ライフサイエンスコーパス: photovoltaic

1 e this system interesting as a ferroelectric photovoltaic.

2 are important for the development of tandem photovoltaics.

3 optoelectronic devices that span far beyond photovoltaics.

4 cs and are used in light-emitting diodes and photovoltaics.

5 on technologies, such as thermoelectrics and photovoltaics.

6 n areas such as electronics, spintronics and photovoltaics.

7 ty, multiferroicity, mangetoresistivity, and photovoltaics.

8 ls-an important process for third-generation photovoltaics.

9 ts to direct charge flow in perovskite-based photovoltaics.

10 will aid the development of next generation photovoltaics.

11 tocatalysis, supercapacitors, batteries, and photovoltaics.

12 ter processes for kef recycling and low cost photovoltaics.

13 lly established alternative to silicon-based photovoltaics.

14 QD-based sensors or photocurrent in QD-based photovoltaics.

15 ly important as charge-transfer materials in photovoltaics.

16 ntial for optoelectronic applications beyond photovoltaics.

17 ive, and stable NIR-selective molecular salt photovoltaics.

18 ass of materials for organic and transparent photovoltaics.

19 to be a poor photocatalyst, is promising for photovoltaics.

20 s to overcome the Shockley-Queisser limit in photovoltaics.

21 librium hot-carrier generation, sensing, and photovoltaics.

22 r cations in the high-performance perovskite photovoltaic absorbers, methylammonium lead iodide (MAPb

23 results represent the first demonstration of photovoltaic action from an ion-exchange membrane and of

24 ts were not likely the cause of the observed photovoltaic action from photoacid-modified membranes.

25 dicted, making photoferroelectrics promising photovoltaic alternatives.

26 rk, through systematic photoluminescence and photovoltaic analysis, a new ideal bandgap (1.35 eV) abs

27 nductivity and colossal magnetoresistance to photovoltaic and catalytic activities.

28 nic materials with excellent efficiencies in photovoltaic and light-emitting applications.

29 Despite rapid developments in both photovoltaic and light-emitting device performance, the

30 s essential for developing new materials for photovoltaic and photocatalytic applications.

31 Here, we directly characterize the local photovoltaic and photoconductive properties of 71 degree

32 indings are promising for practical flexible photovoltaic and photodetector applications ranging from

33 Storage of photovoltaic and wind electricity in batteries could sol

34 the same reduction could be achieved through photovoltaic and wind power generation constituting 60%

35 plications in areas such as nanoelectronics, photovoltaics and catalysis.

36 conductors is crucial for the development of photovoltaics and efficient photonic devices.

37 a variety of organic semiconductors used in photovoltaics and field-effect transistors.

38 velop novel applications in optoelectronics, photovoltaics and green chemistry.

39 e so far reported for fullerene-free organic photovoltaics and is inspiring for the design of new ele

40 hts that may assist in the design of organic photovoltaics and light-emission devices with longer lif

41 e perovskites in the research communities of photovoltaics and light-emitting diodes.

42 he development of high-efficiency perovskite photovoltaics and low-cost lasers.

43 sed towards effective development of organic photovoltaics and molecular electronics.

44 es with single-walled carbon nanotube (SWNT) photovoltaics and nanostructured devices is maintaining

45 rge carriers is a key cross-cutting issue in photovoltaics and optoelectronics.

46 nt light-absorbing materials for solid-state photovoltaics and other applications.

47 nic and hybrid halide double perovskites for photovoltaics and other optoelectronics.

48 ocesses are central to the fields of organic photovoltaics and photocatalysis, where it is necessary

49 w-cost and environment-friendly material for photovoltaics and photocatalysis.

50 he near-infrared photons to be harnessed for photovoltaics and photocatalysis.

51 ly exceeding the Shockley-Queisser limit for photovoltaics and photocatalysis.

52 ient electron transport material for organic photovoltaics and related devices, such as perovskite so

53 to extend to applications of other thin film photovoltaics and semiconductor devices.

54 r potential applications in optoelectronics, photovoltaics and thermoelectrics.

