A three-stage process starting with the deposition of
(In,Ga)<sub>2</sub>Se<sub>3</sub> precursor films has been successful in
the fabrication of graded band-gap Cu(In,Ga)Se<sub>2</sub> thin films.
In this work we examine (1) the reaction of Cu+Se with (In,Ga)<sub>2
</sub>Se<sub>3</sub>, which leads to a spontaneous grading in the Ga
content as a function of depth through the film, and (2) modification of
the Ga content in the surface region of the film through a final
deposition of In+Ga+Se. We show how band-gap grading can be enhanced by
the formation of nonuniform precursors, how counterdiffusion limits the
degree of grading possible in the surface region, and how the Cu<sub>x
</sub>Se secondary phase acts to homogenize the film composition
Several factors that may affect the net discoloration rate of the
ethylene-vinyl acetate (EVA) copolymer encapsulants used in
crystalline-Si photovoltaic (c-Si PV) modules upon accelerated exposure
have been investigated by employing UV-visible spectrophotometry,
spectrocolorimetry, and fluorescence analysis. A number of laminated
films, including the two typical EVA formulations, A9918 and 15295, were
studied. The results indicate that the rate of EVA discoloration is
affected by the: (1) curing agent and curing conditions; (2) presence
and concentration of curing-generated, UV-excitable chromophores; (3) UV
light intensity; (4) loss rate of the UV absorber, Cyasorb UV 5311; (5)
lamination; (6) film thickness; and (7) photobleaching rate due to the
diffusion of air into the laminated films. In general, the loss rate of
the UV absorber and the rate of discoloration from light yellow to brown
follow a sigmoidal pattern. A reasonable correlation for net changes in
transmittance at 420 nm, yellowness index, and fluorescence peak area
(or intensity) ratio is obtained as the extent of EVA discoloration
progressed
The actual efficiency of photovoltaic generators is often lower
than predicted by standard test conditions (STC) or standard operating
conditions (SOC). This is caused mainly by an underestimation of
reflection losses and solar cell temperature in the module. The authors
describe how, in order to obtain more accurate results in predicting the
performance of PV-modules, the parameters influencing incoming (optical
parameters) and outgoing power flow (electrical and thermal parameters)
were investigated by simulation and some verifying experiments at the
University of New South Wales and the Australian desert
A high-efficiency AlGaAs/Si tandem solar cell is fabricated by
metal-organic chemical vapor deposition (MOCVD). It consists of a
Al<sub>0.15</sub>Ga<sub>0.85</sub>As top cell and a Si bottom cell. The
crystalline quality of the Al<sub>0.15</sub>Ga<sub>0.85</sub>As
heteroepitaxial layer grown on Si is improved using a high-temperature
growth process (800°C) and thermal cycle annealings (300~900°C).
The quantum efficiency of the Si bottom cell in the long wavelength
region is improved by back surface field. The conversion efficiencies of
the tandem solar cell under AMO and 1 sun measurement conditions with
4-terminal and 2-terminal configuration are 20.0% and 19.0%,
respectively. The conversion efficiencies of the tandem solar cell with
graded-band-gap emitter Al<sub>x</sub>Ga<sub>1-x</sub>As layer achieved
20.6% and 19.9% under same condition with 4-terminal and 2-terminal
configuration, respectively
Optimised thicknesses of the individual layers in any thin film a-Si:H solar cell can be obtained using optical analysis methods. By minimising the reflectance using an optimal antireflection coating layer and selecting a suitable rear contact material, a significant increase in the photon collection efficiency at long wavelengths can be achieved. The effect of the variation in thicknesses of different layers on the performance characteristics of a cell is discussed. The calculated results and analyses show that the present method can be used directly to design any thin film solar cell with an optimised structure for a desired possible high efficiency
Silicon solar cell efficiencies of 17.1%, 16.4%, 14.8%, and 14.9%
have been achieved on FZ, Cz, multicrystalline (mc-Si), and dendritic
web (DW) silicon, respectively, using simplified, cost-effective rapid
thermal processing (RTP). These represent the highest reported
efficiencies for solar cells processed with simultaneous front and back
diffusion with no conventional high-temperature furnace steps.
