ライフサイエンスコーパス: solar cell

1 f the dye to the overall photocurrent of the solar cell.

2 ive layers of the p-n junction in a complete solar cell.

3 est power conversion efficiency is 3.1% as a solar cell.

4 ntensity that reaches the active part of the solar cell.

5 e high-performance bulk heterojunction (BHJ) solar cells.

6 unter-intuitive anti-reflective coatings for solar cells.

7 iciency of metal halide perovskite thin film solar cells.

8 rformance and device stability of perovskite solar cells.

9 mately affect the overall performance of PQD solar cells.

10 which is one of the highest among all Pe-QD solar cells.

11 igh power conversion efficiencies in organic solar cells.

12 otential non-fullerene acceptors for organic solar cells.

13 s methods to engineer stable CsPbI(3) -based solar cells.

14 e to the design of efficient singlet fission solar cells.

15 idates as non-fullerene acceptors in organic solar cells.

16 al for the successful application of organic solar cells.

17 tion of MHPs and hole mobility in perovskite solar cells.

18 (3))(0.85)(MAPbBr(3))(0.15) perovskite-based solar cells.

19 ce performance, to compete with conventional solar cells.

20 tingly, 8.25% is a new record for P3HT-based solar cells.

21 ng and imaging to performance improvement of solar cells.

22 na can support the performance of perovskite solar cells.

23 new energy materials such as perovskites for solar cells.

24 gh efficient and stable inorganic perovskite solar cells.

25 rd achieving high-performance perovskite CQD solar cells.

26 e efficiency of perovskite-perovskite tandem solar cells.

27 a strong practical impact in next-generation solar cells.

28 he potential of perovskite-perovskite tandem solar cells.

29 rystalline and single-crystalline perovskite solar cells.

30 ls were embedded, limiting the efficiency of solar cells.

31 ed as the active layer in ultrathin flexible solar cells.

32 make these systems very promising for use in solar cells.

33 rication of high-quality films and efficient solar cells.

34 rds efficient long-term stable materials and solar cells.

35 ilm transistors, light-emitting devices, and solar cells.

36 ht into the interfacial effects in nanoscale solar cells.

37 ells is now comparable to that of commercial solar cells.

38 the nonradiative recombination in perovskite solar cells.

39 cation in the stable operation of perovskite solar cells.

40 iency of 25.7% for perovskite-silicon tandem solar cells.

41 skite-based polycrystalline thin-film tandem solar cells.

42 rganic field-effect transistors, and organic solar cells.

43 ency approaching 15% for CsPbI(3) -PQD-based solar cells.

44 dustry-relevant textured crystalline silicon solar cells.

45 skite single-crystalline and polycrystalline solar cells.

46 lue of 1.46 eV, suitable for single junction solar cells.

47 ternary, flexible, and OSC/perovskite hybrid solar cells.

48 energy-density batteries and high-efficiency solar cells.

49 the long-debated ideality factor in organic solar cells.

50 the performance and stability of perovskite solar cells.

51 ty and voltage issues inherent in perovskite solar cells.

52 ich is promising for incorporation of GeH in solar cells.

53 issue that leads to a loss of efficiency in solar cells.

54 extraction layers in metal-halide perovskite solar cells.

55 widespread attention in optoelectronics and solar cells.

56 ion and improve the performance of CuInSe(2) solar cells.

57 vskites have a bandgap well suited to tandem solar cells(1) but suffer from an undesired phase transi

58 Searching for Pb-free perovskite solar cell absorbers is currently an attractive research

59 And the all-polymer solar cell (all-PSC) based on PBDB-T:PTPBT-ET(0.3) achie

60 All-polymer solar cells (all-PSCs) exhibit excellent stability and r

61 ucial role in the performance of all-polymer solar cells (all-PSCs).

62 e-of-the-art CdS in Cu(In,Ga)Se(2) thin-film solar cells, alternatives rarely exceed reference device

63 mes, in addition to photovoltaic devices and solar cells, among a vast multitude of other usages.