55 ood candidates for low-cost, high efficiency photovoltaic, and light-emitting devices.

56 n photocatalysis, (photo)sensors, photonics, photovoltaics, and drug delivery demonstrate the vast po

57 , including heterogeneous catalysis, organic photovoltaics, and nanoelectronics, yet they are rarely

58 the active layers in light-emitting diodes, photovoltaics, and other devices.

59 ications such as efficient electrocatalysts, photovoltaics, and sensors.

60 highly efficient solar absorber material for photovoltaic application.

61 n in the design of lead-free perovskites for photovoltaic application.

62 r microfluidic cooling of chips, vias, MEMS, photovoltaic applications and photonic devices that matc

63 conclude that 1 is a promising material for photovoltaic applications and represents a new type of l

64 An ideal network window electrode for photovoltaic applications should provide an optimal surf

65 cently emerged as novel active materials for photovoltaic applications with power conversion efficien

66 to be promising semiconductor materials for photovoltaic applications, have been made into atomicall

67 nstrate that optical properties suitable for photovoltaic applications, in addition to spatial electr

68 en studied primarily in the context of their photovoltaic applications, when synthesized as colloidal

69 Cs) show significant promise in a variety of photovoltaic applications.

70 ial long-range charge-transfer materials for photovoltaic applications.

71 ogy of the charge separation layer in future photovoltaic applications.

72 to be a revolutionary material for low-cost photovoltaic applications.

73 of ca. 660 ns, which is very encouraging for photovoltaic applications.

74 lver coating effectiveness for the thin-film photovoltaic applications.

75 curity ink and enhanced energy harvesting in photovoltaic applications.

76 lloyed material, which is very promising for photovoltaic applications.

77 o not have bandgaps energies well-suited for photovoltaic applications.

78 ght-absorbing materials has been utilized in photovoltaic applications.

79 ing high-performance conjugated polymers for photovoltaic applications.

80 in organic light-emitting diodes and organic photovoltaics are compared.

81 ications, to date, in organic and perovskite photovoltaics are reviewed, and insights as to how the a

82 Building integrated photovoltaics (BIPV) have attracted considerable interes

83 In photovoltaic blends, charge transfer can occur from the

84 in boosting the performance of polymer:ITIC photovoltaic bulk heterojunction blends.

85 egration of ZnO nanotubes as photoanode in a photovoltaic cell and as a photonic oxygen gas sensor.

86 tted from (90)Sr, and a high efficiency c-Si photovoltaic cell is used as the converter.

87 temperature on an InGaP (GaInP) (55)Fe X-ray photovoltaic cell prototype for a radioisotope microbatt

88 g heat exactly at the bandgap frequency of a photovoltaic cell).

89 ement of the number of charges in an organic photovoltaic cell, while avoiding non-geminate recombina

90 scent modes from the thermal radiator to the photovoltaic cell.

91 Metal halide perovskite photovoltaic cells could potentially boost the efficienc

92 Field-effect transistors and photovoltaic cells demonstrate that BTSA is a promising

93 Photovoltaic cells exhibit a high open circuit voltage (

94 l0.2Ga0.8As (55)Fe radioisotope microbattery photovoltaic cells over the temperature range -20 degree

95 via singlet fission offers the potential for photovoltaic cells that exceed the Shockley-Quiesser lim

96 re used to fabricate colloidal perovskite QD photovoltaic cells with an open-circuit voltage of 1.23

97 aterials are used as electrodes in displays, photovoltaic cells, and touchscreens; they are also used

98 s for organic light-emitting diodes (OLEDs), photovoltaic cells, chemical sensors, and bioimaging.

99 rs and silver-backed semiconductor-thin-film photovoltaic cells.

100 of the twin boundaries in polycrystalline Si photovoltaic cells.

101 ch is commonly used as a protective glass in photovoltaic cells.

102 Photovoltaic characteristics and j-V curve demonstrated

103 (68% visible transmittance) to an absorbing, photovoltaic colored state (less than 3% visible transmi

104 s for device prototypes, as evidenced by the photovoltaics community's focus on detailed balance.

