3470:
5035:
5046:
shaded area under the red line represents the maximum work done by ideal infinite multi-junction solar cells. Hence, the limiting efficiency of ideal infinite multi-junction solar cells is evaluated to be 68.8% by comparing the shaded area defined by the red line with the total photon-flux area determined by the black line. (This is why this method is called "graphical" QE analysis.) Although this limiting efficiency value is consistent with the values published by
Parrott and Vos in 1979: 64% and 68.2% respectively, there is a small gap between the estimated value in this report and literature values. This minor difference is most likely due to the different ways how to approximate the photon flux over 0–0.3096
3803:
28:
5687:
415:
3826:
their bandgap energy. This assumption accounts for the first intrinsic loss in the efficiency of solar cells, which is caused by the inability of single-junction solar cells to properly match the broad solar energy spectrum. However, the current graphical QE analysis still cannot reflect the second intrinsic loss in the efficiency of solar cells, radiative recombination. To take the radiative recombination into account, we need to evaluate the radiative current density,
8394:
5799:
1146:
98:(c-Si) solar cells had efficiencies up to 27.1%, while lab examples of multi-junction cells have demonstrated performance over 46% under concentrated sunlight. Commercial examples of tandem cells are widely available at 30% under one-sun illumination, and improve to around 40% under concentrated sunlight. However, this efficiency is gained at the cost of increased complexity and manufacturing price. To date, their higher price and higher
5813:
139:
1303:
tunneling region, the negative differential resistance region and the thermal diffusion region. The region where electrons can tunnel through the barrier is called the tunneling region. There, the voltage must be low enough so that energy of some electrons who are tunneling is equal to energy states available on the other side of the barrier. Consequently, current density through the tunnel junction is high (with maximum value of
519:
8406:
5268:, is increased. Hence, the voltage is lower than that of the InGaP tunnel junction. GaAsSb heterojunction tunnel diodes offer other advantages. The same current can be achieved by using a lower doping. Secondly, because the lattice constant is larger for GaAsSb than Ge, one can use a wider range of materials for the bottom cell because more materials are lattice-matched to GaAsSb than to Ge.
1447:
5371:) and the total photon flux density. It can be shown that a high (low) value for APE means low (high) wavelengths spectral conditions and higher (lower) efficiencies. Thus APE is a good indicator for quantifying the effects of the solar spectrum variations on performances and has the added advantage of being independent of the device structure and the absorption profile of the device.
3253:
number of photons/m·s). To do that, it is necessary to carry out an intermediate unit conversion from the power of electromagnetic radiation incident per unit area per photon energy to the photon flux per photon energy (i.e., from to ). For this intermediate unit conversion, the following points have to be considered: A photon has a distinct energy which is defined as follows.
2072:
5426:
However, the downside of the concentrator approach is that efficiency drops off very quickly under lower lighting conditions. In order to maximize its advantage over traditional cells and thus be cost competitive, the concentrator system has to track the sun as it moves to keep the light focused on the cell and maintain maximum efficiency as long as possible. This requires a
5418:
non-concentrated version of the same design, one might expect a three-layer cell of 30% efficiency. This is not enough of an advantage over traditional silicon designs to make up for their extra production costs. For this reason, almost all multi-junction cell research for terrestrial use is dedicated to concentrator systems, normally using mirrors or
Fresnel lenses.
1476:, these cannot jump above the barrier formed by the heterojunction because they don't have enough energy, as illustrated in figure E. Hence, electrons (holes) cannot recombine with holes (electrons) and cannot diffuse through the barrier. By the way, window and BSF layers must be transparent to wavelengths absorbed by the next pn junction; i.e.,
2667:
3242:
3791:
1682:
1853:
985:, the trapping of the light in the material (because photons cannot easily get out the MJ structure due to pyramids) and therefore, the path length of photons in the material. On the one hand, the thickness of each AR layer is chosen to get destructive interferences. Therefore, the reflection coefficient
5704:
Measurements on MJ solar cells are usually made in the laboratory, using light concentrators (this is often not the case for the other cells) and under standard test conditions (STCs). STCs prescribe, for terrestrial applications, the AM1.5 spectrum as the reference. This air mass (AM) corresponds to
5417:
m equal 10000 cm), produces the highest efficiencies seen to date. Three-layer cells are fundamentally limited to 63%, but existing commercial prototypes have already demonstrated over 40%. These cells capture about 2/3 of their theoretical maximum performance, so assuming the same is true for a
5066:
The majority of multi-junction cells that have been produced to date use three layers (although many tandem a-Si:H/mc-Si modules have been produced and are widely available). However, the triple junction cells require the use of semiconductors that can be tuned to specific frequencies, which has led
5045:
Now, we can fully use Henry's graphical QE analysis, taking into account the two major intrinsic losses in the efficiency of solar cells. The two main intrinsic losses are radiative recombination, and the inability of single junction solar cells to properly match the broad solar energy spectrum. The
510:
Conveniently, light of a particular wavelength does not interact strongly with materials that are of bigger bandgap. This means that you can make a multi-junction cell by layering the different materials on top of each other, shortest wavelengths (biggest bandgap) on the "top" and increasing through
476:
Combining all of these factors, the maximum efficiency for a single-bandgap material, like conventional silicon cells, is about 34%. That is, 66% of the energy in the sunlight hitting the cell will be lost. Practical concerns further reduce this, notably reflection off the front surface or the metal
3825:
eV are not available. Regardless of this data unavailability, however, the graphical QE analysis can be done using the only available data with a reasonable assumption that semiconductors are opaque for photon energies greater than their bandgap energy, but transparent for photon energies less than
1334:
too. This is why tunnel junctions are ideal for connecting two pn junctions without having a voltage drop. When voltage is higher, electrons cannot cross the barrier because energy states are no longer available for electrons. Therefore, the current density decreases and the differential resistance
472:
spectrum, although that represents almost half of the power coming from the sun. Conversely, photons with more energy than the bandgap, say blue light, initially eject an electron to a state high above the bandgap, but this extra energy is lost through collisions in a process known as "relaxation".
1302:
Hence, electrons can easily tunnel through the depletion region. The J-V characteristic of the tunnel junction is very important because it explains why tunnel junctions can be used to have a low electrical resistance connection between two pn junctions. Figure D shows three different regions: the
1128:
by matching currents of the three subcells. As example, because the current generated by the bottom cell is greater than the currents generated by the other cells, the thickness of AR layers is adjusted so that the infrared (IR) transmission (which corresponds to the bottom cell) is degraded while
3252:
We can estimate the limiting efficiency of ideal infinite multi-junction solar cells using the graphical quantum-efficiency (QE) analysis invented by C. H. Henry. To fully take advantage of Henry's method, the unit of the AM1.5 spectral irradiance should be converted to that of photon flux (i.e.,
550:
The more difficult solution is the "monolithically integrated" cell, where the cell consists of a number of layers that are mechanically and electrically connected. These cells are much more difficult to produce because the electrical characteristics of each layer have to be carefully matched. In
5425:
m would require 625 16 cm cells, but for a concentrator system only a single cell is needed, along with a concentrator. The argument for concentrated Multi-junction cells has been that the high cost of the cells themselves would be more than offset by the reduction in total number of cells.
1842:
is the product of the thermal recombination currents of the two cells. Note that the values inserted for both short circuit currents and thermal recombination currents are those measured or calculated for the cells when they are placed in a multijunction stack (not the values measured for single
5775:
eV. This results in too little current in the GaAs junction, and hampers the overall efficiency since the InGaP junction operates below MPP current and the GaAs junction operates above MPP current. To improve current match, the InGaP layer is intentionally thinned to allow additional photons to
498:
For instance, if one had a cell with two bandgaps in it, one tuned to red light and the other to green, then the extra energy in green, cyan and blue light would be lost only to the bandgap of the green-sensitive material, while the energy of the red, yellow and orange would be lost only to the
5290:
The theoretical efficiency of MJ solar cells is 86.8% for an infinite number of pn junctions, implying that more junctions increase efficiency. The maximum theoretical efficiency is 37, 50, 56, 72% for 1, 2, 3, 36 additional pn junctions, respectively, with the number of junctions increasing
5228:
semiconductor. Its bandgap can be tuned by varying the amount of indium in the alloy from 0.7 eV to 3.4 eV, thus making it an ideal material for solar cells. However, its conversion efficiencies because of technological factors unrelated to bandgap are still not high enough to be
2359:
For maximum efficiency, each subcell should be operated at its optimal J-V parameters, which are not necessarily equal for each subcell. If they are different, the total current through the solar cell is the lowest of the three. By approximation, it results in the same relationship for the
5682:
is to use thin films instead of thick layers in order to decrease the cost efficiency ratio. As of 2010, MJ solar panels are more expensive than others. These differences imply different applications: MJ solar cells are preferred in space and c-Si solar cells for terrestrial applications.
1165:
and optically low-loss connection between two subcells. Without it, the p-doped region of the top cell would be directly connected with the n-doped region of the middle cell. Hence, a pn junction with opposite direction to the others would appear between the top cell and the middle cell.
4841:
1297:
3480:
Based on the above result from the intermediate unit conversion, we can derive the photon flux by numerically integrating the photon flux per photon energy with respect to photon energy. The numerically integrated photon flux is calculated using the trapezoidal rule, as follows.
125:, as opposed to conventional crystalline silicon, to produce a cell with about 10% efficiency that is lightweight and flexible. This approach has been used by several commercial vendors, but these products are currently limited to certain niche roles, like roofing materials.
5291:
exponentially to achieve equal efficiency increments. The exponential relationship implies that as the cell approaches the limit of efficiency, the increase cost and complexity grow rapidly. Decreasing the thickness of the top cell increases the transmission coefficient
5737:
As of 2010, the cost of MJ solar cells was too high to allow use outside of specialized applications. The high cost is mainly due to the complex structure and the high price of materials. Nevertheless, with light concentrators under illumination of at least 400 suns,
2354:
2486:
5712:
Consequently, the performance of MJ solar cells in outdoor environments is inferior to that achieved in the laboratory. Moreover, MJ solar cells are designed such that currents are matched under STC, but not necessarily under field conditions. One can use
3056:
3445:
5393:
optics. Thanks to these devices, light arriving on a large surface can be concentrated on a smaller cell. The intensity concentration ratio (or "suns") is the average intensity of the focused light divided by 1 kW/m (reasonable value related to
5208:
Indium phosphide-based cells have the potential to work in tandem with gallium arsenide cells. The two cells can be optically connected in series (with the InP cell below the GaAs cell), or in parallel through the use of spectra splitting using a
3488:
5310:) multi-junction technologies including tandems and triple- and quadruple-junction modules that typically use III–V semiconductors, with promising power conversion efficiency that rival and even outperform the benchmark silicon solar cells.
2067:{\displaystyle J={\frac {1}{2}}\left(J_{\text{SC,1}}+J_{\text{SC,2}}\right)+{\frac {1}{2}}T^{-}\Delta J_{\text{SC}}-\left(1-T^{+}\right){\sqrt {{\frac {1}{4}}{\Delta J_{\text{SC}}}^{2}+{\tilde {J}}_{0}^{2}\mathrm {e} ^{\frac {qV}{kT}}}}.}
1534:
4599:
4039:
4158:
The current density delivered to the load is the difference of the current densities due to absorbed solar and thermal radiation and the current density of radiation emitted from the top surface or absorbed in the substrate. Defining
494:
Cells made from multiple materials layers can have multiple bandgaps and will therefore respond to multiple light wavelengths, capturing and converting some of the energy that would otherwise be lost to relaxation as described above.
4427:
5275:
in each layer better matches lattice constants of the different layers. Without it, there is about 0.08 percent of mismatching between layers, which inhibits performance. Adding aluminium to the top cell increases its band gap to
962:. This provides an electrical connection to a load or other parts of a solar cell array. They are usually on two sides of the cell. And are important to be on the back face so that shadowing on the lighting surface is reduced.
422:
for the efficiency of a single-junction solar cell. It is essentially impossible for a single-junction solar cell, under unconcentrated sunlight, to have more than ~34% efficiency. A multi-junction cell, however, can exceed that
1121:/4 to have opposite phase for reflected fields. On the other hand, the thickness of each AR layer is also chosen to minimize the reflectance at wavelengths for which the photocurrent is the lowest. Consequently, this maximizes
4328:
3925:
603:) to transmit to the lower sub-cells. Therefore, suitable bandgaps must be chosen such that the design spectrum will balance the current generation in each of the sub-cells, achieving current matching. Figure C(b) plots
5449:
A new technique was announced that year that allowed such cells to use a substrate of glass or steel, lower-cost vapors in reduced quantities that was claimed to offer costs competitive with conventional silicon cells.
5161:
Current efficiencies for commercial InGaP/GaAs/Ge cells approach 40% under concentrated sunlight. Lab cells (partly using additional junctions between the GaAs and Ge junction) have demonstrated efficiencies above 40%.
485:
spectrum, shows the best balance is reached at about 1.1 eV (about 1100 nm, in the near infrared), which happens to be very close to the natural bandgap in silicon and a number of other useful semiconductors.
5034:
1079:
4682:
1419:
4153:
5298:
An InGaP hetero-layer between the p-Ge layer and the InGaAs layer can be added in order to create automatically the n-Ge layer by scattering during MOCVD growth and increase significantly the quantum efficiency
621:. It is plotted together with the maximum conversion efficiency for every junction as a function of the wavelength, which is directly related to the number of photons available for conversion into photocurrent.
480:
Lower, also called narrower, bandgap materials will convert longer wavelength, lower energy photons. Higher, or wider bandgap materials will convert shorter wavelength, higher energy light. An analysis of the
4701:
1180:
534:
Producing a tandem cell is not an easy task, largely due to the thinness of the materials and the difficulties extracting the current between the layers. The easy solution is to use two mechanically separate
2740:, i.e. the number of photons absorbed per unit of length by a material. If it is assumed that each photon absorbed by a subcell creates an electron/hole pair (which is a good approximation), this leads to:
2821:
1840:
3012:
5763:
The environment in space is quite different. Because there is no atmosphere, the solar spectrum is different (AM0). The cells have a poor current match due to a greater photon flux of photons above 1.87
3469:
6033:
465:, and the associated problem that it cannot extract any power at all from certain photons. This is due to the fact that the photons must have enough energy to overcome the bandgap of the material.
5250:-based heterojunction tunnel diodes, instead of conventional InGaP highly doped tunnel diodes described above, have a lower tunneling distance. Indeed, in the heterostructure formed by GaAsSb and
551:
particular, the photocurrent generated in each layer needs to be matched, otherwise electrons will be absorbed between layers. This limits their construction to certain materials, best met by the
499:
bandgap of the red-sensitive material. Following analysis similar to those performed for single-bandgap devices, it can be demonstrated that the perfect bandgaps for a two-gap device are at 0.77
5002:
574:
which contain a small degree of lattice mismatch. However, a greater degree of mismatch or other growth imperfections can lead to crystal defects causing a degradation in electronic properties.