64 The proof-of-concept solar cell and light-emitting diode devices based on the

65 aging and sensing systems, in dye-sensitized solar cells and as photocatalysts are presented.

66 lopments in almost all aspects of perovskite solar cells and discoveries of some fascinating properti

67 gy conversion devices such as dye-sensitized solar cells and dye-sensitized photoelectrosynthesis cel

68 f over 10% have been achieved for perovskite solar cells and LEDs, respectively.

69 generation of high-performance materials for solar cells and light emitting diodes.

70 in optoelectronic applications, particularly solar cells and light-emitting devices (LEDs), and for t

71 for various optoelectronic devices including solar cells and light-emitting diodes for improved stabi

72 strate immense potential for next-generation solar cells and other optoelectronic devices.

73 of perovskites for more efficient and stable solar cells and other optoelectronic devices.

74 sign of clean energy technologies, including solar cells and photocatalytic water splitting.

75 arious optoelectronic applications including solar cells and photodetectors.

76 uences for our current understanding of both solar cells and photodiodes - in the latter case definin

77 sion to increase the efficiencies of silicon solar cells and reduce the cost of the energy that they

78 mal annealing effects in high-efficiency NFA solar cells and tasks for future materials design.

79 parameters are significantly enhanced in the solar cells and the devices also show excellent stabilit

80 erformance of single-junction narrow-bandgap solar cells and, potentially, to give a highly efficient

81 ite, including super capacitors, biosensors, solar cells, and corrosion protection studies.

82 cations such as supercapacitors, biosensors, solar cells, and corrosion studies.

83 efore, it can be used in catalysis, sensors, solar cells, and p-type semiconductors.

84 suitable for applications in photovoltaics, solar cells, and photo-catalysis.

85 nter with perovskite materials for the first solar cell application, which should inspire young resea

86 in perovskite films for the state-of-the-art solar cell applications.

87 As monofacial, single-junction solar cells approach their fundamental limits, there has

88 Up to now, no solar cell architecture has exhibited above-Lambertian s

89 efficiency in thin film crystalline silicon solar cell architectures relies essentially on solar abs

90 onstrate two types of photonic crystal (PhC) solar cells architectures that exceed Lambertian light a

91 stability of the hot-cast layered perovskite solar cells are also discussed to provide guidelines for

92 ters for active layers in silicon (Si) wafer solar cells are determined from free carrier optical abs

93 These solar cells are generally based on multication mixed-hal

94 developing successful ternary or quaternary solar cells are likely very different for D18 than for o

95 ists for lithography or perovskite films for solar cells, are either amorphous or polycrystalline.

96 , and printable supercapacitors and embedded solar cells as energy sources, is successfully demonstra

97 ic properties and environmental stability of solar cells as the solution-processing of perovskite fil

98 eal candidates for light absorbers in tandem solar cells as well as fluorescent materials in light-em

99 Perovskite solar cells, as an emerging high-efficiency and low-cost

100 The processing window of perovskite solar cells, as defined by the latest time the anti-solv

101 Integrating solar cell at the window edge, we find an electrical con

102 splaying the state-of-the-art binary organic solar cells at present.

103 cate high efficiency and low-cost perovskite solar cells at speed.

104 fetimes to improve performance attributes of solar cells based on conjugated organic materials presen

105 tors but also good performance (for example, solar cells based on lead-tin-gradient structures with a

106 hich has resulted in the highest performance solar cells based on mixtures of Cs, methylammonium, and

107 Organic solar cells based on non-fullerene acceptors can show hi

108 Solar cells based on organo-metal halide perovskites hav

109 while it is found challenging in perovskite solar cells because of the difficulty in doping perovski

110 d to impact next generation high performance solar cells because of their extraordinary charge transp

111 ide perovskites are especially attractive in solar cells because of their superior charge transport p

112 racts the interest to design high-efficiency solar cells beyond the pn junction paradigm.

