ライフサイエンスコーパス: photocurrent

1 emical quenching induced by DCBQ mirrors the photocurrent.

2 uminol chemiluminescence, which enhanced the photocurrent.

3 subsurface vibration, parallels that of the photocurrent.

4 es photon spin and thus the direction of the photocurrent.

5 ound to be similar to those determined using photocurrent.

6 ayer generates a directional, spin-polarized photocurrent.

7 the desensitization of the rod outer segment photocurrent.

8 ominant mechanism for the helicity-dependent photocurrent.

9 cking and a gate-dependent modulation of the photocurrent.

10 ing without spending intense effort to match photocurrent.

11 ave narrower bandgap and thus enhance device photocurrent.

12 n desensitization with the rod outer segment photocurrent.

13 ows p-type semiconductor character and large photocurrent.

14 y of ways of reducing bandgaps and enhancing photocurrent.

15 /hole pairs and causes a detectable local AC photocurrent.

16 kinetics, and spectral sensitivity of their photocurrents.

17 on spectrum peaking at 610 nm for stationary photocurrents.

18 ' and approached the upper bound set by cone photocurrents.

19 photoelectrochemical sensor presented a TBHQ photocurrent about 13-fold higher and a charge transfer

20 Because of their greater photocurrents, ACRs permitted complete inhibition of car

21 t fast response times, as well as a constant photocurrent against the induced bias.

22 ent spectral response functions and measured photocurrents along the length of the nanowire.

23 opy, electrochemical impedance spectroscopy, photocurrent analysis and incident photon-to-electron co

24 est performance observed at 17.6 mA/cm(2) of photocurrent and 7.5% PCE for a cosensitized device with

25 ime, displaying a tenfold enhancement in the photocurrent and a twofold decrease in the response time

26 Taking advantage of the improved photocurrent and diminished charge transfer resistance,

27 norganic perovskite photodetectors with high photocurrent and fast response time, displaying a tenfol

28 n technique to address the trade-off between photocurrent and fill factor in thick bulk heterojunctio

29 s the simultaneous recording of the produced photocurrent and fluorescence signals from the photosynt

30 ial is responsible for the markedly enhanced photocurrent and largely shortened response time.

31 ectrode surface gives rise to a quantifiable photocurrent and leads to the generation of a redox cycl

32 electron acceptor in devices to obtain high photocurrent and low dark current.

33 ms enabling significant improvements in both photocurrent and onset potential.

34 rage of solar energy, through improving both photocurrent and photocharging depth.

35 gen evolution catalyst (OEC) to increase the photocurrent and reduce the onset potential.

36 mediators play a major role determining the photocurrent and the photovoltage in dye-sensitized sola

37 aforementioned sensor was monitored with the photocurrent and the relative photocurrent variation, wh

38 o different experimental techniques based on photocurrent and ultrafast spectroscopy measurements.

39 Notably, the photocurrent and various photocycle intermediates were r

40 e development of ChR2 variants with improved photocurrents and more selective ion permeability using

41 Here we analyze laser flash-induced photocurrents and photochemical conversions in Guillardi

42 le spectroscopic measurements to investigate photocurrents and photochemical properties of ReaChR.

43 IR) is one of the key factors to ensure high photocurrents and thus high efficiency.

44 chloride-conducting channels displayed small photocurrents and were not tested for optogenetic inhibi

45 h IDIC layers yield higher photovoltages and photocurrents, and 45% enhanced efficiency compared with

46 ing of bulk heterojunctions to realize large photocurrents, and examine the formed morphology in thre

47 Nanoscale photocurrents are mapped under a series of biases using

48 Because photocurrents are near the theoretical maximum, our focu

49 Onsets of photocurrents are observed at potentials as positive as

50 ed to a 40-fold enhancement of the catalytic photocurrent as compared to planar devices, resulting in

51 oxidation of 1-thioglycerol (TG), generating photocurrent as the readout signal.

52 ed light emission and polarization-dependent photocurrent, as well as anisotropic conductivities and

53 ticle resolution (about 390 nanometres), the photocurrent associated with water oxidation, and find t

54 nic conditions, we concluded that the PsChR1 photocurrent at physiological conditions is strongly inw

55 o the creation of ChRs that have high cation photocurrent but pass fewer calcium ions and protons.

