`ata saa[iT`k eisaz

p`NaalaI kI tulanaa maoM kma qaI.jabaik,, f`I roizkola p`itik`yaa maoM saUxmakNa ka ]%pad SaUV qaa, yaaina A%yaiQak

p`itkarkao sao vaMicat. [sa AQyayana maoM, 60-200 nm Aakar ko saUxmakNa kI ]%pi<a kI ga[^,, jaao Ai@sajaona sao

inaiYk`ya qaI.plsa roiDAaolaa[isasa p`NaalaI maoM salvaoToD [lao@T/na ka svaNa^ Aayana ko saaqa p`itik`yaa ka p`aqaimak Anaupat

7.9x109 M-1 s-1 inaiScat ikyaa gayaa.

User
Text Box
Page 6: GOLD NANOPARTICLES: GENERATION & CHARACTERIZATION

0

GOLD NANOPARTICLES: Generation & Characterization

G.R. Dey

Radiation & Photochemistry Division, Chemistry Group,

Bhabha Atomic Research Centre, Trombay, Mumbai 400085

Summary

The reduction of Au3+ ions through chemical reaction and free radical reaction under

different experimental conditions in aqueous and non-aqueous systems was studied.

During chemical reduction of Au3+ with citric acid (CA) and ascorbic acid (AA), the

spectral nature in two different systems was different with respect to the main absorption

peak (λmax 530 nm). In the case of AA, the band at 530 nm was broader and less intense in

comparison to CA system, which is due to the different size of nanoparticles. In CA

system, the particle sizes observed were smaller (60 nm) than those measured in AA

system (100 nm). While in free radical reduction of Au3+ with esolv-, the yield of

nanoparticles is pure i.e. free from extra reactants (reducing agent), which is normally

observed in chemical reduction processes. However, in no PVA (a stabilizer) system, the

product from free radical reduction was not so impressive. Under this condition the DLS

signal obtained was poor and the size of nanoparticle was not determined, whereas in

presence of PVA the particles sizes are better with respect to polydispersity.

During pulse radiolysis, the rate constant for esolv- reaction with Au3+ was determined

following the decay of solvated electrons in methanol (kbimol = 7.6x109 M-1 s-1). In

principle, initially the reduction of Au3+ ion leads to Au(II) ion intermediate, which later

produces transients Au(I) ion, atomic gold (Auo), etc. through their subsequent reactions.

On further reaction through nucleation reactions, perhaps gold nanoparticles were

generated. Under esolv- - Au3+ ion reaction, the spectrum recorded during short pulse

irradiation exhibits three-absorption peaks with three maxima at 270, 370, and 470 nm.

The nature of all these absorption peaks follows uniformity i.e. decrease in absorbance

with time, moreover with different kinetics. Under the study, 60-200 nm-sized particles

were generated, which are stable even in presence of oxygen.

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1

INTRODUCTION

Metal nanoclusters are important materials because of their role in surface-enhanced

processes. The unique properties of metal clusters, such as collective electronic and lattice

excitations depend on the size and geometry of the particle1 and have various applications

in the field of catalysis2. Study on nanometric particles of metals is also of interest to

understand their growth mechanism in photographic and catalytic sciences. Metals and

their alloys are known to act as catalysts in a wide variety of applications since ages.

Imaging as well as photographic development involves in application of clusters growth.

A number of reports on metal nanoparticles exist in the literature, which deal with the

mechanism of nucleation and growth process in photography3-5.

In the field of catalysis, metals show enhancing support for the propagation of chemical

reactions. This is mostly due to the involvement of free electrons available in metal

atoms/clusters. These electrons and their counter metal cations eventually interact with

themselves and with other reactants, producing various reaction intermediates through

different reaction channels. Metal nanoparticle provides a large surface to mass ratio as

compared to the bulk-metal, which is the primary reason for its superior catalytic activity6.

Even those materials exhibit negligible reactivity on their bulk scales are found to be

extraordinarily active in their small clusters (nanometric particles) forms. For example:

gold is an inert metal due to its non-reactive nature in the bulk state. However, its small

clusters are catalytically active due to different electronic and chemical properties,

including the size and different oxidation states of the nanoparticles. The redox potential

values for bulk gold metal and its atom are different to each other EoAu+∝/Au•

∝ = +1.68 V

and EoAu+/Au• = -1.5 V vs NHE7,8, which results in the higher reactivity of a gold atom

than the bulk gold.

The present work has been carried out to generate gold nanoparticle in water and methanol

(non-aqueous) through two different reduction techniques such as chemical and radiation

induced free radical reactions. In chemical reaction citric acid and ascorbic acids were

used as reducing agents in both aqueous and methanol systems, whereas under radiation-

induced free radical reaction studies, methanol (an alcohol) was used as reaction medium

in which two strongly reducing radicals viz. solvated electron (esolv-) and alcohol radical

(•CH2OH) are generated on radiolysis of the solvent take part in metal ion reduction.