2202:
5359:
are not necessarily matched and the total current becomes lower. These variations can be quantified using the average photon energy (APE) which is the ratio between the spectral irradiance
2662:{\displaystyle QE_{i}(\lambda )={\frac {J_{{\text{SC}}i}(\lambda )}{q\phi _{i}(\lambda )}}\Rightarrow J_{{\text{SC}}i}=\int _{0}^{\lambda 2}q\phi _{i}(\lambda )QE_{i}(\lambda )\,d\lambda }
2881:
3237:{\displaystyle J_{i}=J_{0i}\left(e^{\frac {qV_{i}}{kT}}-1\right)-J_{{\text{SC}}i}\Rightarrow V_{{\text{OC}}i}\approx {\frac {kT}{q}}\ln \left({\frac {J_{{\text{SC}}i}}{J_{0i}}}\right)}
5729:) contains no information on the matching of currents of subcells. An important alternative comparison point is the output power per unit area generated with the same incident light.
6373:
2946:
1424:
In order to avoid the reduction of the MJ solar cell performances, tunnel junctions must be transparent to wavelengths absorbed by the next photovoltaic cell, the middle cell, i.e.
4491:
1174:. In order to decrease this effect, a tunnel junction is used. It is simply a wide band gap, highly doped diode. The high doping reduces the length of the depletion region because
2170:
1769:
3359:
2738:
3048:
2709:
468:
If the photon has less energy than the bandgap, it is not collected at all. This is a major consideration for conventional solar cells, which are not sensitive to most of the
1739:
1712:
3786:{\displaystyle n_{\text{ph}}(E_{g})=\int _{E_{\text{g}}}^{\infty }{\frac {dn_{\text{ph}}}{dhv}}\,dhv=\sum _{i=E_{\text{g}}}^{\infty }(hv_{i+1}-hv_{i}){\frac {1}{2}}\left\,}
5421:
Using a concentrator also has the added benefit that the number of cells needed to cover a given amount of ground area is greatly reduced. A conventional system covering 1
2197:
522:
Figure C. (a) The structure of an MJ solar cell. There are six important types of layers: pn junctions, back surface field (BSF) layers, window layers, tunnel junctions,
5678:. Physically, the main property of a MJ solar cell is having more than one pn junction in order to catch a larger photon energy spectrum while the main property of the
1677:{\displaystyle J={\frac {1}{2}}\left(J_{\text{SC,1}}+J_{\text{SC,2}}\right)-{\sqrt {{\frac {1}{4}}{\Delta J_{\text{SC}}}^{2}+J_{0}^{2}\mathrm {e} ^{\frac {qV}{kT}}}},}
5701:
The efficiencies of solar cells and Si solar technology are relatively stable, while the efficiencies of solar modules and multi-junction technology are progressing.
3802:
1462:. Similarly, a back-surface field (BSF) layer reduces the scattering of carriers towards the tunnel junction. The structure of these two layers is the same: it is a
563:
The choice of materials for each sub-cell is determined by the requirements for lattice-matching, current-matching, and high performance opto-electronic properties.
2129:
2102:
1328:
4500:
3932:
4344:
3463:
As a result of this intermediate unit conversion, the AM1.5 spectral irradiance is given in unit of the photon flux per photon energy, , as shown in Figure 1.
1847:-characteristic for two ideal (operating at the radiative limit) cells that are allowed to exchange luminesence, and thus are radiatively coupled, is given by
547:'s products use three such layers to reach efficiencies around 9%. Lab examples using more exotic thin-film materials have demonstrated efficiencies over 30%.
7381:
6778:
Kuykendall, T.; Ulrich, Philipp; Aloni, Shaul; Yang, Peidong (2007). "Complete compositional tunability of InGaN nanowires using a combinatorial approach".
2131:
are transfer coefficients that describes the exchange of photons between the cells. The transfer coefficients depend on the refractive index of the cells.
7247:
5385:
Light concentrators increase efficiencies and reduce the cost/efficiency ratio. The three types of light concentrators in use are refractive lenses like
7357:(DOE)'s Lawrence Berkeley National Laboratory (Berkeley Lab) has led to record-breaking sunlight-to-electricity conversion efficiencies in solar cells.
4244:
3849:
117:
Tandem fabrication techniques have been used to improve the performance of existing designs. In particular, the technique can be applied to lower cost
7242:
C. Zhang, J. Gwamuri, R. Andrews, and J. M. Pearce, (2014). Design of Multi-Junction
Photovoltaic Cells Optimized for Varied Atmospheric Conditions,
1133:
transmission (which corresponds to the top cell) is upgraded. Particularly, an AR coating is very important at low wavelengths because, without it,
220:
that hit the top of the solar cell are either reflected or transmitted into the cell. Transmitted photons have the potential to give their energy,
5783:
eV, better balancing the junction currents. Radiation particles that are no longer filtered can damage the cell. There are two kinds of damage:
577:
Since each sub-cell is connected electrically in series, the same current flows through each junction. The materials are ordered with decreasing
17:
1024:
624:
Finally, the layers must be electrically optimal for high performance. This necessitates usage of materials with strong absorption coefficients
570:
of each material must be closely matched, resulting in lattice-matched devices. This constraint has been relaxed somewhat in recently developed
4606:
1341:
8299:
7976:
4080:
6380:
5139:(Ge) can be fabricated on germanium wafers. Early cells used straight gallium arsenide in the middle junction. Later cells have utilized In
4836:{\displaystyle W_{\text{m}}={\frac {J_{\text{m}}V_{\text{m}}}{n_{\text{ph}}}}={\frac {eV_{\text{m}}}{1+kT/eV_{\text{m}}}}=eV_{\text{m}}-kT}
1454:
of a window layer. The surface recombination is reduced. (b) Layers and band diagram of a BSF layer. The scattering of carriers is reduced.
1292:{\displaystyle l_{\text{depl}}={\sqrt {{\frac {2\epsilon (\phi _{0}-V)}{q}}{\frac {N_{\text{A}}+N_{\text{D}}}{N_{\text{A}}N_{\text{D}}}}}}}
199:
with metallic contacts deposited on the top and bottom. The doping is normally applied to a thin layer on the top of the cell, producing a
6056:
1330:, the peak current density) and the slope near the origin is therefore steep. Then, the resistance is extremely low and consequently, the
7945:
7781:
6261:
Strehlke, S; Bastide, S; Guillet, J; Levyclement, C (2000). "Design of porous silicon antireflection coatings for silicon solar cells".
91:
of 33.16%. Theoretically, an infinite number of junctions would have a limiting efficiency of 86.8% under highly concentrated sunlight.
7654:
7195:
5624:
6374:"AlGaAs Tunnel Junction for high efficiency multi-junction solar cells: simulation and measurement of temperature-dependent operation"
6134:
3796:
As a result of this numerical integration, the AM1.5 spectral irradiance is given in unit of the photon flux, , as shown in Figure 2.
2442:) is utilized. It measures the ratio between the amount of electron-hole pairs created and the incident photons at a given wavelength
6951:
Yamaguchi, M; Takamoto, T; Araki, K; Ekinsdaukes, N (2005). "Multi-junction III–V solar cells: current status and future potential".
250:
accelerates both electrons and holes towards their respective n-doped and p-doped regions (up and down, respectively). The resulting
6906:
Proceedings of 1994 IEEE 1st World
Conference on Photovoltaic Energy Conversion - WCPEC (A Joint Conference of PVSC, PVSEC and PSEC)
6285:
2746:
1774:
8116:
5787:
and atomic displacement. Still, MJ cells offer higher radiation resistance, higher efficiency and a lower temperature coefficient.
5318:
Solar spectrum at the Earth surface changes constantly depending on the weather and sun position. This results in the variation of
2951:
530:
1.5 solar spectrum, together with the maximum electricity conversion efficiency for every junction as a function of the wavelength.
84:
allows the absorbance of a broader range of wavelengths, improving the cell's sunlight to electrical energy conversion efficiency.
6015:
5254:, the valence band of GaAsSb is higher than the valence band of the adjoining p-doped layer. Consequently, the tunneling distance
8083:
8078:
7412:
6304:
5224:(InGaN) is a semiconductor material made of a mix of gallium nitride (GaN) and indium nitride (InN). It is a ternary group III–V
7335:
6903:
J.C. Zolper; Plut; Tigges; et al. (1994). "GaAsSb-based heterojunction tunnel diodes for tandem solar cell interconnects".
7823:
7259:
D. Crisp; A. Pathareb; R. C. Ewell (2004). "The performance of gallium arsenide/germanium solar cells at the
Martian surface".
571:
7341:
7324:
6922:
6468:
Peharz, G.; Siefer, G.; Bett, A.W. (2009). "A simple method for quantifying spectral impacts on multi-junction solar cells".
6187:
6162:
1153:
of the tunnel junction. Because the length of the depletion region is narrow and the band gap is high, electrons can tunnel.
7216:
Albuflasa, H; Gottschalg, R; Betts, T (2007). "Modeling the effect of varying spectra on multi junction A-SI solar cells".
6822:
6075:
5690:
7177:
5942:
8121:
5779:
In terrestrial concentrating applications, the scatter of blue light by the atmosphere reduces the photon flux above 1.87
5709:
W/m. Therefore, spectral variations of incident light and environmental parameters are not taken into account under STC.
4853:
2349:{\displaystyle {\tilde {J}}_{0}^{2}=\left(1+2n_{\text{r}}^{2}\right)\left(J_{0,2}+2n_{\text{r}}^{2}J_{0,1}\right)J_{0,1}}
1335:
is negative. The last region, called thermal diffusion region, corresponds to the J-V characteristic of the usual diode:
6868:
Yam, F.K.; Hassan, Z. (2008). "InGaN: An overview of the growth kinetics, physical properties and emission mechanisms".
8137:
7489:
5103:
P serve as the high band gap alloy. This alloy range provides for the ability to have band gaps in the range 1.92–1.87
646:
The favorable values in the table below justify the choice of materials typically used for multi-junction solar cells:
8265:
8200:
8142:
7639:
7158:
7118:
5443:
5202:
695:
443:
6743:
Green, M.A.; Emery, K.; Hishikawa, Y.; Warta, W.; Dunlop, E.D. (2012). "Solar cell efficiency tables (version 40)".
5470:, contains technologies that are still in the research or development phase and are not listed in the table below.
5409:
Using concentrations on the order of 500 to 1000, meaning that a 1 cm cell can use the light collected from 0.1
8270:
8033:
7514:
5303:(λ) of the bottom cell. InGaP is advantageous because of its high scattering coefficient and low solubility in Ge.
973:(AR) coating is generally composed of several layers in the case of MJ solar cells. The top AR layer has usually a
691:
eV). The use of Ge is mainly due to its lattice constant, robustness, low cost, abundance, and ease of production.
4237:
equation. Thus, we will neglect this term to simplify the following discussion. Then we can express J as follows.
8284:
7791:
7649:
7530:
6325:
Yamaguchi, M; Takamoto, T; Araki, K (2006). "Super high-efficiency multi-junction and concentrator solar cells".
5826:
5600:
2837:
73:
7467:
6106:
R.Delamare, O.Bulteel, D.Flandre, Conversion lumière/électricité: notions fondamentales et exemples de recherche
473:
This lost energy turns into heat in the cell, which has the side-effect of further increasing blackbody losses.
339:
is current density, i.e. current per unit area) of a solar cell under illumination are obtained by shifting the
8442:
8409:
8235:
7761:
7555:
7504:
5866:
427:
The theoretical performance of a solar cell was first studied in depth in the 1960s, and is today known as the
6698:
6542:
Henry, C. H. (1980). "Limiting efficiencies of ideal single and multiple energy gap terrestrial solar cells".
8068:
6503:
Liu, Lei; Chen, Nuofu; Bai, Yiming; Cui, Ming; Zhang, Han; Gao, Fubao; Yin, Zhigang; Zhang, Xingwang (2008).
5888:
Rühle, Sven (2016-02-08). "Tabulated Values of the
Shockley–Queisser Limit for Single Junction Solar Cells".
5040:
Figure 3. Maximum work by ideal infinite multi-junction solar cells under standard AM1.5 spectral irradiance.
511:
the body of the cell. As the photons have to pass through the cell to reach the proper layer to be absorbed,
3440:{\displaystyle {\frac {dn_{\text{ph}}}{dhv}}={\frac {E}{E_{\text{ph}}}}={\frac {E}{\frac {hc}{\lambda }}}\,}
2897:
446:, this loss accounts for about 7% of the power. The second is an effect known as "recombination", where the
300:
appear. The expression for this photocurrent is obtained by adding generation and scattering photocurrents:
8355:
8335:
7715:
7474:
7095:
6091:
4449:
2134:
1744:
1504:. Furthermore, the lattice constant must be close to the one of InGaP and the layer must be highly doped (
694:
Because the different layers are closely lattice-matched, the fabrication of the device typically employs
271:
accelerates holes (electrons) towards the p-doped (n-doped) region, which gives a scattering photocurrent
8245:
7720:
7405:
6904:
512:
461:
However, the dominant loss mechanism is the inability of a solar cell to extract all of the power in the
428:
419:
6988:"Life cycle energy use and environmental implications of high-performance perovskite tandem solar cells"
6577:
Shockley, W; Queisser, H.A. (1961). "Detailed
Balance Limit of Efficiency of p-n Junction Solar Cells".
8437:
8255:
8108:
8097:
7971:
7818:
7776:
7756:
5831:
5739:
5380:
2714:
114:(CPV), but cannot compete with single junction solar panels unless a higher power density is required.
111:
99:
3021:
2675:
7735:
7669:
7644:
7354:
5836:
1717:
1690:
7375:
1520:
In a stack of two cells, where radiative coupling does not occur, and where each of the cells has a
8170:
8152:
8043:
7889:
7876:
7871:
7771:
5124:
5084:
819:
77:
5158:
eV), the current match is very poor, with the Ge junction operated significantly current limited.
2175:
8260:
8180:
8058:
8028:
7786:
7766:
7695:
7581:
7576:
7545:
7540:
5804:
5523:
5251:
5243:
5186:
5132:
970:
912:
552:
523:
7097:
Impact of spectral effects on the electrical parameters of multijunction amorphous silicon cells
8398:
8240:
8210:
8175:
8162:
8048:
7624:
7614:
7509:
7398:
6053:
5467:
5221:
699:
193:
7310:
6423:
Strandberg, Rune (2020). "An
Analytic Approach to the Modeling of Multijunction Solar Cells".
2172:
also depend on the refractive index of the cells. If the cells have the same refractive index
154:
give their energy to electrons in the depletion or quasi-neutral regions. These move from the
8215:
8205:
8185:
8038:
7861:
7664:
7462:
7196:"High Efficiency Solar Cells for the Price of Conventional Ones | MIT Technology Review"
5694:
5571:
5307:
4594:{\displaystyle eV_{\text{m}}=eV_{\text{OC}}-kT\ln \left(1+{\frac {eV_{\text{m}}}{kT}}\right)}
1162:
458:
left behind by previous excitations. In silicon, this accounts for another 10% of the power.
