ライフサイエンスコーパス: quantum efficiency

1 nsport and charge separation with near unity quantum efficiency.

2 actor (not exceeding 50) provide significant quantum efficiency.

3 e; yet, some OPV blends achieve near-perfect quantum efficiency.

4 results in a 5.5-fold-improved fluorescence quantum efficiency.

5 f 37 cd A(-1), 14 lm W(-1), and 11% external quantum efficiency.

6 l thermal disturbance and the photodetection quantum efficiency.

7 g extremely-dim brightness due to low (0.1%) quantum efficiency.

8 examples nevertheless demonstrate near-unity quantum efficiency.

9 ining barriers to be attacked with near 100% quantum efficiency.

10 d to a significant reduction in the internal quantum efficiency.

11 c organisms harvest sunlight with near unity quantum efficiency.

12 ring adducts, but with a significantly lower quantum efficiency.

13 otons to the reaction center with remarkable quantum efficiency.

14 showed a bathochromic shift and increase in quantum efficiency.

15 a site of charge separation with near unity quantum efficiency.

16 This process occurs with near-perfect quantum efficiency.

17 nd dark current operation, and good internal quantum efficiency.

18 s (CSS) with unusually and consistently high quantum efficiency.

19 which do not produce measurable decreases in quantum efficiency.

20 maintaining the potential for unity internal quantum efficiency.

21 nce and dark current, while maintaining high quantum efficiency.

22 ction efficiency, in agreement with the high quantum efficiency.

23 in photosynthesis are rapid events with high quantum efficiencies.

24 py; such structures exhibit anomalously high quantum efficiencies.

25 environmental compatibility, and near-unity quantum efficiencies.

26 orange) isomer A quantitatively, with a high quantum efficiency (0.60-0.75).

27 r(-1) m(-2)) eight times higher and external quantum efficiencies (2.0%) two times higher than the hi

28 mes the hydrogen evolution rate and apparent quantum efficiency (400 nm), respectively, compared with

29 hydrogen evolution i.e. 4848 mumol/h/0.1 g (quantum efficiency 6.8%).

30 e (PCE = 6.3%, Jsc = 18.6 mA/cm(2), external quantum efficiency = 91%).

31 onalities by at least 10(4), while retaining quantum efficiencies above 50%, and demonstrate evidence

32 ementary absorbing materials, resulting in a quantum efficiency above 75% between 400 and 720 nm.

33 omplexes exhibit far-red emission, with high quantum efficiencies and brightness and also exhibit exc

34 can be isolated in less than 3 min with high quantum efficiencies and elliptical morphologies.

35 ion architecture show greater total external quantum efficiencies and enhanced wide-angle light captu

36 The quantum efficiencies and the ultimate extents of reactan

37 achieves efficiencies of 27.3% for external quantum efficiency and 74.5 lm W(-1) for power efficienc

38 le match with the commercial UV chips, 73.2% quantum efficiency and 90.9% thermal stability at 150 de

39 and the upper lasing level for high internal quantum efficiency and a broadband gain.

40 gy, enabling devices with near 100% internal quantum efficiency and a high power conversion efficienc

41 of a large enhancement in photoluminescence quantum efficiency and a potential route to valleytronic

42 itting diode (OLED) with 24.8% peak external quantum efficiency and CIE coordinates of (0.147, 0.079)

43 Clear improvements in measured detective quantum efficiency and combined energy resolution/energy

44 between electroluminescence and photovoltaic quantum efficiency and conclude that the emission from t

45 ss broadband-enhanced light absorption, high quantum efficiency and desirable power conversion effici

46 ect electron detectors with higher detective quantum efficiency and fast read-out marks the beginning

47 anization that is necessary both for maximum quantum efficiency and for photoprotective dissipation o

48 the current - voltage measurements, external quantum efficiency and impedance analysis.

49 his addition of two carbon atoms doubles the quantum efficiency and improves the photon yield of the

50 ng to faster recovery of high photosystem II quantum efficiency and increased CO2 assimilation.

