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(Research in solar cell)
Perovskite solar cells:
Perovskitesolar cells are solar cells that include
a perovskite structured material as the active layer.
Most commonly, this is a solution-processed hybrid
organic-inorganic tin or lead halide based material.
Efficiencies have increased from below 5% at their
first usage in 2009 to over 20% in 2014, making them
a very rapidly advancing technology and a hot topic in
the solar cell field. Perovskite solar cells are also
forecast to be extremely cheap to scale up, making
them a very attractive option for commercialisation.
(Perovskite solar cell research cell efficiency progress)
Liquid inks
In 2014, researchers at California nano system institute discovered using kestirite
and perovskite improved electric power conversion efficiency for solar cells.
Upconversion and Downconversion:
Photon upconversion is the process of using two low-energy (e.g., infrared) photons to produce
one higher energy photon; down conversion is the process of using one high energy photon
(e.g.,, ultraviolet) to produce two lower energy photons. Either of these techniques could be used
to produce higher efficiency solar cells by allowing solar photons to be more efficiently used.
The difficulty, however, is that the conversion efficiency of existing phosphors exhibiting up- or
down-conversion is low, and is typically narrow band.
One up conversion technique is to incorporate lathanides doped materials
taking advantage of their luminescence to convert infrared radiation to visible light.
Upconversion process occurs when two infrared photons are absorbed by rare-earth ions to
generate a (high-energy) absorbable photon. As example, the energy transfer upconversion
process (ETU), consists in successive transfer processes between excited ions in the near
infrared. The upconverter material could be placed below the solar cell to absorb the infrared
light that passes through the silicon. Useful ions are most commonly found in the trivalent
state. Er+ ions have been the most used. Er3+
ions absorb solar radiation around 1.54 µm. Two Er3+
ions that have absorbed this radiation can interact with each other through an upconversion
process. The excited ion emits light above the Si bandgap that is absorbed by the solar cell and
creates an additional electron–hole pair that can generate current. However, the increased
efficiency was small. In addition, fluoroindate glasses have low phonon energy and have been
proposed as suitable matrix doped with Ho3+
ions.
Light-absorbing dyes Dye-sensitized solar cells (DSSCs) are made of low-cost materials
and do not need elaborate manufacturing equipment, so they can be made in a DIY fashion. In
bulk it should be significantly less expensive than older solid-state cell designs. DSSC's can be
engineered into flexible sheets and although its conversion efficiency is less than the best thin
film cells, its price/performance ratio may be
high enough to allow them to compete
with fossil fuel electrical generation.
Typically a ruthenium metalorganic dye (Ru-
centered) is used as a monolayer of light-
absorbing material. The dye-sensitized solar
cell depends on a mesoporous layer
of nanoparticulate titanium dioxide to greatly
amplify the surface area (200–300 m2/g TiO
2, as compared to approximately 10 m2/g of
flat single crystal). The photogenerated
electrons from the light absorbing dye are
passed on to the n-type TiO
2 and the holes are absorbed by
an electrolyte on the other side of the dye. The
circuit is completed by a redox couple in the electrolyte, which can be liquid or solid. This type
of cell allows more flexible use of materials and is typically manufactured by screen
printing or ultrasonic nozzles, with the potential for lower processing costs than those used for
bulk solar cells. However, the dyes in these cells also suffer from degradation under heat
and UV light and the cell casing is difficult to seal due to the solvents used in assembly. The first
commercial shipment of DSSC solar modules occurred in July 2009 from G24i Innovations.[56]
Quantum dots
Quantum dot solar cells (QDSCs) are based on the Gratzel cell, or dye-sensitized solar
cell architecture, but employ low band gap semiconductor nanoparticles, fabricated with
crystallite sizes small enough to form quantum dots (such as CdS, CdSe, Sb
2S
3, PbS, etc.), instead of organic or organometallic
dyes as light absorbers. QD's size quantization allows
for the band gap to be tuned by simply changing
particle size. They also have high extinction
coefficients and have shown the possibility
of multiple exciton generation.[57]
In a QDSC, a mesoporous layer of titanium
dioxide nanoparticles forms the backbone of the cell,
much like in a DSSC. This TiO
2 layer can then be made photoactive by coating with
semiconductor quantum dots using chemical bath deposition, electrophoretic deposition or
successive ionic layer adsorption and reaction. The electrical circuit is then completed through
the use of a liquid or solid redox couple. The efficiency of QDSCs has increased to over 5%
shown for both liquid-junction and
solid state cells. In an effort to decrease
production costs, the Prashant
Kamat research group demonstrated a
solar paint made with TiO
2 and CdSe that can be applied using a
one-step method to any conductive
surface with efficiencies over 1%.