Appropriate diffusion temperature coupled with the added in-situ anneal
resulted in suitable minority-carrier lifetime and diffusion profiles
for high-efficiency cells. The cooling rate associated with the in-situ
anneal can improve the lifetime and lower the reverse saturation current
density (J<sub>o</sub>), however, this effect is material and base
resistivity specific. PECVD antireflection (AR) coatings provided low
reflectance and efficient front surface and bulk defect passivation.
Conventional cells fabricated on FZ silicon by furnace diffusions and
oxidations gave an efficiency of 18.8% due to greater short wavelength
response and lower J<sub>o</sub>
Improvements in the stabilized efficiency of single-junction and
multi-junction a-Si solar cells are studied. It has been found that the
stabilized efficiency can be improved by suppressing the oxygen and
nitrogen content in the i-layer. The defect density and conversion
efficiency are strongly correlated with the content of hydrogen having
an SiH<sub>2</sub> configuration rather than with the total hydrogen
content in a-Si i-layers. A practical estimation method, which considers
the variation of the I-V characteristics of each component cell, is also
developed in order to optimize multi-junction cells. The world's highest
stabilized efficiency of 8.8% for a single-junction a-Si solar cell and
10.6% for an a-Si/a-SiGe double-junction solar cell are achieved for 1
cm<sup>2</sup> cells
Solar cells based on Cu(In,Ga)Se<sub>2</sub> were prepared
replacing the `standard buffer layer' CdS with a In<sub>x</sub>(OH,S)
<sub>y</sub> thin film. The film is deposited in a chemical bath (CBD)
process using an aqueous solution containing InCl<sub>3</sub> and
thioacetamide. X-ray photoemission spectroscopy measurements were
performed in order to characterize the growth kinetics and the chemical
composition. The influence of different concentrations of InCl<sub>3
</sub> and thioacetamide in the solution on the electrical properties of
the solar cells was studied by measuring the j-V characteristics and the
spectral quantum efficiencies. Capacitance-voltage (C-V) measurements
indicate that the high V<sub>oc</sub> values of devices with the novel
buffer layer are correlated with narrower space charge widths and higher
effective carrier concentrations in the absorber materials. The achieved
conversion efficiency of approximately 15% using the cadmium free
In<sub>x</sub>(OH,S)<sub>y</sub> buffer demonstrates the potential of
this process as an alternative to the standard chemical bath deposition
of CdS
The alignment of energy bands in a Mo/CIS/CdS/ZnO solar cell
structure is presented. Special attention is paid to the surface
chemistry of the molybdenum coated substrate. In this study we have
performed in situ analyses on polycrystalline thin films starting from
the molybdenum coated soda lime glass. The different films have been
deposited sequentially under ultra high vacuum conditions and analyzed
with photoelectron spectroscopy techniques. We have found that Mo
surface is significantly oxidized. Air annealing at 200°C leads to a
diffusion of sodium through the Mo layer. Mo-O and Mo-Se compounds are
formed and present during the evolution of the Mo-CIS interface. Band
lineups have been determined for the CIS/CdS/ZnO interfaces of the solar
cell structure. We have found no indication for band discontinuities
deteriorating the solar cell device performance
This paper explores the possibility of measuring the open-circuit voltage as a function of wavelength as a tool for device characterization. Computer simulations show that the spectral response of the open-circuit voltage exhibits a similar dependence to the spectral response of the short-circuit current. Experimental studies on silicon solar cells confirmed the strong spectral dependence of the open-circuit voltage. The spectral measurements have been performed using a quasi-steady state open-circuit voltage method, which also allows to determine the spectral response of the maximum power voltage. The advantages of this new technique over conventional spectral response measurements include its applicability directly after junction formation and its simple apparatus.
This paper addresses the problem of preparing a good p-layer
contact with zinc oxide as TCO (transparent conducting oxide). Our
approach was to deposit pin cells with different p-layer recipes on ZnO
coated SnO<sub>2</sub>:F and on uncoated SnO<sub>2</sub>:F in one run.
