ライフサイエンスコーパス: solar cell

1 bine promising perovskite material with c-Si solar cell.

2 hen surface plasmon is located in front of a solar cell.

3 dots to improve the performance of a silicon solar cell.

4 rect bandgap of 1.95 eV, suited for a tandem solar cell.

5 ve this including crystalline silicon (c-Si) solar cell.

6 phenomenon in semiconductor devices such as solar cells.

7 earth-abundant sensitizers in dye-sensitized solar cells.

8 or application in low-cost silicon thin film solar cells.

9 n-fullerene candidates for "all-polymer" BHJ solar cells.

10 e hole-transporting materials for perovskite solar cells.

11 substrates integrated with amorphous silicon solar cells.

12 fect transistors, light-emitting diodes, and solar cells.

13 design and optimization of stable perovskite solar cells.

14 junction ZnO nanowire/a-Si:H p-i-n thin-film solar cells.

15 eisser limit of conventional single-junction solar cells.

16 iencies approaching 20% in planar perovskite solar cells.

17 -effective approach for the manufacturing of solar cells.

18 d backward scattering in plasmonic thin film solar cells.

19 voltage in several types of high efficiency solar cells.

20 of the bottom cell of all-perovskite tandem solar cells.

21 ove the power conversion efficiency (PCE) of solar cells.

22 ganic, photovoltaics (OPV)/perovskite hybrid solar cells.

23 potential for applications in tandem organic solar cells.

24 y offer lead-free alternatives in perovskite solar cells.

25 s an efficient BHJ for OPV/perovskite hybrid solar cells.

26 served in metal-oxide-based inverted polymer solar cells.

27 mong the best for solution-processed organic solar cells.

28 and diffusion lengths observed in perovskite solar cells.

29 xploring the ultimate performance of organic solar cells.

30 t photovoltaics to compete with conventional solar cells.

31 , including bioimaging and in dye-sensitized solar cells.

32 been used to produce Cu(In,Ga)(S,Se)2 (CIGS) solar cells.

33 ncy, stability, or scalability of perovskite solar cells.

34 anar silicon heterojunction and homojunction solar cells.

35 to probe the charging effects in perovskite solar cells.

36 rent-voltage hysteresis in hybrid perovskite solar cells.

37 egies to obtain record-efficiency perovskite solar cells.

38 ing materials for vacuum processable organic solar cells.

39 proach in characterization of dye sensitized solar cells.

40 uch efficient IMLs for more efficient tandem solar cells.

41 in inverted planar heterojunction perovskite solar cells.

42 ving the performance of perovskite thin-film solar cells.

43 ned and synthesized for efficient perovskite solar cells.

44 er conversion efficiencies for both LEDs and solar cells.

45 is used to make semi-transparent perovskite solar cells.

46 pon photovoltaic performance of MAPbI3 based solar cells.

47 the corresponding polycrystalline thin-film solar cells.

48 e for a new generation of easily processable solar cells.

49 nificantly affects the efficiency of organic solar cells.

50 w-cost high-performance tin-based perovskite solar cells.

51 graphene nanoribbons and their properties in solar cells.

52 iency of 17.8% for single crystal perovskite solar cells.

53 ith aspect-ratios up to 8, on the surface of solar cells.

54 tor devices, such as transistors, diodes and solar cells.

55 is an electron transport material in organic solar cells.

56 -free HTL for lead-free tin-based perovskite solar cells.

57 ise for boosting the PCE of third generation solar cells.

58 avenue in low cost fabrication of thin-film solar-cells.

59 ons in the movie provide insight into future solar cells, 2D materials and other semiconductor device

60 ovskite films into the planar heterojunction solar cells, a power conversion efficiency of 20.15% is

61 as less toxic analogs of the lead perovskite solar-cell absorbers APbX3 (A = monovalent cation; X = B

62 ymer acceptors" in bulk-heterojunction (BHJ) solar cells achieve >7 % efficiency when used in conjunc

63 sulting alpha-bis-PCBM-containing perovskite solar cells achieve better stability, efficiency, and re

64 r, Ta-WO x -doped interface-based perovskite solar cells achieve maximum efficiencies of 21.2% and of

65 All-polymer solar cells (all-PSCs) offer unique morphology stability

66 units is designed and applied in all-polymer solar cells (all-PSCs).