Organic/polymer solar cells
Organic solar cells and polymer solar
cells are built from thin films (typically
100 nm) of organic
semiconductors including polymers,
such as polyphenylene vinylene and
small-moliculecompounds like copper
phthalocyanine (a blue or green
organic pigment) and carbon
fullerenes and fullerene derivatives
such as PCBM.
They can be processed from liquid
solution, offering the possibility of a
simple roll-to-roll printing process,
potentially leading to inexpensive,
large-scale production. In addition,
these cells could be beneficial for some
applications where mechanical
flexibility and disposability are
important. Current cell efficiencies are, however, very low, and practical devices are essentially
non-existent.
( Swapping tellurium for sulfur improves light absorption in organic solar cells)
Energy conversion efficiencies achieved to date using conductive polymers are very low
compared to inorganic materials. However, Konarka Power Plastic reached efficiency of
8.3%[63] and organic tandem cells in 2012 reached 11.1%.
The active region of an organic device consists of two materials, one electron donor and one
electron acceptor. When a photon is converted into an electron hole pair, typically in the donor
material, the charges tend to remain bound in the form of an exciton, separating when the exciton
diffuses to the donor-acceptor interface, unlike most other solar cell types. The short exciton
diffusion lengths of most polymer systems tend to limit the efficiency of such devices.
Nanostructured interfaces, sometimes in the form of bulk heterojunctions, can improve
performance.
In 2011, MIT and Michigan State researchers developed solar cells with a power efficiency close
to 2% with a transparency to the human eye greater than 65%, achieved by selectively absorbing
the ultraviolet and near-infrared parts of the spectrum with small-molecule
compounds. Researchers at UCLA more recently developed an analogous polymer solar cell,
following the same approach, that is 70% transparent and has a 4% power conversion
efficiency. These lightweight, flexible cells can be produced in bulk at a low cost and could be
used to create power generating windows.
In 2013, researchers announced polymer cells with some 3% efficiency. They used block
copolymers, self-assembling organic materials that arrange themselves into distinct layers. The
research focused on P3HT-b-PFTBT that separates into bands some 16 nanometers wide.
Adaptive cells
Adaptive cells change their absorption/reflection characteristics depending to respond to
environmental conditions. An
adaptive material responds to the
intensity and angle of incident light.
At the part of the cell where the
light is most intense, the cell surface
changes from reflective to adaptive,
allowing the light to penetrate the
cell. The other parts of the cell
remain reflective increasing the
retention of the absorbed light
within the cell.
( Solar cell as lighter as soap
bubble)
In 2014 a system was developed that combined an adaptive surface with a glass substrate that
redirect the absorbed to a light absorber on the edges of the sheet. The system also includes an
array of fixed lenses/mirrors to concentrate light onto the adaptive surface. As the day continues,
the concentrated light moves along the surface of the cell. That surface switches from reflective
to adaptive when the light is most concentrated and back to reflective after the light moves along.