105 been a long-standing question in the organic photovoltaics community.

106 ng the main possibilities towards economical photovoltaic conversion of the solar energy.

107 tille polycondensation methods for producing photovoltaic copolymers, this DARP protocol eliminates t

108 synthesis of high-performance pi-conjugated photovoltaic copolymers.

109 This photoconduction facilitated local photovoltaic current is likely to be a universal propert

110 ements demonstrate that domain wall enhanced photovoltaic current originates from its high conduction

111 ies and their effects upon the conduction of photovoltaic current still remain elusive.

112 Local photovoltaic current, proven to be driven by the bulk ph

113 ion has been proposed as a possible cause of photovoltaic current-voltage hysteresis in hybrid perovs

114 the fundamental design paradigms in organic photovoltaic device engineering is based on the idea tha

115 in the preparation of a bulk-heterojunction photovoltaic device increases its power conversion effic

116 High efficiency polymer:fullerene photovoltaic device layers self-assemble with hierarchic

117 investigate regioisomeric effects on organic photovoltaic device performance.

118 surface-engineered GQD-incorporated polymer photovoltaic device shows enhanced power conversion effi

119 indows with energy conversion by producing a photovoltaic device with a switchable absorber layer tha

120 erential resistance, tunnelling transistors, photovoltaic devices and so on.

121 as gone towards maximizing the efficiency of photovoltaic devices based on shift currents.

122 as competitive semiconducting materials for photovoltaic devices due to their high performance and l

123 Planar photovoltaic devices from optimized ACI perovskite films

124 The implementation of intermolecular SF in photovoltaic devices has achieved an external quantum ef

125 e slow photocurrent degradation in thin-film photovoltaic devices is due to the formation of light-ac

126 the efficiency of P3HT:IC60BA-based organic photovoltaic devices is enhanced when using hydrogen-dop

127 tured a large portion of the total market of photovoltaic devices mostly due to their relatively high

128 , enabling the realization of ultrathin-film photovoltaic devices or systems for hydrogen production.

129 Moreover, photostability of photovoltaic devices up to 10-Suns is observed, which is

130 rovskites that have yielded highly efficient photovoltaic devices, however, it remains unclear whethe

131 lead to their successful implementation into photovoltaic devices, NIR optical switches and smart win

132 film formation, enables single-layer organic photovoltaic devices, processed at room temperature, wit

133 deformable technologies, including flexible photovoltaic devices, sensors, and displays.

134 n impressive V OC of over 1 V is recorded in photovoltaic devices, suggesting that ITCC has great pot

135 an be precisely controlled in thin films for photovoltaic devices, the synthesis of perovskite nanost

136 in the ease of processing of thin films for photovoltaic devices, there have been suggestions that m

137 description of the fundamental processes in photovoltaic devices, with the main emphasis on the char

138 lifetimes are mapped in polycrystalline CdTe photovoltaic devices.

139 e-carrier transport and on the efficiency of photovoltaic devices.

140 ate-of-art hybrid lead halide perovskites in photovoltaic devices.

141 the systems of artificial photosynthesis and photovoltaic devices.

142 ferroelectric materials lead to their use as photovoltaic devices.

143 s recently been explored for applications in photovoltaic devices.

144 which can raise the open circuit voltage of photovoltaic devices.

145 for use as epitaxial templates for thin film photovoltaic devices.

146 t on integrated optics, optical sensors, and photovoltaic devices.

147 ularly attractive for efficient and low-cost photovoltaic devices.

148 f the main purpose of push-pull polymers for photovoltaic devices.

149 ctronics, organic light emitting diodes, and photovoltaic devices.

150 pplications such as NIR optical switches and photovoltaic devices.

151 fficient single-junction, solution-processed photovoltaic devices.

152 is important for the development of organic photovoltaic diodes (PVDs).

153 t the performance of such promising class of photovoltaic diodes.