51 todetection, but only with very low external quantum efficiency and no spectral selectivity.

52 cells there is an empirical relation between quantum efficiency and photon energy loss that presently

53 rix demonstrate a significant enhancement in quantum efficiency and short-circuit current density, su

54 ty, molecular recognition, high fluorescence quantum efficiency and signal transduction.

55 report a dramatic enhancement of the overall quantum efficiency and spectral selectivity that enables

56 with dye regeneration, reducing the internal quantum efficiency and the electron lifetime of the DSC.

57 we examined the photocatalytic H2 generation quantum efficiency and the rates of elementary charge se

58 otoenergy to chemical energy with near unity quantum efficiency and under high light intensities by s

59 ncement of out-coupling efficiency, internal quantum efficiency, and color purity in thermally activa

60 Their emission intensity, quantum efficiency, and color quality can be systematica

61 The internal quantum efficiencies approach 100% in 3-millimeter-thick

62 in solution, however photoluminescence (PL) quantum efficiency (approximately 6%) is considerably lo

63 SrTaO2 N nanoplates, with a record apparent quantum efficiency (AQE) of 6.1 % for OER compared to th

64 Quantum efficiencies are dramatically higher than in pre

65 External quantum efficiencies are enhanced about 2.5 fold around

66 the short-circuit current (Jsc) and external quantum efficiency are even higher than reported values

67 pants displayed electroluminescence external quantum efficiencies as high as 10%.

68 terials, respectively, we show that external quantum efficiencies as high as 16% can be obtained for

69 wish green electroluminescence with external quantum efficiency as high as 4.6% (15.7 cd A(-1)).

70 trollable white color, and a down-conversion quantum efficiency as high as 82%.

71 nic light emitting diode exhibiting external quantum efficiency as high as 9.1%.

72 e, where for the best films the luminescence quantum efficiency as high as 92% was measured.

73 The photoresponse reaches up to 50% external quantum efficiency at 1000 nm and extends to 1200 nm.

74 NPB singlet manifold, yielding 2.7% external quantum efficiency at 450 nm.

75 tion-processed OLEDs with near-100% internal quantum efficiency at high brightness.

76 The quantum efficiency-bandwidth product of 105 GHz is the h

77 emit in the visible region with the greatest quantum efficiencies being 8.97 x 10(-2) (monomer) and 2

78 reatly enhance the photocurrent and external quantum efficiency by up to 1,500%.

79 we observed large variations in luminescence quantum efficiency (ca. 0-0.6), lambdamax for absorbance

80 ults suggest a two-pathway mechanism: a high quantum efficiency charge-transfer pathway to H2ase gene

81 is an ultrafast process, which occurs with a quantum efficiency close to unity.

82 ary modes, thus achieving photoisomerization quantum efficiencies comparable to those seen in visual

83 The associated internal quantum efficiency (corrected for reflection and absorpt

84 example, exhibited a loaded Q of 4,300, 25% quantum efficiency (corresponding to a responsivity of 0

85 The abrupt transition in quantum efficiency data for wavelengths above the absorp

86 The published external quantum efficiency data of the world-record CdTe solar c

87 ge selective diode fabrication, and internal quantum efficiency determinations were carried out to ob

88 s permitted highly reproducible upconversion quantum efficiency determinations while permitting the e

89 The TET quantum efficiencies determined by ultrafast transient a

90 dard method for measurement of the detective quantum efficiency (DQE) of digital radiography systems,

91 a direct correlation between their external quantum efficiencies (EQE) in organic solar cells and th

92 The soft salts yielded maximal external quantum efficiencies (EQE) ranging from 0.2% to 4.7%.

93 ty up to 0.77 A W(-1) due to a high external quantum efficiency (EQE) in exceeding 90%, which represe

94 imer-based white devices achieve an external quantum efficiency (EQE) of 24.5%, coordinates of (0.37,

95 H3 NH3 PbI3 perovskite LEDs with an external quantum efficiency (EQE) of 5.9% as a platform, it is sh

96 (EL) peak at 325 nm and achieved an external quantum efficiency (EQE) of about 0.03%, for a deep UV-L

97 External quantum efficiency (EQE) of up to 10% is achieved in a s

98 sable OLEDs with an extremely small external quantum efficiency (EQE) roll-off has been demonstrated.