Surface texturing
For the past years, researchers have been trying to reduce the price of solar cells while
maximizing efficiency. Thin-film solar cell is a cost-effective second generation solar cell with
much reduced thickness at the expense of light absorption efficiency. Efforts to maximize light
absorption efficiency with reduced thickness have been made. Surface texturing is one of
techniques used to reduce optical losses to maximize light absorbed. Currently, surface texturing
techniques on silicon photovoltaics are drawing much attention. Surface texturing could be done
in multiple ways. Etching single crystalline silicon substrate can produce randomly distributed
square based pyramids on the surface using anisotropic etchants. Recent studies show that c-Si
wafers could be etched down to form nano-scale inverted pyramids. Multicrystalline silicon solar
cells, due to poorer crystallographic quality, are less effective than single crystal solar cells, but
mc-Si solar cells are still being used widely due to less manufacturing difficulties. It is reported
that multicrystalline solar cells can be surface-textured to yield solar energy conversion
efficiency comparable to that of monocrystalline silicon cells, through isotropic etching or
photolithography techniques. Incident light rays onto a textured surface do not reflect back out to
the air as opposed to rays onto a flat surface. Rather some light rays are bounced back onto the
other surface again due to the geometry of the surface. This process significantly improves light
to electricity conversion efficiency, due to increased light absorption. In 2012, researchers at
MIT reported that c-Si films textured with nanoscale inverted pyramids could achieve light
absorption comparable to 30 times thicker planar c-Si. In combination with anti-reflective
coating, surface texturing technique can effectively trap light rays within a thin film silicon solar
cell. Consequently, required thickness for solar cells decreases with the increased absorption of
light rays.
 Ref…………………..
1. Shockley, William; Queisser, Hans J. (1961). “detailed balance limit of efficiency of
p-n junction solar cells” Journal of Applied Physics. 32 (3):
510. dio:10.1063/1/736034.
2. solar cell. chemistryexplained.co
3. Technology road map “solar photovoltaic energy’. IEA. 2014. Archived from the
original on 7 October 2014. Retrieved 7 October 2014.
4. "Light sensitive device " U.S. Patent 2,402,662 Issue date: June 1946
5. Williams, Neville (2005). Chasing the Sun: Solar Adventures Around the
World. New Society Publishers. p. 84. ISBN 9781550923124

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research in solar cell

  • 1. (Research in solar cell) Perovskite solar cells: Perovskitesolar cells are solar cells that include a perovskite structured material as the active layer. Most commonly, this is a solution-processed hybrid organic-inorganic tin or lead halide based material. Efficiencies have increased from below 5% at their first usage in 2009 to over 20% in 2014, making them a very rapidly advancing technology and a hot topic in the solar cell field. Perovskite solar cells are also forecast to be extremely cheap to scale up, making them a very attractive option for commercialisation. (Perovskite solar cell research cell efficiency progress) Liquid inks In 2014, researchers at California nano system institute discovered using kestirite and perovskite improved electric power conversion efficiency for solar cells. Upconversion and Downconversion: Photon upconversion is the process of using two low-energy (e.g., infrared) photons to produce one higher energy photon; down conversion is the process of using one high energy photon (e.g.,, ultraviolet) to produce two lower energy photons. Either of these techniques could be used to produce higher efficiency solar cells by allowing solar photons to be more efficiently used. The difficulty, however, is that the conversion efficiency of existing phosphors exhibiting up- or down-conversion is low, and is typically narrow band. One up conversion technique is to incorporate lathanides doped materials taking advantage of their luminescence to convert infrared radiation to visible light. Upconversion process occurs when two infrared photons are absorbed by rare-earth ions to generate a (high-energy) absorbable photon. As example, the energy transfer upconversion process (ETU), consists in successive transfer processes between excited ions in the near infrared. The upconverter material could be placed below the solar cell to absorb the infrared light that passes through the silicon. Useful ions are most commonly found in the trivalent state. Er+ ions have been the most used. Er3+ ions absorb solar radiation around 1.54 µm. Two Er3+ ions that have absorbed this radiation can interact with each other through an upconversion process. The excited ion emits light above the Si bandgap that is absorbed by the solar cell and creates an additional electron–hole pair that can generate current. However, the increased efficiency was small. In addition, fluoroindate glasses have low phonon energy and have been proposed as suitable matrix doped with Ho3+ ions.