56 ing electrodes, hence influencing the device photocurrent, but also act as protective barriers agains

57 ve flow of electrolytes greatly enhanced the photocurrent by 5 times comparing to that with stagnant

58 quilibrium mid-gap traps which contribute to photocurrent by a non-linear process of optical release,

59 the pressure on the junction to 23 MPa, the photocurrent can be enhanced by a factor of four through

60 oanodes with oxygen evolution catalysts, the photocurrent can be enhanced; however, current systems f

61 The photocurrent can be reversed and switched by controllabl

62 The photoresponsivity and photocurrent can be varied by more than one order of mag

63 These photocurrents can be used to detect the carrier-envelope

64 ed with anti-AFP through the analysis of the photocurrent change.

65 unit 2 (KA2) to the recently discovered high-photocurrent channelrhodopsin CoChR restricted expressio

66 ionally characterized ChRs, we designed high-photocurrent ChRs with high light sensitivity.

67 Despite generating less photocurrent, Co(II/III)(pz-py-pz)2 devices achieved max

68 te electrodes demonstrate a higher reductive photocurrent compared to the photocurrent registered at

69 owed a higher signal-to-noise ratio (SNR) of photocurrents compared to the traditional DC response, w

70 endent photocurrent generation and prolonged photocurrent decay, originated from charge trapping in t

71 The PEC sensing principle is based on the photocurrent decline due to the blocking effect of SCCA

72 Here we show that the slow photocurrent degradation in thin-film photovoltaic devic

73 ith a forward gradient produce record AM 1.5 photocurrent densities for CuBi2O4 up to -2.5 mA/cm(2) a

74 The mediated photocurrent densities generated by the biofilm were 2 o

75 s design approach led to anodic and cathodic photocurrent densities of + 38.41 mA cm(-2) (+ 0.76 V(RH

76 ode behavior has been observed with negative photocurrent densities of around -10 muA/cm(2) at 0 V vs

77 These photocathodes demonstrate photocurrent densities on the order of -1.0 mA/cm(2) at

78 on, Ag nanoparticle electrodes achieved high photocurrent densities, surpassing 2 mA cm(-2) with an i

79 the ability to obtain substantially improved photocurrent densities.

80 x based redox mediators without compromising photocurrent densities.

81 ectrodes, leading to a drastically increased photocurrent density ( Jph ).

82 ability was gained with RuO(2) where initial photocurrent density (>8 mA cm(-2)) deceased only 15% or

83 In an attempt to enhance the photocurrent density achievable by pigment proteins, her

84 n efficiency (5.01%) in the series with high photocurrent density and open circuit voltage.

85 r = 31.2 muC cm(-2) ) and a largely enhanced photocurrent density approximately two orders of magnitu

86 t 1.3 V vs. RHE for 10 h, 90% of the initial photocurrent density are retained, whereas the photoacti

87 ted hematite showed a substantially enhanced photocurrent density compared to untreated samples.

88 .2 V vs. RHE for CO production and a partial photocurrent density for CO at -0.11 V vs. RHE (j(-0.11,

89 charge-modulation system exhibits increased photocurrent density from 0.68 to 4.75 mA cm(-2) and pro

90 design concept by achieving an unprecedented photocurrent density in PEC water splitting over 5 mA cm

91 p-Si/AZO/TiO(2) /CoP(2) photocathode shows a photocurrent density of -16.7 mA cm(-2) at 0 V versus re

92 A record photocurrent density of -9.8 mA cm(-2) at 0 V versus RHE

93 rmance under simulated sunlight, achieving a photocurrent density of 10 mA cm(-2) at +0.13 V vs RHE.

94 bon nitride (G-CN) photoanode, with a record photocurrent density of 103.2 muA cm(-2) at 1.23 V vs. R

95 We achieve a photocurrent density of 15.1 mA cm(-2) at 1.23 V vs. rev

96 al Cu foam exhibits a record H(2) -evolution photocurrent density of 370 muA cm(-2) at 0.3 V vs. reve

97 A photocurrent density of 4.48 mA.cm(-2) at 1.23 V vs reve

98 perovskite solar cell exhibits an operating photocurrent density of 6.84 mA cm(-2) and stable gas pr

99 surface, this photoanode shows a remarkable photocurrent density of 7.32 mA cm(-2) at a potential of

100 osited silicon films show about 40 to 50% of photocurrent density of a commercial silicon wafer by ph

101 The Sb(2)Se(3) photocathode exhibits a high photocurrent density of almost 30 mA cm(-2) at 0 V again

102 Under minimally optimized conditions, a photocurrent density of as high as 115 muAcm(-2) and a F

103 exhibits a 14-fold and 2-fold enhancement in photocurrent density under simulated sunlight compared w

104 oated with a MoS(3):MoP composite gave 1 Sun photocurrent density up to 8.7 mA cm(-2) at 0 V vs RHE (

105 2D CCP-Th presents a superb H(2) -evolution photocurrent density up to ~7.9 uA cm(-2) at 0 V versus

106 guration, namely, high transparency and high photocurrent density.