67 s, here we report a ribbon that integrates a solar cell and a supercapacitor.

68 opto-electronic applications from displays, solar cells and bio-medical imaging to single-electron d

69 based on the performance of organic bilayer solar cells and careful modeling.

70 uilding on regenerative photoelectrochemical solar cells and emerging electrochemical redox flow batt

71 acement of precious metals in dye-sensitized solar cells and in luminescent devices by earth-abundant

72 dyes for charge injection into semiconductor solar cells and in sensitizer-catalyst assemblies for ph

73 Despite their importance in solar cells and infrared (IR) light-emitting diodes and

74 lend them to application in high-efficiency solar cells and light-emission devices.

75 optoelectronic semiconductor devices such as solar cells and light-emitting diodes.

76 eloping highly efficient ferroelectric-based solar cells and novel optoelectronic memory devices.

77 perovskites are promising semiconductors for solar cells and optoelectronic applications.

78 stability problem for their applications in solar cells and other optoelectronics.

79 aics and related devices, such as perovskite solar cells and photocatalytic devices, it is important

80 es over laborious layer-by-layer methods for solar cells and photodetectors, while opening the door t

81 ient solar energy harvesting in both organic solar cells and photosynthetic systems.

82 s for much improved optical control in LEDs, solar cells, and also toward applications as optical dev

83 r solar cells, organometal halide perovskite solar cells, and finally some photocatalytic systems.

84 eneration environmentally friendly germanium solar cells, and near-to-mid infrared (1.8-2.0 mum) lase

85 ations in art, architecture, semitransparent solar cells, and security features in anticounterfeiting

86 nor:acceptor blends that are used in organic solar cells, and which are generally comprised of a comp

87 of attention CH3NH3PbI3 has received for its solar cell application, intrinsic properties of this mat

88 the potential of the ACI perovskites toward solar cell applications, we studied the (C(NH2)3)(CH3NH3

89 C-H/C-H green catalysis with dye-sensitized solar cell applications.

90 ed as possible lower toxicity alternates for solar cell applications.

91 tronic (light-emitting devices, transistors, solar cells) applications, we end with an assessment of

92 ability to perform various enabling roles in solar cell architectures, leading to overall improvement

93 approach and its compatibility with current solar cell architectures.

94 ance in both regular and inverted structured solar cell architectures.

95 and mechanically stacked tandems on silicon solar cells are 18.0% efficient.

96 Furthermore, PffBT4T-2OD:EH-IDTBR solar cells are found to be substantially more stable un

97 igher stability, but the efficiencies of the solar cells are limited by the confinement of excitons.

98 Efficient wide-bandgap (WBG) perovskite solar cells are needed to boost the efficiency of silico

99 While the basic principles of conventional solar cells are well understood, little attention has go

100 ng devices were determined by completing the solar cells as follows: Mo/CZTSSe/CdS/i-ZnO/Al:ZnO/Ni/Al

101 rly double those of previously reported BiOI solar cells, as well as other bismuth halide and chalcoh

102 The best-performing FASnI3 PHJ solar cell assembled by this protocol exhibits a power c

103 addition, a flexible FASnI3 -based flexible solar cell assembled on a polyethylene naphthalate-indiu

104 ds material design and processing of organic solar cells, assisting to realize their purported promis

105 oor and outdoor stability testing of organic solar cells based on a blend between a donor-acceptor po

106 cost-effective manufacturing process for Si solar cells based on electrodeposition.

107 g the further commercialization of thin-film solar cells based on hybrid organohalide lead perovskite

108 Solar cells based on hybrid perovskites have shown high

109 buffer layers at the front and rear side of solar cells based on selenium; Todorov et al., reduce in

110 Solar cells based on this new perovskite show power conv

111 Solar-cells based on Schottky junctions between metals a

112 A bendable integrated solar cell-battery system charged by light with stable o

113 n with regards to the functioning of polymer solar cells because these species are long-lived and que

114 d as attractive alternatives to conventional solar cell building blocks.