  • 2. Light-absorbing dyes Dye-sensitized solar cells (DSSCs) are made of low-cost materials and do not need elaborate manufacturing equipment, so they can be made in a DIY fashion. In bulk it should be significantly less expensive than older solid-state cell designs. DSSC's can be engineered into flexible sheets and although its conversion efficiency is less than the best thin film cells, its price/performance ratio may be high enough to allow them to compete with fossil fuel electrical generation. Typically a ruthenium metalorganic dye (Ru- centered) is used as a monolayer of light- absorbing material. The dye-sensitized solar cell depends on a mesoporous layer of nanoparticulate titanium dioxide to greatly amplify the surface area (200–300 m2/g TiO 2, as compared to approximately 10 m2/g of flat single crystal). The photogenerated electrons from the light absorbing dye are passed on to the n-type TiO 2 and the holes are absorbed by an electrolyte on the other side of the dye. The circuit is completed by a redox couple in the electrolyte, which can be liquid or solid. This type of cell allows more flexible use of materials and is typically manufactured by screen printing or ultrasonic nozzles, with the potential for lower processing costs than those used for bulk solar cells. However, the dyes in these cells also suffer from degradation under heat and UV light and the cell casing is difficult to seal due to the solvents used in assembly. The first commercial shipment of DSSC solar modules occurred in July 2009 from G24i Innovations.[56] Quantum dots Quantum dot solar cells (QDSCs) are based on the Gratzel cell, or dye-sensitized solar cell architecture, but employ low band gap semiconductor nanoparticles, fabricated with crystallite sizes small enough to form quantum dots (such as CdS, CdSe, Sb 2S 3, PbS, etc.), instead of organic or organometallic dyes as light absorbers. QD's size quantization allows for the band gap to be tuned by simply changing particle size. They also have high extinction coefficients and have shown the possibility of multiple exciton generation.[57] In a QDSC, a mesoporous layer of titanium dioxide nanoparticles forms the backbone of the cell, much like in a DSSC. This TiO 2 layer can then be made photoactive by coating with semiconductor quantum dots using chemical bath deposition, electrophoretic deposition or successive ionic layer adsorption and reaction. The electrical circuit is then completed through the use of a liquid or solid redox couple. The efficiency of QDSCs has increased to over 5%
  • 3. shown for both liquid-junction and solid state cells. In an effort to decrease production costs, the Prashant Kamat research group demonstrated a solar paint made with TiO 2 and CdSe that can be applied using a one-step method to any conductive surface with efficiencies over 1%. Organic/polymer solar cells Organic solar cells and polymer solar cells are built from thin films (typically 100 nm) of organic semiconductors including polymers, such as polyphenylene vinylene and small-moliculecompounds like copper phthalocyanine (a blue or green organic pigment) and carbon fullerenes and fullerene derivatives such as PCBM. They can be processed from liquid solution, offering the possibility of a simple roll-to-roll printing process, potentially leading to inexpensive, large-scale production. In addition, these cells could be beneficial for some applications where mechanical flexibility and disposability are important. Current cell efficiencies are, however, very low, and practical devices are essentially non-existent. ( Swapping tellurium for sulfur improves light absorption in organic solar cells) Energy conversion efficiencies achieved to date using conductive polymers are very low compared to inorganic materials. However, Konarka Power Plastic reached efficiency of 8.3%[63] and organic tandem cells in 2012 reached 11.1%. The active region of an organic device consists of two materials, one electron donor and one electron acceptor. When a photon is converted into an electron hole pair, typically in the donor material, the charges tend to remain bound in the form of an exciton, separating when the exciton diffuses to the donor-acceptor interface, unlike most other solar cell types. The short exciton diffusion lengths of most polymer systems tend to limit the efficiency of such devices.
