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Van Thi Thanh Ho Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 6, ( Part -1) June 2016, pp.21-24
www.ijera.com 21 | P a g e
Growth and Dispersion the Silica Particle on the Glass via
Modified Stöber Method and Spray Technique
Van Thi Thanh Ho*
1
Hochiminh City University of Natural Resources and Environment (HCMUNRE), Vietnam
ABSTRACT
We presented the fabrication of a novel geometric light trapping structure based on silica particle. This light
trapping structure with good morphology was fabricated through modified Stöber method and spray technique.
More importantly, the silica particles were dispersed onto glass by using bottom-up or chemical approach
involves a common route used to synthesis silica particles from atomic or molecular scale. An optimized
synthesis condition is a combination of optimal values of each reaction parameter of Stöber method that could
produce homogenous and mono-dispersed silica nanoparticles with uniform size. The diameter of silica particles
can be varied from 200, 430, 560, 460 nm by increasing concentrations of ammonia from 2.33 mM to 4.65 mM,
9.31 mM and 13.96 mM, respectively. We found that the silica particle size was well controlled and uniform
from ~200 nm to 560 nm by controlling the ammonia concentration. These results open up the possibility to
further fabricate geometric light trapping structure with high scattering level (haze) and subsequently to increase
the short circuit current density (Jsc) in the solar cells.
Keywords: SiO2, Stöber method, dispersion, growth, TCO
I. INTRODUCTION
Colloidal silica spheres occupy a
prominent position in scientific and technological
research, because of their unique optical, biological
significances, as well as their important industrial
applications such as catalysis, pigments, pharmacy
and thin film substrates [1-4]. The specific
applications of SiO2 nanoparticles are highly
dependent on their size and size distribution. In
1968, Stöber, et al. [5] reported a method for the
synthesis of spherical silica nanoparticles from
aqueous alcohol solutions of silicon alkoxides in
the presence of ammonium hydroxide as a catalyst,
with the size of the particles depending on the type
of silicon alkoxide and alcohol. They reported that
the smallest particles were those prepared in
methanol solutions, and that the particle size
increases with the chain length of the alcohol, from
50 nm to 1 µm. Various works have being
published confirming that the choice of precursor
and reaction conditions govern the final form of the
silica spheres [6-8].
Transparent conductive oxides (TCOs)
with rough textured surface play a critical role in
the silicon based thin film solar cells. As a top
electrode for thin film silicon solar cells, textured
surface is required to scatter the incident light for
effective light trapping, and subsequently to
increase the short circuit current density (Jsc) in the
solar cells. Several techniques are used for
obtaining an optimized surface texture such as
chemical etching and natural growth using
chemical vapor deposition (CVD). The first
approach of chemical etching is to make the film
surface bumpy by using chemicals such as crater-
like (ZnO:Al film after etching in acids). This
approach can make the surface structures of
ZnO:Al films for effective light scattering,
however, the uniformly textured surface is hard to
be obtained by this way and also complicated
treatment is needed to obtain textured topography,
like soaking in an acid solution, lithography, etc.
which increases the fabrication cost and increase
the risk of introducing unexpected impurities. The
second approach of natural growth is to make the
grains at the film surface present pyramidal by
atmosphere pressure CVD of F doped SnO2, and
low pressure CVD of B doped ZnO by controlling
the growth process. [9-14] This method is highly-
efficient and can avoid the poor uniformity in the
corrosion method. Recently, novel types of high
haze SnO2:F TCO superstrates with double-texture
(W-texture) surface morphology have been also
developed. [15-19] These TCO superstrates
obtained by natural growth are aiming to boost the
scattering level (haze), especially at longer
wavelengths (λ>600 nm), however, generally
requires the vacuum and needs expensive metal
organic salts. Therefore, the cost is high by this
method. In order to reduce the cost and achieve
large scale industrial production, we develop an
effective way to fabricate a light-trapping TCO
structure based on dispersed Silica particles onto
glass for effective light trapping in thin film silicon
solar cells. More importantly, the silica particles
RESEARCH ARTICLE OPEN ACCESS
Van Thi Thanh Ho Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 6, ( Part -1) June 2016, pp.21-24
www.ijera.com 22 | P a g e
were dispersed onto glass by the bottom-up or
chemical approach involves a common route used
to synthesis silica particles from atomic or
molecular scale. Some of the widely used methods
to synthesize silica nanoparticles are sol-gel
process, reverse microemulsion, and flame
synthesis. The high temperature flame
decomposition of metal-organic precursors can be
produced silica nanoparticles but this process is
difficult in controlling the particle size,
morphology, and phase composition.