107:
88:
4034:{\displaystyle A={\frac {2\pi \,\exp \left(n^{2}+1\right)E_{\text{g}}^{2}kT}{h^{3}c^{2}}}\,}
8432:
8250:
8230:
8225:
8220:
8195:
8190:
7705:
7634:
7479:
7447:
7316:
7268:
6960:
6877:
6834:
6787:
6664:
6621:
6586:
6551:
6477:
6235:
5897:
5746:
5679:
5463:
2107:
2080:
1306:
1167:
536:
527:
451:
118:
6655:
Parrott, J. (1979). "The limiting efficiency of an edge-illuminated multigap solar cell".
5280:
eV, covering a larger part of the solar spectrum and obtain a higher open-circuit voltage
4422:{\displaystyle eV_{\text{OC}}=E_{\text{g}}-kT\ln \left({\frac {A}{en_{\text{ph}}}}\right)}
539:
and then wire them together separately outside the cell. This technique is widely used by
431:. The limit describes several loss mechanisms that are inherent to any solar cell design.
8:
7904:
7884:
7851:
7659:
7595:
7535:
7494:
6308:
6226:
Miles, R (2006). "Photovoltaic solar cells: Choice of materials and production methods".
5517:
5459:
788:
604:
435:
147:
95:
7272:
6964:
6881:
6838:
6791:
6668:
6625:
6590:
6555:
6505:"Quantum efficiency and temperature coefficients of GaInP/GaAs dual-junction solar cell"
6481:
6239:
5901:
3475:
Figure 1. Photon flux per photon energy from standard solar energy spectrum (AM of 1.5).
27:
7940:
7899:
7846:
7619:
7499:
7363:
7074:
7020:
6987:
6928:
6850:
6823:"Progress in Indium Gallium Nitride Materials for Solar Photovoltaic Energy Conversion"
6760:
6680:
6637:
6524:
6450:
6432:
5984:
5964:
5745:
As less expensive multi-junction materials become available other applications involve
5438:
As of 2014 multi-junction cells were expensive to produce, using techniques similar to
5390:
7280:
6270:
76:. Each material's p–n junction will produce electric current in response to different
7966:
7961:
7894:
7690:
7629:
7560:
7550:
7320:
7114:
7078:
7066:
7045:
7025:
7007:
6932:
6918:
6803:
6684:
6676:
6641:
6633:
6612:
Vos, A. D. (1980). "Detailed balance limit of the efficiency of tandem solar cells".
6454:
6286:"Antireflection coating design for multi-junction, series interconnected solar cells"
6183:
6158:
6001:
5576:
540:
122:
35:
6854:
6764:
6528:
6356:
J.F.Klem, S.Park, J.C.Zolper, Semiconductor tunnel junction with enhancement layer,
5988:
4055:
is evaluated to be 3.6, the value for GaAs. The incident absorbed thermal radiation
526:
and metallic contacts. (b) Graph of spectral irradiance E vs. wavelength λ over the
8023:
8007:
7991:
7981:
7452:
7276:
7225:
7104:
7058:
7046:"Life cycle assessment of recycling strategies for perovskite photovoltaic modules"
7015:
6999:
6968:
6910:
6885:
6842:
6795:
6752:
6672:
6629:
6594:
6559:
6516:
6485:
6442:
6334:
6300:
6266:
6243:
5976:
5905:
5170:
5128:
5068:
850:
251:
200:
69:
6972:
6489:
6208:
6034:"30.2 Percent Efficiency – New Record for Silicon-based Multi-junction Solar Cell"
5909:
5458:
There are four main categories of photovoltaic cells: conventional mono- and poly-
5071:(GaAs) compounds, often germanium for the bottom-, GaAs for the middle-, and GaInP
7935:
7866:
7181:
6446:
6338:
6247:
6115:
6079:
6060:
5980:
5466:(a-Si, CIGS and CdTe), and multi-junction (MJ) solar cells. The fourth category,
5210:
4323:{\displaystyle J=en_{\text{ph}}-A\exp \left({\frac {eV-E_{\text{g}}}{kT}}\right)}
3920:{\displaystyle J_{\text{rad}}=A\exp \left({\frac {eV-E_{\text{g}}}{kT}}\right)\,}
1158:
286:
159:
7229:
6504:
6072:
5147:
As, due to the better lattice match to Ge, resulting in a lower defect density.
8345:
8320:
7986:
7838:
7740:
7730:
7700:
7457:
7174:
7062:
6889:
6136:
High-efficiency multi-junction solar cells: current status and future potential
5938:
5439:
5395:
5225:
1467:
1463:
566:
For optimal growth and resulting crystal quality, the crystal lattice constant
397:
6914:
6846:
6723:"The World's leading provider of compound semiconductor and lighting products"
6520:
6358:
354:. Since solar cells are designed to supply power and not absorb it, the power
8426:
7930:
7920:
7833:
7725:
7442:
7421:
7070:
7011:
6002:"Solar Junction Breaks Concentrated Solar World Record with 43.5% Efficiency"
5818:
5750:
5427:
5271:
Chemical components can be added to some layers. Adding about one percent of
1458:
A window layer is used in order to reduce the surface recombination velocity
455:
439:
240:
167:
110:
is desirable. In terrestrial applications, these solar cells are emerging in
81:
414:
8375:
8330:
8063:
7029:
7003:
6807:
6722:
5674:
MJ solar cells and other photovoltaic devices have significant differences
5386:
1451:
1150:
261:
178:
155:
143:
1074:{\displaystyle n_{\text{L2}}=n_{\text{AlInP}}^{\frac {1}{2}}n_{\text{L1}}}
8370:
8340:
8315:
8073:
7710:
7685:
5547:
5173:
may be used as a substrate to fabricate cells with band gaps between 1.35
4677:{\displaystyle J_{\text{m}}={\frac {en_{\text{ph}}}{1+kT/eV_{\text{m}}}}}
2883:
is the percentage of incident light which is not absorbed by the subcell
1130:
31:
5261:
is reduced and so the tunneling current, which exponentially depends on
3813:
There are no photon flux data in the small photon energy ranges 0–0.3096
1414:{\displaystyle J=J_{S}\left(\exp \left({\frac {qV}{kT}}\right)-1\right)}
515:
need to be used to collect the electrons being generated at each layer.
7856:
7828:
7606:
5846:
5784:
5757:
5686:
5083:
Dual junction cells can be made on gallium arsenide wafers. Alloys of
4148:{\displaystyle J_{th}=A\exp \left({\frac {-E_{\text{g}}}{kT}}\right)\,}
955:
615:
518:
65:
44:
6598:
6305:
10.1002/1099-159X(200011/12)8:6<563::AID-PIP327>3.0.CO;2-8
6180:
Third generation photovoltaics : advanced solar energy conversion
6118:, Technical Information Office, Solar Energy Research Institute (1982)
5705:
a fixed position of the sun in the sky of 48° and a fixed power of 833
3808:
Figure 2. Photon flux from standard solar energy spectrum (AM of 1.5).
8147:
8053:
7925:
7109:
6799:
6756:
6563:
5841:
5136:
1741:
are the short circuit currents of the individual cells in the stack,
1145:
881:
677:
544:
103:
5798:
138:
8360:
8350:
8325:
7337:
Berkeley Lab
Research Sparks Record-Breaking Solar Cell Performance
6437:
2434:
directly from the total J-V characteristic, the quantum efficiency
959:
469:
447:
225:
163:
5367:) (the power density of the light source in a specific wavelength
5197:
As) is lattice matched to Indium
Phosphide with a band gap of 0.74
8365:
6950:
6260:
5812:
1331:
978:
958:
that make contact with the semiconductor layers. They are often
703:
578:
204:
196:
50:
Solar power cell with multiple band gaps from different materials
7390:
5925:
Third Generation Photovoltaics: Advanced Solar Energy Conversion
2459:) be the photon flux of corresponding incident light in subcell
5272:
5247:
662:
217:
151:
7258:
7175:"NREL Solar Cell Sets World Efficiency Record at 40.8 Percent"
2816:{\displaystyle QE_{i}(\lambda )=1-e^{-\alpha (\lambda )d_{i}}}
1835:{\displaystyle J_{0}^{2}=J_{\mathrm {0,1} }J_{\mathrm {0,2} }}
6016:"Sharp Hits Concentrator Solar Cell Efficiency Record, 43.5%"
3007:{\displaystyle V_{\text{OC}}=\sum _{i=1}^{3}V_{{\text{OC}}i}}
2402:) is the short-circuit current density at a given wavelength
1171:
647:
482:
462:
344:
264:. In the quasi-neutral region, the scattering electric field
87:
Traditional single-junction cells have a maximum theoretical
5205:
can be lattice matched for any band gap in between the two.
1771:
is the difference between these short circuit currents, and
1446:
7043:
Tian, Xueyu; Stranks, Samuel D.; You, Fengqi (2021-06-24).
5108:
974:
6986:
Tian, Xueyu; Stranks, Samuel D.; You, Fengqi (July 2020).
5389:, reflective dishes (parabolic or cassegraine), and light
5014:(red line) is plotted in Figure 3 for different values of
3817:
eV because the standard (AM1.5) solar energy spectrum for
2711:
is obtained by linking it with the absorption coefficient
438:, a loss mechanism that affects any material object above
6777:
5721:) to compare performances of different technologies, but
7215:
6742:
477:
terminals, with modern high-quality cells at about 22%.
243:
pair. In the depletion region, the drift electric field
192:
Traditional photovoltaic cells are commonly composed of
5881:
7184:, National Renewable Energy Laboratory, 13 August 2008
6324:
5150:
Due to the huge band gap difference between GaAs (1.42
1441:
6902:
5965:"Four-Junction Wafer Bonded Concentrator Solar Cells"
5453:
5050:
eV. Here, we approximated the photon flux as 0–0.3096
4856:
4704:
4609:
4503:
4452:
4347:
4247:
4083:
3935:
3852:
3491:
3362:
3059:
3024:
2954:
2900:
2840:
2749:
2717:
2678:
2489:
2205:
2178:
2137:
2110:
2083:
1856:
1777:
1747:
1720:
1693:
1537:
1466:
which catches electrons (holes). Indeed, despite the
1344:
1309:
1183:
1081:
to have the same amplitudes for reflected fields and
1027:
7261:
Progress in Photovoltaics: Research and Applications
6745:
Progress in Photovoltaics: Research and Applications
6293:
Progress in Photovoltaics: Research and Applications
5794:
3833:, first. According to Shockley and Queisser method,
102:
have limited their use to special roles, notably in
5216:
4997:{\displaystyle W_{\text{m}}=E_{\text{g}}-kT\left\,}
1170:would be lower than if there would be no parasitic
7044:
4996:
4835:
4676:
4593:
4485:
4421:
4322:
4147:
4033:
3919:
3785:
3439:
3247:
3236:
3042:
3006:
2940:
2875:
2815:
2732:
2703:
2661:
2348:
2191:
2164:
2123:
2096:
2066:
1843:junction cells of the respective cell types.) The
1834:
1763:
1733:
1706:
1676:
1413:
1322:
1291:
1073:
981:in order to increase the transmission coefficient
5446:but on "chip" sizes on the order of centimeters.
1524:-characteristic given by the diode equation, the
8424:
7312:Handbook of Photovoltaic Science and Engineering
6820:
6576:
6467:
614:), which is the source power density at a given
94:As of 2024 the best lab examples of traditional
8107:
4230:eV, as can be shown by evaluation of the above
989:decreases to 1%. In the case of two AR layers L
7309:Luque, Antonio; Hegedus, Steven, eds. (2003).
7042:
6985:
6283:
6132:
5430:system, which increases yield, but also cost.
365:must be negative. Hence, the operating point (
8300:List of countries by photovoltaics production
7977:Solar-Powered Aircraft Developments Solar One
7406:
6502:
5756:MJ cells are currently being utilized in the
5374:
5306:Currently, there are several commercial (non-
5165:
5078:
4493:. The familiar result of this calculation is
4333:The open-circuit voltage is found by setting
698:(MOCVD). This technique is preferable to the
7353:Theoretical research by scientists with the
7308:
7293:
7145:
7133:
6699:"CPV Solar Cells—Azurspace Power Solar GmbH"
6407:
6371:
5181:eV. Indium Phosphide has a band gap of 1.35
4846:Combining the last three equations, we have
2360:short-circuit current of the MJ solar cell:
285:). Consequently, due to the accumulation of
7782:Photovoltaic thermal hybrid solar collector
6116:"Basic Photovoltaic Principles and Methods"
5232:
2948:, the following approximation can be used:
2876:{\displaystyle e^{-\alpha (\lambda )d_{i}}}
2476:) be the quantum efficiency of the subcell
7655:Copper indium gallium selenide solar cells
7413:
7399:
6827:Metallurgical and Materials Transactions A
6422:
3050:are then given by the J-V diode equation:
965:
954:The metallic contacts are low-resistivity
7108:
7103:. Loughborough University. January 2003.
7019:
6867:
6821:McLaughlin, D.V.P.; Pearce, J.M. (2013).
6436:
6418:
6416:
5054:eV as the same as the photon flux at 0.31
4993:
4476:
4144:
4030:
3951:
3916:
3782:
3573:
3436:
3337:Then the photon flux per photon energy, d
2652:
1528:-characteristic of the stack is given by
8117:Grid-connected photovoltaic power system
6203:
6201:
6199:
5941:. National Renewable Energy Laboratory.
5685:
5406:higher under concentrated illumination.
1445:
1144:
517:
413:
137:
133:
26:
8084:Victorian Model Solar Vehicle Challenge
8079:Hunt-Winston School Solar Car Challenge
6654:
6073:"Concentrating Photovoltaic Technology"
5962:
4694:) done per absorbed photon is given by
2413:Because of the impossibility to obtain
696:metal-organic chemical vapor deposition
489:
14:
8425:
7333:
7193:
6413:
6327:Solar Energy Materials and Solar Cells
6013:
5342:) and thus the short-circuit currents
5313:
5118:
3348:ν, with respect to certain irradiance
2941:{\displaystyle V=\sum _{i=1}^{3}V_{i}}
944:
188:, which gives scattering photocurrent.
7394:
7342:Lawrence Berkeley National Laboratory
7159:"Solar cell breaks efficiency record"
7090:
7088:
6946:
6944:
6942:
6657:Journal of Physics D: Applied Physics
6614:Journal of Physics D: Applied Physics
6541:
6403:
6401:
6399:
6397:
6395:
6393:
6352:
6350:
6348:
6225:
6196:
6177:
6152:
6128:
6126:
6124:
6102:
6100:
5939:"Best Research-Cell Efficiency Chart"
5922:
5887:
5352:. As a result, the current densities
4486:{\displaystyle {\frac {dJV}{dV}}\,=0}
4446:) is found by setting the derivative
1515:
8405:
7244:International Journal of Photoenergy
7151:
6509:Science China Technological Sciences
5753:with varied atmospheric conditions.