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2

EXPERIMENTAL

Gold ions as HAuCl4 (99.9% purity) from Arora-Mathey chemicals, citric acid (>99%

purity) from LOBA Chemie, India and ascorbic acid (GR grade) from E Merck and

methanol (99.8% purity) from SRL, India were used as received. The UV-vis spectra of

the clusters produced during γ-radiolysis were recorded using Hitachi U-2001

Spectrophotometer. Prior to the desire experiments, UV-vis spectra of 0.2 mM Au3+ ions in

water, methanol and water-methanol mixture solvents were recorded separately and the

spectra obtained are shown in Figure 1. It was noticed from the figure that the spectral

nature of Au3+ ion changes appreciably at 300 nm region with methanol concentrations.

For better understanding, the absorbances at 310 nm were plotted against methanol

percentage in water and the plot is shown as inset of figure 1. It is noticed that the

absorption at λmax = 310 nm is minimum when there is no methanol, however, it increases

with methanol concentration and reaches maximum around 40% of methanol and remains

steady (see inset figure 1). Hence in the present work, >90% methanol was used for

carrying out all desire experiments assuming at this concentration, the nature of the parent

Au3+ ions remains identical.

RESULTS & DISCUSSION

Chemical Reaction

Generation of gold nanoparticles through chemical reduction

A chemical reaction is a process that always results in the inter conversion of chemical

substances. The substance(s) initially involved in a chemical reaction are called

reactant(s). Chemical reactions are usually characterized by a chemical change, and they

yield to one or more products, which are in general different from the reactant(s). The

performance of these reactions mostly depends on four parameters viz. temperature,

concentration, surface area and catalyst. Under this direction, the chemical reduction of

Au3+ ions (one reactant) to gold nanoparticles (product) was studied using ascorbic acid

and citric acid as reducing agent (another reactant) at room temperature (25oC) separately.

Observations during the course of reaction are discussed below.

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Reduction with CA

HAuCl4 (0.1 mM) solution in water was mixed with 0.1 mM CA at its natural pH (pH ≈ 3)

under aerated condition in which oxygen concentration present in the solution was 0.2

mM. With time, the initial light yellow colour solution changed to wine red colour

indicating the formation of gold nanoparticles possibly due to chemical reaction between

Au3+ ions with CA. The UV-vis spectrum recorded shown in Figure 2A exhibits absorption

maximum at 530 nm, which is similar to the reported spectrum for gold nanoparticles9-12.

Different concentration ratios of Au3+ ions to CA were employed to observe the different

behavior with respect to color intensity, kinetics, etc. exists if any during the study. The

peak at 530 nm did not change appreciably when the concentration of CA was tripled,

however, when the concentration of CA increased to 1 mM (10 times as compared to 0.1

mM), the absorption intensity at 530 nm was increased to three fold with a red shift to 550

nm. As mentioned above, the chemical reactions depend on concentration (one of the four

parameters) of at least one of the reactant, which is also supported by the experimental

results obtained at higher concentration of CA, a reactant in the Au3+ ions system. It is

interesting to note here that instantaneous development of color occurred as soon as the

concentration of CA increased to 10 time reveals that the kinetics of the reaction became

faster on increase in reactant (CA) concentration. Furthermore, lower concentration of CA

(0.1 and 0.3 mM) was not sufficient to reduce entire Au3+ ions to gold nanoparticles,

which is the possible reason to observe low yields (less absorbance at 530 nm).

Similar experiments were carried out in presence of 1 mM PVA, a stabilizer and the UV-

vis spectra obtained are shown in Figure 2B. The difference between the spectra observed

in with and without PVA systems was the band intensity. In presence of PVA, 1:1 and 1:3

ratios of Au3+ ions to CA, the peak at 530 nm was remain almost steady whereas at 1:10

Au3+ ions to CA ratio the absorbance value was doubled (0.45 to 1.1). The sizes of the

nanoparticles were measured using DLS (Dynamic Light Scattering) technique and listed

in Table 1. Particle size and the spectral properties (peak sharpness & intensity) together

reveal that CA under the study acts a stabilizer of gold nanoparticles, as there is no

influence of PVA. Both in presence and absence of PVA the particle size (~60 nm) and

peak intensity (Abs546 nm ~ 1.1) remain identical.