In this work, we present an effective and
reliable method to growth sub-micrometer mono-
disperse and multi-layer disperse silica on glass
through Stöber method and spray technique as a
chemical approach based on silica with uniform
size. Significantly, the pure silica particles were
produced through without using any surfactant
and/or stabilizer.
II. EXPERIMENTAL SECTION
II.1. Materials and characterizations
Ethanol 99.5% from Shimakyu’s pure
chemicals, 1-butanol 99%, isopropanol 99% and
tetraethoxysilane (TEOS), 98% was purchased
from Acros. Ammonium hydroxide (35%) was
purchased from Fisher Scientific, Spin-on-glass
(SOG) 211 from Honeywell. All chemicals were
used without further purification. The silica
particles size were characterized using scanning
electron microscopy (SEM, JEOL JSM-6500F).
II.2. Synthesis of silica sphere on glass via
modified Stöber method and spray technique
Figure1. The process for preparation SiO2 via
modified Stöber method and Spray technique
The textured surface based on silica for
effective light trapping was fabricated in this work.
First, the silica particles were synthesized through
Stöber method as a chemical approach. For a
typical synthesis procedure, 0.037 mmol was added
to a solution containing 11 ml of ethanol and 5 ml
of deionized water to form ammonia concentration
of 2.3 mM , followed by the addition of 0.088
mmol of TEOS in 10 mL ethanol to the solution
with vigorous stirring at room temperature. After
20 min reaction time, the resulting mixture was
changed from transparent solution to turbid
solution, suggesting silica colloidal is formed by
hydrolysis and condensation of tetraethoxysilane in
the presence of NH3 play as a catalyst and in water-
alcohol as a solvent. Next, the silica colloidal was
dispersed onto glass substrate through spray
technique. Corning EAGLE 2000 glasses was
served as a substrate, had been cleaned through
sonication in acetone for 5 min, cleaning in ethanol
for 5 min, rinsing with DI water, and then blowing
dry under N2 before using. Substrate temperature
was kept constant at room temperature during
spraying. The silica colloidal was sprayed with the
flow rate about ~2 mL/min. Final, textured
structure based on silica dispersion was formed by
heating it in the air at 200 o
C for 20 min.
III. RESULTS AND DISCUSSION
The silica particles (SiO2) are growth and
dispersed directly on the glass via modified Stöber
method and spray technique as Figure 2. The
formation mono-dispersed or multi-dispersed layer
of SiO2 on glass depends on the times of spraying.
Figure2. The process to fabricate texture surface
based on silica particle on glass through Stöber
method and spray technique.
Figure 3 shows all the silica spheres
preserve a spherical morphology and mono-
dispersion onto glass without aggregation between
particles or overlap to form layer-by-layer. We can
see that the SiO2 particles formation on the glass is
distributed uniformly. The diameter of spherical
silica is uniform at approximately 200 nm. It is
clearly observed that the SiO2 dispersed mono-
layer and could not observe the big aggregation for
all samples with different scale bar. This result can
be explained due to facile method to the prepare
Van Thi Thanh Ho Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 6, ( Part -1) June 2016, pp.21-24
www.ijera.com 23 | P a g e
SiO2 as well as highly controlled the step of spray
SiO2 on the glass. The good distribution and highly
uniformly as-synthesized SiO2 could open the new
wat to present an effective and reliable method to
growth sub-micrometer mono-disperse silica onto
glass through Stöber method as a chemical
approach, allowing one to attain a light-strapping
structure based on silica with uniform size and can
be obtained the high diffuse transmittance. More
important, the mono-layer or multi-layer of pure
silica particles on glass substrate can produce and
control by control the times of spray step.