115 aining optimal morphologies not only for BHJ solar cells but also for any other solution-processed so

116 t as promising materials for next-generation solar cells, but serious issues related to long-term sta

117 s finding provides a novel concept to design solar cell by sacrificing part of sunlight to provide "e

118 otential to overcome thermodynamic limits in solar cells by converting the energy of a single absorbe

119 opic TiO2 layer in a metal halide perovskite solar cell can influence the overall power conversion ef

120 The crucial separation of photocarriers in solar cells can be efficiently driven by contacting semi

121 essible solar energy; however, the output of solar cells can be non-continuous and unstable.

122 a solid standing point, on which perovskite solar cells can be understood more accurately and their

123 s quite limited because very few such hybrid solar cells can simultaneously show high short-circuit c

124 e time for carrier extraction in hot carrier solar cells.Carrier-carrier scattering rates determine t

125 In conventional semiconductor solar cells, carriers are extracted at the band edges an

126 ne major limitation of VOC in WBG perovskite solar cells comes from the nonmatched energy levels of c

127 In a tandem solar cell comprising a NIR BODIPY subcell and a matchin

128 Silicon solar cells comprising this encapsulation architecture s

129 The a-Si:H solar cells constructed on such nanopatterned substrates

130 hes for development of inexpensive, nontoxic solar cell contacting pastes.

131 of cost effectiveness, if failed, perovskite solar cells could be collected and recycled; reuse of th

132 d perovskite-based single bandgap and tandem solar cell designs have yielded impressive performances.

133 tizers are readily prepared and submitted to solar cell device fabrications, giving the power convers

134 llenges associated with long-term perovskite solar cell device stability include the role of testing

135 8.1% is achieved for the flexible perovskite solar-cell devices made on an indium tin oxide/poly(ethy

136 re applied as photoanode in a dye-sensitized solar cell (DSC).

137 for NIR photon absorption in dye-sensitized solar cells (DSCs) when used as a pi-bridge.

138 ayer candidates for lightweight and flexible solar cells due to their low-temperature process capabil

139 on (TTA-UC) and increase maximum theoretical solar cell efficiencies from 33% to >43%.

140 The Shockley-Queisser limit for solar cell efficiency can be overcome if hot carriers ca

141 ling effect is significant enough to improve solar cell efficiency.

142 trically functional components (transistors, solar cells, emitters, etc.) that can enable a diversity

143 ency, stability, and photophysics of organic solar cells employing poly[(5,6-difluoro-2,1,3-benzothia

144 The fabrication of a new type of solar cell encapsulation architecture comprising a perio

145 , polymeric antioxidants and nanocrystalline solar cells, etc.

146 tches the SiNx antireflective-coating on the solar cell, exposing the Si surface.

147 However, to date, no solar cell fabricated on graphene electrodes has out-per

148 Inverted PffBT4T-2OD:EH-IDTBR blend solar cell fabricated without any processing additive ac

149 al quantum efficiency spectra of the polymer solar cells fabricated with either [60]PCBM or [70]PCBM

150 s via a simple process, and pave the way for solar cell fabrication via scalable methods in the near

151 of 21.6% is achieved for crystalline silicon solar cells featuring a full-area TiO2 -based electron-s

152 n be efficiently harvested by the perovskite solar cells for electric power generation.

153 Solar cell generates electrical energy from light one vi

154 ve electrolyte species in the dye-sensitized solar cell has a significant impact on the rate of regen

155 The best-performing {en}MASnI3 solar cell has achieved a high efficiency of 6.63% with

156 e that the choice of redox mediator in these solar cells has a profound influence on both the light h

157 The meteoric rise of the field of perovskite solar cells has been fueled by the ease with which a wid

158 Most research on perovskite solar cells has focused on improving power-conversion ef

159 he power conversion efficiency of perovskite solar cells has improved rapidly, a rational path for fu

160 interfacial electron transfer in sensitized solar cells has mostly been probed by visible-to-teraher

161 ncy of polymer:fullerene bulk heterojunction solar cells has recently surpassed 11%, as a result of s