99 hoto)electrochemical transients and external quantum efficiency (EQE), are extracted, and prospects f

100 d excellent efficiencies up to 16 % external quantum efficiency (EQE).

101 We achieve external quantum efficiencies (EQEs) up to 1.1%, the highest valu

102 Large enhancements of the internal quantum efficiencies (eta(int)) were measured when silve

103 D device that showed an outstanding external quantum efficiency (eta = 6.31%) with blue emission [CIE

104 000 cd/m(2) luminance, 1.6% forward external quantum efficiency (eta(ext)), and 5 V turn-on voltages

105 All three devices showed external quantum efficiencies exceeding 100% and we report a maxi

106 m-waveguide organic solar concentrators with quantum efficiencies exceeding 50% and projected power c

107 The external quantum efficiency exceeds 80%.

108 dride reduction work in opposition regarding quantum efficiencies for (1)O2 and (3)DOM* production bu

109 significantly enhanced external and internal quantum efficiencies for conversion of photons into coll

110 large TPA cross-sections coupled with modest quantum efficiencies for initiation reveal the unique po

111 al and internal photon to collected electron quantum efficiencies for the new polymers as a function

112 The experimentally determined external quantum efficiencies for these synthesized candidates we

113 he great potential of improving the internal quantum efficiency for mid- and deep-UV device applicati

114 ion of a 50-ps excitation lifetime and a 95% quantum efficiency for one of the model membranes, and d

115 (M260) mutant, which lacks Q(A), to the 100% quantum efficiency for Phi(A) along the A-branch in the

116 onstrate a marked decrease in photosynthetic quantum efficiency, from 98% to below 72%, if the unprod

117 decreased FV, yielding a large loss in PS II quantum efficiency (FV/FM).

118 al size-tunable optical resonances, external quantum efficiencies greater than unity, and current den

119 benzene solutions, extremely stable and high quantum efficiency green (Phi(UC) = 0.0313 +/- 0.0005) a

120 ) and fill factors of 62% with high external quantum efficiencies >70% across the spectral regime of

121 ganic light-emitting diodes exhibit external quantum efficiency >45% at 10,000 cd m(-2) with colour r

122 ganic light-emitting diodes exhibit external quantum efficiency >60%, while phosphorescent white orga

123 Highly enhanced emission quantum efficiency (>1%) in plasmonic silicon, along wit

124 larify the necessary means to achieve device quantum efficiency higher than the state-of-the-art GaN:

125 h organic photovoltaic cells would have poor quantum efficiencies if every encounter led to recombina

126 substituents have the highest photochemical quantum efficiencies in the presence of an alkene trap,

127 ilicon devices, exhibiting voltage-dependent quantum efficiencies in the range of a few 10 s of %, fe

128 Well defined cut-offs and high quantum efficiency in each channel are achieved.

129 The diffusion length determines PSII's high quantum efficiency in ideal conditions, as well as how i

130 ndent studies further show that the internal quantum efficiency in one-layer MoS2 can reach a maximum

131 the field of view and increase the effective quantum efficiency in single-molecule switching nanoscop

132 nce (lambda(PL) = 490-556 nm) with a high PL quantum efficiency in solution (Phi = 5 to 90%).

