Determining the Size and Shape of Gold Nanoparticles
Carthage College
Ashley Wulf 11/17/2011
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Abstract:
Gold nanoparticles (GNPs) are studied because they have unique optical
properties making them very useful for things such as diagnostics. GNPs were
synthesized using cetyltrimethylammonium bromide (CTAB) to create icosahedral
shapes and were then studied based on their Surface Enhanced Raman Scattering
(SERS). Various imaging techniques were used in order to better understand the
structure of GNPs and to prove a high yield for the controlled synthesis. Through the
work by Haiss, et al. spherical gold nanoparticles were also synthesized and size was
determined through UV-Visible spectroscopy (UV-Vis) and surface plasmon resonance
(SPR). In another study by Kwon, et al. transmission electron microscope (TEM),
scanning electron microscope (SEM), X-ray diffraction (XRD), and UV-vis were used to
study the GNPs synthesized to determine the size and shape. Equations were
developed based on the diameter of the particle through SPR and UV-vis spectra data
which allowed one to be able to quickly and easily calculate size and concentration of
GNPs. In conclusion, GNPs were synthesized using two different methods to produce
spherical and icosahedral shapes and then were studied to determine size and their
SERS properties.
Introduction:
Gold nanoparticles (GNPs) are the most stable metal nanoparticle and their
unique optical and electrical properties make many researchers believe that they will be
among the key materials and building blocks for nano-materials in the 21st century 1.
Determining the shape and diameter of nanoparticles is important because their uses in
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optical 2, electronic, magnetic and catalytic applications are dependent upon shape and
size 1 . Nanoparticles can be prepared in numerous shapes such as rods, prisms, and
wires 2, but high yields have never resulted from these syntheses. This thesis will
examine a new high-yield synthesis of icosahedral GNPs and will present a study that
characterizes the size of spherical GNPs.
In the article by Kwon, et al., cetyltrimethylammonium bromide (CTAB) was used
to control particle aggregation in a icosahedral GNPs synthesis 3. CTAB stops the
growing process because it can act as a capping agent. The capping between the
CTAB molecules and GNPs occur due to electrostatic interactions. If the GNPs were not
capped then they could fuse into larger particles because GNPs experience dispersion
interactions which increase their tendency to fuse. CTAB counteracts this fusing
process by overcoming the electrostatic repulsion. Therefore, once the driving forces for
growth by GNPs and the CTAB counteracting interactions are in equilibrium, the GNPs
stop growing 1.
In the article by Kwon, et al. Gold particles of 3.5nm size were used as seeds to
grow larger nanoparticles with CTAB. A controlled synthesis was then preformed to
produce GNPs of 10 to 90nm in size. Five synthesized samples were labeled A-E and
had increasing particle size. Each of the five solutions contained the following: 9.0 mL of
growth solution containing 2.5x10-4 M HAuCl4, 0.10 M CTAB solutions and 50 µL of 0.10
M ascorbic acid. Of the seed solution 1.0 mL was mixed with solution A. Then 1.0 mL
was taken from solution A and added to solution B. Again 1.0 mL of solution B was
added to solution C and the same process was used to solutions D, and E. The
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concentrations of the GNPs were calculated and are listed in Table 1. The five different
samples were then studied using
microscopy and spectroscopy 3.
To examine the five samples,
transmission electron microscopy
(TEM) was used to capture images of
the GNPs. In TEM, an electron beam
interacts with and is transmitted through
a thin sample, and then projected onto
a florescent screen. An image of the
sample is thus produced and the brighter regions of the image represent areas where
more electrons have passed through the sample; whereas the darker regions represent
areas where fewer electrons have been passed through due to higher sample density.