162 The efficiency of perovskite solar cells has surged in the past few years, while the

163 Organic-inorganic perovskite solar cells have attracted tremendous attention because

164 compelling device efficiencies of perovskite solar cells have been achieved, investigative efforts ha

165 Amorphous silicon (a-Si:H) solar cells have been constructed on nanoholes array tex

166 Silicon solar cells have captured a large portion of the total m

167 Solution-processed organometallic perovskite solar cells have emerged as one of the most promising th

168 The efficiencies of perovskite solar cells have gone from single digits to a certified

169 ic-inorganic hybrid perovskite multijunction solar cells have immense potential to realize power conv

170 Solar cells hold promise as energy conversion devices du

171 e Shockley-Queisser limit of single-junction solar cells; however, they are limited by large nonideal

172 ersion efficiency (PCE) of the 3-dimensional solar cells improved by up to 60% compared to using AZO

173 Selenium was used in the first solid state solar cell in 1883 and gave early insights into the phot

174 within a ultrathin microcrystalline silicon solar cell, in enhancing broadband light trapping capabi

175 y photons are absorbed at the surface of the solar cell, in the heavily doped region, and the photo-g

176 create stratified bulk heterojunction (BHJ) solar cells, in which the two BHJ layers are spin cast s

177 Inverted polymer solar cells incorporating the post-treated TiO2 :TOPD el

178 o enhance the efficiency of perovskite-based solar cells, instead of using tandem devices or near inf

179 nally, a four-terminal all-perovskite tandem solar cell is demonstrated by combining this low-bandgap

180 High performance of organic tandem solar cell is largely dependent on transparent and condu

181 conversion efficiency of ITIC2-based organic solar cells is 11.0%, much higher than that of ITIC1-bas

182 The efficiency of dye sensitized solar cells is a function of the interaction of a dye wi

183 methylammonium lead triiodide single crystal solar cells is extended to 820 nm, 20 nm broader than th

184 e layer of bulk heterojunction (BHJ) organic solar cells is paramount to achieve high-efficiency devi

185 light absorption enhancement in thin film Si solar cells is performed.

186 ever, the efficiency of tin-based perovskite solar cells is still low and they exhibit poor air stabi

187 Furthermore, a "field-effect solar cell" is successfully developed and implemented by

188 All-inorganic solar cells (ITO|NiOx |BiOI|ZnO|Al) with negligible hyst

189 y of a variety of electronic devices such as solar cells, LEDs, sensors, and possible future bioelect

190 numerous optoelectronic applications such as solar cells, light-emitting diodes, and displays.

191 version by showing remarkable performance of solar cells made with HaPs, especially tetragonal methyl

192 of a photogenerated electron-hole pair in a solar cell material, charges of opposite sign have to be

193 NCs) have emerged as promising phosphors and solar cell materials due to their remarkable optoelectro

194 GaAs based optoelectronic devices (e.g. solar cells, modulators, detectors, and diodes) used in

195 ted Lewis base is introduced into perovskite solar cells, namely, indacenodithiophene end-capped with

196 in the fabrication of natural dye sensitized solar cells (NDSSC).

197 with j sc, V oc, FF and eta of the optimized solar cell of 29.30 mA cm(-2), 0.564 V, 65.59% and 10.83

198 rials as functional components of perovskite solar cells offers the expanded flexibility for engineer

199 on process, known to provide high efficiency solar cells, on semitransparent indium tin oxide (ITO) a

200 ideal bandgap of 1.3 eV for single-junction solar cell operation is achieved in the rationally-tailo

201 applications in white light emitting diodes, solar cells, optical codes, biomedicine and so on.

202 Organic solar cell optimization requires careful balancing of cu

203 ), organic field-effect transistors (OFETs), solar cells or other light harvesting devices.

204 structure-activity relationships in optical (solar cells) or (photo)catalytic performance and their r

205 tized solar cells, polymer-fullerene polymer solar cells, organometal halide perovskite solar cells,

206 eveloped so far for high-performance organic solar cells (OSCs) are designed in planar molecular geom

207 Furthermore, nonfullerene organic solar cells (OSCs) based on fluorinated ITIC-Th1 electro

208 d-ring electron acceptor (IOIC2) for organic solar cells (OSCs).