Dynamic Light Scattering (DLS) Measurements: This technique is also called as ‘quasi

elastic light scattering technique’, which provides rapid detection of the precise size and

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4

size distribution of materials with nano to micro range particles. When light (from Laser

source) is made incident on the solution, light scatters in all direction. Thus an analyzer

(fast photon counter) kept at a specific angle detects the analyzer beam and hence these

time dependent fluctuations in the scattering intensity are seen. These fluctuations are due

to the small molecules in the solution undergoing Brownian movement and are directly

related to the rate of diffusion of the molecule through the solvent. Hence, these

fluctuations are analyzed to determine the hydrodynamic radius of the particles present in

the solution. A typical plot from DLS measurement is shown in Figure 3A wherein a

representative change of the electric field correlation function g1(τ) for the gold

nanoparticle in aqueous phase is recorded at a scattering angle of 90˚. The solid line is a fit

of the experimental data using the method of cumulants13. The particles were found to be

highly poly-disperse in nature and the polydispersity index (ratio of variance and square of

mean decay rate13) obtained from cumulant analysis. Figure 3B represents the particles

distributions in the solution and the peak position corresponds to the dominating size of

the nanoparticles.

Similarly, TEM and SEM analyses are used for size determination and image

monitoring14,15 of nanometric particles.

Reduction with AA

In addition to the generation of gold nanoparticles using CA, the chemical reduction of

Au3+ ions with AA (another reducing agent) has also been carried out under identical

conditions. The UV-vis spectra recorded for without and with PVA are shown in Figure 4.

In absence of PVA, the peak around 550 nm because of gold nanoparticles was shifted

towards red with respect to AA concentration, which is due to increase in particle size.

However, in presence of PVA the peak was relatively sharper when the concentration of

AA increased to 1 mM (10 times) (Figure 4B). The particle sizes measured by DLS

method are listed in Table 1.

Particle size and the spectral properties (peak sharpness & intensity) together reveal that

AA under the study does not act as a stabilizer of gold nanoparticles, since there is

significant change in peak intensity (Abs535 nm ~ 0.93 from 0.6 for 1:10 ratio) and the

particle size (~140 to 100 nm) in presence of PVA. Hence AA under the study is not a

potential stabilizer as CA does.

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Similar experiments on chemical reduction of Au3+ ions were also carried out in methanol

medium using both CA and AA separately. It was observed that even after 72 hr of mixing

of two reactants, the solution color did not change to wine red, an indication of chemical

reaction of Au3+ ions with CA/AA in aqueous systems or vis-à-vis gold nanoparticle

formation, which designates negligible or a very slow reaction (if any) in methanol solvent

with these reactants. This dissimilar reaction behavior of gold nanoparticle formation in

methanol and water systems could be explained with the difference in solvent properties

viz. a low dielectric constant of the solvent methanol (32.63) as compared to water

(78.25)16.

The reactions taking place during the formation of gold nanoparticles through chemical

reduction of Au3+ ions with CA and AA are:

2HAuCl4 + Citrate ion gold particles + CO2 + HCOOH + etc. (1)

2HAuCl4 + 3C6H8O6 2Auo + C6H6O6 + 8HCl (2)

Where C6H8O6 and C6H6O6 represent ascorbic acid and dehydroascorbic acid respectively.

Soon after Auo takes part in nanoparticle formation.

Similarly, using other reducing agents such as sodium borohydride (NaBH4)17, aldehydes

(RCHO)18, and Carbon monoxide (CO)19, metal nanoparticleds are also generated through

chemical reduction method.

Radiolytic Reaction

Generation of gold nanoparticles through radiation induced free radical reaction

In radiation chemical research, high-energy ionizing radiation is generally used as

the energy source, whereas a light source is used in photochemical studies. The high

ionizing radiation emitting sources generally used for such work are radioactive nuclides

viz. 60Co, 90Sr, 3H and 137Cs in addition neutron source from nuclear reactors is also used.

In laboratory, machine sources such as X-ray tubes, Van de graaff generators, cyclotron,

synchrotrons betatron, febetron and other electron accelerators are used as high-energy

ionizing radiation sources. Therefore, in addition to an electronic excitation routinely

occur in the later type studies, ionization and super excitation of molecules are caused by

high-energy ionizing radiation20,21. Temporally, starting at femto-second time scale,

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6

interaction of radiations with matter produces electrons in a high and wide energy range.

These electrons lose energy through various physical processes and lead to the formation

of low energy (eV) electrons. Interaction of matter with such low-energy electrons

produce ionic and/or excited species, which disappear through different processes such as

dissociation, recombination, luminescence, internal conversion, intersystem crossing, ion

molecule reactions and solvation, generating various end-products. In water/aqueous

medium, the primary transient species produced due to the interaction of high-energy

radiation in picosecond time scale and diffused homogeneously throughout the medium

within 0.1 μs time are eaq-, H•, •OH, H2, H2O2, H3O

+. Amongst these, eaq- and H• are

reducing in nature and their reduction potentials are: eaq- + H+/½H2 = –2.9 V and H• + e- +