TEM was also used because images are able to be magnified up to 500,000 times thus
producing a high resolution, highly magnified, image.4,5, 6
A scanning electron microscope (SEM) was also used to study the synthesized
GNPs. In SEM, a set of coils moves the electron beam across a sample in a two
dimensional grid. When the electron beam across over the sample, different interactions
occur. Some of the electrons from the surface material kick of their electrons by the
beam thus producing secondary electrons. These secondary electrons can then be
detected by the secondary electron detector on a SEM. An image is then produced at
the surface of the sample and is projected. Similarly to TEM, SEM images can be
magnified up to 100,000 times while maintaining a high resolution. 5,4,6
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Both TEM and SEM are electron microscopes and require an electron source.
The most common electron source used is a tungsten filament. When the filament is
heated, electrons are produced and are attracted by the anode where they are pushed
down the column of the apparatus to interact with the sample. 6 Although SEM and TEM
both use electron beams to produce images of particles, the techniques have a few
important differences. For example, in TEM an electron beam passes through a thin
sample whereas in SEM the electron beam scans the entire surface of the sample.
Also, in TEM the samples are very thin, and in SEM the sample can be of any
thickness. Lastly, TEM images are shown on fluorescent screens and SEM images are
shown on television monitors.
X-Ray diffraction (XRD) was also used to also examine the synthesized GNPs.
In XRD, x-rays that are produced by the x-ray beam get scattered by the atoms in the
sample. Waves are then scattered spherically from the atoms which causes the
intensity of the scattered radiation to show minimum and maximums in different
directions. XRD allows a better visual of the structure of the observed atoms because it
shows axes, shape, size and position of the atoms 7. In the article of Kwon, et al., XRD
was used to show that particle growth occurs through adding more gold atoms down the
preferential plane of the five solutions 3.
Surface-enhanced Raman scattering (SERS) is a more advanced spectroscopic
technique which is a form of Raman spectroscopy. Raman scattering is a type of
molecular vibration that can occur between light and molecules. If the energy of light is
not enough to excite the molecules from the ground state to the lowest electronic state,
the molecule is then instead excited to a virtual state between the two. SERS was
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discovered by accident when a researcher was trying to do Raman scattering and
produced a Raman scattering more intense than expected. This strong signal was then
coined SERS. Therefore, SERS is a technique that enhancing Raman scattering by
molecules adsorbed on a rough surface. SERS can occur when molecules are brought
to the surface of metals and can be observed from silver, gold and copper. Also, if metal
nanoparticles are used in SERS, the particle size needs to be from 20-300 nm. 3,8
Surface plasmon resonance (SPR) was used and involved light being directed
onto a thin surface which contains gold. Some of the lights electric field can leak onto
the surface if the angle of light causes it to be reflected. The electric field excites the
surface plasmon waves in the metal. A surface plasmon is an electron wave that travels
along the surface of the gold film. The wavelength of this plasmon wave is then
detected in the SPR experiment.9,10
Ultraviolet-visible spectroscopy (UV-Vis) involves the absorption of light by
molecules in ultraviolet-visible region. The absorption in the visible range directly
corresponds to the color of the chemicals involved. UV-Vis can be used to determine
the concentration of the solution based on the absorbance. UV-Vis uses a
spectrophotometer which measures the intensity of light that passes through a given
sample (I). The instrument then compares the measurement to the intensity of light
before it passes through the sample (I0). A percent transmittance is then determined by
using I/I0. Next, from the percent transmittance, an absorbance can be calculated by
using Equation 1.
A= -log (%Transmittance / 100%) (1)
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Uv-Vis thus allows a concentration and absorbance to be calculated depending on the
wavelength of the particle or solution studied 11.
In a second study by Haiss, et al. UV-Vis and TEM were used to determine the
size of spherical gold nanoparticles. GNPs in aqueous solutions with diameters of three
to 120 nm were studied. Through UV-Vis spectroscopy and SPR, particle diameters
were determined which are important for depending on the application of GNPs.
Equations are developed that correlate UV-vis absorbance and SPR to particle size
thus yielding a simple and quick method to determine size. 11 In the Haiss, et al. study
Gold hydrosols were studied; a hydrosol is a colloidal system where the dispersion
medium is water. The phase for this dispersion can be a solid, gas or another liquid 12. A
colloidal system is a substance which is dispersed throughout another substance 13.