113 time the anti-solvent drip yields efficient solar cells, broadened with the increasing complexity of

114 emerged as a promising material not only for solar cells but also for lighting and display applicatio

115 Thermophotovoltaic cells are similar to solar cells, but instead of converting solar radiation t

116 ture of a commercial polycrystalline silicon solar cell by 17 degrees C under one sun condition and e

117 e Pb(2+) leaked from the degraded perovskite solar cells by forming water-insoluble solids.

118 ience positive-intrinsic-negative perovskite solar cells by incorporating a piperidinium-based ionic

119 ide a strategic advantage to singlet fission solar cells by suppressing singlet dissociation at optim

120 ility of hybrid organic-inorganic perovskite solar cells by using different organic agents as additiv

121 that the recent advances of 2D materials for solar cells can be employed for formulating the future r

122 to enhance the performances in electronics, solar cells, catalysis, sensors, and energy conversion a

123 sis in the fields of biosensors, fuel cells, solar cells, catalytic mechanism studies, and bioelectro

124 orted to date for single junction perovskite solar cells, corresponding to a voltage deficit of 0.37

125 and lead contamination issues in perovskite solar cells could greatly improve the feasibility of lar

126 he PCE should be able to rise further if the solar cells could use narrower-band gap absorbers (1.2-1

127 and in delivering insights in, for example, solar cell degradation mechanisms via phase separation,

128 Our findings open new avenues for organic solar cell design where material energetics are tuned th

129 Solar cell device performance parameters including photo

130 Moreover, examination of solar cell devices based on the bismuth-based compound 5

131 y means of an electronic characterization of solar cell devices in combination with ultrafast broadba

132 o a SnO(2)/FTO electrode in a dye-sensitized solar cell (DSSC) architecture.

133 s of the photovoltaic cell, a dye sensitized solar cell (DSSC), and better electrocatalytic features

134 a photovoltaic cell that is a dye sensitized solar cell (DSSC), in which one of the electrodes is the

135 Previously, textile dye sensitised solar cells (DSSCs) woven using photovoltaic (PV) yarns

136 fective counter electrode for dye-sensitized solar cells (DSSCs); where M denotes monoclinic crystal

137 tems for nonlinear optics and dye-sensitized solar cells, DTT polymers in light-emitting diodes, orga

138 property variations in colloidal quantum dot solar cells due to film defects, physical damage, and co

139 much attention for application in perovskite solar cells due to their high carrier mobility and tunab

140 emendous attention in the field of thin-film solar cells due to their wide range of applications, esp

141 ction and recombination processes that limit solar cell efficiencies.

142 Shockley-Queisser limit for single-junction solar cell efficiency through the production of two elec

143 As a result, the solar cell efficiency was increased to 23.25 % from 21.0

144 In metal halide perovskite solar cells, electron transport layers (ETLs) such as Ti

145 This paper presents perovskite solar cells employed with WO(3) nanoparticles embedded c

146 Consequently, solar cells employing mixed 2D DJ 3AMP-based and 3D MA(0

147 ammonium (MA)/formaminidium (FA)) perovskite solar cells from ~19.2% (reference) to 20.8% (using 1 vo

148 Optimized n = 4 RPP solar cells had PCEs of 13% with significant potential f

149 State-of-the-art halide perovskite solar cells have bandgaps larger than 1.45 eV, which res

150 However, wide-band gap perovskite solar cells have been fundamentally limited by photoindu

151 Perovskite solar cells have developed into a promising branch of re

152 Thin-film solar cells have great potential to overtake the current

153 Specifically, non-fullerene small-molecule solar cells have recently shown a high power conversion

154 skite-based polycrystalline thin-film tandem solar cells have the potential to deliver efficiencies o

155 sses an optimal band gap for single junction solar cells; however, the synthetic literature on this q

156 and public health risk when using perovskite solar cells in building-integrated photovoltaics(17-23).

157 IGS (copper indium gallium selenide) used in solar cells in just about a decade.

158 ive a highly efficient alternative to bottom solar cells in tandem devices.