H+/H2 = -2.3 V vs. NHE respectively whereas •OH is an oxidizing radical, which

possesses reduction potential •OH + H+ + e-/H2O = 2.72 V in acidic solution and •OH + e-

/OH- = 1.89 V vs. NHE in basic solutions (pKa •OH O- + H+ is 11.9)20. The yields of

primary species in water radiolysis vary with pH of the solution. The yield in radiation

chemistry is generally expressed as G-value (G), which is the number of species generated

or destroyed per 100 eV of absorbed dose. In SI unit, G is expressed in mol J-1. At near

neutral pH, the primary species of water radiolysis with G-values (in μmol J-1) are given

as:

eaq- (0.28), H• (0.062), •OH (0.29), H2O2 (0.07), H2 (0.05), H3O

+ H2O

(0.33)20, thus allowing quantitative measurement of the ensuing chemical change.

Similarly, the radiolysis of non-aqueous solvents generates a number of species

through different reactions. The generation of two strong reducing species such as solvated

electrons (esolv-) and alcohol radical along with other species during the radiolysis of

alcohol such as methanol, ethanol, 2-propanol is well known22-27. The different species

generated in radiolysis of methanol are presented below:

esolv-, CH3OH2

+, CH3O-, H•, H2, CH3O

•, •CH2OH (3) CH3OH

In the absence of any added solute, the transient absorption spectrum obtained on

radiolysis has an absorption maximum at 620 nm caused by esolv- species [21].

In this system, H• or H-atom produced on radiolysis reacts with methanol producing •CH2OH radicals (reaction rate constant = 2.6 x106 M-1 s-1 in aqueous system)28. H• +

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7

CH3OH •CH2OH + H2 and CH3O• + H2. Hence, the existence of H• is negligible in

methanol system. Moreover, H• does not react directly with low concentration of the

solute present in methanol. •CH2OH, a reducing radical, generated during radiolysis as

well as through H• scavenging reaction with methanol has a reduction potential of –1.18 V

vs. NHE at neutral pH29.

Steady state radiolysis

Generation of Au nanoparticles in methanol

In our laboratory, for the generation of gold nanoparticles, 60Co γ-source was used for

steady state radiolysis. Typical Fricke’s dosimetry is employed to determine the dose

absorbed by the solution under identical experiments conditions20. Deoxygenated solution

of 0.2 mM Au3+ in methanol was γ-irradiated using the available 60Co γ-source at

Radiation and Photochemistry division, BARC (dose rate ~ 29 Gy/min in methanol) for

different time intervals. It was found that up to 3.5 kGy the intensity of yellow color

experimental solution decreases. On further irradiation (beyond 3.5 kGy dose), a purple

color solution was observed which is quite similar to the color reported for gold

nanoparticles. The absorption spectra of all samples before and after irradiation were

recorded, and shown in Figure 5. From figure 5, the absorption at 220 and 320 nm was

found to be decreasing with irradiation time, whereas after irradiation to 3.5 kGy dose, a

new broad band with absorbance maximum around 525 – 550 nm was appeared. This band

is due to the gold nanoparticles, and their size was >400 nm with high polydispersity.

Generation of Au-nanoparticles in methanol in presence of stabilizer

The effect of stabilizer in the generation of Au-nanoparticles through free radical induced

reaction was also studied. For which a solution of 0.2 mM Au3+ in methanol containing 1

mM PVA (a stabilizer) was irradiated using 60Co γ-source under Ar-purged conditions.

Figure 6 represents the spectra recorded for irradiated samples along with non-irradiated

one. It was observed that after γ-irradiation to 300 Gy dose, the solution color starts

changing to purple, this became more intense after 3.5 kGy dose. The peak at 530 nm in

PVA system is quite different than that observed in without PVA system (see figure 5).

Under DLS measurements the size of Au-nanoparticles was found to be ~100 nm, which is

more stable in contrast to without PVA under identical conditions. The reaction for the

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formation of nanoparticle including coagulation is fairly controlled in PVA containing

system due to the increase in solution density; as a result smaller-sized nanoparticles were

produced.

Later the gold nanoparticles in both solutions (with and without PVA) were exposed to air

(oxygen) and the observed spectra were found to be identical to their respective spectra

recorded before the exposure to air. This study suggests that the gold nanoparticle

generated in methanol during radiolysis is stable and inactive to oxygen in contrast to

silver nanoparticle in methanol30.

Pulse radiolysis

Pulse radiolysis technique is a well-accepted method for studying kinetics and the spectral

properties of the short-lived transient and/or reaction intermediate species (≥ ns life-

time)31. Such studies have been carried out using 7 MeV electron pulses of 50, 100, 200 ns

and 2 μs durations from a linear electron accelerator (Forward Industries, UK). The

experimental set up is currently available at Radiation and Photochemistry Division,

BARC for pulse radiolysis studies and its detail has been reported earlier32. The schematic

diagram of pulse radiolysis set-up is shown in Figure 7. In brief, an electron pulse beam

irradiates the sample contained in a 10 mm X 10 mm ‘‘Suprasil’’ square cuvette kept at a

distance of ~120 mm from the exit window, where the electron beam diameter is ~10 mm.