107 rements correspond to the maximum-achievable-photocurrent-density (MAPD), under AM1.5G illumination a

108 However, direct photocurrent detection of different OAM modes has not ye

109 igh as 43 times due to a smaller bandgap and photocurrent direction alignment for all absorption ener

110 ast light response time and with a very high photocurrent dissymmetry factor (g(ph) = 1.27 +/- 0.06)

111 The photocurrent distributions are independent of electric f

112 However, angular photocurrent distributions in nanoplasmonic systems rema

113 For the PbI2-deficient samples, the photocurrent dropped, which could be attributed to accum

114 ven nanorod--even though more improvement in photocurrent efficiency correlates with less reduction i

115 oltaic photocurrents in graphene(12-20): the photocurrent emerges exclusively at the charge neutralit

116 r, the optimal catalyst deposition sites for photocurrent enhancement are the lower-activity sites, a

117 Here, two-dimensional photocurrent excitation spectroscopy, a novel non-linear

118 iderably less than that of the outer segment photocurrent following equivalent pigment bleaching.

119 ity retaining more than 80% of their initial photocurrent for approximately 1 h under continuous illu

120 The enhancement of the total photocurrent for different spacings between the Ni-conta

121 nsor showed selectivity to TBHQ, with a high photocurrent for this antioxidant compared to the photoc

122 efficient of 3.5 x 10(-15) cm(3) s(-1) and a photocurrent gain >10(6) in the perovskite thin films.

123 aneously provide information about the local photocurrent generated at the sample under irradiation a

124 The photocurrent generated by the antibody-coated sensor was

125 rum above the bandgap reveals spin-polarized photocurrent generated by ultrafast relaxation of excite

126 matches the energy of incident photons, the photocurrent generated can be significantly enhanced (up

127 Kinetic modeling of photocurrents generated from ChR2 proteins with conserva

128 n beyond 800 nm into the NIR should increase photocurrent generation and further improve photovoltaic

129 ity owing to its quasi-linear time-dependent photocurrent generation and prolonged photocurrent decay

130 In this work, we demonstrate robust photocurrent generation at the edge of T(d)-WTe(2), a ty

131 As far as we know, the largest photocurrent generation by luminol chemiluminescence was

132 The high photocurrent generation by this dye is reasoned to it ex

133 Photodetectors are typically based either on photocurrent generation from electron-hole pairs in semi

134 The role of Channel II photocurrent generation has often been neglected due to

135 Here we report the layer-number-dependent photocurrent generation in graphene/MoS2/graphene hetero

136 lecular factors determining the mechanism of photocurrent generation in low-donor-content organic sol

137 Photocurrent generation in organic bulk heterojunction (

138 Photocurrent generation is enhanced by directional energ

139 Two photocurrent generation mechanisms of photovoltaic and p

140 ter utilize triplet charge transfer mediated photocurrent generation or increasing the donor-acceptor

141 to energetic electron-hole pairs, useful for photocurrent generation or photocatalysis.

142 semiconductor nanorods allow both efficient photocurrent generation through a photovoltaic response

143 hode using an electron acceptor that enables photocurrent generation under anaerobic conditions as th

144 as key factors determining the efficiency of photocurrent generation.

145 -matter interaction and selectively enhanced photocurrent generation.

146 photoelectrochemical electrode for enhanced photocurrent generation.

147 mainly determined by the bias dependence of photocurrent generation.

148 and a GaN nanowire/Si photocathode with high photocurrents (>5 mA cm(-2) ).