159 here has been significant interest in tandem solar cells in the presence of concentrated sunlight or

160 Pb-based halide perovskite solar cells, in particular, currently stand at a record

161 Solar cell investigation of devices based on 1 were cond

162 ffective charge separation in perovskite CQD solar cells is developed.

163 he alkali metal cations in halide perovskite solar cells is not well understood.

164 ersion efficiency (PCE) of halide perovskite solar cells is now comparable to that of commercial sola

165 es for high-efficiency and stable perovskite solar cells is reported.

166 s recombination and hysteresis in perovskite solar cells, is revealed.

167 ve emerged as a series of star materials for solar cells, lasers and detectors.

168 ide perovskite nanocrystals (NCs) for use in solar cells, light emitting diodes, lasers, and photodet

169 significant demand in applications including solar cells, light-emitting diodes, and touch panels.

170 for applications such as solution-processed solar cells, light-emitting diodes, detectors and lasers

171 properties and device applications, such as solar cells, light-emitting diodes, white-light emitters

172 Despite the notable progress in perovskite solar cells, maintaining long-term operational stability

173 ded invaluable insights for many crystalline solar cell materials, and we used this method to success

174 hybrid perovskites at the forefront of novel solar cell materials, with CH(3) NH(3) PbI(3) being an a

175 ow very much accepted that halide perovskite solar cells may have a strong practical impact in next-g

176 The perovskite solar cell modified with a metal-organic framework could

177 lymers is important for nonfullerene organic solar cells (NF-OSCs), as state-of-the-art nonfullerene

178 to nonfullerene-based small-molecule organic solar cells (NFSM-OSCs) to achieve a very high power con

179 harge dynamics in systems such as perovskite solar cells, organic-, and nanostructure-based photovolt

180 upling by embedding a fullerene-free organic solar cell (OSC) photo-active layer into an optical micr

181 A major challenge for organic solar cell (OSC) research is how to minimize the tradeof

182 Organic solar cells (OSCs) are one of the most promising cost-ef

183 n solution-processed semitransparent organic solar cells (OSCs) are presented.

184 Organic solar cells (OSCs) based on D18:Y6 have recently exhibit

185 vice fabrication, the performance of organic solar cells (OSCs) has improved markedly in recent years

186 rphology tuning of the blend film in organic solar cells (OSCs) is a key approach to improve device e

187 ed, non-fullerene-based, and ternary organic solar cells (OSCs) over a wide range of interlayer thick

188 er conversion efficiencies (PCEs) in organic solar cells (OSCs).

189 an integral part of high performance organic solar cells over the last 20 years, however their inhere

190 rformance of NiO-based p-type dye-sensitized solar cells (p-DSCs), the function of the surface states

191 Overall, we find that organic solar cells packaged in an inert atmosphere can be extre

192 recycling of the photoactive materials from solar cells paves a path for more sustainable green ener

193 As a result, we achieve greatly enhanced solar cell performance for the optimized AVA-based devic

194 e materials have shown rapid improvements in solar cell performance, surpassing the top efficiency of

195 contact, however, results in extremely poor solar cell performance.

196 ly improved CsPbI(3) PQD synthetic yield and solar-cell performance through surface ligand management

197 h can be attractive for energy conversion in solar cells, photocatalysis and hydrogen generation.

198 develop the optimal bulk heterojunction for solar-cell, photodetector, and photocatalytic applicatio

199 nt of other optoelectronic devices including solar cells, photodetectors, and light-emitting diodes.