The transient changes in the absorbance of the solution caused by the electron beam are

monitored with the help of a collimated light beam from a pulsed 450 W Xenon arc lamp.

The analyzing light has been detected in PMT (Hamamatsu, R-955) placed at the exit of

monochromator (Kratos, model GMA 252). The output signal from PMT is fed to 100

MHz 1 GS/s Tektronix TDS 220 Storagescope. Spectral and kinetic data acquisition and

analysis has been carried out with the help of an IBM compatible PC33. Aerated 10 mM

potassium thiocyanate solution is used for determining the absorbed dose using a value of

2.59x10-4 m2 J-1 for Gε at 475 nm34. Pulse doses are 10, 20, 40 and 80 Gy respectively for

50, 100, 200 ns and 2 μs pulses. The pulse doses are variable and the desired dose can be

achieved by changing instrumental parameters. Care need to be taken while preparing the

methanolic solutions so that the water content always remains less than 1%. The water

contamination in alcohols plays an important role in radiolysis25 and the possible effects

are: i) change in matrix properties; ii) change in reaction rate constants. Anhydrous CuSO4

was used to test the water content in alcohols27. If the anhydrous CuSO4 (white) failed to

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transform into blue color in alcohols then the presence of negligible or very low water

contamination (within the limit permissible for such studies) was indicated. Presently, to

reconfirm its’ purity, the yield and kinetics profiles of transient are additionally checked

by adding 1% water to alcohol. Unchanged kinetic behavior confirms the suitability of the

methanol solvent and permissible for such experiments. High concentrated (24 mM) Au3+

ion stock solution in water prepared previously is mixed with neat methanol to formulate

desired experimental solutions of <1% water as impurity.

Reduction of Au3+ ions in methanol The time resolved spectra due to the transient species generated during electron pulse

irradiation on deoxygenated methanol are shown in Figure 8. The spectra at 0.4 and 0.8 μs

time after electron pulse are due to solvated electron and the spectra are matching well

with the reported one21. The decay of esolv- was faster in the presence of Au3+ ions in

methanol than measured in neat (without Au3+ ions) solvent, which authenticate the

reaction between Au3+ ions and esolv-. The decay time profiles obtained in different conc.

of Au3+ ions are shown in Figure 9. The reaction rate constant (kbimol) was determined by

following the change in pseudo first order decay (kϕ) of esolv- absorption at 620 nm21 with

respect to Au3+ ions concentrations. From the slope of the plot kϕ vs. [HAuCl4], (shown as

inset of Figure 9), the bimolecular reaction rate constant was evaluated to be 7.6×109 dm3

mol-1 s-1.

The time resolved spectra recorded during the course of esolv- reaction with Au3+ ions (0.2

mM HAuCl4) are shown in Figure 10, which exhibit three absorption maxima at 270, 370

and 470 nm. The nature of the absorbing species at these three wavelengths is quite

similar; at each peak position the absorption intensity decreases with time. The inset of

Figure 10 represents the time profiles obtained at 470 and 270 nm in electron pulse

irradiated deoxygenated 0.2 mM Au3+ ions in methanol. The 470 nm time profile shows

the faster decay of esolv- initially which is due to solvated electron reaction with Au3+ ions

followed by the formation of reduced Au3+ ions intermediate species. The decay of esolv-

attains its minimum value around 1.5 μs whereas the formation of reduced Au3+

intermediate species is completed within 10 μs after the electron pulse. This observation

concludes that the formation of the species absorbing at 470 nm is not only due to simple

first reduction species but also consisting different intermediate species originating from

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10

the solvated electron reaction. At longer time (up to 5 ms) also no intermediate species

absorbing within the measurement region were generated after the subsequent decay of

reduced Au3+ ion species absorbing at 470 nm. Similar observation in 2-propanol system

has been reported recently35. Moreover, it is difficult to interpret that these three peaks are

due to one species. Comparing the reducing radical yields in methyl viologen (MV2+)

systems containing with and without Au3+ ions and the transient spectrum observed in 2-

propanol system, the spectrum of very first reduced Au3+ species (i.e. Au2+•) has been

derived and discussed earlier35.

The overall reactions taking place during the formation of gold nanoparticles through free

radical induced Au3+ ions reduction are:

In deoxygenated (Ar/N2-purged) system:

The initial species Au•++, Au(I) and Auo possessing optical absorption in 250-720 nm

wavelength region generated during the course of reaction of esolv- with Au3+ ions as

discussed above are shown below through reactions 4-7.