Fig.3. The SEM micrographs for the spherical
silica in overview and high resolution images
(showing different the scale bar) prepared at
concentrations of ammonia about 2.3 mM (A-C).
The diameter of spherical silica is uniform at
approximately 200 nm.
Figure 4 shows the multi-layer of SiO2
particles on the glass by controlling the times of
spray step. The spraying times is increased 2 times
to control the SiO2 layers. From the Figure 4, we
can observe that the SiO2 particles formed layer by
layer on the glass substrate. Interestingly, the SiO2
particles formed multi-layer on the glass substrate
however, there did not observe the aggregation
between SiO2 particles. Depend on the times of
SiO2 layers that we want; it is facile to control the
spraying time which could improve the scattering
level (haze) of glass substrate. This result suggests
that the SiO2 particles was grown and dispersed the
silica particle on the glass via modified Stöber
method and spray technique is promising way to
fabricate the a novel geometric light trapping
structure based on silica particle that can enhance
the scattering level (haze) and subsequently to
increase the short circuit current density (Jsc) in the
solar cells.
Fig.4. The SEM micrographs for the multi-layer
spherical silica in overview and high resolution
images (showing different the scale bar) prepared
at concentrations of ammonia about 2.3 mM (A-B).
The diameter of spherical silica is uniform at
approximately 200 nm.
For the mechanism of SiO2 particles
formation, it is indicate that depending on the
particle formation mechanism in the sol -
precipitation process a large number of primary
particles is first nucleated in the initial high
supersaturated solution which called the induction
period. Then, the primary particles are rapidly
aggregated to form stable particles, which grow
with the further aggregation of primary particles.
After this particle induction period, any further
primary particles generated under supersaturation
are consumed for the growth of stable particles. In
this case, the resulting particles in the product
suspension were highly monodispersed in size and
spherical in shape, But, if the generation of primary
particles by supersaturation exceeds the
consumption of primary particles for the growth of
stable particles during sol -precipitation, new stable
particles are spontaneously formed by the self -
aggregation of the extra primary particles and a
multi modal distribution of particle. The
mechanism of SiO2 particles formation using the
Stöber method is shown below:
IV. CONCLUSIONS
We presented the fabrication of a novel
geometric light trapping structure based on silica
particle. This light trapping structure with good
morphology was fabricated through Stöber method
and spray technique. The silica particle size was
well controlled and uniform from ~200 nm. These
Van Thi Thanh Ho Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 6, ( Part -1) June 2016, pp.21-24
www.ijera.com 24 | P a g e
results open up the possibility to further fabricate
geometric light trapping structure with high
scattering level (haze) and subsequently to increase
the short circuit current density (Jsc) in the solar
cells.
ACKNOWLEGMENT: We would like to thank
Professor Lu-Sheng Hong, National Taiwan
University of Science and Technology Dr. Nam
Giang Nguyen, Department of Engineering, Alstom
PhuMy Power Service, Vietnam, Dr. Long Giang
Bach, NTT Institute of Hi-Technology, Nguyen Tat
Thanh University, Ho Chi Minh City, Vietnam
were supported for this work.
REFERENCES
[1] R.K. Iler, The Colloid Chemistry of Silica
and Silicates, Cornell University Press,
Ithaca, New York, USA, 1955, pp. 730-787.
[2] G. Herberg, Synthesis of monodispersed
silica powders II. Controlled growth reaction
and continuous production process, J. Eur.
Ceram. Soc. 14 (3) (1994) 205-214.
[3] U. Jeong, Y. Wang, M. Ibisate, Y. Xia,
Some new developments in the synthesis,
functionalization, and utilization of
monodisperse colloidal spheres, Adv. Funct.
Mater. 15 (12) (2005) 1907-1921.
[4] J.D. Wright, N.A.J.M. Sommerdijk, Sol-Gel
Materials: Chemistry and Applications,
Gordon and Breach Science Publishers,
Amsterdam, 2001, pp. 1-20.