149 Ionic migration, polarization, and photocurrent hysteresis are thus directly correlated at

150 onradiative charge recombination, and induce photocurrent hysteresis, all of which limit the efficien

151 The photocurrent images reveal strongly reduced GP wavelengt

152 Here by using photocurrent imaging we report experimental evidence of

153 omprehensive study of the helicity-dependent photocurrent in (Bi1-x Sb x )2Te3 thin films as a functi

154 mploy detailed quantum transport modeling of photocurrent in graphene field-effect transistors (inclu

155 we report on the observation of an intrinsic photocurrent in graphene, which occurs in a different pa

156 c semiconductors can potentially enhance the photocurrent in photovoltaic devices.

157 QDs to amplify signal in QD-based sensors or photocurrent in QD-based photovoltaics.

158 ght-harvesting efficiency can lead to higher photocurrent in solar cells that are limited by sub-opti

159 energy of 166 meV dominates the persistence photocurrent in the devices.

160 anic chromophore, these solar cells generate photocurrent in the NIR beyond the band edge of the pero

161 to generate a directional helicity-dependent photocurrent in three-dimensional topological insulators

162 Measurements of the rod outer segment photocurrent in transgenic mice, which have only rod fun

163 However, it is challenging to achieve high photocurrents in a device setup due to limitations impos

164 -chip CEP detection via optical-field-driven photocurrents in a monolithic array of electrically-conn

165 observed photothermoelectric or photovoltaic photocurrents in graphene(12-20): the photocurrent emerg

166 driving, switching, and steering femtosecond photocurrents in nanoelectronic devices and pulsed elect

167 spite recent reports on optical-field-driven photocurrents in various nanoscale solid-state materials

168 portant properties such as light adaptation, photocurrent inactivation, and alteration of the ion sel

169 The AC photocurrent increased as a result of the adsorption of

170 ) and a bistable variant (SwiChR++) with net photocurrents increased more than 15-fold under physiolo

171 inescence emission of luminol, a substantial photocurrent increment was observed due in part to the s

172 The below-bandgap photocurrent indicates that CTEs are vital states formed

173 f magnitude enhancement of the short-circuit photocurrent is achieved in Bi(2) WO(6) /SrTiO(3) at roo

174 The spin-polarized photocurrent is achieved through the valley-dependent op

175 and at a -0.45% compressive strain, the PD's photocurrent is dramatically enhanced from approximately

176 Whilst the overall photocurrent is found to be low, the photocurrent stabil

177 A mirror process also occurs in which photocurrent is generated through photoexcitation of the

178 ctroscopy studies revealed that the enhanced photocurrent is partly due to improved efficiency of cha

179 erlying mechanism for the helicity-dependent photocurrent is still not understood.

180 ude that, for the device series studied, the photocurrent loss with thick active layers is primarily

181 duced calcium rise precedes the onset of the photocurrent, making it a candidate in the activation ch

182 with electrical read-out, allowing infrared photocurrent mapping at length scales of tens of nanomet

183 High-resolution real-space photocurrent maps are used to investigate the plasmon pr

184 Photocurrent measurements also reveal a substantial enha

185 Using a combination of steady-state photocurrent measurements and time-delayed collection fi

186 Magnetic-field-dependent photocurrent measurements of polytetracene-based devices

187 We present indium-tin-oxide-based photocurrent measurements that reveal a light-induced si

188 ort carrier lifetime obtained from transient photocurrent measurements, indicates an exciton diffusio

189 Here, using time-resolved photocurrent measurements, we identify an efficient out-

190 nduced absorption spectroscopy and transient photocurrent measurements.

191 is-NIR diffuse reflectance spectra (DRS) and photocurrent measurements.

192 elength- and polarization-dependent scanning photocurrent measurements.

193 inside the junction was monitored by in situ photocurrent measurements.

194 escence, these states are often probed using photocurrent methods that require efficient charge colle

195 Here, using the scanning photocurrent microscopy, we find that twin boundaries ha

196 junctions in the films, which we study with photocurrent microscopy.

197 hat end, we introduce nanoscale-resolved THz photocurrent near-field microscopy, where near-field exc

198 enhanced near p-n or contact junctions, the photocurrent observed in our work arises near the edges/

199 ble light, the photobioanode shows an anodic photocurrent of 1.95 muA cm(2) at attractively low poten

200 lectrodes is delayed for about 36 times; The photocurrent of bR integrated CuSCN electrodes is enhanc

201 A photocurrent of over 6.8 mA cm(-2) and an accordingly hi

202 The photocurrent of the nanostructures shows an NADH-depende

203 m the contribution of the dye to the overall photocurrent of the solar cell.