Michael Faraday a famous chemists known for contributing to electrochemistry
and electromagnetism first noted how to form red solutions when a reduction of
chloroaurate (AuCl4-) occurred 1. In order to synthesis the gold hydrosols used in the
article by Haiss, et al. HAuCl4 was used along with water. GNPs seeds were
synthesized using citrate to reduce Au3+ and had an approximate diameter of 17-20nm.
The synthesized GNP seeds were then used as seed particles for the synthesis of
GNPs larger than 20nm. This method allowed Au3+ to be reduced on the surface. Gold
needs to be reduced on the surface of GNPs because it increases their diameter
depending on the side of the seed particle and the amount of gold reduced. The gold
was then studied using UV-Vis spectroscopy in the wavelength range of 350 to 800
nm.11
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The total amount of gold used for synthesis, measured particle diameter, and
volume of synthesized solutions were all used to then calculate the density of particles.
Commercial GNPs were also used for comparison with the synthesized GNPs. The
manufactures of the commercial GNPs provided the size and density of these GNPs.
Through UV-vis and TEM, the synthesized and manufactured GNPs were compared
and size and concentration were determined 11.
In conclusion, gold nanoparticles were synthesized via two methods to create
two different shaped particles. Spherical gold nanoparticles were synthesized and the
size was characterized. Icosahedral particles were also synthesized in order to study
their SERS properties. Other techniques such as TEM, SEM, XRD, UV-Vis were used
to image the particles and to determine size and shape of GNPs. Therefore, through
these two studies gold nanoparticles were synthesized and their size, and shape we
characterized.
Results and Discussion:
Gold seeds were used in a synthesis to create gold nanoparticles with diameters
ranging from 10 to 90 nm. The synthesis also used cetyltrimethylammonium bromide
(CTAB) and ascorbic acid. The starting oxidation state of gold in the synthesis was Au3+
and the final oxidation state was Au0. As a result, a reducing agent was needed in
order to first reduce gold to Au+ from Au3+. The reducing agent used in this synthesis
was ascorbic acid. It allowed larger sized particles to be grown with the growth seeds 3.
The reduction of gold was confirmed because the color changed when ascorbic acid
was added. For example, before CTAB was added the solution color was orange and
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once ascorbic acid was added, the orange color disappeared. Gold was not reduced to
the Au0 because ascorbic acid is too weak to reduce the gold further because it is a
weak acid, with a pka of 4.2. 14, 15
Gold seeds were also used in the synthesis because they act as nucleation
centers which allow the gold to be reduced. The particle size of the gold seeds were
around 3.5 nm 15. The gold seed particles help the synthesis to reduce Au+ to Au0
because they act as nucleation centers. Growth solution containing HAuCl4 and CTAB
was added to ascorbic acid and in labeled vials a-e. Each of the five solutions
contained the following: 9.0 mL of growth solution containing 2.5x10-4 M HAuCl4, 0.10 M
CTAB solutions and 50 µL of 0.10 M ascorbic acid. One millimeter of the seed solution
was mixed with solution A. Then 1.0 mL was taken from solution A and added to
solution B. Again 1.0 mL of solution B was added to solution C and the same process
was used for solutions D, and E. Therefore, after the reducing agents had been added
gold atoms form in the solution and particles begin to form .3 This nucleation process
allows the remaining gold atoms to attach to these nucleation sites. As a result of the
reducing agent and nucleation process, the growth of large nanoparticles was achieved.
In this experiment, five different solutions labeled a-e were prepared of varying
sizes of gold nanoparticles. Imaging measurements were used to determine the particle
size of each solution of gold nanoparticles. Each solution a-e increased in particle size
as shown through Figure 1 3. TEM images were obtained for the five solutions. TEM
uses electrons as the light source to produce images of the particles examined 5,4 .
Figure 1 shows the TEM images of the CTAB-stabilized gold nanoparticles from
solutions a-e. As seen from Figure 1, hexagonal shapes are seen in all solutions.