154 for designing transparent conductors used in photovoltaics, displays and solid-state lighting is the

155 s, for the first time, achieved on inorganic photovoltaic double perovskites through high pressure tr

156 s (PDs) have long been realized by utilizing photovoltaic effect and their performances can be effect

157 a new approach to enhance the ferroelectric photovoltaic effect by introducing the polarization-depe

158 This field-switchable photovoltaic effect can be explained by the formation of

159 power conversion efficiency of ferroelectric photovoltaic effect currently reported is far below the

160 from first principles that substantial bulk photovoltaic effect enhancement can be achieved by nanol

161 s up the possibility for control of the bulk photovoltaic effect in ferroelectric materials by nanosc

162 However, the mechanism underpinning their photovoltaic effect is still far from understood, which

163 aic current, proven to be driven by the bulk photovoltaic effect, has been probed over the whole illu

164 Rectification and photovoltaic effects are observed in chemically homogene

165 plied strain on the pyro-phototronic and the photovoltaic effects are thoroughly investigated.

166 Optimal materials to induce bulk photovoltaic effects should lack inversion symmetry and

167 ibits clear diode rectification behavior and photovoltaic effects, indicating promise for application

168 oelectric, flexoelectric, thermoelectric and photovoltaic effects.

169 or sunlight spectrum absorption and original photovoltaic effects.

170 ed from the deposited Si film exhibits clear photovoltaic effects.

171 erroics a promising candidate to induce bulk photovoltaic effects.

172 mendous attention because of their excellent photovoltaic efficiencies.

173 state heterojunction solar cells raising the photovoltaic efficiency to 20% within the last 5 years.

174 y, for applications such as touch sensors or photovoltaic electrode structures.

175 Here we report a photovoltaic-electrolysis system with the highest STH ef

176 These results demonstrate the potential of photovoltaic-electrolysis systems for cost-effective sol

177 light emitting diodes, photodetector arrays, photovoltaics, energy storage elements, and bare die int

178 mance and robust state-of-the-art perovskite photovoltaics, especially for the air-sensitive tin-base

179 exceptional electron acceptors, and organic photovoltaics fabricated with the ribbons show efficienc

180 ach to identify two classes of shift current photovoltaics, ferroelectric polymer films and single-la

181 signing high performance, flexible thin film photovoltaics for the realization of building-integrated

182 The field of organic photovoltaics has developed rapidly over the last 2 deca

183 n efficiency (PCE) of lead halide perovskite photovoltaics has reached 22.1% with significantly impro

184 cts are studied through the point of view of photovoltaics-however, the results have important implic

185 O surfaces at molecular interfaces in hybrid photovoltaic (hPV) and organic photovoltaic (OPV) device

186 systems are described-a solar thermoelectric-photovoltaic hybrid system and a vehicle waste heat harv

187 ndidates for high efficiency low cost tandem photovoltaics, in part because they have band gaps that

188 semiconductor, flat panel display, and solar photovoltaic industries.

189 Powering distributed HS-DAC with photovoltaics (instead of coal) while including recaptur

190 water photolysis, exciton fission and novel photovoltaics involving low-dimensional nanomaterials, h

191 ted such that the maximum power point of the photovoltaic is well matched to the operating capacity o

192 remarkable performance of hybrid perovskite photovoltaics is attributed to their long carrier lifeti

193 and hybrid organic-inorganic heterojunction photovoltaics is often limited by high carrier recombina

194 copper refining, which is critical to solar photovoltaics, is chosen as a case study, and three comm

195 For multi-layer organic photovoltaics, it is desirable for the molecules to have

196 toelectronic applications, such as memories, photovoltaics, logic rectifiers and logic optoelectronic

197 systematically tuned to design a new hybrid photovoltaic material predicted to exhibit very low reco

198 ed to design and characterize a new class of photovoltaic materials composed of layered transition me

199 Bulk-heterojunction organic photovoltaic materials containing nonfullerene acceptors

200 perovskites have emerged as high-performance photovoltaic materials with their extraordinary optoelec

201 perovskites have emerged as high-performance photovoltaic materials.

202 ganic-inorganic perovskites high-performance photovoltaic materials.

203 y boost the efficiency of commercial silicon photovoltaic modules from approximately 20 toward 30% wh

204 Technological deployment of organic photovoltaic modules requires improvements in device lig

205 ould reduce the price per watt of perovskite photovoltaic modules.