5691:National Renewable Energy Laboratory
5123:Triple junction cells consisting of
2165:{\displaystyle {\tilde {J}}_{0}^{2}}
1764:{\displaystyle \Delta J_{\text{SC}}}
949:
706:quality and large scale production.
8122:List of photovoltaic power stations
6611:
6263:Materials Science and Engineering B
5945:from the original on March 14, 2023
5776:penetrate to the lower GaAs layer.
1442:Window layer and back-surface field
1140:
632:), high minority carrier lifetimes
24:
8138:Rooftop photovoltaic power station
7541:Polycrystalline silicon (multi-Si)
7490:Third-generation photovoltaic cell
7302:
7139:
7085:
6939:
6390:
6372:J.F.Wheeldon; et al. (2009).
6345:
6318:
6121:
6097:
5454:Comparison with other technologies
3609:
3538:
2480:. By definition, this equates to:
2034:
1985:
1929:
1748:
1644:
1604:
1137:would be strongly reduced to 70%.
558:
409:
25:
8454:
8143:Building-integrated photovoltaics
7640:Carbon nanotubes in photovoltaics
7546:Monocrystalline silicon (mono-Si)
7420:
6870:Superlattices and Microstructures
5444:metalorganic vapour phase epitaxy
5203:indium gallium arsenide phosphide
2733:{\displaystyle \alpha (\lambda )}
977:surface texturation with several
444:standard temperature and pressure
379:) is located in the region where
74:different semiconductor materials
43:triple-junction gallium arsenide
8404:
8393:
8392:
7515:Polarizing organic photovoltaics
6014:Shahan, Zachary (May 31, 2012).
5832:Concentrator photovoltaics (CVP)
5811:
5797:
5440:semiconductor device fabrication
5217:Indium gallium nitride substrate
5033:
3842:can be approximated as follows.
3801:
3468:
3043:{\displaystyle V_{{\text{OC}}i}}
2830:is the thickness of the subcell
2704:{\displaystyle QE_{i}(\lambda )}
442:. In the case of solar cells at
434:The first are the losses due to
7650:Cadmium telluride photovoltaics
7531:List of semiconductor materials
7287:
7252:
7236:
7209:
7187:
7168:
7127:
7036:
6979:
6896:
6861:
6814:
6771:
6736:
6715:
6691:
6648:
6605:
6570:
6535:
6496:
6461:
6365:
6277:
6254:
6219:
6171:
6146:
6109:
6085:
6066:
5827:List of semiconductor materials
5732:
5242:Many MJ photovoltaic cells use
5111:junction has a band gap of 1.42
3248:Theoretical limiting efficiency
1734:{\displaystyle J_{\text{SC,2}}}
1707:{\displaystyle J_{\text{SC,1}}}
18:Multijunction photovoltaic cell
7762:Incremental conductance method
7556:Copper indium gallium selenide
7505:Thermodynamic efficiency limit
6178:Green, Martin (11 July 2003).
6155:Third Generation Photovoltaics
6047:
6026:
6007:
5995:
5956:
5931:
5916:
5859:
5433:
5067:to most of them being made of
3774:
3758:
3722:
3700:
3652:
3614:
3515:
3502:
3352:can be calculated as follows.
3152:
2858:
2852:
2798:
2792:
2769:
2763:
2727:
2721:
2698:
2692:
2649:
2643:
2627:
2621:
2569:
2563:
2557:
2539:
2533:
2509:
2503:
2213:
2145:
2015:
1227:
1208:
702:(MBE) because it ensures high
588:, allowing sub-bandgap light (
128:
13:
1:
8069:South African Solar Challenge
7281:10.1016/S0094-5765(02)00287-4
6973:10.1016/j.solener.2004.09.018
6909:. Vol. 2. p. 1843.
6490:10.1016/j.solener.2009.05.009
6425:IEEE Journal of Photovoltaics
6271:10.1016/S0921-5107(99)00272-X
6092:"Uni-Solar Energy Production"
5969:IEEE Journal of Photovoltaics
5910:10.1016/j.solener.2016.02.015
5853:
396:, and chosen to maximize the
162:. Depending on the location,
7716:Photovoltaic mounting system
7194:Bullis, Kevin (2014-06-09).
6447:10.1109/JPHOTOV.2020.3013974
6339:10.1016/j.solmat.2006.06.028
6248:10.1016/j.vacuum.2006.01.006
6036:. Fraunhofer ISE. 2016-11-09
5981:10.1109/jphotov.2015.2501729
5402:then the MJ current becomes
5237:
5061:
4219:for all semiconductors with
4212:, is negligible compared to
2192:{\displaystyle n_{\text{r}}}
7:
7721:Maximum power point tracker
7334:Yarris, Lynn (7 Nov 2011).
7230:10.1016/j.desal.2007.04.012
5790:
5229:competitive in the market.
5201:eV. A quaternary alloy of
4687:Finally, the maximum work (
10:
8459:
7972:Solar panels on spacecraft
7819:Solar-powered refrigerator
7777:Concentrated photovoltaics
7757:Perturb and observe method
7536:Crystalline silicon (c-Si)
7063:10.1038/s41893-021-00737-z
6890:10.1016/j.spmi.2007.05.001
6677:10.1088/0022-3727/12/3/014
6634:10.1088/0022-3727/13/5/018
6579:Journal of Applied Physics
6544:Journal of Applied Physics
5381:Concentrator photovoltaics
5378:
5375:Use of light concentrators
5166:Indium phosphide substrate
5079:Gallium arsenide substrate
5007:Using the above equation,
112:concentrator photovoltaics
100:price-to-performance ratio
8388:
8308:
8292:
8283:
8161:
8130:
8096:
8016:
8000:
7954:
7913:
7811:
7804:
7749:
7678:
7670:Heterojunction solar cell
7645:Dye-sensitized solar cell
7605:
7594:
7569:
7523:
7485:Multi-junction solar cell
7475:Nominal power (Watt-peak)
7435:
7428:
7355:U.S. Department of Energy
6915:10.1109/WCPEC.1994.520724
6847:10.1007/s11661-013-1622-1
6521:10.1007/s11431-008-0203-9
5923:Green, Martin A. (2003).
5837:Organic photovoltaic cell
5570:
5516:
4432:The maximum power point (
4051:is in electron volts and
1450:Figure E: (a) Layers and
680:for the bottom sub-cell (
665:for the middle sub-cell (
239:, generating an electron-
177:, which gives generation
8153:Strasskirchen Solar Park
8044:American Solar Challenge
7890:Solar-powered flashlight
7877:Solar-powered calculator
7872:Solar cell phone charger
7561:Amorphous silicon (a-Si)
7294:Luque & Hegedus 2003
7146:Luque & Hegedus 2003
7134:Luque & Hegedus 2003
6408:Luque & Hegedus 2003
6182:. Springer. p. 61.
5849:(a-Si/μc-Si tandem-cell)
5767:eV vs those between 1.87
5233:Performance improvements
5125:indium gallium phosphide
5085:indium gallium phosphide
3295:is the Planck constant (
993:(the top layer, usually
347:in the dark downward by
260:is called the generated
82:semiconducting materials
8059:Frisian Solar Challenge
8029:List of solar car teams
7787:Space-based solar power
7767:Constant voltage method
7696:Solar charge controller
7582:Timeline of solar cells
7577:Growth of photovoltaics
6284:Daniel J.Aiken (2000).
6133:N.V.Yastrebova (2007).
5963:Dimroth, Frank (2016).
5927:. Springer. p. 65.
5805:Renewable energy portal
5187:Indium gallium arsenide
5133:indium gallium arsenide
966:Anti-reflective coating
572:metamorphic solar cells
524:anti-reflective coating
429:Shockley–Queisser limit
420:Shockley–Queisser limit
8049:Formula Sun Grand Prix
7881:Solar-powered fountain
7824:Solar air conditioning
7625:Quantum dot solar cell
7615:Nanocrystal solar cell
7510:Sun-free photovoltaics
7198:. Technologyreview.com
7004:10.1126/sciadv.abb0055
6054:"ZTJ Space Solar Cell"
5698:
5468:emerging photovoltaics
5222:Indium gallium nitride
4998:
4837:
4678:
4595:
4487:
4423:
4324:
4149:
4035:
3921:
3787:
3613:
3441:
3238:
3044:
3008:
2988:
2942:
2927:
2877:
2817:
2734:
2705:
2663:
2350:
2193:
2166:
2125:
2098:
2068:
1836:
1765:
1735:
1708:
1678:
1455:
1415:
1324:
1293:
1154:
1075:
700:molecular beam epitaxy
650:for the top sub-cell (
639:, and high mobilities
531:
513:transparent conductors
424:
189:
80:. The use of multiple
47:
8443:Semiconductor devices
8039:World Solar Challenge
7862:Photovoltaic keyboard
7792:PV system performance
7665:Perovskite solar cell
7463:Solar cell efficiency
7317:John Wiley & Sons
7051:Nature Sustainability
6359:U.S. patent 5,679,963
5695:solar cell efficiency
5689:
5676:(see the table above)
5648:Multi-junction cells
5572:Thin film solar cells
5464:thin film solar cells
4999:
4838:
4679:
4596:
4488:
4424:
4325:
4150:
4036:
3922:
3788:
3586:
3442:
3239:
3045:
3009:
2968:
2943:
2907:
2878:
2818:
2735:
2706:
2664:
2351:
2194:
2167:
2126:
2124:{\displaystyle T^{+}}
2099:
2097:{\displaystyle T^{-}}
2077:Here, the parameters
2069:
1837:
1766:
1736:
1709:
1679:
1449:
1416:
1325:
1323:{\displaystyle J_{P}}
1294:
1163:electrical resistance
1149:Figure D: Layers and
1148:
1076:
537:thin film solar cells
521:
417:
343:characteristics of a
141:
134:Basics of solar cells
119:thin-film solar cells
108:power-to-weight ratio
30:
8309:Individual producers
8017:Solar vehicle racing
7706:Solar micro-inverter
7635:Plasmonic solar cell
7480:Thin-film solar cell
7448:Photoelectric effect
6333:(18–19): 3068–3077.
6153:Green, M.A. (2003).
5680:thin film solar cell
4854:
4702:
4607:
4501:
4450:
4345:
4245:
4081:
3933:
3850:
3489:
3360:
3057:
3022:
2952:
2898:
2838:
2747:
2715:
2676:
2487:
2203:
2176:
2135:
2108:
2081:
1854:
1775:
1745:
1718:
1691:
1535:
1342:
1307:
1181:
1161:is to provide a low
1025:
553:III–V semiconductors
490:Multi-junction cells
452:photoelectric effect
146:illustration of the
78:wavelengths of light
7905:Solar traffic light
7885:Solar-powered radio
7852:Solar-powered watch
7660:Printed solar panel
7495:Solar cell research
7273:2004AcAau..54...83C
6965:2005SoEn...79...78Y
6882:2008SuMi...43....1Y
6839:2013MMTA...44.1947M
6792:2007NatMa...6..951K
6669:1979JPhD...12..441P
6626:1980JPhD...13..839D
6591:1961JAP....32..510S
6556:1980JAP....51.4494H
6482:2009SoEn...83.1588P
6240:2006Vacuu..80.1090M
6213:www.superstrate.net
6157:. Springer-Verlag.
5902:2016SoEn..130..139R
5869:. Dutch Space. 2007
5867:"Dawn Solar Arrays"
5747:bandgap engineering
5518:Crystalline silicon
5460:crystalline silicon
5398:). If its value is
5314:Spectral variations
5244:III–V semiconductor
5119:Germanium substrate
3998:
3542:
3311:is speed of light (
2891:Similarly, because
2607:
2308:
2261:
2229:
2161:
2031:
1792:
1641:
1060:
945:Structural elements
605:spectral irradiance
436:blackbody radiation
400:of the power |
293:and a photocurrent
170:are accelerated by
148:photovoltaic effect
96:crystalline silicon
7941:The Quiet Achiever
7900:Solar street light
7847:Solar-powered pump
7620:Organic solar cell
7500:Thermophotovoltaic
7468:Quantum efficiency
7180:2008-09-17 at the
7157:Michael Kanellos,
6725:. Spectrolab. 2009
6078:2011-08-22 at the
6059:2011-09-28 at the
5742:become practical.
5699:
5075:for the top-cell.
4994:
4833:
4674:
4591:
4483:
4419:
4320:
4145:
4031:
3984:
3917:
3783:
3521:
3437:
3330:is frequency, and
3291:is photon energy,
3234:
3040:
3004:
2938:
2873:
2813:
2730:
2701:
2659:
2590:
2346:
2294:
2247:
2206:
2189:
2162:
2138:
2121:
2094:
2064:
2008:
1832:
1778:
1761:
1731:
1704:
1674:
1627:
1516:J-V characteristic
1456:
1411:
1320:
1289:
1166:Consequently, the
1155:
1071:
1041:
532:
425:
203:with a particular
190:
48:
8438:Energy conversion
8420:
8419:
8384:
8383:
8279:
8278:
8092:
8091:
7967:Mauro Solar Riser
7962:Electric aircraft
7895:Solar-powered fan
7800:
7799:
7691:Balance of system
7679:System components
7630:Hybrid solar cell
7590:
7589:
7551:Cadmium telluride
7326:978-0-471-49196-5
7296:, pp. 414 ff
7246:,514962, pp. 1-7.
7165:, 6 December 2006
7148:, pp. 449 ff
6924:978-0-7803-1460-3
6599:10.1063/1.1736034
6234:(10): 1090–1097.
6189:978-3-540-40137-7
6164:978-3-540-26562-7
5672:
5671:
5577:Amorphous silicon
5154:eV), and Ge (0.66
4975:
4963:
4924:
4920:
4877:
4864:
4821:
4806:
4802:
4770:
4752:
4749:
4738:
4728:
4712:
4672:
4668:
4636:
4617:
4584:
4572:
4530:
4514:
4474:
4413:
4409:
4371:
4358:
4314:
4302:
4264:
4205:The second term,
4138:
4126:
4028:
3991:
3910:
3898:
3860:
3756:
3741:
3698:
3683:
3663:
3604:
3571:
3556:
3533:
3499:
3455:/(1.998 × 10 ) =
3434:
3433:
3411:
3408:
3391:
3376:
3315: =
3228:
3208:
3186:
3163:
3145:
3120:
3033:
2997:
2962:
2580:
2567:
2526:
2301:
2254:
2216:
2186:
2148:
2059:
2056:
2018:
1995:
1981:
1939:
1917:
1898:
1885:
1871:
1758:
1728:
1701:
1669:
1666:
1614:
1600:
1579:
1566:
1552:
1394:
1287:
1285:
1281:
1271:
1259:
1246:
1234:
1191:
1157:The main goal of
1068:
1058:
1048:
1035:
1021:), there must be
950:Metallic contacts
942:
941:
541:amorphous silicon
335:characteristics (
123:amorphous silicon
106:where their high
16:(Redirected from
8450:
8408:
8407:
8396:
8395:
8290:
8289:
8131:Building-mounted
8109:PV power station
8105:
8104:
8034:Solar challenges
8024:Solar car racing
7992:Solar Challenger
7982:Gossamer Penguin
7809:
7808:
7603:
7602:
7453:Solar irradiance
7433:
7432:
7415:
7408:
7401:
7392:
7391:
7384:R&D Magazine
7379:
7373:
7369:
7367:
7359:
7350:
7348:
7330:
7297:
7291:
7285:
7284:
7256:
7250:
7240:
7234:
7233:
7213:
7207:
7206:
7204:
7203:
7191:
7185:
7172:
7166:
7155:
7149:
7143:
7137:
7136:, pp. 61 ff
7131:
7125:
7124:
7112:
7102:
7092:
7083:
7082:
7048:
7040:
7034:
7033:
7023:
6998:(31): eabb0055.