133 y toward methane C-H bond activation and the quantum efficiency increased linearly as a function of l

134 transfer processes display a remarkably high quantum efficiency, indicating a near-complete inhibitio

135 lar spectrum LSCs suffer from moderately low quantum efficiency, intrinsically small absorption cross

136 been tested by conversion efficiency (J-V), quantum efficiency (IPCE), electrochemical impedance spe

137 alysis of limiting factors for high internal quantum efficiencies (IQE) are accomplished through the

138 d that, contrary to intuition, high internal quantum efficiency (IQE) can be obtained in polymer/full

139 lar spectrum, but nevertheless, the internal quantum efficiency (IQE) has not been reported to be hig

140 blends, our study reveals that the internal quantum efficiency (IQE) is essentially independent of w

141 The internal quantum efficiency (IQE) of an electrically-driven GaN:E

142 As such, the internal quantum efficiency (IQE) of the solar cell may likewise

143 High internal quantum efficiencies (IQEs) are estimated for photoelect

144 The corresponding internal quantum efficiency is (160 +/- 10)%.

145 High quantum efficiency is achieved for some of these compoun

146 oactivated charge separation with near unity quantum efficiency is not fundamentally understood.

147 A sharp increase in phosphorescence quantum efficiency is observed in a variety of polymer m

148 der of magnitude enhancement of the external quantum efficiency is observed without reduction in the

149 The quantum efficiency is temperature-independent from 298 t

150 The improved understanding of the quantum efficiency issue through current injection effic

151 om lasers provide new possibilities for high quantum efficiency lasing that could potentially be wide

152 The total internal quantum efficiency loss due to geminate recombination is

153 in H2O (lambdairr = 400 nm), but with a low quantum efficiency (<1%).

154 inates of (0.15, 0.17) with maximum external quantum efficiency (max.

155 easurements correlate well with the external quantum efficiencies measured for a series of polymer ph

156 We report the highest external quantum efficiency measured on hematite (alpha-Fe(2)O(3)

157 exhibit distinct photoluminescence (PL) with quantum efficiency measured up to 42%.

158 Furthermore, external quantum efficiency measurements of the charge-transfer s

159 External quantum efficiency measurements show that PDPPTe2T produ

160 tance spectroscopies, combined with external quantum efficiency measurements, provided structure-prop

161 lymer absorption, as verified using external quantum efficiency measurements.

162 e tunable molecular sensitizers, and exhibit quantum efficiencies near unity.

163 m upon excitations at 449 nm and 980 nm with quantum efficiencies of 6.3% and 1.1%, respectively.

164 123 mA cm(-2), giving external and internal quantum efficiencies of 0.1% and 0.4%, respectively.

165 A cm(-2), with highest external and internal quantum efficiencies of 0.76% and 3.4%, respectively.

166 High luminescence quantum efficiencies of 20-30% for near-infrared emittin

167 EBL-based OLEDs achieve current and external quantum efficiencies of 52 cd A(-1) and 14.3%, a ca. 50%

168 EBL-based OLEDs achieve current and external quantum efficiencies of 52 cd A-1 and 14.3%, a ca. 50% p

169 itons and biexcitons by 109 and 100 folds at quantum efficiencies of 60 and 70%, respectively, in ver

170 white-light emissions with photoluminescence quantum efficiencies of approximately 20% for the bulk s

171 y utilized photosensitizers and had relative quantum efficiencies of hydrogen production up to 37 tim

172 was observed to be most effective, yielding quantum efficiencies of initiation of >5%.

173 er/PCBM (1:4 by weight) devices and external quantum efficiencies of more than 10% have been observed

174 Thus, the internal quantum efficiencies of the devices approach 100% in the

175 Hence, the quantum efficiencies of the perovskite light-emitting di

176 The ECL quantum efficiencies of the series, compared to that of

177 coated emissive layers exhibit high external quantum efficiencies of up to 15%.

178 a single-junction device shows high external quantum efficiency of >60% and spectral response that ex

179 Changes in the quantum efficiency of (1)O(2) production upon dilution o

180 cal trapping scheme, we show a peak external quantum efficiency of (109 +/- 1)% at wavelength lambda

181 This compound was photolyzed with a quantum efficiency of 0.09 at pH 7.4.

182 s, Nb-VNA and Nv-VNA, are photoreleased with quantum efficiency of 0.13 and 0.041, respectively.

183 s O(2)(a(1)Delta(g)) with the uniquely large quantum efficiency of 0.25 +/- 0.03.