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However, in solutions a and e hexagonal shapes are not as visible due to image quality.
Particles in solution a are too small
to determine a shape and particles
in solution e are too large to show
the hexagonal shape. Solutions b-
d have good image quality and
show recognizable hexagonal
shapes 3. Gold particles that are
icosahedral may show hexagonal
shapes under TEM imagining
because the shape of fine gold
seeds in CTAB solutions is faceted
with (111) faces. The differences
between an icosahedron with (111)
faces and a cube with (100) faces
is illustrated in Figure 2 16. Also,
lower CTAB and higher ascorbic
acid concentrations favor faster formation and deposition of neutral gold onto the (111)
faces. This leads to the disappearance and formation of (100) faces and as a result
produces cubic instead of spherical shapes. If the CTAB concentration was similar or
slightly higher and the ascorbic acid concentration was slightly lower, then there would
be a truncated octahedral which would contain both (100) and (111) faces 17. Therefore,
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solutions a and e are
not as visible as
compared to b-d
because TEM only
gives a projected
image of objects.
Next, from the
TEM measurements, nanoparticles diameters were measured for CTAB gold
nanoparticles solutions a-e. Table 2,
shows the mean particle diameters in nm
for the 5 solutions 3. Table 2 and Figure 1,
both show that the particle size increases
greatly from solutions a-e using.
Therefore TEM was successfully used to
study the shape and diameter of the
CTAB-stabilized gold nanoparticles.
Scanning Electron Microscopy, (SEM) was also used in order to further examine
the five solutions and see the definite structure of gold nanoparticles. In SEM, a set of
coils moves the electron beam across a sample. When the electron beam moved
across the sample, different interactions occurred. Some of the electrons from the
surface material kick of their electrons by the beam thus producing secondary electrons
and a image of the sample. 5,4 Solution D was analyzed with TEM and further used to
show the shape of the gold nanoparticles. The SEM image of solution D is displayed in
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Figure 3 3. The image shows that the nanoparticles have an icosahedral shape. Also, in
Figure 3 the inset shows all of
the (111) facets of an
icosahedral GNPs. Solution D
was then examined again using
TEM to obtain a high-resolution
image for better understanding
the shape of the particles.
Solution D was used because it
offered the best images of the
hexagonal shape which is the
most useful for studying the gold nanoparticles icosahedral shape.
Figure 4 shows the TEM images of solution D 3. Images, a and b are of solution
D where b is an enlargement of a. The lines drawn on image b represent the two
boundaries which
intersect the two
neighboring facets. To
further confirm the
icosahedron shape, the
d-spacing was found to
be 2.36 Å which is
consistent with the
(111) planes of face
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centered cubic gold 3. D-spacing is important in the identification process. For example,
each particle has a known value for d-spacing and thus when a d-spacing is known it
can help establish which type of facets are observed 18. Through these further studies of
solution D, it was concluded that the
shape of the GNPs was icosahedron by
using TEM and SEM.
X-Ray diffraction (XRD) was also
used to characterize the nanoparticles.
This experiment involves scattering x-
rays through specifically placed atoms
of crystals. In this study XRD was used
to show that particle growth proceeds
by adding more gold atoms on the
preferential planes for each solution.
Figure 5 shows the XRD measurements
for solutions a-e 3.Three peaks were
obtained from each solution. As seen in
Figure 5, solution E shows the largest
peak for the (111) planes as expected
because sample E has the largest
particles. As a result, the particles grow when more gold atoms are added into the
solutions causing an increase in the XRD patterns. The three peaks were assigned to
diffraction peaks of gold metal of (111), (200), (220). The work by Hyunjoon, et al. also
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produced XRD patterns for Pt nanoparticles at facets of (111), (200) and (220) 19.
Equation 1 was used to calculate the intensities ratios of the 5 solutions 3.