Au3+ + esolv- Au•++ (4)

Au•++ + Au•++ (Au•++)2 Au3+ + Au•+ (5)

Au•+ + Au•++ Au3+ + Auo (6)

Au•+ + Au•+ Au•++ + Auo (7)

The absorption of (Au•++)2 and Au•++ species as shown earlier in 2-propanol systems30 are

formed during the reduction of Au3+ ions, undergoes decay successively. These reactions

continued to the formation of gold nanoparticles. Hence, the absorption shown in figure 10

is quite similar to 2-propanol system, which is due to the contribution of Au•++, Au•+ and

Auo intermediate species. These intermediate species are stabilized with solvent molecules

or the species generated from alcohol radiolysis. For a single pulse (~30 Gy) irradiation,

the formation of the gold nanoparticle was not observed whereas purple coloration due to

gold nanoparticle appeared after either long time radiolysis or repetitive pulse irradiation

up to dose ≥ 400 Gy.

In conclusion, two different systems (water and methanol) were used for the generation of

gold nanoparticles using chemical as well as free radical induced reduction processes. In

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chemical reduction reaction, AA & CA both generate nanoparticles in aqueous systems

whereas their chemical reactions in methanol are quite slow, highlighting the importance

of solvent properties. In free radical induced Au3+ ions reduction, there are many reports in

aqueous systems available in the literature; hence it is not discussed in this presentation.

Moreover, as compared to radical (esolv- and •CH2OH) reaction with Au3+ in water,

reaction rates in methanol are diffusion controlled.

Acknowledgement: The author would like to thank Ms. D.G. Deepanjali (M.Sc student from Pune University) and Dr. R. Ganguli of Chemistry Division, BARC for their assistance during the course of studies/experiments. He also thanks the LINAC maintenance team for their help during pulse radiolysis measurements. REFERENCES

1. Kreibig U., Voller M., Optical properties of metal clusters, Springer-Verlag, Berlin, 1995. 2. Henglein A., “Small-particle research: Physicochemical properties of extremely small

colloidal metal and semiconductor particles”, Chemical Review, 89 (1989): 1861-1873. 3. Gurney, R.W., Mott, N.F. “The theory of the photolysis of silver bromide and

photographic latent image, Proc. Roy. Soc. London, Sect. A, 164 (1938): 151-167 4. Lewis, L.N. “Chemical catalysis by colloids & clusters”, Chem.Rev. 93 (1993): 2693–

2730. 5. Hailstone, R.K., Liebert, N.B., Levy, M., McCleary, R.T., Girolmo, S.R., Jeanmaire, D.L.,

Boda, C.B. “Achieving high quantum sensitivities with hydrogen hyper sensitisation measurement”, J.Image.Sci. 32 (1988): 113–124.

6. Eustis, S., El-Sayed, M.A. “Why gold nanoparticles are more precious than pretty gold: Noble metal surface Plasmon resonance and its enhancement of the radiative and nonradiative properties of nanocrystals of different shapes”, Chem Soc Rev, 35 (2006): 209-217.

7. Weast, R.C. CRC Handbook in Chemistry and Physics, 65th Edition, CRC Press, Inc. Boca Raton, Florida, D-155, 1984-85.

8. Mosseri, S., Henglein, A., Janata, E. Reduction of Au(CN)2- in aqueous solution.

Formation of nonmetallic clusters and colloidal gold, J. Phys.Chem. 93 (1989): 6791-6795.

9. Dey, G.R. “Radiation Induced free radical chemistry:in homo & heterogeneous media”, Eds. G.R. Dey, Research Signpost, India, 159-171, 2008.

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11. Dey, G.R. “Gold and gold-copper nanoparticles in 2-propanol: a radiation chemical study”, Radiat. Phys. Chem., 80 (2011): 1216-1221.

12. Dey, G.R. “Generation of mono and bimetallic nanoparticles in 2-propanol through radiation induced reactions”, ISRAPS Bulletin, 25 (2013): 38-45.

13. Hassan, P.A., Kulshreshtha, S.K. “Modification to the cumulant analysis of polydispersity in quasielastic light scattering data”, J Colloid Interface Sci, 300 (2006): 744-748.

14. http://www.en.wikipedia.org/wiki/transmission_electron_microscopy 15. http://www.en.wikipedia.org/wiki/scanning_electron_microscopy 16. Lide, D.R., Handbook of Physics and Chemistry, 74th edition. CRC Press, Florida. 1993–

94.

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17. Daniel, M.C., Astruc, D. “Gold nanoparticles: assembly, supramolecular chemistry, quantum-size-related properties, and applications towards biology, catalysis, and nanotechnology”, Chem Rev., 104 (2004): 293-346.