200 re paired with those of experts in thin-film solar cell preparation at the cutting edge of current de

201 Consequently, the resulting perovskite solar cells present a power conversion efficiency of 21.

202 tely resulting in high-efficiency perovskite solar cells produced with ease and with high reproducibi

203 the current-voltage hysteresis in perovskite solar cells (PSCs) and, in turn, to impact the interfaci

204 Metal-halide perovskite solar cells (PSCs) are one of the most promising photovo

205 ectron-transport-layer (ETL)-free perovskite solar cells (PSCs) are still inferior to ETL-containing

206 Perovskite solar cells (PSCs) composed of organic polymer-based hol

207 tate-of-the-art, high-performance perovskite solar cells (PSCs) contain a large amount of iodine to r

208 trinsic degradation mechanisms of perovskite solar cells (PSCs) containing unreacted PbI(2) has been

209 The photovoltaic efficiency of perovskite solar cells (PSCs) depends drastically on the charge-car

210 Environmental stability of perovskite solar cells (PSCs) has been improved by trial-and-error

211 of cesium lead iodide (CsPbI(3) ) perovskite solar cells (PSCs) has generated enormous interest in th

212 The operational instability of perovskite solar cells (PSCs) is known to mainly originate from the

213 Surface passivation of perovskite solar cells (PSCs) using a low-cost industrial organic p

214 iro-OMeTAD, allowing us fabricate perovskite solar cells (PSCs) with a champion reverse scan power co

215 istine TiO(2) -based devices, the perovskite solar cells (PSCs) with acid-treated TiO(2) ETL exhibit

216 Currently, blade-coated perovskite solar cells (PSCs) with high power conversion efficienci

217 n photoconversion efficiencies of perovskite solar cells (PSCs).

218 were synthesized and employed in perovskite solar cells (PSCs).

219 conductivity in triple cation 2D perovskite solar cells (PSCs).

220 (PCEs) in bulk heterojunction (BHJ) polymer solar cells (PSCs).

221 ance and operational stability of perovskite solar cells (PSCs).

222 mprove photovoltaic efficiency of perovskite solar cells (PSCs).

223 on transport materials (ETMs) for perovskite solar cells (PSCs); however, experimental evidence is la

224 Although organic-inorganic hybrid perovskite solar cells (PVSCs) have achieved dramatic improvement i

225 All-inorganic perovskite solar cells (PVSCs) have drawn increasing attention beca

226 radiative recombination losses in perovskite solar cells (PVSCs).

227 er great opportunities for hybrid perovskite solar cells (PVSCs).

228 S sites when the OPV device is operated as a solar cell rather than as a light-emitting diode.

229 Lead (Pb)-halide perovskite solar cells reach 24.2% power conversion efficiency, ren

230 Though perovskite solar cells reached comparable efficiency to that of cry

231 all NFSM-OSCs and all small-molecule binary solar cells reported so far.

232 Organo-lead halide perovskite solar cells represent a revolutionary shift in solar pho

233 also a significant driver in the perovskite solar cell research.

234 copy, where MAPbBr(3) - and CsPbBr(3) -based solar cells respond at very different frequencies.

235 Typical lead-based perovskites solar cells show an onset of photogeneration around 800

236 The resulting perovskite CQD solar cell shows a power conversion efficiency approachi

237 e doping of semiconductors in heterojunction solar cells shows tremendous success in enhancing the pe

238 all effect using the diode equation and PC1D solar cell simulations.

239 icularly challenging in the present best CQD solar cells, since these employ a p-type hole-transport

240 lithic-structured solid-state dye sensitized solar cell (ssDSSC) on textile using all solution based

241 ons show that the simplified single nanowire solar cell structure can minimize the interface area and

242 thickness in strained multiple quantum well solar cell structures suggests that apparent radiative e

243 vertake the currently dominant silicon-based solar cell technologies in a strongly growing market.

244 Silicon dominates contemporary solar cell technologies(1).

245 of the emerging lead (Pb) halide perovskite solar cell technology still faces significant challenges

246 ates the immense potential of this thin-film solar cell technology to become a low-cost alternative t

247 cations involving light-emitting devices and solar cell technology.