The pin cells prepared on the ZnO surface exhibit a lower fill factor
(FF). Our experiments demonstrate that the hydrogen interaction with the
ZnO surface plays the most decisive role for the ZnO/p contact. We
explain the observed effects using a band diagram of the ZnO/p interface
and show that the accumulation layer at the ZnO surface-caused by atomic
hydrogen in the plasma-is responsible for the low FF in pin cells. Based
on this model the contact problem is solved by introducing a μc-n-Si
intralayer between ZnO and p layer resulting in an identical high FF on
both ZnO and SnO<sub>2</sub> substrates
Preliminary research into the development of single-junction Ga
<sub>x</sub>In<sub>1-x</sub>As thermophotovoltaic (TPV) power converters
is reviewed. The devices structures are grown epitaxially on
single-crystal InP substrates. Converter band gaps of 0.50 -0.74 eV have
been considered in accordance with modeling calculations. A 1-sun, AMO
efficiency of 12.8% is reported for a lattice-matched, 0.74-eV
converter. Converters with lower band gaps are fabricated using
lattice-mismatched, compositionally graded structures. Functional TPV
converters with good performance characteristics have been demonstrated
for band gaps as low as 0.5 eV
Thin films based on Cu(In,Ga)Se<sub>2</sub> prepared on alkali
free substrates are compared to films prepared on soda lime glass. On
the latter, the presence of sodium species as detected with X-ray
photoelectron spectroscopy is correlated with an enhanced formation of
Se-O, In-O and Ga-O bonds at the surface after several days air
exposure. The electrical conductivity is also one order of magnitude
higher on soda lime glass and solar cells prepared on molybdenum-coated
substrates exhibit increased open circuit voltages. Capacitance-voltage
characteristics on junctions prepared on alkali free substrates show an
increased space charge width. The observations can be explained in terms
of an increased net acceptor density in polycrystalline
Cu(In,Ga)Se<sub>2</sub> when prepared on soda lime glass substrates. An
alkali-metal-promoted oxidation of the surface is discussed
The thermal oxidation of CuInSe<sub>2</sub> single crystals and
bulk polycrystalline plates of n- and p-type conductivity with polished
facets have been carried out at elevated temperatures 400 to 610°C
in dry oxygen/air atmosphere. All the crystals demonstrated an
enhancement in hole conductivity near the surface. Additionally,
transparent layers of In<sub>2</sub>O<sub>3</sub> chemical composition
have been grown on the surface. Electron-probe analysis, Rutherford
backscattering, X-ray diffraction, optical and photoelectric
experimental data have provided a basis to develop a physico-chemical
model thermal oxidation of CuInSe<sub>2</sub> crystals. The model
includes the In<sub>2</sub>O<sub>3</sub> compound appearance, V<sub>Se
</sub>, V<sub>Cu</sub> vacancy absorption, Se<sub>i</sub>,
Cu<sub>i</sub> extra atom and Cu<sub>x</sub>Se generation. The chemical
reactions are accompanied by arising dislocations and mechanical
stresses at the In<sub>2</sub>O<sub>3</sub>/CuInSe<sub>2</sub> interface
This paper reports the effect of solvent and dopant impurities on
the performance of LPE silicon solar cells. For LPE layers grown from Sn
and In based solutions and having similar surface morphology and
resistivity, the performance of solar cells made on LPE layers grown
from In was always higher than that of cells made on LPE layers grown
using Sn as solvent. Consistently higher performance was also obtained
from solar cells fabricated upon Ga-doped LPE layers than from cells
made on Al-doped LPE silicon. The best cell was fabricated upon a
Ga-doped LPE layer grown from In solution and had a total area
efficiency of 16.4% confirmed by Sandia measurements. The observed
phenomena are explained on the basis of Hall mobilities and minority
carrier lifetimes of LPE layers grown from different solutions, and also
the oxidation difference of these layers during cell processing
Presents results of the role of the oxygen partial pressure (p<sub>02</sub>) used on the properties exhibited by doped μc silicon oxycarbide films produced by a two consecutive decomposition and deposition chamber (TCDDC) system, where a spatial separation between the plasma and the growth regions is achieved. The films produced are highly conductive and transparent with suitable properties for optoelectronic applications. The film's structure, composition, morphology and optoelectronic properties were analysed by means of grazing X-ray diffraction, electron secondary chemical analysis (ESCA), secondary ion mass spectroscopy (SIMS) as a function of temperature (T) and optical absorption (ranging from 300 to 80 K) measurements