206 -harvesting systems, like photocatalytic and photovoltaic ones.

207 anic thin-film transistors (TFT) and organic photovoltaic (OPV) cells.

208 ces in hybrid photovoltaic (hPV) and organic photovoltaic (OPV) devices is presented.

209 Solution-processed organic photovoltaics (OPV) offer the attractive prospect of low

210 is essential for highly efficient, organic, photovoltaics (OPV)/perovskite hybrid solar cells.

211 on molecular semiconductors, such as organic photovoltaics (OPVs) and artificial photosynthetic syste

212 A new type of window electrode for organic photovoltaics (OPVs) based on an ultra-thin bilayer of c

213 cy (PCE), commercial applications of organic photovoltaics (OPVs) can be foreseen in near future.

214 Among the photovoltaic technologies, organic photovoltaics (OPVs) demonstrate a cheap, flexible, clea

215 migration character, applicable not only to photovoltaic or display-destined organic semiconductors

216 ion of the energy of light to electricity in photovoltaics, or to energy-rich molecules (solar fuel)

217 Application of this coating to photovoltaic p(+)n-Si junctions yields best reported per

218 Flat-plate photovoltaic panels also have a much higher theoretical

219 derstanding of previously reported excellent photovoltaic parameters in these systems and their super

220 sses caused by the metal contacts in silicon photovoltaics, particularly the optical and resistive lo

221 Technologies for biofuel and photovoltaic paths are evolving; it is critical to consi

222 s bridged with heterocycles exhibit superior photovoltaic performance compared to their unfused semif

223 weight (Mn) on the blend film morphology and photovoltaic performance of all-polymer solar cells (APS

224 erent polymer purification procedures on the photovoltaic performance of bulk heterojunction solar ce

225 The high photovoltaic performance of Cu-based redox mediators und

226 act of the structural phase transitions upon photovoltaic performance of MAPbI3 based solar cells.

227 , and electron mobility, and finally enhance photovoltaic performance of nonfullerene acceptors.

228 Photovoltaic performance of solar cells was investigated

229 ated conducting polymer, which determine the photovoltaic performance of the corresponding solar cell

230 0.1 perovskite can substantially enhance the photovoltaic performance of the derived hole-conductor-f

231 g explored, it is becoming apparent that the photovoltaic performance of the halide perovskites is ju

232 vskites could potentially provide comparable photovoltaic performance with enhanced stability compare

233 under selenium vapor resulted in the optimum photovoltaic performance, with j sc, V oc, FF and eta of

234 materials recently investigated show limited photovoltaic performance.

235 ermally converted perovskite films and their photovoltaic performance.

236 40 s at 170 degrees C without affecting the photovoltaic performance.

237 The good general photovoltaic performances obtained with the three dyes h

238 d in CZTSSe compounds to further improve the photovoltaic performances of related devices.

239 Perovskite CH3NH3PbI3 exhibits outstanding photovoltaic performances, but the understanding of the

240 at the heart of many applications, including photovoltaics, photocatalysis, and photodetection.

241 ication set has cross-cut energy conversion (photovoltaics, photocatalysis, thermoelectrics), energy

242 the next generation of solution-processable photovoltaics, photodetectors, and thermoelectric device

243 in many optoelectronic applications such as photovoltaics, photoelectrochemical cells and light emit

244 uccessful optoelectronic materials with high photovoltaic power conversion efficiencies and low mater

245 Following the unprecedented rise in photovoltaic power conversion efficiencies during the pa

246 as plasmonically-enhanced photocatalytic or photovoltaic processes.

247 , have been proven to play a crucial role in photovoltaic properties of ferroelectrics.

248 Photovoltaic properties of the resulting devices were de

249 structural development of the thin film, its photovoltaic properties undergo dramatic enhancement dur

250 iour with a rectification ratio of 10(4) and photovoltaic properties with a power conversion efficien

251 al properties (for example, charge mobility, photovoltaic properties, gas adsorption capacity or lith

252 s on 2D InSe with improved rectification and photovoltaic properties, without requiring heterostructu

253 materials with excellent optoelectronic and photovoltaic properties.