6992:Science Advances
6983:
6977:
6976:
6948:
6937:
6936:
6900:
6894:
6893:
6865:
6859:
6858:
6833:(4): 1947–1954.
6818:
6812:
6811:
6800:10.1038/nmat2037
6780:Nature Materials
6775:
6769:
6768:
6757:10.1002/pip.2267
6740:
6734:
6733:
6731:
6730:
6719:
6713:
6712:
6710:
6709:
6695:
6689:
6688:
6652:
6646:
6645:
6609:
6603:
6602:
6574:
6568:
6567:
6564:10.1063/1.328272
6539:
6533:
6532:
6515:(5): 1176–1180.
6500:
6494:
6493:
6476:(9): 1588–1598.
6465:
6459:
6458:
6440:
6431:(6): 1701–1711.
6420:
6411:
6410:, p. 390 ff
6405:
6388:
6387:
6385:
6379:. Archived from
6378:
6369:
6363:
6361:
6354:
6343:
6342:
6322:
6316:
6315:
6313:
6307:. Archived from
6290:
6281:
6275:
6274:
6265:. 69–70: 81–86.
6258:
6252:
6251:
6223:
6217:
6216:
6205:
6194:
6193:
6175:
6169:
6168:
6150:
6144:
6143:
6141:
6130:
6119:
6113:
6107:
6104:
6095:
6089:
6083:
6070:
6064:
6051:
6045:
6044:
6042:
6041:
6030:
6024:
6023:
6011:
6005:
5999:
5993:
5992:
5960:
5954:
5953:
5951:
5950:
5935:
5929:
5928:
5920:
5914:
5913:
5885:
5879:
5878:
5876:
5874:
5863:
5821:
5816:
5815:
5807:
5802:
5801:
5782:
5774:
5770:
5766:
5708:
5473:
5472:
5424:
5416:
5412:
5279:
5200:
5184:
5180:
5176:
5171:Indium phosphide
5157:
5153:
5129:gallium arsenide
5114:
5106:
5069:gallium arsenide
5057:
5053:
5049:
5037:
5003:
5001:
5000:
4995:
4992:
4988:
4981:
4977:
4976:
4974:
4966:
4965:
4964:
4961:
4951:
4929:
4925:
4923:
4922:
4921:
4918:
4905:
4879:
4878:
4875:
4866:
4865:
4862:
4842:
4840:
4839:
4834:
4823:
4822:
4819:
4807:
4805:
4804:
4803:
4800:
4791:
4773:
4772:
4771:
4768:
4758:
4753:
4751:
4750:
4747:
4741:
4740:
4739:
4736:
4730:
4729:
4726:
4719:
4714:
4713:
4710:
4683:
4681:
4680:
4675:
4673:
4671:
4670:
4669:
4666:
4657:
4639:
4638:
4637:
4634:
4624:
4619:
4618:
4615:
4600:
4598:
4597:
4592:
4590:
4586:
4585:
4583:
4575:
4574:
4573:
4570:
4560:
4532:
4531:
4528:
4516:
4515:
4512:
4492:
4490:
4489:
4484:
4475:
4473:
4465:
4454:
4428:
4426:
4425:
4420:
4418:
4414:
4412:
4411:
4410:
4407:
4394:
4373:
4372:
4369:
4360:
4359:
4356:
4329:
4327:
4326:
4321:
4319:
4315:
4313:
4305:
4304:
4303:
4300:
4284:
4266:
4265:
4262:
4229:
4154:
4152:
4151:
4146:
4143:
4139:
4137:
4129:
4128:
4127:
4124:
4114:
4096:
4095:
4040:
4038:
4037:
4032:
4029:
4027:
4026:
4025:
4016:
4015:
4005:
3997:
3992:
3989:
3983:
3979:
3972:
3971:
3943:
3926:
3924:
3923:
3918:
3915:
3911:
3909:
3901:
3900:
3899:
3896:
3880:
3862:
3861:
3858:
3824:
3816:
3805:
3792:
3790:
3789:
3784:
3781:
3777:
3773:
3772:
3757:
3755:
3744:
3743:
3742:
3739:
3729:
3721:
3720:
3699:
3697:
3686:
3685:
3684:
3681:
3671:
3664:
3656:
3651:
3650:
3635:
3634:
3612:
3607:
3606:
3605:
3602:
3572:
3570:
3559:
3558:
3557:
3554:
3544:
3541:
3536:
3535:
3534:
3531:
3514:
3513:
3501:
3500:
3497:
3472:
3446:
3444:
3443:
3438:
3435:
3429:
3421:
3417:
3412:
3410:
3409:
3406:
3397:
3392:
3390:
3379:
3378:
3377:
3374:
3364:
3325:
3323:
3320:
3306:
3304:
3243:
3241:
3240:
3235:
3233:
3229:
3227:
3226:
3214:
3213:
3209:
3206:
3199:
3187:
3182:
3174:
3169:
3168:
3164:
3161:
3151:
3150:
3146:
3143:
3133:
3129:
3122:
3121:
3119:
3111:
3110:
3109:
3096:
3085:
3084:
3069:
3068:
3049:
3047:
3046:
3041:
3039:
3038:
3034:
3031:
3013:
3011:
3010:
3005:
3003:
3002:
2998:
2995:
2987:
2982:
2964:
2963:
2960:
2947:
2945:
2944:
2939:
2937:
2936:
2926:
2921:
2882:
2880:
2879:
2874:
2872:
2871:
2870:
2869:
2822:
2820:
2819:
2814:
2812:
2811:
2810:
2809:
2762:
2761:
2739:
2737:
2736:
2731:
2710:
2708:
2707:
2702:
2691:
2690:
2668:
2666:
2665:
2660:
2642:
2641:
2620:
2619:
2606:
2598:
2586:
2585:
2581:
2578:
2568:
2566:
2556:
2555:
2542:
2532:
2531:
2527:
2524:
2516:
2502:
2501:
2406:for the subcell
2355:
2353:
2352:
2347:
2345:
2344:
2329:
2325:
2324:
2323:
2307:
2302:
2299:
2287:
2286:
2266:
2262:
2260:
2255:
2252:
2228:
2223:
2218:
2217:
2209:
2198:
2196:
2195:
2190:
2188:
2187:
2184:
2171:
2169:
2168:
2163:
2160:
2155:
2150:
2149:
2141:
2130:
2128:
2127:
2122:
2120:
2119:
2103:
2101:
2100:
2095:
2093:
2092:
2073:
2071:
2070:
2065:
2060:
2058:
2057:
2055:
2047:
2039:
2037:
2030:
2025:
2020:
2019:
2011:
2004:
2003:
1998:
1997:
1996:
1993:
1982:
1974:
1972:
1970:
1966:
1965:
1964:
1941:
1940:
1937:
1928:
1927:
1918:
1910:
1905:
1901:
1900:
1899:
1896:
1887:
1886:
1883:
1872:
1864:
1841:
1839:
1838:
1833:
1831:
1830:
1829:
1813:
1812:
1811:
1791:
1786:
1770:
1768:
1767:
1762:
1760:
1759:
1756:
1740:
1738:
1737:
1732:
1730:
1729:
1726:
1713:
1711:
1710:
1705:
1703:
1702:
1699:
1683:
1681:
1680:
1675:
1670:
1668:
1667:
1665:
1657:
1649:
1647:
1640:
1635:
1623:
1622:
1617:
1616:
1615:
1612:
1601:
1593:
1591:
1586:
1582:
1581:
1580:
1577:
1568:
1567:
1564:
1553:
1545:
1511:
1420:
1418:
1417:
1412:
1410:
1406:
1399:
1395:
1393:
1385:
1377:
1360:
1359:
1329:
1327:
1326:
1321:
1319:
1318:
1298:
1296:
1295:
1290:
1288:
1286:
1284:
1283:
1282:
1279:
1273:
1272:
1269:
1262:
1261:
1260:
1257:
1248:
1247:
1244:
1237:
1235:
1230:
1220:
1219:
1200:
1198:
1193:
1192:
1189:
1159:tunnel junctions
1141:Tunnel junctions
1080:
1078:
1077:
1072:
1070:
1069:
1066:
1059:
1051:
1049:
1046:
1037:
1036:
1033:
1020:
1019:
1018:
1004:
1003:
1002:
743:
741:
709:
708:
690:
675:
660:
506:
502:
405:
395:
385:
42:
21:
8458:
8457:
8453:
8452:
8451:
8449:
8448:
8447:
8423:
8422:
8421:
8416:
8380:
8304:
8275:
8157:
8126:
8099:
8088:
8012:
8001:Water transport
7996:
7950:
7936:Solar golf cart
7909:
7867:Solar road stud
7796:
7750:System concepts
7745:
7674:
7597:
7586:
7565:
7519:
7424:
7419:
7371:
7370:
7361:
7360:
7346:
7344:
7327:
7305:
7303:Further reading
7300:
7292:
7288:
7257:
7253:
7241:
7237:
7214:
7210:
7201:
7199:
7192:
7188:
7182:Wayback Machine
7173:
7169:
7156:
7152:
7144:
7140:
7132:
7128:
7121:
7100:
7094:
7093:
7086:
7041:
7037:
6984:
6980:
6949:
6940:
6925:
6901:
6897:
6866:
6862:
6819:
6815:
6786:(12): 951–956.
6776:
6772:
6741:
6737:
6728:
6726:
6721:
6720:
6716:
6707:
6705:
6697:
6696:
6692:
6653:
6649:
6610:
6606:
6575:
6571:
6540:
6536:
6501:
6497:
6466:
6462:
6421:
6414:
6406:
6391:
6383:
6376:
6370:
6366:
6357:
6355:
6346:
6323:
6319:
6311:
6288:
6282:
6278:
6259:
6255:
6224:
6220:
6207:
6206:
6197:
6190:
6176:
6172:
6165:
6151:
6147:
6139:
6131:
6122:
6114:
6110:
6105:
6098:
6090:
6086:
6080:Wayback Machine
6071:
6067:
6061:Wayback Machine
6052:
6048:
6039:
6037:
6032:
6031:
6027:
6012:
6008:
6000:
5996:
5961:
5957:
5948:
5946:
5937:
5936:
5932:
5921:
5917:
5886:
5882:
5872:
5870:
5865:
5864:
5860:
5856:
5817:
5810:
5803:
5796:
5793:
5780:
5772:
5768:
5764:
5740:MJ solar panels
5735:
5706:
5524:Monocrystalline
5499:
5490:
5456:
5436:
5422:
5414:
5410:
5383:
5377:
5357:
5351:
5316:
5286:
5277:
5267:
5260:
5240:
5235:
5219:
5211:dichroic filter
5198:
5196:
5192:
5182:
5178:
5174:
5168:
5155:
5151:
5146:
5142:
5121:
5112:
5107:eV. The lower
5104:
5102:
5098:
5094:
5090:
5087:in the range In
5081:
5074:
5064:
5055:
5051:
5047:
5041:
5038:
5027:
5020:
5013:
4967:
4960:
4956:
4952:
4950:
4943:
4939:
4917:
4913:
4909:
4904:
4900:
4893:
4889:
4874:
4870:
4861:
4857:
4855:
4852:
4851:
4818:
4814:
4799:
4795:
4787:
4774:
4767:
4763:
4759:
4757:
4746:
4742:
4735:
4731:
4725:
4721:
4720:
4718:
4709:
4705:
4703:
4700:
4699:
4693:
4665:
4661:
4653:
4640:
4633:
4629:
4625:
4623:
4614:
4610:
4608:
4605:
4604:
4576:
4569:
4565:
4561:
4559:
4552:
4548:
4527:
4523:
4511:
4507:
4502:
4499:
4498:
4466:
4455:
4453:
4451:
4448:
4447:
4445:
4438:
4406:
4402:
4398:
4393:
4389:
4368:
4364:
4355:
4351:
4346:
4343:
4342:
4306:
4299:
4295:
4285:
4283:
4279:
4261:
4257:
4246:
4243:
4242:
4236:
4227:
4225:
4218:
4211:
4201:
4194:
4187:
4172:
4165:
4130:
4123:
4119:
4115:
4113:
4109:
4088:
4084:
4082:
4079:
4078:
4068:
4061:
4050:
4021:
4017:
4011:
4007:
4006:
3993:
3988:
3967:
3963:
3962:
3958:
3944:
3942:
3934:
3931:
3930:
3902:
3895:
3891:
3881:
3879:
3875:
3857:
3853:
3851:
3848:
3847:
3841:
3832:
3822:
3814:
3809:
3806:
3768:
3764:
3745:
3738:
3734:
3730:
3728:
3710:
3706:
3687:
3680:
3676:
3672:
3670:
3669:
3665:
3655:
3646:
3642:
3624:
3620:
3608:
3601:
3597:
3590:
3560:
3553:
3549:
3545:
3543:
3537:
3530:
3526:
3525:
3509:
3505:
3496:
3492:
3490:
3487:
3486:
3476:
3473:
3422:
3416:
3405:
3401:
3396:
3380:
3373:
3369:
3365:
3363:
3361:
3358:
3357:
3343:
3334:is wavelength.