(2)
Next, by examining Figure 5 and using Equation 2, the intensity ratios of the five
solutions were calculated and are shown below in Table 2. Although, solution A was
studied and shows a XRD pattern, the intensity could not be obtained due to poor
spectral quality. Table 2 and Figure
5, clearly show that intensity ratios
decrease as particle size
increases. The peak for the (111)
is always the largest peak
compared to the (200) and (220)
peaks because the ratio is less
than one. The (220) peak is the
smallest in most samples except for solution e because e has the GNPs size 3. From
these ratios it was concluded that the gold nanoparticles are primarily composed of
(111) facets. In other words, the five solutions have the highest intensities of the (111)
peak and thus have an icosahedron shape. Therefore, the XRD, SEM and TEM results
all point to gold nanoparticles with an icosahedral shape.
Next, in order to further study gold nanoparticles, Ultraviolet-visible spectroscopy
(UV-Vis) was used to determine the wavelength maximum of the five solutions. UV-vis
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was used because gold nanoparticles have strong plasmon resonance absorption which
is dependent on size and
shape of the particles 3.
Plasmon resonance
absorption occurs because
of d-d band transitions.
Plasmon excitation occurs
with the whole particle
jumping through transition
bands. Also, the resonance
frequency can be affected
by four factors: density of
electrons, electron mass, mass and size of the charge. The UV-vis spectra of the 5
solutions were then compared to the gold seed used in the growth system. The
literature value for Plasmon bands is
usually a between 520 and 530 nm for
spherical gold nanoparticles 3. Figure
6 shows the visible spectra of the five
solutions (a-e) and the gold seed.
From the data in Figure 5, Table 3
constructed to show the wavelength
maxima for solutions a-e. The data
shows that for solutions a-e,
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wavelength increases, steadily. The wavelengths increase with each sample because
the particle size also increases. Larger particles show plasmon absorbance at longer
wavelengths.
Finally, Surface Enhanced Raman Scattering, (SERS) spectra were used to
study gold nanoparticles and investigate further the spherical and icosahedral shapes 3.
SERS enhances the Raman signal from Raman-active molecules that have been
absorbed on metal surfaces. Spherical gold nanoparticles were compared to the
icosahedral gold nanoparticles through SERS. Noble metallic nanostructures exhibit
SERS in which the scattering
cross-sections are
dramatically enhanced for
molecules adsorbed on.
Figure 7 3, shows the spectra
of two gold nanoparticle
shapes under three different
concentrations. The average
particle size for the spherical
gold nanoparticles was 3.5
nm, the same as the
icosahedral. Figure 6a shows
the spectrum of 1 x 10-4 M 4-
nitrobenzenethiol (4-NBT), Figure6b shows the spectrum of 1 x 10-4 M 2-
mercaptopyridine (2-MP), and lastly Figure 6c shows the spectrum of 1 x 10-6 M
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rhodamine 6G (R6G). Therefore, the three spectras in Figure 6 are of solution c and the
three organic molecules used. Not only is the size important but the morphology or
shape of the particles is also important because it has a great effect on SERS activities
of organic molecules. In each of the three spectra in Figure 7, the upper line refers to
the icosahedral particles and the lower line refers to the spherical particles. The
icosahedral particles used in the SERS experiment were from solution c. Particles from
solution c were used because they produced the strongest Raman shift for the SERS
spectrum of 1 x 10-4 M 4-nitrobenzenethiol (4-NBT). In all the spectra, the icosahedral
particles show intensities nearly four times that of the spherical particles. Icosahedral
particles give higher intensities because they have very well-defined edges and corners
and thus sharper features as compared to spherical particles. The detailed shape
difference between icosahedral and spherical particles could be because of the larger
localized field enhancement 3. Therefore, the SERS studies showed the intensities for
two different shaped nanoparticles of gold. It was concluded that the icosahedral
shapes gives stronger signals for intensities as compared to spherical gold
nanoparticles.
In conclusion, TEM, XRD, SEM, SERS, and UV-Vis spectroscopy techniques
were used to study GNPs. In all experiments the nanoparticles synthesized were
shown to have an icosahedral shape. Also, spherical particles were compared to the
icosahedral particles using SERS. This study is related to the work by Haiss, et al.
which deals with spherical GNPs. Haiss, et al. determined the size and concentration of
spherical GNPs. This work also used UV-Vis and TEM to characterize the GNPs.