254 faltering attention owing to their excellent photovoltaic properties.

255 ide perovskites (MHPs) as solution-processed photovoltaic (PV) absorbers.

256 potential of at least 17348 TWh year(-1) for photovoltaic (PV) and 2213 TWh year(-1) for concentratin

257 them promising candidates for application in photovoltaic (PV) and related optoelectronic devices.

258 Solar photovoltaic (PV) electricity generation is expanding ra

259 One possible approach is photovoltaic (PV) energy delivery using optical illumina

260 nd economic effects of large levels of solar photovoltaic (PV) penetration within the services areas

261 State-of-the-art photovoltaic (PV) performance is reported with power con

262 While photovoltaic (PV) renewable energy production has surged

263 ite (HaP) semiconductors are revolutionizing photovoltaic (PV) solar energy conversion by showing rem

264 lead toxicity issue confronting the current photovoltaic (PV) standout, CH3 NH3 PbI3 .

265 We examine the utility of solar photovoltaic (PV) system deployment on urban rooftops to

266 d important progress in associated thin-film photovoltaic (PV) technology, while avoiding scarce and/

267 PECs) can be as low as 0.8%, tandem PECs and photovoltaic (PV)-electrolyzers can operate at 7.2% unde

268 properties of semiconductors, especially in photovoltaics (PVs), due to their effects on electron-ho

269 Exploitation of natural photovoltaic reaction center pigment proteins in biohybr

270 nd by metastable radical pair formation when photovoltaic reaction centers are embedded throughout li

271 ell as other bismuth halide and chalcohalide photovoltaics recently explored by many groups.

272 perties as well as the detailed mechanism of photovoltaics requires a reliable and accessible electro

273 ic-organic hybrid halides has revolutionised photovoltaic research.

274 ng and subsequent applications in artificial photovoltaic research.

275 efficient photocurrent generation through a photovoltaic response and electroluminescence within a s

276 Room temperature photovoltaic response with a cut-off wavelength of 3.4 m

277 The devices show hysteresis-free photovoltaic response, which had been a fundamental bott

278 n perovskites are distinct from conventional photovoltaic semiconductors.

279 aphene-based devices such as photodetectors, photovoltaics, sensors, batteries, and supercapacitors.

280 High-efficiency small-molecule-based organic photovoltaics (SM-OPVs) using two electron donors (p-DTS

281 All-organic-based photovoltaic solar cells have attracted considerable att

282 of a broad array of technologies, including photovoltaics, solar fuel systems and energy storage.

283 Coupling this hybrid device to existing photovoltaic systems would yield a CO2 reduction energy

284 ctrodes play a fundamental role in far-field PhotoVoltaic systems, but have never been thoroughly inv

285 le to those obtained with several commercial photovoltaic technologies in a remarkably short period o

286 erging as one of the most promising low cost photovoltaic technologies, addressing "secure, clean and

287 Among the photovoltaic technologies, organic photovoltaics (OPVs)

288 ability characteristics of leading thin-film photovoltaic technologies.

289 The third generation of photovoltaic technology aims to reduce the fabrication c

290 S) is presently the most efficient thin-film photovoltaic technology with efficiencies exceeding 22%.

291 erged as one of the most promising thin-film photovoltaic technology.

292 great promise as a low-cost, high-efficiency photovoltaic technology.

293 es have triggered the latest breakthrough in photovoltaic technology.

294 synthesis, humans can wear the as-fabricated photovoltaic textile to harness solar energy for powerin

295 wearable manner by fabricating an all-solid photovoltaic textile.

296 ion technology with microfluidic systems and photovoltaics that natively use silicon materials, while

297 ustrate the great potential of shift current photovoltaics to compete with conventional solar cells.

298 films and potential in applications such as photovoltaics, touch panels, liquid crystal displays, an

299 State-of-the-art photovoltaics use high-purity, large-area, wafer-scale s

300 This work validates a photovoltaic window technology that circumvents the fund