209 iciency among all parallel connected organic solar cells (OSCs).

210 ) is known as a challenging issue in organic solar cells (OSCs).

211 olymer are used to fabricate ternary organic solar cells (OSCs).

212 evolution of the dye adsorption capacity and solar cells parameters are explored as a function of the

213 temperature may be a key to achieve superior solar cell performance.

214 ted approximately 50% enhancement in maximum solar cell performance.

215 of the absorber and it clearly improved the solar cell performance.

216 ignificant interest for applications such as solar cells, photodectors, light-emitting diodes, and la

217 h-performance organic light-emitting diodes, solar cells, photodiodes and transistors, including ohmi

218 In organic solar cells, photoexcitation of the donor or acceptor ph

219 pplications in dye or quantum dot-sensitized solar cells, polymer-fullerene polymer solar cells, orga

220 plasmonic color filter-integrated perovskite solar cells provide 10.12%, 8.17% and 7.72% of power con

221 In this work, a nonfullerene polymer solar cell (PSC) based on a wide bandgap polymer donor P

222 al reflectance, to better understand polymer solar cell (PSC) optimization approaches.

223 mesoporous standard architecture perovskite solar cell (PSC).

224 Mixed ion perovskite solar cells (PSC) are manufactured with a metal-free hol

225 pment of hybrid organic-inorganic perovskite solar cells (PSC) astonished the community.

226 Perovskite solar cells (PSCs) exceeding a power conversion efficien

227 Perovskite solar cells (PSCs) have developed rapidly over the past

228 hole-transporting layer (HTL) in perovskite solar cells (PSCs) provides higher carrier mobility, bet

229 In order to develop high performance polymer solar cells (PSCs), full exploitation of the sun-irradia

230 Since the establishment of perovskite solar cells (PSCs), there has been an intense search for

231 terials (ETMs) in inverted planar perovskite solar cells (PSCs).

232 ular acceptor (SMA) for nonfullerene polymer solar cells (PSCs).

233 Conventional perovskite solar cells (PSCs); however, suffer the issue that lead

234 er improve PCE of single junction perovskite solar cells (PVSCs) because of a better balance between

235 rated in organic-inorganic hybrid perovskite solar cells (PVSCs), critical concerns pertaining to the

236 for efficient conventional n-i-p perovskite solar cells (PVSCs).

237 e efficient, low-cost, and stable perovskite solar cells (PVSCs).

238 Impressive performance of hybrid perovskite solar cells reported in recent years still awaits a comp

239 in both conventional and inverted perovskite solar cells, respectively.

240 The solar cell's photovoltic performance in terms of efficie

241 those in polymers, life sciences, photonics, solar cells, semiconductors, pharmaceuticals, and cultur

242 hin-film-transistors, light-emitting diodes, solar cells, sensors, photorefractive devices, and many

243 TOA-perovskite-based n-i-p planar solar cells show minimal discrepancies between stabilize

244 Fullerene-free organic solar cells show over 11% power conversion efficiency, p

245 ably, while encapsulated PffBT4T-2OD:PC71 BM solar cells show significant efficiency loss under simul

246 tant monolithic perovskite-perovskite tandem solar cell shows a high V oc of 1.98 V (approaching 80%

247 otoinduced trap states, PffBT4T-2OD:EH-IDTBR solar cell shows negligible burn in efficiency loss.

248 oundaries in a high-efficiency Cu(In, Ga)Se2 solar cell shows the matrix and alkali concentrations ar

249 highest efficiencies reported for perovskite solar cells so far have been obtained mainly with methyl

250 Rigorously differing solar cell structures as well as independent photolumine

251 tum efficiency data of the world-record CdTe solar cell suggests that the device uses bandgap enginee

252 They reveal that CdCl2 treatment of CdTe solar cells suppresses nonradiative recombination and en

253 serious low-cost competitor to silicon based solar cell technologies.