For the first time the Si/C interface in poly-Si photovoltaic thin films on graphite substrate is described. The isostatically pressed graphite is covered with a 3-5 μm thick amorphous silicon layer which is recrystallized by the ZMR method (zone melting recrystallization by means of a line electron beam). During ZMR the molten silicon penetrates into the graphite pores, while at the interface β-SiC particles with a size of 50-1000 nm were formed (TEM, SEM analysis). Furthermore there exists a “reaction zone” where Si, SiC and C are found by electron diffraction. As a consequence the poly-Si layer shows an excellent adhesion to the substrate. Since there is no continuous electrically insulating SiC layer formed, highly boron doped seed layers show an ohmic contact to the graphite. The investigated poly-Si thin films on graphite substrate offer a great potential for photovoltaic application after epitaxy up to 50 μm by LPE or CVD
Sub-bandgap spectral response measurements on silicon solar cells
are used to characterise the infrared response of present devices, and
to investigate the impurity photovoltaic (IPV) effect for improving
their infrared response. The former has, aside from establishing a
baseline case, led to an improved determination of the subgap absorption
coefficient of crystalline silicon. Absorption coefficient values as low
as 10<sup>-7</sup> cm<sup>-1</sup> have been determined, revealing
structure due to 3- and 4-phonon assisted absorption. The influences of
free carrier absorption, bandgap narrowing, and the Franz-Keldysh effect
on cell infrared response are considered. Investigation of the IPV
effect of indium in high efficiency bulk and thin film cells reveals
that indium improves their infrared response. The cross-section for
electron photoemission from the indium level, a crucial parameter for
modelling indium's IPV effect, is determined
A new method for the fabrication of a columnar, multicrystalline silicon layer on a graphite substrate is presented. This method basically involves three process steps: (1) deposition of a thin (3-5 μm) silicon layer; (2) zone melting recrystallization of this layer with a line electron beam as the heat source to form a multicrystalline seed layer; and (3) thickening of the seed layer by high temperature, epitaxial chemical vapour deposition (CVD) to a thickness of 20-40 μm. The recrystallization leads to (110)[112]-textured silicon seed layers if sufficiently high scan velocities are applied. The degree of deviation from the ideal (110)[112]-texture increases with decreasing scan velocity. The doping level of the seed layer is found to be only weakly affected by the zone melting recrystallization. The epitaxial layer grown on top of the seed layer exhibits a columnar grain structure
Thin film crystalline silicon solar cells can only achieve high
efficiencies if light trapping can be used to give a long optical path
length, while simultaneously achieving near unity collection
probabilities for all generated carriers. This necessitates a supporting
substrate of a foreign material, with refractive index compatible with
light trapping schemes for the silicon. The resulting inability to
nucleate growth of crystalline silicon films of good crystallographic
quality on such foreign substrates, prevents the achievement of high
efficiency devices using conventional single junction solar cell
structures. The parallel multijunction solar cell provides a new
approach for achieving high efficiencies from very poor quality
material, with near unity collection probabilities for all generated
carriers achieved through appropriate junction spacing. Heavy doping is
used to minimise the dark saturation current contribution from the
layers, therefore allowing respectable voltages. The design strategy,
corresponding advantages, theoretical predictions and experimental
results are presented
We used a 10-kW high-flux solar furnace (HFSF) to diffuse the
front-surface n<sup>+</sup>-p junction and the back-surface p-p<sup>+
</sup> junction of single-crystal silicon solar cells in one processing
step. We found that all of the HFSF-processed cells have better
conversion efficiencies than control cells of identical structures
fabricated by conventional furnace diffusion methods. HFSF processing
offers several advantages that may contribute to improved solar cell
efficiency: (1) it provides a cold-wall process, which reduces