3321:
3318:
3316:
3302:
3300:
3290:
3263:
3250:
3219:
3215:
3205:
3204:
3200:
3198:
3194:
3175:
3173:
3160:
3159:
3155:
3142:
3141:
3137:
3112:
3105:
3101:
3097:
3095:
3091:
3090:
3086:
3077:
3073:
3064:
3060:
3058:
3055:
3054:
3030:
3029:
3025:
3023:
3020:
3019:
2994:
2993:
2989:
2983:
2972:
2959:
2955:
2953:
2950:
2949:
2932:
2928:
2922:
2911:
2899:
2896:
2895:
2865:
2861:
2845:
2841:
2839:
2836:
2835:
2828:
2805:
2801:
2785:
2781:
2757:
2753:
2748:
2745:
2744:
2716:
2713:
2712:
2686:
2682:
2677:
2674:
2673:
2637:
2633:
2615:
2611:
2599:
2594:
2577:
2576:
2572:
2551:
2547:
2543:
2523:
2522:
2518:
2517:
2515:
2497:
2493:
2488:
2485:
2484:
2471:
2454:
2433:
2426:
2419:
2397:
2387:
2380:
2373:
2366:
2334:
2330:
2313:
2309:
2303:
2298:
2276:
2272:
2271:
2267:
2256:
2251:
2237:
2233:
2224:
2219:
2208:
2207:
2204:
2201:
2200:
2183:
2179:
2177:
2174:
2173:
2156:
2151:
2140:
2139:
2136:
2133:
2132:
2115:
2111:
2109:
2106:
2105:
2088:
2084:
2082:
2079:
2078:
2048:
2040:
2038:
2033:
2032:
2026:
2021:
2010:
2009:
1999:
1992:
1988:
1984:
1983:
1973:
1971:
1960:
1956:
1949:
1945:
1936:
1932:
1923:
1919:
1909:
1895:
1891:
1882:
1878:
1877:
1873:
1863:
1855:
1852:
1851:
1819:
1818:
1814:
1801:
1800:
1796:
1787:
1782:
1776:
1773:
1772:
1755:
1751:
1746:
1743:
1742:
1725:
1721:
1719:
1716:
1715:
1698:
1694:
1692:
1689:
1688:
1658:
1650:
1648:
1643:
1642:
1636:
1631:
1618:
1611:
1607:
1603:
1602:
1592:
1590:
1576:
1572:
1563:
1559:
1558:
1554:
1544:
1536:
1533:
1532:
1518:
1509:
1503:
1496:
1489:
1482:
1474:
1444:
1437:
1430:
1386:
1378:
1376:
1372:
1365:
1361:
1355:
1351:
1343:
1340:
1339:
1314:
1310:
1308:
1305:
1304:
1278:
1274:
1268:
1264:
1263:
1256:
1252:
1243:
1239:
1238:
1236:
1215:
1211:
1201:
1199:
1197:
1188:
1184:
1182:
1179:
1178:
1143:
1127:
1120:
1113:
1107:
1100:
1093:
1087:
1065:
1061:
1050:
1045:
1032:
1028:
1026:
1023:
1022:
1017:
1014:
1013:
1012:
1010:
1008:
1001:
998:
997:
996:
994:
992:
971:Anti-reflective
968:
952:
947:
782:
775:
768:
763:
762:
753:
752:
739:
734:
733:
732:Absorption, at
728:
721:
720:
688:
686:
673:
671:
658:
656:
638:
602:
587:
561:
559:Material choice
504:
500:
492:
450:created by the
412:
410:Loss mechanisms
401:
393:
387:
380:
378:
371:
364:
353:
327:
320:
313:
306:
299:
284:
277:
270:
259:
249:
238:
213:
187:
176:
160:conduction band
136:
131:
51:
40:
23:
22:
15:
12:
11:
5:
8456:
8446:
8445:
8440:
8435:
8418:
8417:
8415:
8414:
8402:
8389:
8386:
8385:
8382:
8381:
8379:
8378:
8373:
8368:
8363:
8358:
8353:
8348:
8346:Solar Frontier
8343:
8338:
8333:
8328:
8323:
8321:Hanwha Q CELLS
8318:
8312:
8310:
8306:
8305:
8303:
8302:
8296:
8294:
8287:
8281:
8280:
8277:
8276:
8274:
8273:
8268:
8266:United Kingdom
8263:
8258:
8253:
8248:
8243:
8238:
8233:
8228:
8223:
8218:
8213:
8208:
8203:
8201:Czech Republic
8198:
8193:
8188:
8183:
8178:
8173:
8167:
8165:
8159:
8158:
8156:
8155:
8150:
8145:
8140:
8134:
8132:
8128:
8127:
8125:
8124:
8119:
8113:
8111:
8102:
8094:
8093:
8090:
8089:
8087:
8086:
8081:
8076:
8071:
8066:
8061:
8056:
8051:
8046:
8041:
8036:
8031:
8026:
8020:
8018:
8014:
8013:
8011:
8010:
8004:
8002:
7998:
7997:
7995:
7994:
7989:
7987:Qinetiq Zephyr
7984:
7979:
7974:
7969:
7964:
7958:
7956:
7952:
7951:
7949:
7948:
7943:
7938:
7933:
7928:
7923:
7917:
7915:
7914:Land transport
7911:
7910:
7908:
7907:
7902:
7897:
7892:
7887:
7882:
7879:
7874:
7869:
7864:
7859:
7854:
7849:
7844:
7841:
7839:Solar backpack
7836:
7831:
7826:
7821:
7815:
7813:
7806:
7802:
7801:
7798:
7797:
7795:
7794:
7789:
7784:
7779:
7774:
7769:
7764:
7759:
7753:
7751:
7747:
7746:
7744:
7743:
7741:Synchronverter
7738:
7733:
7731:Solar shingles
7728:
7723:
7718:
7713:
7708:
7703:
7701:Solar inverter
7698:
7693:
7688:
7682:
7680:
7676:
7675:
7673:
7672:
7667:
7662:
7657:
7652:
7647:
7642:
7637:
7632:
7627:
7622:
7617:
7611:
7609:
7600:
7592:
7591:
7588:
7587:
7585:
7584:
7579:
7573:
7571:
7567:
7566:
7564:
7563:
7558:
7553:
7548:
7543:
7538:
7533:
7527:
7525:
7521:
7520:
7518:
7517:
7512:
7507:
7502:
7497:
7492:
7487:
7482:
7477:
7472:
7471:
7470:
7460:
7458:Solar constant
7455:
7450:
7445:
7439:
7437:
7430:
7426:
7425:
7418:
7417:
7410:
7403:
7395:
7389:
7388:
7331:
7325:
7304:
7301:
7299:
7298:
7286:
7251:
7235:
7224:(1–3): 78–85.
7208:
7186:
7167:
7150:
7138:
7126:
7119:
7084:
7057:(9): 821–829.
7035:
6978:
6938:
6923:
6895:
6860:
6813:
6770:
6735:
6714:
6690:
6663:(3): 441–450.
6647:
6620:(5): 839–846.
6604:
6569:
6534:
6495:
6460:
6412:
6389:
6386:on 2009-11-17.
6364:
6344:
6317:
6314:on 2011-07-21.
6299:(6): 563–570.
6276:
6253:
6218:
6209:"Tandem cells"
6195:
6188:
6170:
6163:
6145:
6120:
6108:
6096:
6084:
6065:
6046:
6025:
6006:
5994:
5955:
5930:
5915:
5880:
5857:
5855:
5852:
5851:
5850:
5844:
5839:
5834:
5829:
5823:
5822:
5808:
5792:
5789:
5734:
5731:
5670:
5669:
5667:
5664:
5661:
5658:
5655:
5652:
5649:
5645:
5644:
5642:
5639:
5636:
5633:
5630:
5627:
5621:
5620:
5618:
5615:
5612:
5609:
5606:
5603:
5597:
5596:
5594:
5591:
5588:
5585:
5582:
5579:
5574:
5568:
5567:
5565:
5562:
5559:
5556:
5553:
5550:
5544:
5543:
5541:
5538:
5535:
5532:
5529:
5526:
5521:
5514:
5513:
5510:
5504:
5501:
5497:
5492:
5488:
5483:
5480:
5477:
5462:(c-Si) cells,
5455:
5452:
5435:
5432:
5396:solar constant
5387:Fresnel lenses
5376:
5373:
5355:
5346:
5315:
5312:
5284:
5265:
5258:
5239:
5236:
5234:
5231:
5226:direct bandgap
5218:
5215:
5194:
5190:
5167:
5164:
5144:
5140:
5120:
5117:
5100:
5096:
5092:
5088:
5080:
5077:
5072:
5063:
5060:
5043:
5042:
5039:
5032:
5025:
5018:
5011:
5005:
5004:
4991:
4987:
4984:
4980:
4973:
4970:
4959:
4955:
4949:
4946:
4942:
4938:
4935:
4932:
4928:
4916:
4912:
4908:
4903:
4899:
4896:
4892:
4888:
4885:
4882:
4873:
4869:
4860:
4844:
4843:
4832:
4829:
4826:
4817:
4813:
4810:
4798:
4794:
4790:
4786:
4783:
4780:
4777:
4766:
4762:
4756:
4745:
4734:
4724:
4717:
4708:
4691:
4685:
4684:
4664:
4660:
4656:
4652:
4649:
4646:
4643:
4632:
4628:
4622:
4613:
4601:
4589:
4582:
4579:
4568:
4564:
4558:
4555:
4551:
4547:
4544:
4541:
4538:
4535:
4526:
4522:
4519:
4510:
4506:
4482:
4479:
4472:
4469:
4464:
4461:
4458:
4443:
4436:
4430:
4429:
4417:
4405:
4401:
4397:
4392:
4388:
4385:
4382:
4379:
4376:
4367:
4363:
4354:
4350:
4331:
4330:
4318:
4312:
4309:
4298:
4294:
4291:
4288:
4282:
4278:
4275:
4272:
4269:
4260:
4256:
4253:
4250:
4234:
4223:
4216:
4209:
4203:
4202:
4199:
4192:
4185:
4170:
4163:
4156:
4155:
4142:
4136:
4133:
4122:
4118:
4112:
4108:
4105:
4102:
4099:
4094:
4091:
4087:
4066:
4059:
4048:
4042:
4041:
4024:
4020:
4014:
4010:
4004:
4001:
3996:
3987:
3982:
3978:
3975:
3970:
3966:
3961:
3957:
3954:
3950:
3947:
3941:
3938:
3927:
3914:
3908:
3905:
3894:
3890:
3887:
3884:
3878:
3874:
3871:
3868:
3865:
3856:
3839:
3830:
3811:
3810:
3807:
3800:
3794:
3793:
3780:
3776:
3771:
3767:
3763:
3760:
3754:
3751:
3748:
3737:
3733:
3727:
3724:
3719:
3716:
3713:
3709:
3705:
3702:
3696:
3693:
3690:
3679:
3675:
3668:
3662:
3659:
3654:
3649:
3645:
3641:
3638:
3633:
3630:
3627:
3623:
3619:
3616:
3611:
3600:
3596:
3593:
3589:
3585:
3582:
3579:
3576:
3569:
3566:
3563:
3552:
3548:
3540:
3529:
3524:
3520:
3517:
3512:
3508:
3504:
3495:
3478:
3477:
3474:
3467:
3461:
3460:
3432:
3428:
3425:
3420:
3415:
3404:
3400:
3395:
3389:
3386:
3383:
3372:
3368:
3341:
3288:
3282:
3281:
3261:
3249:
3246:
3245:
3244:
3232:
3225:
3222:
3218:
3212:
3203:
3197:
3193:
3190:
3185:
3181:
3178:
3172:
3167:
3158:
3154:
3149:
3140:
3136:
3132:
3128:
3125:
3118:
3115:
3108:
3104:
3100:
3094:
3089:
3083:
3080:
3076:
3072:
3067:
3063:
3037:
3028:
3018:The values of
3016:
3015:
3001:
2992:
2986:
2981:
2978:
2975:
2971:
2967:
2958:
2935:
2931:
2925:
2920:
2917:
2914:
2910:
2906:
2903:
2889:
2888:
2868:
2864:
2860:
2857:
2854:
2851:
2848:
2844:
2826:
2808:
2804:
2800:
2797:
2794:
2791:
2788:
2784:
2780:
2777:
2774:
2771:
2768:
2765:
2760:
2756:
2752:
2729:
2726:
2723:
2720:
2700:
2697:
2694:
2689:
2685:
2681:
2670:
2669:
2658:
2655:
2651:
2648:
2645:
2640:
2636:
2632:
2629:
2626:
2623:
2618:
2614:
2610:
2605:
2602:
2597:
2593:
2589:
2584:
2575:
2571:
2565:
2562:
2559:
2554:
2550:
2546:
2541:
2538:
2535:
2530:
2521:
2514:
2511:
2508:
2505:
2500:
2496:
2492:
2467:
2450:
2431:
2424:
2417:
2392:
2385:
2378:
2371:
2364:
2343:
2340:
2337:
2333:
2328:
2322:
2319:
2316:
2312:
2306:
2297:
2293:
2290:
2285:
2282:
2279:
2275:
2270:
2265:
2259:
2250:
2246:
2243:
2240:
2236:
2232:
2227:
2222:
2215:
2212:
2182:
2159:
2154:
2147:
2144:
2118:
2114:
2091:
2087:
2075:
2074:
2063:
2054:
2051:
2046:
2043:
2036:
2029:
2024:
2017:
2014:
2007:
2002:
1991:
1987:
1980:
1977:
1969:
1963:
1959:
1955:
1952:
1948:
1944:
1935:
1931:
1926:
1922:
1916:
1913:
1908:
1904:
1894:
1890:
1881:
1876:
1870:
1867:
1862:
1859:
1828:
1825:
1822:
1817:
1810:
1807:
1804:
1799:
1795:
1790:
1785:
1781:
1754:
1750:
1724:
1697:
1685:
1684:
1673:
1664:
1661:
1656:
1653:
1646:
1639:
1634:
1630:
1626:
1621:
1610:
1606:
1599:
1596:
1589:
1585:
1575:
1571:
1562:
1557:
1551:
1548:
1543:
1540:
1517:
1514:
1501:
1494:
1487:
1480:
1472:
1468:electric field
1464:heterojunction
1443:
1440:
1435:
1428:
1422:
1421:
1409:
1405:
1402:
1398:
1392:
1389:
1384:
1381:
1375:
1371:
1368:
1364:
1358:
1354:
1350:
1347:
1317:
1313:
1300:
1299:
1277:
1267:
1255:
1251:
1242:
1233:
1229:
1226:
1223:
1218:
1214:
1210:
1207:
1204:
1196:
1187:
1142:
1139:
1125:
1118:
1111:
1105:
1098:
1091:
1085:
1064:
1057:
1054:
1044:
1040:
1031:
1015:
1006:
999:
990:
967:
964:
951:
948:
946:
943:
940:
939:
936:
933:
930:
927:
924:
921:
918:
915:
909:
908:
905:
902:
899:
896:
893:
890:
887:
884:
878:
877:
874:
871:
868:
865:
862:
859:
856:
853:
847:
846:
843:
840:
837:
834:
831:
828:
825:
822:
816:
815:
812:
809:
806:
803:
800:
797:
794:
791:
785:
784:
777:
770:
765:
760:
755:
750:
745:
730:
723:
718:
713:
684:
669:
654:
636:
600:
585:
560:
557:
491:
488:
456:electron holes
411:
408:
398:absolute value
391:
376:
369:
362:
351:
325:
318:
311:
304:
297:
289:, a potential
282:
275:
268:
257:
247:
236:
211:
185:
174:
135:
132:
130:
127:
68:with multiple
54:Multi-junction
49:
9:
6:
4:
3:
2:
8455:
8444:
8441:
8439:
8436:
8434:
8431:
8430:
8428:
8413:
8412:
8403:
8401:
8400:
8391:
8390:
8387:
8377:
8374:
8372:
8369:
8367:
8364:
8362:
8359:
8357:
8354:
8352:
8349:
8347:
8344:
8342:
8339:
8337:
8334:
8332:
8329:
8327:
8324:
8322:
8319:
8317:
8314:
8313:
8311:
8307:
8301:
8298:
8297:
8295:
8291:
8288:
8286:
8282:
8272:
8269:
8267:
8264:
8262:
8259:
8257:
8254:
8252:
8249:
8247:
8244:
8242:
8239:
8237:
8234:
8232:
8229:
8227:
8224:
8222:
8219:
8217:
8214:
8212:
8209:
8207:
8204:
8202:
8199:
8197:
8194:
8192:
8189:
8187:
8184:
8182:
8179:
8177:
8174:
8172:
8169:
8168:
8166:
8164:
8160:
8154:
8151:
8149:
8146:
8144:
8141:
8139:
8136:
8135:
8133:
8129:
8123:
8120:
8118:
8115:
8114:
8112:
8110:
8106:
8103:
8101:
8095:
8085:
8082:
8080:
8077:
8075:
8072:
8070:
8067:
8065:
8062:
8060:
8057:
8055:
8052:
8050:
8047:
8045:
8042:
8040:
8037:
8035:
8032:
8030:
8027:
8025:
8022:
8021:
8019:
8015:
8009:
8006:
8005:
8003:
7999:
7993:
7990:
7988:
7985:
7983:
7980:
7978:
7975:
7973:
7970:
7968:
7965:
7963:
7960:
7959:
7957:
7955:Air transport
7953:
7947:
7944:
7942:
7939:
7937:
7934:
7932:
7931:Solar roadway
7929:
7927:
7924:
7922:
7921:Solar vehicle
7919:
7918:
7916:
7912:
7906:
7903:
7901:
7898:
7896:
7893:
7891:
7888:
7886:
7883:
7880:
7878:
7875:
7873:
7870:
7868:
7865:
7863:
7860:
7858:
7855:
7853:
7850:
7848:
7845:
7842:
7840:
7837:
7835:
7834:Solar charger
7832:
7830:
7827:
7825:
7822:
7820:
7817:
7816:
7814:
7810:
7807:
7803:
7793:
7790:
7788:
7785:
7783:
7780:
7778:
7775:
7773:
7770:
7768:
7765:
7763:
7760:
7758:
7755:
7754:
7752:
7748:
7742:
7739:
7737:
7734:
7732:
7729:
7727:
7726:Solar tracker
7724:
7722:
7719:
7717:
7714:
7712:
7709:
7707:
7704:
7702:
7699:
7697:
7694:
7692:
7689:
7687:
7684:
7683:
7681:
7677:
7671:
7668:
7666:
7663:
7661:
7658:
7656:
7653:
7651:
7648:
7646:
7643:
7641:
7638:
7636:
7633:
7631:
7628:
7626:
7623:
7621:
7618:
7616:
7613:
7612:
7610:
7608:
7604:
7601:
7599:
7593:
7583:
7580:
7578:
7575:
7574:
7572:
7568:
7562:
7559:
7557:
7554:
7552:
7549:
7547:
7544:
7542:
7539:
7537:
7534:
7532:
7529:
7528:
7526:
7522:
7516:
7513:
7511:
7508:
7506:
7503:
7501:
7498:
7496:
7493:
7491:
7488:
7486:
7483:
7481:
7478:
7476:
7473:
7469:
7466:
7465:
7464:
7461:
7459:
7456:
7454:
7451:
7449:
7446:
7444:
7443:Photovoltaics
7441:
7440:
7438:
7434:
7431:
7427:
7423:
7422:Photovoltaics
7416:
7411:
7409:
7404:
7402:
7397:
7396:
7393:
7386:
7385:
7382:reprinted in
7377:
7365:
7358:
7356:
7343:
7339:
7338:
7332:
7328:
7322:
7318:
7314:
7313:
7307:
7306:
7295:
7290:
7282:
7278:
7274:
7270:
7267:(2): 83–101.