204 soluble AQ salt is employed with the highest photocurrent of up to 0.4 mA cm(-2) and near-quantitativ

205 W cm(-2) white-light illumination, sustained photocurrents of 1.5 mA cm(-2) were measured under an ap

206 The resulting CdTe photoanode generated photocurrents of 1.8 and 5.4 mA cm(-2) at 0.6 and 1.2 V(

207 Immobilized ZnSe NRs on CuCrO(2) generate photocurrents of around -10 muA cm(-2) in an aqueous ele

208 testing, showing p-type behavior and stable photocurrents of up to ~ 0.036 mA/cm(2).

209 sing technique invoked wide range of tunable photocurrent on/off ratio in Si-QD photodetector (rangin

210 Significantly higher photocurrent on/off ratio was achieved up to over 500 co

211 aqueous electrolyte solution (pH 5.5) with a photocurrent onset potential of approximately +0.75 V vs

212 and photocathodes show positive and negative photocurrent onset potentials for water oxidation and re

213 The microscopic mechanism of this large photocurrent originates from separated transport of elec

214 The photocurrent (PC) response is orders of magnitude higher

215 coherence times between the exciton and the photocurrent producing states of 20 fs or less.

216 e, polymer-fullerene blends with contrasting photocurrent properties and enthalpic offsets driving se

217 r properties of MoS2 devices by studying its photocurrent properties on both SiO2 and self-assembled

218 tion and demonstrate a general, device-based photocurrent-ratio measurement to extract the intrinsic

219 on, an organic-soluble AQ is applied and the photocurrent reaches 1.8 mA cm(-2) with faradaic efficie

220 on model to explain the unique light-induced photocurrent recorded in NpHR.

221 Photocurrents recorded from the RubyACR from Aurantiochy

222 a chemical capacitance, we suggest that the photocurrent reduction was primarily caused by the light

223 igher reductive photocurrent compared to the photocurrent registered at pure PbO or Pb3O4-modified el

224 bular geometry had a strong influence on the photocurrent response and a 29.9% improvement of the pho

225 e prepared Si film exhibited ~30-40 % of the photocurrent response of a commercial p-type Si wafer, i

226 order of magnitude increase in the transient photocurrent response relative to CdS alone, an effect a

227 cycles caused a marked deterioration of the photocurrent response to around a third of initial level

228 the nanocomposite components, an outstanding photocurrent response was observed for DA based on PEC s

229 current for this antioxidant compared to the photocurrent responses for other phenolic antioxidants.

230 ficient to explain the complex dependence of photocurrent responses to photostimuli.

231 illumination orientation and simulating the photocurrent responses with an equivalent circuit model

232 s response to 442 nm illumination, including photocurrent, rise time, and fall time.

233 12 to 1.17 V and an efficiency of 23.4% from photocurrent scanning with a stabilized efficiency of 22

234 The flexible photocurrent sensing system was manufactured on a 30-mic

235 The chemiluminescence in the miniaturized photocurrent sensing system was successfully used to det

236 The photocurrent shows a ninefold increase in comparison to

237 of tropomyosin with TROP aptamer probe, the photocurrent signal decreased due to releasing adsorbed

238 6(3+) was adsorbed on aptamer to enhance the photocurrent signal.

239 The photocurrent signals exhibit similar patterns to the lig

240 Coherent oscillations in the photocurrent signals indicate that polaron formation may

241 Intriguingly, the photocurrent signals were eliminated after specific poin

242 In the photocurrent single entity transients, we demonstrate re

243 This AQ-relay DSPEC exhibits the highest photocurrent so far in non-aqueous electrolytes for H(2)

244 The two-dimensional photocurrent spectra are interpreted by introducing a th

245 a, photoluminescence spectroscopy, transient photocurrent spectra, and electrochemical impedance spec

246 ta show no cross-peaks in the twodimensional photocurrent spectra, as predicted by the model for cohe

247 lations, optical absorption measurements and photocurrent spectral response measurements demonstrate

248 current spectroscopy and intensity modulated photocurrent spectroscopy (IMPS).

249 ectrodes were studied by using the transient photocurrent spectroscopy and intensity modulated photoc

250 While device photocurrent spectroscopy can be used to extract the exc

251 nsitions of high-quality bilayer graphene by photocurrent spectroscopy measurement.