contamination; (2) temperature versus time profiles can be precisely
controlled; (3) wavelength, intensity, and spatial distribution of the
incident solar flux can be controlled and changed rapidly, (4) a number
of high-temperature processing steps can be performed simultaneously;
and (5) combined quantum and thermal effects may benefit overall cell
performance. The HFSF has also been successfully used to texture the
surface of silicon wafers and to crystallize a-Si:H thin films on glass
The transitory and erratic nature of shunt currents, whether caused by light-soaking or electrical biasing, in amorphous Si (a-Si) single- and triple-junction solar cells has been a real puzzle and made the study of these cells difficult. The authors present a careful study of the time/voltage dependence of these current transients in several different a-Si solar cell structures and find they reveal more about the basic shunt mechanism. In single-junction cells, they see stepwise current changes that increase in size and number with reverse bias and can be removed with forward bias. This stepwise, on and off switching suggests a discrete shunt path conduction mechanism. The kinetics of these metastable shunt paths show that both the “on-state” and “off-state” possess memory. Cells without (Al)ZnO show no metastable switching. The authors associate the stepwise features with the textured substrate and the switching metastability with contact to (Al)ZnO. Switching in triple-junction cells occurs with hundreds of oscillations at each step
4,7-Bis(2,3-dihydrothieno [3,4-b] [1,4] dioxin-5-yl)-2-dodecyl-2H-benzo [1,2,3] triazole (BEBT) was polymerized both electrochemically (ePBEBT) and chemically (cPBEBT). Since chemical polymerization enabled a soluble polymer in common organic solvents, a single layer electrochromic device of ePBEBT was constructed. The polymer cPBEBT was also used in bulk heterojunction (BHJ) solar cells as the active layer in combination with a soluble fullerene derivative, 1-(3-methoxycarbonyl)-propyl-1-1-phenyl-(6,6)C61 PCBM.
A solution-processable and star-shaped molecule 4-((E)-2-(benzo[1,2,5]thiadiazol-4-yl)vinyl)-N,N-bis(4-((E)-2-(benzo[1,2,5]thiadiazol-7-yl)vinyl)phenyl)benzenamine (TPA-BT) has been designed and synthesized by palladium-catalyzed Heck reaction for the application in organic solar cells (OSCs). The molecule possesses a D–A structure with a triphenylamine core (donor unit) linked with three benzo[1,2,5]thiadiazole (acceptor unit) arms through double bonds. TPA-BT film shows a strong absorption peak in the visible wavelength range from 400 to 560 nm, which could be ascribed to the charge transfer band of the D–A structure of the molecule. The bulk-heterojunction OSCs with the device structure of ITO/PEDOT:PSS/TPA-BT:PCBM/Ca/Al (or Ba/Al) were fabricated by spin-coating the blend solution of TPA-BT and PCBM (1:3, w/w), in which TPA-BT was used as donor and PCBM as acceptor materials. The devices show a high open circuit voltage of ca. 0.9 V and a power conversion efficiency of 0.61%, under the illumination of AM 1.5, 100 mW/cm2. The results indicate that TPA-BT is a promising solution-processable organic photovoltaic material.
Bulk heterojunction solar cells utilizing soluble phthalocyanine derivative, 1,4,8,11,15,18,22,25-octahexylphthalocyanine (C6PcH2) have been investigated. The active layer was fabricated by spin-coating the mixed solution of C6PcH2 and 1-(3-methoxy-carbonyl)-propyl-1-1-phenyl-(6,6)C61 (PCBM). The photovoltaic properties of the solar cell with bulk heterojunction of C6PcH2 and PCBM demonstrated the strong dependence of active layer thickness, and the optimized active layer thickness was clarified to be 120 nm. By inserting MoO3 hole transport buffer layer between the positive electrode and active layer, the FF and energy conversion efficiency were improved to be 0.50 and 3.2%, respectively. The tandem organic thin-film solar cell has also been studied by utilizing active layer materials of C6PcH2 and poly(3-hexylthiophene) and the interlayer of LiF/Al/MoO3 structure, and a high Voc of 1.27 V has been achieved.Highlights► Organic solar cells utilizing phthalocyanine derivative (C6PcH2) have been investigated. ► The photovoltaic properties demonstrated the strong dependence of active layer thickness. ► By inserting MoO3 buffer layer the FF and energy conversion efficiency were improved. ► The tandem solar cell has been investigated by utilizing C6PcH2 and poly(3-hexylthiophene). ► The optimized thickness was 120 nm, and a high Voc of 1.27 V has been achieved in the tandem cell.