7266:
7262:
7255:
7249:
7245:
7239:
7231:
7227:
7223:
7219:
7212:
7197:
7190:
7183:
7179:
7176:
7171:
7164:
7160:
7154:
7147:
7142:
7135:
7130:
7122:
7120:9784990181604
7116:
7111:
7106:
7099:
7098:
7091:
7089:
7080:
7076:
7072:
7068:
7064:
7060:
7056:
7052:
7047:
7039:
7031:
7027:
7022:
7017:
7013:
7009:
7005:
7001:
6997:
6993:
6989:
6982:
6974:
6970:
6966:
6962:
6958:
6954:
6947:
6945:
6943:
6934:
6930:
6926:
6920:
6916:
6912:
6908:
6907:
6899:
6891:
6887:
6883:
6879:
6875:
6871:
6864:
6856:
6852:
6848:
6844:
6840:
6836:
6832:
6828:
6824:
6817:
6809:
6805:
6801:
6797:
6793:
6789:
6785:
6781:
6774:
6766:
6762:
6758:
6754:
6751:(5): 606–14.
6750:
6746:
6739:
6724:
6718:
6704:
6700:
6694:
6686:
6682:
6678:
6674:
6670:
6666:
6662:
6658:
6651:
6643:
6639:
6635:
6631:
6627:
6623:
6619:
6615:
6608:
6600:
6596:
6592:
6588:
6584:
6580:
6573:
6565:
6561:
6557:
6553:
6549:
6545:
6538:
6530:
6526:
6522:
6518:
6514:
6510:
6506:
6499:
6491:
6487:
6483:
6479:
6475:
6471:
6464:
6456:
6452:
6448:
6444:
6439:
6434:
6430:
6426:
6419:
6417:
6409:
6404:
6402:
6400:
6398:
6396:
6394:
6382:
6375:
6368:
6360:
6353:
6351:
6349:
6340:
6336:
6332:
6328:
6321:
6310:
6306:
6302:
6298:
6294:
6287:
6280:
6272:
6268:
6264:
6257:
6249:
6245:
6241:
6237:
6233:
6229:
6222:
6214:
6210:
6204:
6202:
6200:
6191:
6185:
6181:
6174:
6166:
6160:
6156:
6149:
6138:
6137:
6129:
6127:
6125:
6117:
6112:
6103:
6101:
6093:
6088:
6081:
6077:
6074:
6069:
6062:
6058:
6055:
6050:
6035:
6029:
6021:
6020:CleanTechnica
6017:
6010:
6003:
5998:
5990:
5986:
5982:
5978:
5974:
5970:
5966:
5959:
5944:
5940:
5934:
5926:
5919:
5911:
5907:
5903:
5899:
5895:
5891:
5884:
5868:
5862:
5858:
5848:
5845:
5843:
5840:
5838:
5835:
5833:
5830:
5828:
5825:
5824:
5820:
5819:Energy portal
5814:
5809:
5806:
5800:
5795:
5788:
5786:
5777:
5761:
5759:
5754:
5752:
5751:microclimates
5748:
5743:
5741:
5730:
5728:
5724:
5720:
5716:
5710:
5702:
5696:
5692:
5688:
5684:
5681:
5677:
5668:
5665:
5662:
5659:
5656:
5653:
5650:
5647:
5646:
5643:
5640:
5637:
5634:
5631:
5628:
5626:
5623:
5622:
5619:
5616:
5613:
5610:
5607:
5604:
5602:
5599:
5598:
5595:
5592:
5589:
5586:
5583:
5580:
5578:
5575:
5573:
5569:
5566:
5563:
5560:
5557:
5554:
5551:
5549:
5546:
5545:
5542:
5539:
5536:
5533:
5530:
5527:
5525:
5522:
5519:
5515:
5511:
5508:
5505:
5502:
5496:
5493:
5487:
5484:
5481:
5478:
5475:
5474:
5471:
5469:
5465:
5461:
5451:
5447:
5445:
5441:
5431:
5429:
5428:solar tracker
5419:
5407:
5405:
5401:
5397:
5392:
5388:
5382:
5372:
5370:
5366:
5362:
5358:
5350:
5345:
5341:
5337:
5333:
5329:
5325:
5321:
5311:
5309:
5304:
5302:
5296:
5294:
5288:
5283:
5274:
5269:
5264:
5257:
5253:
5249:
5245:
5230:
5227:
5223:
5214:
5212:
5206:
5204:
5188:
5172:
5163:
5159:
5148:
5138:
5135:(InGaAs) and
5134:
5130:
5126:
5116:
5110:
5086:
5076:
5070:
5059:
5036:
5031:
5030:
5029:
5024:
5017:
5010:
4989:
4985:
4982:
4978:
4971:
4968:
4957:
4953:
4947:
4944:
4940:
4936:
4933:
4930:
4926:
4914:
4910:
4906:
4901:
4897:
4894:
4890:
4886:
4883:
4880:
4871:
4867:
4858:
4849:
4848:
4847:
4830:
4827:
4824:
4815:
4811:
4808:
4796:
4792:
4788:
4784:
4781:
4778:
4775:
4764:
4760:
4754:
4743:
4732:
4722:
4715:
4706:
4697:
4696:
4695:
4690:
4662:
4658:
4654:
4650:
4647:
4644:
4641:
4630:
4626:
4620:
4611:
4602:
4587:
4580:
4577:
4566:
4562:
4556:
4553:
4549:
4545:
4542:
4539:
4536:
4533:
4524:
4520:
4517:
4508:
4504:
4496:
4495:
4494:
4480:
4477:
4470:
4467:
4462:
4459:
4456:
4442:
4435:
4415:
4403:
4399:
4395:
4390:
4386:
4383:
4380:
4377:
4374:
4365:
4361:
4352:
4348:
4340:
4339:
4338:
4336:
4316:
4310:
4307:
4296:
4292:
4289:
4286:
4280:
4276:
4273:
4270:
4267:
4258:
4254:
4251:
4248:
4240:
4239:
4238:
4233:
4222:
4215:
4208:
4198:
4191:
4184:
4180:
4176:
4175:
4174:
4169:
4162:
4140:
4134:
4131:
4120:
4116:
4110:
4106:
4103:
4100:
4097:
4092:
4089:
4085:
4076:
4075:
4074:
4072:
4065:
4058:
4054:
4047:
4022:
4018:
4012:
4008:
4002:
3999:
3994:
3985:
3980:
3976:
3973:
3968:
3964:
3959:
3955:
3952:
3948:
3945:
3939:
3936:
3928:
3912:
3906:
3903:
3892:
3888:
3885:
3882:
3876:
3872:
3869:
3866:
3863:
3854:
3845:
3844:
3843:
3838:
3834:
3829:
3820:
3804:
3799:
3798:
3797:
3778:
3769:
3765:
3761:
3752:
3749:
3746:
3735:
3731:
3725:
3717:
3714:
3711:
3707:
3703:
3694:
3691:
3688:
3677:
3673:
3666:
3660:
3657:
3647:
3643:
3639:
3636:
3631:
3628:
3625:
3621:
3617:
3598:
3594:
3591:
3587:
3583:
3580:
3577:
3574:
3567:
3564:
3561:
3550:
3546:
3527:
3522:
3518:
3510:
3506:
3493:
3484:
3483:
3482:
3471:
3466:
3465:
3464:
3458:
3454:
3450:
3430:
3426:
3423:
3418:
3413:
3402:
3398:
3393:
3387:
3384:
3381:
3370:
3366:
3355:
3354:
3353:
3351:
3347:
3340:
3335:
3333:
3329:
3314:
3310:
3299: ≈
3298:
3294:
3287:
3279:
3275:
3271:
3267:
3260:
3256:
3255:
3254:
3230:
3223:
3220:
3216:
3210:
3201:
3195:
3191:
3188:
3183:
3179:
3176:
3170:
3165:
3156:
3147:
3138:
3134:
3130:
3126:
3123:
3116:
3113:
3106:
3102:
3098:
3092:
3087:
3081:
3078:
3074:
3070:
3065:
3061:
3053:
3052:
3051:
3035:
3026:
2999:
2990:
2984:
2979:
2976:
2973:
2969:
2965:
2956:
2933:
2929:
2923:
2918:
2915:
2912:
2908:
2904:
2901:
2894:
2893:
2892:
2886:
2866:
2862:
2855:
2849:
2846:
2842:
2833:
2829:
2806:
2802:
2795:
2789:
2786:
2782:
2778:
2775:
2772:
2766:
2758:
2754:
2750:
2743:
2742:
2741:
2724:
2718:
2695:
2687:
2683:
2679:
2672:The value of
2656:
2653:
2646:
2638:
2634:
2630:
2624:
2616:
2612:
2608:
2603:
2600:
2595:
2591:
2587:
2582:
2573:
2560:
2552:
2548:
2544:
2536:
2528:
2519:
2512:
2506:
2498:
2494:
2490:
2483:
2482:
2481:
2479:
2475:
2470:
2466:
2462:
2458:
2453:
2449:
2445:
2441:
2437:
2430:
2423:
2416:
2411:
2409:
2405:
2401:
2396:
2391:
2384:
2377:
2370:
2363:
2357:
2341:
2338:
2335:
2331:
2326:
2320:
2317:
2314:
2310:
2304:
2295:
2291:
2288:
2283:
2280:
2277:
2273:
2268:
2263:
2257:
2248:
2244:
2241:
2238:
2234:
2230:
2225:
2220:
2210:
2180:
2157:
2152:
2142:
2116:
2112:
2089:
2085:
2061:
2052:
2049:
2044:
2041:
2027:
2022:
2012:
2005:
2000:
1989:
1978:
1975:
1967:
1961:
1957:
1953:
1950:
1946:
1942:
1933:
1924:
1920:
1914:
1911:
1906:
1902:
1892:
1888:
1879:
1874:
1868:
1865:
1860:
1857:
1850:
1849:
1848:
1846:
1826:
1823:
1820:
1815:
1808:
1805:
1802:
1797:
1793:
1788:
1783:
1779:
1752:
1722:
1695:
1671:
1662:
1659:
1654:
1651:
1637:
1632:
1628:
1624:
1619:
1608:
1597:
1594:
1587:
1583:
1573:
1569:
1560:
1555:
1549:
1546:
1541:
1538:
1531:
1530:
1529:
1527:
1523:
1513:
1507:
1500:
1493:
1486:
1479:
1475:
1469:
1465:
1461:
1453:
1448:
1439:
1434:
1427:
1407:
1403:
1400:
1396:
1390:
1387:
1382:
1379:
1373:
1369:
1366:
1362:
1356:
1352:
1348:
1345:
1338:
1337:
1336:
1333:
1315:
1311:
1275:
1265:
1253:
1249:
1240:
1231:
1224:
1221:
1216:
1212:
1205:
1202:
1194:
1185:
1177:
1176:
1175:
1173:
1169:
1164:
1160:
1152:
1147:
1138:
1136:
1132:
1124:
1117:
1110:
1104:
1097:
1090:
1084:
1062:
1055:
1052:
1042:
1038:
1029:
988:
984:
980:
976:
972:
963:
961:
957:
937:
934:
931:
928:
925:
922:
919:
916:
914:
911:
910:
906:
903:
900:
897:
894:
891:
888:
885:
883:
880:
879:
875:
872:
869:
866:
863:
860:
857:
854:
852:
849:
848:
844:
841:
838:
835:
832:
829:
826:
823:
821:
818:
817:
813:
810:
807:
804:
801:
798:
795:
792:
790:
787:
786:
781:
778:
774:
771:
766:
759:
756:
749:
746:
737:
731:
727:
724:
717:
714:
711:
710:
707:
705:
701:
697:
692:
683:
679:
668:
664:
653:
649:
644:
642:
635:
631:
627:
622:
620:
617:
613:
609:
606:
599:
595:
591:
584:
580:
575:
573:
569:
564:
556:
554:
548:
546:
543:solar cells,
542:
538:
529:
525:
520:
516:
514:
508:
496:
487:
484:
478:
474:
471:
466:
464:
459:
457:
453:
449:
445:
441:
440:absolute zero
437:
432:
430:
421:
416:
407:
404:
399:
390:
383:
375:
368:
361:
357:
350:
346:
342:
338:
334:
329:
324:
317:
310:
303:
296:
292:
288:
281:
274:
267:
263:
256:
253:
246:
242:
235:
231:
227:
223:
219:
215:
210:
206:
202:
198:
195:
184:
180:
173:
169:
165:
161:
157:
153:
149:
145:
140:
126:
124:
120:
115:
113:
109:
105:
101:
97:
92:
90:
85:
83:
79:
75:
71:
70:p–n junctions
67:
63:
59:
55:
46:
39:
38:
33:
29:
19:
8410:
8397:
8376:Yingli Solar
8356:Sungen Solar
8331:Motech Solar
8285:PV companies
8246:South Africa
8064:Solar Splash
7805:Applications
7736:Solar mirror
7596:Photovoltaic
7484:
7383:
7352:
7345:. Retrieved
7336:
7311:
7289:
7264:
7260:
7254:
7243:
7238:
7221:
7218:Desalination
7217:
7211:
7200:. Retrieved
7189:
7170:
7162:
7153:
7141:
7129:
7096:
7054:
7050:
7038:
6995:
6991:
6981:
6959:(1): 78–85.