18. Azetsu, A., Koga, H., Yuan, L.-Y., Kitaoka, T. “Direct synthesis of goldcatalysts on tempo oxidised pulp paper containing aldehyde groups”, BioResources, 8 (2013) 3706-3717.

19. Young, J.K., Lewinski, N.A., Langsner, R.J., Kennedy, L.C., Satyanarayan, A., Nammalvar, V., Lin, A.Y., Drezek, R.A. “Size-controlled synthesis on mondispersed gold nanoparticles via carbon monoxide gas reduction”, Nanoscale Research Letters, 6 (2011): 428

20. Spinks, J.W.T., Woods, R.J. “An introduction to radiation chemistry”, 3rd edition, John Wiley, New York, 1990.

21. Tabata, Y., Ito, Y., Tagawa, S. Hand book on radiation chemistry, CRC press, Boca Raton, Florida, 419, 1991.

22. Ferradini, C., Jay-Gerin, J.P. “Quelques aspects actuels de la radiolysis du methanol liquide: Une revue”, Radiat.Phys.Chem., 48 (1996): 473-480.

23. Fowles, P. “Pulse radiolytic induced transient electrical conductance in liquid solutions”, Trans Faraday Soc., 76 (1971): 428-439.

24. Baxendale, J.H., Wardman, P., “Electrons in liquid alcohols at low temperature”, J.Chem.Phys.Faraday Trans. I, 69 (1973): 584-594.

25. Getoff, N., Ritter, A., Schworer, F., Bayer, P. “Primary yields of CH3.O and .CH2OH

radicals resulting in the radiolysis of high purity methanol”, Radiat.Phys.Chem., 41 (1993): 797-801.

26. Dey, G.R. “Reduction of the copper ion to its metal and clusters in alcoholic media: A radiation chemical study”, Radiat.Phys.Chem., 74 (2005): 172-184.

27. Dey, G.R., Kishore, K. “Silver clusters in 2-propanol: A radiation chemical study”, Radiat.Phys.Chem., 72 (2005): 565-573.

28. Buxton, G.V., Greenstock, C.L., Helman, W.P., Ross, A.B. “Critical review of rate constants for reactions of hydrated electron, hydrogen atoms and hydroxyl radicals (OH/O-

) in aqueous solution”, J. Phys. Chem. Ref. Data, 17 (1988) 513-886. 29. Schwarz, H.A., Dodson, R.W. “Reduction potentials of CO2

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30. M. Mostafavi, G.R. Dey, L. Francois, J. Belloni, (2002) J.Phys.Chem. A, 106, 10184 31. Baxendale, J.H., Busi, F. The study of fast processes and transient species by electron

pulse radiolysis, NATO ASI Series, D. Reidel Pub.Co., p. 63, 1982. 32. Guha, S.N., Moorthy, P.N., Kishore, K., Naik, D.B., Rao, K.N. “One electron reduction of

thionine studied by pulse radiolysis”, Proc. Indian Acad. Sci. (Chem. Sci.), 99 (1987): 261-271

33. Panajkar, M.S., Moorthy, P.N., Shirke, N.D. “Programming a micro-computer for on-line data acquisition and processing in pulse radiolysis experiment. Part 1: Kinetic parameters”, BARC-1410, 1988.

34. Buxton, G.V., Stuart, C.R. “Re-evaluation of the thiocyanate dosimeter for pulse radiolysis”, J. Chem. Soc. Faraday Trans. 91 (1995): 279-281.

35. Dey, G.R., El Omar, A.K., Jacob, J.A., Mostafavi, M., Belloni, J. “Mechanism of trivalent gold reduction and reactivity of transient divalent and monovalent gold ions studied by gamma and pulse radiolysis”, J. Phys. Chem. A, 115 (2011): 383-391.

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Table 1

Sizes of the gold nanoparticles generated under different conditions:

Sr. no. Systems Size (nm)

1 0.1 mM Au3+ ions with 0.1 mM CA in water 60

2 0.1 mM Au3+ ions with 0.1 mM CA in water with PVA 57

3 0.1 mM Au3+ ions with 0.3 mM CA in water 72

4 0.1 mM Au3+ ions with 0.3 mM CA in water with PVA 75

5 0.1 mM Au3+ ions with 1 mM CA in water 147

6 0.1 mM Au3+ with 1 mM CA in water PVA 150

7 0.1 mM Au3+ ions with 0.1 mM AA in water 167

8 0.1 mM Au3+ with 0.1 mM AA in water with PVA 104

9 0.1 mM Au3+ ions with 0.3 mM AA in water 111

10 0.1 mM Au3+ ions with 0.3 mM AA in water with PVA 120

11 0.1 mM Au3+ ions with 1 mM AA in water 190

12 0.1 mM Au3+ with 1 mM AA in water PVA 125

13 0.1 mM Au3+ ions on γ-radiolysis in methanol (deaerated) -

14 0.1 mM Au3+ ions on γ-radiolysis in methanol with PVA (deaerated)

100

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240 320 400 480 5600.0

0.3

0.6

0.9

1.2

1.5

0 25 50 75 1000.2

0.3

0.4

0.5

a

d c

Abs

λ (nm)

b

Abs 31

0

% of Methanol

Figure 1. UV-vis spectra of 0.2 mM HAuCl4 recorded in different concentrations of methanol in water. (a) no methanol, (b) 20% methanol, (c) 30% methanol, (d) 40% methanol. Inset: the plot of absorbance at 310 nm vs. % of methanol in the solutions containing 0.2 mM HAuCl4.