254 Herein, dye-synthesized solar cell technology is combined with lithium-ion mater

255 areas such as artificial photosynthesis and solar cell technology.

256 omising applications is semitransparent (ST) solar cells that can be utilized in value-added applicat

257 Highly efficient colored perovskite solar cells that exploit localized surface plasmon reson

258 Using this strategy, we demonstrate solar cells that harvest light in the infrared up to 104

259 monstrated only in the application of a-Si:H solar cells, the ideas are able to extend to application

260 In solar cells, the mismatch between the Sun's emission spe

261 When integrated into polymer solar cells, the polymers show a promising power convers

262 ady led to improvements in the efficiency of solar cells, the processability of transistors and the s

263 To guide the design of plasmonic solar cells, theoretical investigation of core (metal)-s

264 In lead halide perovskite solar cells, there is at least one recycling event of el

265 ens asymmetry in organic-c-Si heterojunction solar cell through molecule alignment process.

266 -dimethoxythiophene) thin films into organic solar cells through a vacuum-based polymer vapor printin

267 re needed to boost the efficiency of silicon solar cells to beyond Schottky-Queisser limit, but they

268 among other similar-structured CH3 NH3 PbBr3 solar cells to date.

269 s set will enable "all-perovskite" thin-film solar cells to reach the highest efficiencies in the lon

270 ropelled by modern applications in thin-film solar cells, transistors and optical sensors.

271 Indoor lifetime testing was performed on solar cells using a solar simulator under a constant irr

272 e we demonstrate highly efficient and stable solar cells using a ternary approach, wherein two non-fu

273 a highly efficient parallel connected tandem solar cell utilizing a nonfullerene acceptor is demonstr

274 t on fabricating highly efficient perovskite solar cells via a simple process, and pave the way for s

275 Organic solar cells were fabricated and showed power conversion

276 ng the charge transport layers in perovskite solar cells when the perovskites have a different compos

277 ngs have relevance in the context of polymer solar cells, where C60 bisadducts have found use as elec

278 ht generation, water-splitting, or thin-film solar cells, where increased response in areas of weak a

279 ith one InGaP/GaAs/GaInNAsSb triple-junction solar cell, which produces a large-enough voltage to dri

280 n state-of-the-art silicon-perovskite tandem solar cells, which highlights the prospects of using per

281 lecular-orbital is needed for WBG perovskite solar cells, while its energy-disorder needs to be minim

282 olution-processable absorber for a thin-film solar cell with a power-conversion efficiency over 20%.

283 With the objective to conceive a plasmonic solar cell with enhanced photocurrent, we investigate th

284 A planar perovskite solar cell with grain boundary and interface passivation

285 We used a lateral-contact solar cell with selective electron- and hole-collecting

286 PCE10), the two mixed acceptors also lead to solar cells with 11.0 +/- 0.4% efficiency and a high ope

287 styrenesulfonate) (PEDOT:PSS) heterojunction solar cells with 16.2% efficiency and excellent stabilit

288 ading to high-performance thick-film polymer solar cells with a V(OC) of 0.88 V and a power conversio

289 ed energetic carriers may enable hot-carrier solar cells with efficiencies exceeding the Shockley-Que

290 mance is also achieved for cesium tin iodide solar cells with en loading, demonstrating the broad sco

291 Here, we report lead-free tin-based solar cells with greatly enhanced performance and stabil

292 WBG perovskite solar cells with ICBA-tran3 show enhanced VOC by 60 mV,

293 nd two-terminal perovskite-perovskite tandem solar cells with ideally matched band gaps.

294 Perovskite solar cells with IDIC layers yield higher photovoltages

295 trategy to improve the efficiency of Silicon solar cells with mass-compatible techniques that could s

296 d rapidly over the last 2 decades, and small solar cells with power conversion efficiencies of 13% ha

297 s and fabricate perovskite-perovskite tandem solar cells with small V oc,loss .

298 dy, we demonstrate graded bandgap perovskite solar cells with steady-state conversion efficiencies av

299 During the 140 h experiment, the solar cells with the Au electrode experience a dramatic,

300 Solar cells with the composite nanowire top contacts att