[5] W. Stöber, A. Fink, E. Bohn, Controlled
growth of monodisperse silica spheres in the
micron size range, J. Colloid Interface Sci.
26 (1) (1968) 62-69
[6] van Blaaderen, J.V. Geest, A. Vrij,
Monodisperse colloidal silica spheres from
tetraalkoxylanes: Particle formation and
growth mechanism, J. Colloid Interface Sci.
154 (2) (1992) 481-501.
[7] Blaaderen, A.P.M. Kentgens, Particle
morphology and chemical microstructure of
colloidal silica spheres made from
alkoxylanes, J. Non-Cryst. Solids 149 (3)
(1992) 161-178.
[8] T. Yokoi, Y. Sakamoto, O. Terasaki, Y.
Kubota, T. Okubo, T. Tatsumi, Periodic
arrangement of silica nanospheres assisted
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[10] Löffl A, Kerber H, Schock H-W, Kluth O,
Houben L, Rech B, Wagner H. Solid State
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Schöpe G, Beneking C, Wagner H, Löffl A,
Schock HW. Thin Solid
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[12] Kluth O, Schöpe G, Hüpkes J, Agashe C,
Müller J, Rech B. Thin Solid
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[13] Hüpkes J, Rech B, Kluth O, Repmann T,
Zwaygardt B, Müller J, Drese R, Wuttig
M. Sol. Energy Mater. Sol.
Cells. 2006;90:3054–3060.
[14] Berginski M, Hüpkes J, Schulte M, Schöpe
G, Stiebig H, Rech B, Wuttig M. J. Appl.
Phys.2007;101:074903.
[15] Zhu H, Hüpkes J, Bunte E, Owen J, Huang
SM. Sol. Energy Mater. Sol.
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[16] Jost G, Bunte E, Worbs J, Siekmann H,
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[17] Fernández S, de Abril O, Naranjo FB,
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Growth and Dispersion the Silica Particle on the Glass via Modified Stöber Method and Spray Technique

  • 1. Van Thi Thanh Ho Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 6, ( Part -1) June 2016, pp.21-24 www.ijera.com 21 | P a g e Growth and Dispersion the Silica Particle on the Glass via Modified Stöber Method and Spray Technique Van Thi Thanh Ho* 1 Hochiminh City University of Natural Resources and Environment (HCMUNRE), Vietnam ABSTRACT We presented the fabrication of a novel geometric light trapping structure based on silica particle. This light trapping structure with good morphology was fabricated through modified Stöber method and spray technique. More importantly, the silica particles were dispersed onto glass by using bottom-up or chemical approach involves a common route used to synthesis silica particles from atomic or molecular scale. An optimized synthesis condition is a combination of optimal values of each reaction parameter of Stöber method that could produce homogenous and mono-dispersed silica nanoparticles with uniform size. The diameter of silica particles can be varied from 200, 430, 560, 460 nm by increasing concentrations of ammonia from 2.33 mM to 4.65 mM, 9.31 mM and 13.96 mM, respectively. We found that the silica particle size was well controlled and uniform from ~200 nm to 560 nm by controlling the ammonia concentration. These results open up the possibility to further fabricate geometric light trapping structure with high scattering level (haze) and subsequently to increase the short circuit current density (Jsc) in the solar cells. Keywords: SiO2, Stöber method, dispersion, growth, TCO I. INTRODUCTION Colloidal silica spheres occupy a prominent position in scientific and technological research, because of their unique optical, biological significances, as well as their important industrial applications such as catalysis, pigments, pharmacy and thin film substrates [1-4]. The specific applications of SiO2 nanoparticles are highly dependent on their size and size distribution. In 1968, Stöber, et al. [5] reported a method for the synthesis of spherical silica nanoparticles from aqueous alcohol solutions of silicon alkoxides in the presence of ammonium hydroxide as a catalyst, with the size of the particles depending on the type of silicon alkoxide and alcohol. They reported that the smallest particles were those prepared in methanol solutions, and that the particle size increases with the chain length of the alcohol, from 50 nm to 1 µm. Various works have being published confirming that the choice of precursor and reaction conditions govern the final form of the silica spheres [6-8]. Transparent conductive oxides (TCOs) with rough textured surface play a critical role in the silicon based thin film solar cells. As a top electrode for thin film silicon solar cells, textured surface is required to scatter the incident light for effective light trapping, and subsequently to increase the short circuit current density (Jsc) in the solar cells. Several techniques are used for obtaining an optimized surface texture such as chemical etching and natural growth using chemical vapor deposition (CVD). The first approach of chemical etching is to make the film surface bumpy by using chemicals such as crater- like (ZnO:Al film after etching in acids). This approach can make the surface structures of ZnO:Al films for effective light scattering, however, the uniformly textured surface is hard to be obtained by this way and also complicated treatment is needed to obtain textured topography, like soaking in an acid solution, lithography, etc. which increases the fabrication cost and increase the risk of introducing unexpected impurities. The second approach of natural growth is to make the grains at the film surface present pyramidal by atmosphere pressure CVD of F doped SnO2, and low pressure CVD of B doped ZnO by controlling the growth process. [9-14] This method is highly- efficient and can avoid the poor uniformity in the corrosion method. Recently, novel types of high haze SnO2:F TCO superstrates with double-texture (W-texture) surface morphology have been also developed. [15-19] These TCO superstrates obtained by natural growth are aiming to boost the scattering level (haze), especially at longer wavelengths (λ>600 nm), however, generally requires the vacuum and needs expensive metal organic salts. Therefore, the cost is high by this method. In order to reduce the cost and achieve large scale industrial production, we develop an effective way to fabricate a light-trapping TCO structure based on dispersed Silica particles onto glass for effective light trapping in thin film silicon solar cells. More importantly, the silica particles RESEARCH ARTICLE OPEN ACCESS
  • 2. Van Thi Thanh Ho Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 6, ( Part -1) June 2016, pp.21-24 www.ijera.com 22 | P a g e were dispersed onto glass by the bottom-up or chemical approach involves a common route used to synthesis silica particles from atomic or molecular scale. Some of the widely used methods to synthesize silica nanoparticles are sol-gel process, reverse microemulsion, and flame synthesis. The high temperature flame decomposition of metal-organic precursors can be produced silica nanoparticles but this process is difficult in controlling the particle size, morphology, and phase composition. In this work, we present an effective and reliable method to growth sub-micrometer mono- disperse and multi-layer disperse silica on glass through Stöber method and spray technique as a chemical approach based on silica with uniform size. Significantly, the pure silica particles were produced through without using any surfactant and/or stabilizer. II. EXPERIMENTAL SECTION II.1. Materials and characterizations Ethanol 99.5% from Shimakyu’s pure chemicals, 1-butanol 99%, isopropanol 99% and tetraethoxysilane (TEOS), 98% was purchased from Acros. Ammonium hydroxide (35%) was purchased from Fisher Scientific, Spin-on-glass (SOG) 211 from Honeywell. All chemicals were used without further purification. The silica particles size were characterized using scanning electron microscopy (SEM, JEOL JSM-6500F). II.2. Synthesis of silica sphere on glass via modified Stöber method and spray technique Figure1. The process for preparation SiO2 via modified Stöber method and Spray technique The textured surface based on silica for effective light trapping was fabricated in this work. First, the silica particles were synthesized through Stöber method as a chemical approach. For a typical synthesis procedure, 0.037 mmol was added to a solution containing 11 ml of ethanol and 5 ml of deionized water to form ammonia concentration of 2.3 mM , followed by the addition of 0.088 mmol of TEOS in 10 mL ethanol to the solution with vigorous stirring at room temperature. After 20 min reaction time, the resulting mixture was changed from transparent solution to