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300 400 500 600 700 8000.0

0.3

0.6

0.9

1.2

1.5

300 400 500 600 700 8000.0

0.3

0.6

0.9

1.2

1.5

1:11:3

1:10

Abs

orba

nce

λ / nm

B

1:3

1:1

1:10

A

A

bsor

banc

e

λ / nm

Figure 2. UV-vis spectra of the gold nanoparticles generated during the reaction of CA with Au3+. Systems used are: 1:10, 1:3 & 1:1 ratios of Au3+ ions to CA without (A) & with (B) 1 mM PVA in aerated water.

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10-1 100 101 102 103 104

0.0

0.2

0.4

0.6

0.8

10 100 10000

3

6

9

12

15

A

Cor

rela

tion

Fun

ctio

n (g

1 (τ))

Time (μSec)

B

Num

ber

Size

Figure 3. (A): Plot of correlation function vs. time for gold nanoparticles. (B): The distribution of particles of the same sample for figure 3 A.

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300 400 500 600 700 8000.0

0.3

0.6

0.9

1.2

1.5

1.8

300 400 500 600 700 8000.0

0.3

0.6

0.9

1.2

1.5

B

1:1

1:3

1:10

Abs

orba

nce

λ / nm

A

1:1

1:3

1:10

Abs

orba

nce

λ / nm

Figure 4. UV-vis spectra of the gold nanoparticles generated during the reaction of AA with Au3+. Systems used are: 1:10, 1:3 & 1:1 ratios of Au3+ ions to AA without (A) & with (B) PVA in aerated water.

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300 400 500 600 700 8000.0

0.3

0.6

0.9

1.2

1.5

b

cd

e

a

Ab

s

λ (nm)

Figure 5. UV-vis spectra of gold nanoparticles generated during γ-radiolysis of deaerated 0.2 mM Au3+ ion solution in methanol before (a) and after (b) 150 Gy; (c) 600 Gy; (d) 3.5 kGy and (e) 5 kGy irradiation.

Figure 6. UV-vis spectra of gold nanoparticles generated during γ-radiolysis of deaerated 0.2 mM Au3+ ion solution in methanol containing 1 mM PVA before a) and after (b) 450 Gy; (c) 1.7 kGy; (d) 3.5 kGy and (e) 5 kGy irradiation.

200 300 400 500 600 700 8000.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

1.6

ed

ba

Ab

sorb

an

ce

λ / nm

c

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400 500 600 700 800

0.000

0.006

0.012

0.018

0.024

7 μs

0.8 μs

ΔA

λ / nm

0.4 μs

Figure 7. Typical pulse radiolysis setup.

Figure 8. The time resolved spectra obtained during electron beam irradiation of deoxygenated methanol.

XeLamp L L M PM T

PC

7M ev electro n pulse beam

O scilloscope

Sam pleShutter

M – MonochromatorL - LensX e – X enon arc la m pPC – C om puterPMT – Photomult ip lier tube

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0 2 4 6 8-0.005

0.000

0.005

0.010

0.015

0.020

0.0 0.1 0.2 0.3 0.40

10

20

30

40

k φ /105 s

-1

[HAuCl4] / 10-3 M

d

c

b

a

ΔA

Time / μs

0 5 10 15 20

-0.02

0.00

0.02

0.04

0.06

0 5 10 15 20-0.002

0.000

0.002

0.004

0.006

300 400 500 600 700

-0.02

0.00

0.02

0.04

0.06

Time (μs)

ΔA

270 nm

Time (μs)

470 nm

4

20 μs

2

0.8

ΔA

λ (nm)

Figure 9. The time profiles at 620 nm obtained during electron beam irradiation of deoxygenated methanol in absence (a) and in presence of different concentrations of Au(III) ions (b: 0.01 mM; c: 0.025 mM and d: 0.4 mM). Inset: plot of kφ vs. concentration of HAuCl4

Figure 10. The time resolved spectra obtained in electron pulse irradiated deoxygenated 0.2 mM HAuCl4 solutions in methanol after 0.8 to 20 μs (Dose/pulse 16 Gy). Inset: time profiles at 270 and 470 nm.