248 sting should be performed to rapidly develop solar cells that are both extraordinarily efficient and

249 fficiency (PCE) of perovskite/silicon tandem solar cells that can exceed the Shockley-Queisser single

250 Microbial solar cells that mainly rely on the use of photosynthesi

251 Tandem solar cells that pair silicon with a metal halide perovs

252 After applying PT-TPA into perovskite solar cells, the doping-induced band bending in perovski

253 rid organic-inorganic lead halide perovskite solar cells, the energy loss is strongly associated with

254 spatial charge collection efficiency in CQD solar cells, the key materials interface dominating the

255 the tremendous interest in halide perovskite solar cells, the structural reasons that cause the all-i

256 Known technologies-such as solar cells, thermoelectric devices and mechanical gener

257 For next generation organic solar cells, this involves intermolecular charge-transfe

258 on lifetime and boosts the efficiency of the solar cells to 21.1%.

259 ties to apply the knowledge accrued from BHJ solar cells to generate free charges for use in promisin

260 emiconductors to pair with silicon in tandem solar cells to pursue the goal of achieving power conver

261 rgy-harvesting/storage devices, ranging from solar cells to rechargeable batteries.

262 ons, including ultrathin flexible materials, solar cells, touch-screen panels, nanotextured surfaces

263 performance perovskite-based photodetectors, solar cells, transistors, scintillators, etc.

264 erence to their target applications, namely: solar cells, transparent film heaters, sensors, and disp

265 fs involved in the design of bifacial tandem solar cells under arbitrary concentration and series res

266 tial rapid degradation of CH(3) NH(3) PbI(3) solar cells under illumination.

267 rapid degradation of encapsulated perovskite solar cells under illumination.

268 monstration of long-term operational, stable solar cells under intense conditions is a key step towar

269 te a stability enhancement of the perovskite solar cells upon supramolecular modulation, without comp

270 light is possible by sensitizing the silicon solar cell using singlet exciton fission, in which two e

271 Organic solar cells usually utilise a heterojunction between ele

272 o improve the cell performance of perovskite solar cells via the combination of internal doping by a

273 minal wide-bandgap perovskite/silicon tandem solar cell was made possible by the ideal combination of

274 s acceptor materials for bulk heterojunction solar cell were demonstrated.

275 Early heterojunction-based solar cells were limited to relatively modest efficienci

276 Solar cells were made with n = 3 giving an efficiency of

277 ining to the design of "thin film multilayer solar cells", where the goal is to maximize the external

278 rent generation in low-donor-content organic solar cells, where the active layer is composed of vacuu

279 terfacial charge recombination in perovskite solar cells which is in complimentary to broadly applied

280 e efficiency is by fabricating multijunction solar cells, which can split the solar spectrum, reducin

281 g the performance of many types of inorganic solar cells, while it is found challenging in perovskite

282 The photoactive layer of bulk heterojunction solar cell, whose performance is strongly correlated to

283 The deployment of perovskite solar cells will rely on further progress in the operati

284 We developed a stable perovskite solar cell with a bandgap of ~1.7 electron volts that re

285 s leads to a cesium-based ternary perovskite solar cell with stabilized power output of 21.32% at max

286 ine, yielding high-performance p-i-structure solar cells with a stabilized efficiency of 21.4%.

287 deposition of perovskite QDs, we demonstrate solar cells with abrupt compositional changes throughout

288 realize high-performance P3HT-based polymer solar cells with an efficiency over 8%.

289 leads to alpha-6T based homojunction organic solar cells with an external quantum efficiency reaching

290 of concentrated sunlight or tandem bifacial solar cells with back-reflected albedo.

291 Stacking solar cells with decreasing band gaps to form tandems pr

292 nic lead-halide perovskites that have led to solar cells with extremely high photoconversion efficien

293 We analyse organic solar cells with four different photoactive blends exhib

294 2D perovskite solar cells with high stability and high efficiency have

295 rection for achieving low-bandgap perovskite solar cells with high stability.

296 and electron mobility than NDI-CI, affording solar cells with higher efficiencies.

297 help advancing our understanding and lead to solar cells with higher efficiency.

298 tron and hole transport layers in perovskite solar cells with ideal energy levels, high charge mobili

299 As a consequence, perovskite solar cells with organic chromophore exhibit an enhanced

300 More importantly, solar cells with the new HTMs are hysteresis-free and de