252 of excitons in bilayer graphene (BLG) using photocurrent spectroscopy of high-quality BLG encapsulat

253 Mott-Schottky plots, and intensity-modulated photocurrent spectroscopy show that such enhancement is

254 Using ultrafast electro-optical pump-push-photocurrent spectroscopy, we find the yield of free ver

255 overall photocurrent is found to be low, the photocurrent stability is shown to be excellent, with li

256 photovoltaic detectors have shown excellent photocurrent stability under bending induced stress up t

257 The bias and temperature effects on the photocurrent strength and the signal-to-noise ratio have

258 ular photodetector was developed as the core photocurrent system through chemiluminescence for hydrog

259 ion photoanode results into a 10-fold higher photocurrent than bulk graphitic carbon nitride (G-CN) p

260 s, we obtained a ChR, ChromeQ, with improved photocurrent that possesses order-of-magnitude reduction

261 photogalvanic effect (CPGE) is the part of a photocurrent that switches depending on the sense of cir

262 the rate of both of these is limited by the photocurrents that can be generated from the solar flux.

263 and gives relatively stable photoanodes with photocurrents that reach to 1.7 mA cm(-2) with an optimi

264 To maintain the photocurrent, the reduction of oxidized dye by the redox

265 n purified wild-type and mutant ACRs, and of photocurrents they generate in HEK293 cells.

266 ement for the fabrication of efficient, high photocurrent, thick organic solar cells.

267 f a microalgae living biosensor by enhancing photocurrent through nanocavities formed between copper

268 odel to relate the directional nature of the photocurrent to asymmetric optical transitions between t

269 try, electrochemical impedance spectroscopy, photocurrent transient analysis) demonstrated better per

270 Simulation of the photovoltage and photocurrent transients shows that hysteresis requires t

271 aneously collects photoluminescence spectra, photocurrent transients, and photovoltage transients.

272 As a result of a balance between VOC and the photocurrent, tuning of the interface energy gap is nece

273 Unlike other photocurrent types that are enhanced near p-n or contact

274 complex and thus generating enhanced anodic photocurrent under visible light for signaling.

275 Remarkably, PyTz-COF exhibited a photocurrent up to 100 muA cm(-2) at 0.2 V vs. RHE and c

276 iation, which is expressed as the changes in photocurrent upon the formation of antibody-antigen comp

277 The experiment showed the relative photocurrent variation is directly proportional to the l

278 The photocurrent variation related to the specific recogniti

279 tored with the photocurrent and the relative photocurrent variation, which is expressed as the change

280 ieved by tuning photoexcitation of ultrafast photocurrents via the photogalvanic effect.

281 the traditional DC response, while a steeper photocurrent-voltage (I-V) curve than that of LAPS with

282 The PVSCs exhibit small photocurrent-voltage hysteresis and high reproducibility

283 zation on the direction and magnitude of the photocurrent was also demonstrated.

284 Photocurrent was measured when the sensor was excited by

285 onceive a plasmonic solar cell with enhanced photocurrent, we investigate the role of plasmonic nanos

286 However, passive photocurrents were only observed in leak mutants if the

287 Light-evoked excitatory photocurrents were reliably obtained from SST-ChR2-YFP n

288 originated from the optical helicity-induced photocurrent which is shown to be enhanced, reduced, tur

289 otovoltage with respect to the outer segment photocurrent, which is eliminated upon internal dialysis

290 -near-infrared (NIR) region to generate high photocurrent, which leads to the significant reduction o

291 ation) was observed because of the increased photocurrent, which was attributed to enhancement of lig

292 ally, the dual-plasmon device produces a net photocurrent whose polarity is determined by the balance

293 tron-hole pairs give rise to a stable anodic photocurrent whose potential- and pH-dependences exhibit

294 devices also exhibit sizable X-ray generated photocurrent with a high mutau product of ~1.2 x 10(-4)

295 Whereas the helicity dependent photocurrent with below-gap excitation is due to spin-ga

296 The nature of variation of photocurrent with temperature confirms that the trap sta

297 er interactions lead to optical-field-driven photocurrents with an attosecond-level temporal response

298 3 as the redox mediator produced the highest photocurrent yet generated from TTA-UC (0.158 mA cm(-2))

299 These disparate photocurrents, yet similar yields for nonradiative excit

300 n perylenediimides and rubrene show a higher photocurrent yield (+50%) and extended spectral coverage