6956:
6953:Solar Energy
6952:
6905:
6898:
6873:
6869:
6863:
6830:
6826:
6816:
6783:
6779:
6773:
6748:
6744:
6738:
6727:. Retrieved
6717:
6706:. Retrieved
6702:
6693:
6660:
6656:
6650:
6617:
6613:
6607:
6582:
6578:
6572:
6547:
6543:
6537:
6512:
6508:
6498:
6473:
6470:Solar Energy
6469:
6463:
6428:
6424:
6381:the original
6367:
6330:
6326:
6320:
6309:the original
6296:
6292:
6279:
6262:
6256:
6231:
6227:
6221:
6212:
6179:
6173:
6154:
6148:
6135:
6111:
6087:
6068:
6049:
6038:. Retrieved
6028:
6019:
6009:
5997:
5972:
5968:
5958:
5947:. Retrieved
5933:
5924:
5918:
5893:
5890:Solar Energy
5889:
5883:
5871:. Retrieved
5861:
5778:
5762:
5755:
5744:
5736:
5733:Applications
5726:
5722:
5718:
5714:
5711:
5703:
5700:
5675:
5673:
5506:
5494:
5485:
5457:
5448:
5437:
5420:
5408:
5403:
5399:
5384:
5368:
5364:
5360:
5353:
5348:
5343:
5339:
5335:
5331:
5327:
5323:
5319:
5317:
5305:
5300:
5297:
5292:
5289:
5281:
5270:
5262:
5255:
5241:
5220:
5207:
5169:
5160:
5149:
5122:
5095:P through In
5082:
5065:
5044:
5022:
5015:
5008:
5006:
4845:
4688:
4686:
4440:
4433:
4431:
4334:
4332:
4231:
4220:
4213:
4206:
4204:
4196:
4189:
4182:
4178:
4167:
4160:
4157:
4070:
4063:
4062:is given by
4056:
4052:
4045:
4043:
3836:
3835:
3827:
3818:
3812:
3795:
3479:
3462:
3459:× 5.03 × 10
3456:
3452:
3448:
3349:
3345:
3338:
3336:
3331:
3327:
3312:
3308:
3305:10 J⋅Hz
3296:
3292:
3285:
3283:
3277:
3273:
3269:
3265:
3258:
3251:
3017:
2890:
2884:
2831:
2824:
2671:
2477:
2473:
2468:
2464:
2460:
2456:
2451:
2447:
2443:
2439:
2435:
2428:
2421:
2414:
2412:
2407:
2403:
2399:
2394:
2389:
2382:
2375:
2368:
2361:
2358:
2076:
1844:
1686:
1525:
1521:
1519:
1505:
1498:
1491:
1484:
1477:
1470:
1459:
1457:
1452:band diagram
1432:
1425:
1423:
1301:
1168:photovoltage
1156:
1151:band diagram
1134:
1122:
1115:
1108:
1102:
1095:
1088:
1082:
986:
982:
969:
953:
779:
772:
757:
747:
735:
725:
715:
693:
681:
666:
651:
645:
640:
633:
629:
625:
623:
618:
611:
607:
597:
593:
589:
582:
576:
567:
565:
562:
549:
533:
509:
497:
493:
479:
475:
467:
460:
433:
426:
402:
388:
381:
373:
366:
359:
355:
348:
340:
336:
332:
330:
322:
315:
308:
301:
294:
290:
279:
272:
265:
262:photocurrent
254:
244:
233:
229:
221:
216:
208:
201:p–n junction
191:
182:
179:photocurrent
171:
156:valence band
144:Band diagram
116:
93:
86:
61:
57:
53:
52:
36:
8433:Solar cells
8371:Trina Solar
8316:First Solar
8256:Switzerland
8236:Netherlands
8074:Tour de Sol
7772:Fill factor
7711:Solar cable
7686:Solar panel
7607:Solar cells
7372:|work=
7248:open access
6876:(1): 1–23.
6550:(8): 4494.
6094:, Uni-Solar
6004:. Cnet.com.
5975:: 343–349.
5896:: 139–147.
5771:eV and 1.42
5548:Polysilicon
5479:Technology
5476:Categories
5434:Fabrication
5246:materials.
5177:eV and 0.74
1436:gMiddleCell
1131:ultraviolet
503:eV and 1.70
129:Description
66:solar cells
62:solar cells
45:solar cells
32:Black light
8427:Categories
8293:By country
8163:By country
8098:Generation
8008:Solar boat
7857:Solar Tuki
7843:Solar tree
7829:Solar lamp
7812:Appliances
7436:Technology
7202:2014-08-17
6729:2015-08-04
6708:2014-08-17
6585:(3): 510.
6438:2001.08553
6040:2016-11-15
5949:2023-03-28
5854:References
5847:Micromorph
5785:ionisation
5760:missions.
5758:Mars rover
5697:over time.
5442:, usually
5379:See also:
5308:Perovskite
5131:(GaAs) or
4173:, we have
956:electrodes
616:wavelength
142:Figure A.
89:efficiency
8171:Australia
8148:Solar Ark
8054:Solar Cup
7946:Sunmobile
7926:Solar car
7524:Materials
7374:ignored (
7364:cite book
7163:CNET News
7110:2134/8216
7079:235630649
7071:2398-9629
7012:2375-2548
6933:136718230
6703:Azurspace
6685:250869484
6642:250782402
6455:210860788
5842:PIN diode
5693:graph of
5238:Structure
5137:germanium
5127:(InGaP),
5062:Materials
4937:
4898:
4881:−
4825:−
4546:
4534:−
4387:
4375:−
4293:−
4277:
4268:−
4117:−
4107:
3956:
3949:π
3889:−
3873:
3821:< 0.31
3637:−
3610:∞
3588:∑
3539:∞
3523:∫
3431:λ
3324: m⋅s
3192:
3171:≈
3153:⇒
3135:−
3124:−
2970:∑
2909:∑
2856:λ
2850:α
2847:−
2796:λ
2790:α
2787:−
2779:−
2767:λ
2725:λ
2719:α
2696:λ
2657:λ
2647:λ
2625:λ
2613:ϕ
2601:λ
2592:∫
2570:⇒
2561:λ
2549:ϕ
2537:λ
2507:λ
2214:~
2146:~
2090:−
2016:~
1986:Δ
1954:−
1943:−
1930:Δ
1925:−
1749:Δ
1605:Δ
1588:−
1401:−
1370:
1222:−
1213:ϕ
1206:ϵ
1009:(usually
938:100–1000
767:Hardness
754:(cm/V·s)
712:Material
678:Germanium
676:eV), and
657:= 1.8–1.9
545:Uni-Solar
454:meet the
448:electrons
164:electrons
104:aerospace
8399:Category
8361:Sunpower
8351:Solyndra
8326:JA Solar
8261:Thailand
8181:Bulgaria
7429:Concepts
7178:Archived
7030:32789177
6855:13952749
6808:17965718
6765:93809051
6529:55197753
6076:Archived
6063:, emcore
6057:Archived
5989:47576267
5943:Archived
5873:July 18,
5791:See also
2388:) where
1502:gEmitter
1488:gEmitter
979:pyramids
960:aluminum
637:minority
579:bandgaps
470:infrared
406:|.
226:electron
224:, to an
207:energy,
181:, or by
72:made of
34:test of
8411:Commons
8366:Suntech
8241:Romania
8211:Germany
8176:Belgium
8100:systems
7570:History
7269:Bibcode
7021:7399695
6961:Bibcode
6878:Bibcode
6835:Bibcode
6788:Bibcode
6665:Bibcode
6622:Bibcode
6587:Bibcode
6552:Bibcode
6478:Bibcode
6236:Bibcode
5898:Bibcode
5413:m (as 1
2199:, then
1481:gWindow
1429:gTunnel
1332:voltage
1005:) and L
920:0.5868
889:0.5657
858:0.5653
827:0.5451
814:0.1–60
796:0.5431
776:(μm/K)
769:(Mohs)
744:(1/μm)
704:crystal
287:charges
252:current
218:Photons
205:bandgap
197:silicon
158:to the
152:Photons
8216:Greece
8206:France
8186:Canada
7598:system
7347:10 Dec
7323:
7117:
7077:
7069:
7028:
7018:
7010:
6931:
6921:
6853:
6806:
6763:
6683:
6640:
6527:
6453:
6362:(1997)
6228:Vacuum
6186:
6161:
6082:, NREL
5987:
5781:
5773:
5769:
5765:
5707:
5611:0.029
5587:0.089
5555:0.615
5520:cells
5512:Ref's
5482:η (%)
5423:
5415:
5411:
5278:
5273:Indium
5266:tunnel
5259:tunnel
5252:InGaAs
5248:GaAsSb
5199:
5183:
5179:
5175:
5156:
5152:
5113:
5105:
5056:
5052:
5048:
4228:
4044:where
3823:
3815:
3284:where
2823:where
2446:. Let
2367:= min(
1687:where
1510:
913:InGaAs
799:0.102
783:(m/s)
740:
689:
687:= 0.67
674:
663:InGaAs
659:
505:
501:
423:limit.
394:< 0
384:> 0
326:pscatt
319:nscatt
283:nscatt
276:pscatt
121:using
41:'s
8341:Sharp
8251:Spain
8231:Japan
8226:Italy
8221:India
8196:China
8191:Chile
7101:(PDF)
7075:S2CID
6929:S2CID
6851:S2CID
6761:S2CID
6681:S2CID
6638:S2CID
6525:S2CID
6451:S2CID
6433:arXiv
6384:(PDF)
6377:(PDF)
6312:(PDF)
6289:(PDF)
6140:(PDF)
5985:S2CID
5660:1.81
5654:40.7
5629:19.5
5608:0.86
5605:16.5
5584:0.63
5581:11.1
5558:8.35
5552:20.3
5528:24.7
5509:(μm)
5391:guide
5185:eV.
5145:0.985
5141:0.015
4850:(13)
4698:(12)
4603:(11)
4497:(10)
4337:= 0.
4226:≥ 0.3
4073:= 0.
4069:with
3301:6.626
1512:cm).
1497:>
1483:>
1431:>
1172:diode
1047:AlInP
935:5.66
926:1200
907:1000
898:1000
895:3900
886:0.65
864:8500
824:1.86
820:InGaP
802:1400
793:1.12
764:(μs)
738:= 0.8
729:(nm)
722:(eV)
672:= 1.4
661:eV),
648:InGaP
596:<
483:AM1.5
463:light
345:diode
269:scatt
248:drift
194:doped
186:scatt
175:drift
168:holes
7376:help
7349:2011
7321:ISBN
7115:ISBN
7067:ISSN
7026:PMID
7008:ISSN
6919:ISBN
6804:PMID
6184:ISBN
6159:ISBN
5875:2011
5749:for
5666:140
5663:476
5657:2.6
5625:CIGS
5601:CdTe
5564:200
5561:211
5540:100
5534:0.8
5531:0.5
5503:W/m
5500:(A)
5491:(V)
5276:1.96
5195:0.47
5191:0.53
5115:eV.
5109:GaAs
5101:0.47
5097:0.53
5058:eV.
5021:(or
4341:(9)
4241:(8)
4177:(7)
4077:(6)
3929:(5)
3846:(4)
3485:(3)
3356:(2)
3257:(1)
2834:and
2463:and
2104:and
1897:SC,2
1884:SC,1
1727:SC,2
1714:and
1700:SC,1
1578:SC,2
1565:SC,1
1508:≥ 10
1495:gBSF
1490:and
1190:depl
1129:the
975:NaOH
917:1.2
870:4–5
861:0.9
855:1.4
851:GaAs
842:5.3
833:500
811:2.6
789:c-Si
507:eV.
418:The
386:and
331:The
241:hole
166:and
64:are
37:Dawn
8336:REC
7277:doi
7226:doi
7222:209
7105:hdl
7059:doi
7016:PMC
7000:doi
6969:doi
6911:doi
6886:doi
6843:doi
6796:doi
6753:doi
6673:doi
6630:doi
6595:doi
6560:doi
6517:doi
6486:doi
6443:doi
6335:doi
6301:doi
6267:doi
6244:doi
5977:doi
5906:doi
5894:130
5651:MJ
5590:33
5537:63
5334:),
5326:),
5189:(In
5093:0.5
5089:0.5
5028:).
4274:exp
4200:rad
4104:exp
4067:rad
3953:exp
3870:exp
3859:rad
3840:rad
3831:rad
3326:),
3322:458
3319:792
3317:299
3307:),
2432:SC3
2425:SC2
2418:SC1
2386:SC3
2379:SC2
2372:SC1
1367:exp
1119:min
1099:min
1094:= 4
1011:TiO
995:SiO
923:30
876:50
845:50
341:J-V
333:J-V
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