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Gold nanoparticles (GNPs) can be used in a number of applications due to their
optical properties. The applications include diagnostics, therapeutics, catalysis, and
optical sensing1. Wolfgang, et al. studied the optical properties of spherical gold
nanoparticles, ranging in size from 3 to 120 nanometers 11. Through this work UV-
Visible spectroscopy allowed the researchers to calculate particle size and to determine
particle concentration.
The Haiss, et al. study investigated particles with diameters ranging from three
to 120 nanometers 11. Transmission electron microscopy (TEM) was used as in the
previous study by Kwon, et al., to record images of gold particles and the gold
hydrosols. In a hydrosol particles
are uniformly dispensed in water
12. In this study, TEM was also
used to image at least 100
particles from each particle size
group. The size distribution of
gold nanoparticles from the TEM
images can be seen in Figure 8
11.The histogram was generated
from 617 measurements of
particle size 11. The inset shows
a representative TEM image of
the spherical gold nanoparticles. From the data in the histogram, the average diameter
of spherical gold nanoparticles was found to be 60±9 nm.
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Spherical GNPs were also studied with surface plasmon resonance or SPR. In
the SPR experiment, light is directed onto a thin surface containing gold. If the angle of
light causes it to
all be reflected,
some of the light’s
electric field leaks
onto the surface.
This electric field
can then excite
surface plasmon
waves in the
metal. A surface
plasmon is an
electron wave that
travels across the surface of the gold film. The wavelength of this plasmon wave is
detected in the SPR experiment. The wavelength has been shown to depend on the
size of the nanoparticles on the surface. Previous work has shown that GNPs produce
surface plasmon waves with wavelengths of 520 nm 9,10. Figure 9 shows a diagram of
the surface plasmon resonance (SPR) experiment.
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The overall goal of this experiment was to correlate the size of GNPs to the
wavelength of the surface plasmon wave. Therefore, the wavelength of SPR (λspr) was
examined as a function of the diameter of the particles. The results are shown in Figure
10 11. The calculated
wavelengths of surface plasmon
peaks are shown as circles and
the experimental data is shown
as triangles. The upward
triangles represent particles that
were synthesized in house and
the downward triangles represent
the commercial gold
nanoparticles 11. The error bars in
this figure are horizontal and
show the errors in the diameters
of the particles used. The error
bars are only shows for the in-house synthesized particles. As seen in the figure, the
calculated and experimental wavelengths are in perfect agreement with one another.
Wavelengths vs. diameters data for particles that were larger than 25nm were fit
to the exponential function shown in Equation (3) 11.
λspr= λo + L1 exp (L2d) (3)
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λspr was the surface plasmon resonance wavelength and d was the diameter. The fit to
the data in Figure 10 gave values for the free parameters to be λ0 = 512, L1= 6.53, and
L2 = 0.0216. The error in the fit was three percent. Next, with the three values
established, Equation (3) was rearranged to solve for d. This expression is shown in
Equation (4). With the relationship between λspr and d now established, Equation (4) can
be used to calculate nanoparticles size (d) from the measurements of SPR
wavelengths.
λ λ
(4)
However, the equation cannot be used for particles smaller than 25nm because
the experimentally observed wavelength is lower than what would be expected 11.
Recall that the SPR wavelength for spherical GNPs is usually around 540 nm 20 and this
experiment had a range of 520-580 nm 11. However, when particles were smaller than
25 nm, the wavelength of SPR was smaller than 520 nm. The wavelength may be
smaller for particles smaller than 25 nm because of the increase of the ratio of surface
atoms to bulk atoms for small particle diameters 11.
Since the data for GNPs smaller than 35 nm did not show an experimental
dependence of λspr on d, the size cannot be estimated by Equation (3). Therefore, UV-
vis spectroscopy had to be used to incorporate particles that are smaller than 35 nm
into the study. UV-Vis spectra were collected for GNPs as a function of size. Data
plotted on Figure 11 (a) 11.