turbid solution, suggesting silica colloidal is formed by hydrolysis and condensation of tetraethoxysilane in the presence of NH3 play as a catalyst and in water- alcohol as a solvent. Next, the silica colloidal was dispersed onto glass substrate through spray technique. Corning EAGLE 2000 glasses was served as a substrate, had been cleaned through sonication in acetone for 5 min, cleaning in ethanol for 5 min, rinsing with DI water, and then blowing dry under N2 before using. Substrate temperature was kept constant at room temperature during spraying. The silica colloidal was sprayed with the flow rate about ~2 mL/min. Final, textured structure based on silica dispersion was formed by heating it in the air at 200 o C for 20 min. III. RESULTS AND DISCUSSION The silica particles (SiO2) are growth and dispersed directly on the glass via modified Stöber method and spray technique as Figure 2. The formation mono-dispersed or multi-dispersed layer of SiO2 on glass depends on the times of spraying. Figure2. The process to fabricate texture surface based on silica particle on glass through Stöber method and spray technique. Figure 3 shows all the silica spheres preserve a spherical morphology and mono- dispersion onto glass without aggregation between particles or overlap to form layer-by-layer. We can see that the SiO2 particles formation on the glass is distributed uniformly. The diameter of spherical silica is uniform at approximately 200 nm. It is clearly observed that the SiO2 dispersed mono- layer and could not observe the big aggregation for all samples with different scale bar. This result can be explained due to facile method to the prepare
  • 3. Van Thi Thanh Ho Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 6, ( Part -1) June 2016, pp.21-24 www.ijera.com 23 | P a g e SiO2 as well as highly controlled the step of spray SiO2 on the glass. The good distribution and highly uniformly as-synthesized SiO2 could open the new wat to present an effective and reliable method to growth sub-micrometer mono-disperse silica onto glass through Stöber method as a chemical approach, allowing one to attain a light-strapping structure based on silica with uniform size and can be obtained the high diffuse transmittance. More important, the mono-layer or multi-layer of pure silica particles on glass substrate can produce and control by control the times of spray step. Fig.3. The SEM micrographs for the spherical silica in overview and high resolution images (showing different the scale bar) prepared at concentrations of ammonia about 2.3 mM (A-C). The diameter of spherical silica is uniform at approximately 200 nm. Figure 4 shows the multi-layer of SiO2 particles on the glass by controlling the times of spray step. The spraying times is increased 2 times to control the SiO2 layers. From the Figure 4, we can observe that the SiO2 particles formed layer by layer on the glass substrate. Interestingly, the SiO2 particles formed multi-layer on the glass substrate however, there did not observe the aggregation between SiO2 particles. Depend on the times of SiO2 layers that we want; it is facile to control the spraying time which could improve the scattering level (haze) of glass substrate. This result suggests that the SiO2 particles was grown and dispersed the silica particle on the glass via modified Stöber method and spray technique is promising way to fabricate the a novel geometric light trapping structure based on silica particle that can enhance the scattering level (haze) and subsequently to increase the short circuit current density (Jsc) in the solar cells. Fig.4. The SEM micrographs for the multi-layer spherical silica in overview and high resolution images (showing different the scale bar) prepared at concentrations of ammonia about 2.3 mM (A-B). The diameter of spherical silica is uniform at approximately 200 nm. For the mechanism of SiO2 particles formation, it is indicate that depending on the particle formation mechanism in the sol - precipitation process a large number of primary particles is first nucleated in the initial high supersaturated solution which called the induction period. Then, the primary particles are rapidly aggregated to form stable particles, which grow with the further aggregation of primary particles. After