  • 4. Nanostructured interfaces, sometimes in the form of bulk heterojunctions, can improve performance. In 2011, MIT and Michigan State researchers developed solar cells with a power efficiency close to 2% with a transparency to the human eye greater than 65%, achieved by selectively absorbing the ultraviolet and near-infrared parts of the spectrum with small-molecule compounds. Researchers at UCLA more recently developed an analogous polymer solar cell, following the same approach, that is 70% transparent and has a 4% power conversion efficiency. These lightweight, flexible cells can be produced in bulk at a low cost and could be used to create power generating windows. In 2013, researchers announced polymer cells with some 3% efficiency. They used block copolymers, self-assembling organic materials that arrange themselves into distinct layers. The research focused on P3HT-b-PFTBT that separates into bands some 16 nanometers wide. Adaptive cells Adaptive cells change their absorption/reflection characteristics depending to respond to environmental conditions. An adaptive material responds to the intensity and angle of incident light. At the part of the cell where the light is most intense, the cell surface changes from reflective to adaptive, allowing the light to penetrate the cell. The other parts of the cell remain reflective increasing the retention of the absorbed light within the cell. ( Solar cell as lighter as soap bubble) In 2014 a system was developed that combined an adaptive surface with a glass substrate that redirect the absorbed to a light absorber on the edges of the sheet. The system also includes an array of fixed lenses/mirrors to concentrate light onto the adaptive surface. As the day continues, the concentrated light moves along the surface of the cell. That surface switches from reflective to adaptive when the light is most concentrated and back to reflective after the light moves along. Surface texturing For the past years, researchers have been trying to reduce the price of solar cells while maximizing efficiency. Thin-film solar cell is a cost-effective second generation solar cell with much reduced thickness at the expense of light absorption efficiency. Efforts to maximize light absorption efficiency with reduced thickness have been made. Surface texturing is one of techniques used to reduce optical losses to maximize light absorbed. Currently, surface texturing techniques on silicon photovoltaics are drawing much attention. Surface texturing could be done
  • 5. in multiple ways. Etching single crystalline silicon substrate can produce randomly distributed square based pyramids on the surface using anisotropic etchants. Recent studies show that c-Si wafers could be etched down to form nano-scale inverted pyramids. Multicrystalline silicon solar cells, due to poorer crystallographic quality, are less effective than single crystal solar cells, but mc-Si solar cells are still being used widely due to less manufacturing difficulties. It is reported that multicrystalline solar cells can be surface-textured to yield solar energy conversion efficiency comparable to that of monocrystalline silicon cells, through isotropic etching or photolithography techniques. Incident light rays onto a textured surface do not reflect back out to the air as opposed to rays onto a flat surface. Rather some light rays are bounced back onto the other surface again due to the geometry of the surface. This process significantly improves light to electricity conversion efficiency, due to increased light absorption. In 2012, researchers at MIT reported that c-Si films textured with nanoscale inverted pyramids could achieve light absorption comparable to 30 times thicker planar c-Si. In combination with anti-reflective coating, surface texturing technique can effectively trap light rays within a thin film silicon solar cell. Consequently, required thickness for solar cells decreases with the increased absorption of light rays.  Ref………………….. 1. Shockley, William; Queisser, Hans J. (1961). “detailed balance limit of efficiency of p-n junction solar cells” Journal of Applied Physics. 32 (3): 510. dio:10.1063/1/736034. 2. solar cell. chemistryexplained.co 3. Technology road map “solar photovoltaic energy’. IEA. 2014. Archived from the original on 7 October 2014. Retrieved 7 October 2014. 4. "Light sensitive device " U.S. Patent 2,402,662 Issue date: June 1946 5. Williams, Neville (2005). Chasing the Sun: Solar Adventures Around the World. New Society Publishers. p. 84. ISBN 9781550923124