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Figure 11 (a) shows a plot of the ratio of the absorbance at two wavelengths vs. particle
diameter.11 For example, the circles in the image represent the ratio of the absorbance
at the wavelength of SPR wave
to the absorbance at 450.
Unlike the square, diamonds
and triangles, these data points
increase at a steady rate with
increasing diameter. Therefore
the ratio of the absorbance at
the SPR wavelength to the
absorbance at 450 nm may be
useful in measuring particle
sizes less than 35 nm.
Since none of the lines
have a strong linearity, Figure
11 (a) is not very useful
because only one line out of the
five could be used for further
analysis of the ratio of absorbencies to diameters. As a result, the data represented by
the circles in Figure 11 (a) was used to construct, Figure 11 (b) 11. In Figure 11 (b) the
absorbance ratio is plotted vs. the natural log of the GNPs diameter.
Therefore, Figure 11 (b) is more useful in showing agreement between
theoretical and experimental results when the absorbance ratios are in the wavelength
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region below 600 nm. The particle diameters used were in the size range of 5 to 80 nm.
The circles in the graph are the theoretical data points produced and can be fitted to a
line with a R2 value of 0.9999. The triangles in the graph again represent the
experimentally in-house and commercial GNPs. Since a strong linear correlation was
produced in the graph the ratio Aspr/A450 can be used to calculate the particle diameter
with Equation (5). 11
(5)
In the equation, B1 is the inverse slope, and B2=B0/m where B0 is the intercept. The
values obtained for B1 and B2 are shown in Table 4. The equation had an error of 18%
when the theoretical data for B1 and B2 were used to calculate particle diameter.
However, if the experimental values for B1 and B2 were used, the error in determining
particle size was 11%. Table 4 shows a comparison of experimental and theoretical
data for B1 and B2.11 As a result, Equation (5) can be used to determine the particle
diameter of particles between 5 to 80 nm.
In conclusion, the particle diameters can be determined through experimental
techniques. The best technique to use depends on the size of the particles. For
example Equation (3) from SPR can be used to calculate particle diameters for particles
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that are between 35 to 100 nm. Equation (4) from UV-Vis spectroscopy can be used to
calculate diameters of the particles when the absorbance ratio is known. Therefore,
these experiments offered efficient methods to calculate particle diameter for spherical
GNPs. If scientists are thus working with gold hydrosols, a quick method for size
determination can be applied due to this experiment because it offers researchers a
way to determine the size and concentration from either the SPR wavelength or UV-Vis
spectrum.
Conclusion:
This thesis has shown the importance of gold nanoparticles because of their size
and shape. The shape and size of GNPs is important for their uses in optical, electronic,
magnetic and catalytic properties. Therefore, through the work by Kwon, et al., GNPs of
icosahedral shape were synthesized and studied. The GNPs were studied through
TEM, SEM, XRD, UV-Vis to focus on the size of each particle synthesized and their
icosahedral properties. The icosahedral particles were also studied to examine their
surface-enhanced Raman scattering properties. In this thesis spherical GNPs were also
studied through the work of Haiss, et al. to determine the size of spherical particles. The
particles were synthesized and studied through UV-Vis, and TEM to develop equations
to calculate the concentration. In essence, icosahedral and spherical GNPs were
synthesized and studied to determine the size, shape, and their surface-enhanced
Raman scattering properties.
Further research could be done to see if the GNP shape affected the correlation
observed. Since GNPs can form numerous shapes; such as prisms and rods, can
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equation to calculate the diameters of these particles can be developed. Another idea to
focus on for further research could be which shape is better for different applications.
For example, each shape of GNPs have different physical properties thus making it
useful to determine which shape is better in areas such as diagnostics, therapeutics,
catalysis, optical sensing, and in further nanotechnology. Thus, a study could be
conducted to learn how shape affects the application GNPs used.
References:
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