this particle induction period, any further primary particles generated under supersaturation are consumed for the growth of stable particles. In this case, the resulting particles in the product suspension were highly monodispersed in size and spherical in shape, But, if the generation of primary particles by supersaturation exceeds the consumption of primary particles for the growth of stable particles during sol -precipitation, new stable particles are spontaneously formed by the self - aggregation of the extra primary particles and a multi modal distribution of particle. The mechanism of SiO2 particles formation using the Stöber method is shown below: IV. CONCLUSIONS We presented the fabrication of a novel geometric light trapping structure based on silica particle. This light trapping structure with good morphology was fabricated through Stöber method and spray technique. The silica particle size was well controlled and uniform from ~200 nm. These
  • 4. Van Thi Thanh Ho Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 6, ( Part -1) June 2016, pp.21-24 www.ijera.com 24 | P a g e results open up the possibility to further fabricate geometric light trapping structure with high scattering level (haze) and subsequently to increase the short circuit current density (Jsc) in the solar cells. ACKNOWLEGMENT: We would like to thank Professor Lu-Sheng Hong, National Taiwan University of Science and Technology Dr. Nam Giang Nguyen, Department of Engineering, Alstom PhuMy Power Service, Vietnam, Dr. Long Giang Bach, NTT Institute of Hi-Technology, Nguyen Tat Thanh University, Ho Chi Minh City, Vietnam were supported for this work. REFERENCES [1] R.K. Iler, The Colloid Chemistry of Silica and Silicates, Cornell University Press, Ithaca, New York, USA, 1955, pp. 730-787. [2] G. Herberg, Synthesis of monodispersed silica powders II. Controlled growth reaction and continuous production process, J. Eur. Ceram. Soc. 14 (3) (1994) 205-214. [3] U. Jeong, Y. Wang, M. Ibisate, Y. Xia, Some new developments in the synthesis, functionalization, and utilization of monodisperse colloidal spheres, Adv. Funct. Mater. 15 (12) (2005) 1907-1921. [4] J.D. Wright, N.A.J.M. Sommerdijk, Sol-Gel Materials: Chemistry and Applications, Gordon and Breach Science Publishers, Amsterdam, 2001, pp. 1-20. [5] W. Stöber, A. Fink, E. Bohn, Controlled growth of monodisperse silica spheres in the micron size range, J. Colloid Interface Sci. 26 (1) (1968) 62-69 [6] van Blaaderen, J.V. Geest, A. Vrij, Monodisperse colloidal silica spheres from tetraalkoxylanes: Particle formation and growth mechanism, J. Colloid Interface Sci. 154 (2) (1992) 481-501. [7] Blaaderen, A.P.M. Kentgens, Particle morphology and chemical microstructure of colloidal silica spheres made from alkoxylanes, J. Non-Cryst. Solids 149 (3) (1992) 161-178. [8] T. Yokoi, Y. Sakamoto, O. Terasaki, Y. Kubota, T. Okubo, T. Tatsumi, Periodic arrangement of silica nanospheres assisted by amino acids, J. Am. Chem. Soc. 128 (42) (2006) 13664-13665. [9] Anna Selvan JA. IMT Progress Report. III. IMT: Neuchatel; 1995. pp. 1–7. [10] Löffl A, Kerber H, Schock H-W, Kluth O, Houben L, Rech B, Wagner H. Solid State Phenomena.1999;67–68:277–282. [11] Kluth O, Rech B, Houben L, Wieder S, Schöpe G, Beneking C, Wagner H, Löffl A, Schock HW. Thin Solid Films. 1999;351:247–253. [12] Kluth O, Schöpe G, Hüpkes J, Agashe C, Müller J, Rech B. Thin Solid Films. 2003;442:80–85. [13] Hüpkes J, Rech B, Kluth O, Repmann T, Zwaygardt B, Müller J, Drese R, Wuttig M. Sol. Energy Mater. Sol. Cells. 2006;90:3054–3060. [14] Berginski M, Hüpkes J, Schulte M, Schöpe G, Stiebig H, Rech B, Wuttig M. J. Appl. Phys.2007;101:074903. [15] Zhu H, Hüpkes J, Bunte E, Owen J, Huang SM. Sol. Energy Mater. Sol. Cells. 2011;95:964–968. [16] Jost G, Bunte E, Worbs J, Siekmann H, Hüpkes J. Proceedings of the 25th European Photovoltaic Solar Energy Conference and Exhibition. WIP: Munich; 2010. pp. 3078– 3082. [17] Fernández S, de Abril O, Naranjo FB, Gandía JJ. Sol. Energy Mater. Sol. Cells. 2011;95:2281–2286. [18] Johnson EV, Prod′homme P, Boniface C, Huet K, Emeraud T, Cabarrocas PRocai. Sol. Energy Mater. Sol. Cells. 2011;95:2823–2830. [19] Pust SE, Becker J-P, Worbs J, Klemm SO, Mayrhofer KJJ, Hüpkes J. J. Electrochem. Soc.2011; 158:413–419. D.