184 m radiant flux of 1.7 W m(-2) at an external quantum efficiency of 0.44%.

185 toward an unprecedentedly high fluorescence quantum efficiency of 0.60 in hexane.

186 ronic ground state but was photolyzed with a quantum efficiency of 0.78.

187 A high quantum efficiency of 1.4% was recorded for the noble- a

188 eeding 100% and we report a maximum external quantum efficiency of 122% for cells consisting of the s

189 nover frequency of 76 h(-1), and an external quantum efficiency of 15% (lambda = 360 +/- 10 nm).

190 000 cd m(-2) , while maintaining an external quantum efficiency of 15.3% at such high brightness, dem

191 n the emissive layer gave a maximum external quantum efficiency of 16.1%, demonstrating that triplet

192 efficiency of 61.6 cd A(-1) and an external quantum efficiency of 17.8%, which are the highest effic

193 ngly to optical irradiation with an external quantum efficiency of 25% and fast photoresponse <15 mus

194 om cut-off wavelength at 77 K and exhibits a quantum efficiency of 31% for a 2 microm-thick absorptio

195 emitter can reach an extremely high external quantum efficiency of 31.9% with a pure blue emission.

196 A quantum efficiency of 4.2% is obtained (pH = 7.5).

197 urrent density of 7.78 mA/cm(2) and external quantum efficiency of 47% are also the best such photovo

198 ably long lifetime of 0.28 s and a very high quantum efficiency of 5 % was thus obtained under ambien

199 hows a strong photoresponse with an external quantum efficiency of 52.7% and a response time of 66 ms

200 external gate to achieve a maximum external quantum efficiency of 55% and internal quantum efficienc

201 of cyclic alkanes gave an excellent apparent quantum efficiency of 6.0% under visible light illuminat

202 rrent density of 10.5 mA cm(-2) and external quantum efficiency of 61.3% are also the best reported i

203 inant from 15 to 300 K, with a high internal quantum efficiency of 62% even at room temperature.

204 An external quantum efficiency of 67% and fill-factor of 65% are ach

205 on-optimized NYS:0.10Sm(3+) exhibited a high quantum efficiency of 73.2%, and its luminescence intens

206 ier with weak measurements, obtaining a high quantum efficiency of 75% (70% including noise added by

207 measured decay time of 3 ms and an estimated quantum efficiency of 78%, which is comparable to Er dop

208 mpere per watt (corresponding to an external quantum efficiency of above 30%).

209 trochemical water splitting with an internal quantum efficiency of approximately 2.3% using blue ligh

210 ed strong and persistent RTP emission with a quantum efficiency of approximately 20 % and a lifetime

211 resence of 2,3-dimethyl-1,3-butadiene with a quantum efficiency of approximately 38%.

212 otenoid is transferred to the retinal with a quantum efficiency of approximately 40%.

213 intensity, which indicates a high radiative quantum efficiency of approximately 50%.

214 th a large Stokes shift of 332 nm and a high quantum efficiency of around 46 %.

215 l rates up to 0.96 mumol min(-1), and with a quantum efficiency of at least 0.19% (measured at 530 nm

216 t is converted to the 362 nm species, with a quantum efficiency of ca. 0.2.

217 d rate of photosynthesis, and higher maximum quantum efficiency of CO(2) assimilation.

218 his work, we redetermine the chemiexcitation quantum efficiency of dimethyl-1,2-dioxetanone, a more a

219 the overall photochemical reactivity, as the quantum efficiency of ET defines the upper limit on the

220 n CdS NRs by directly measuring the rate and quantum efficiency of ET from photoexcited CdS NRs to Ca

221 , with values of 10(7) s(-1), resulting in a quantum efficiency of ET of 42% for complexes with the a

222 CuPC domains, combine to reduce the internal quantum efficiency of free polaron formation in the bulk

223 r the previously unexplained decrease in the quantum efficiency of isoprene emission with increasing

224 crucial for understanding limitations on the quantum efficiency of larger CP materials.

225 nd inexpensive way to determine the absolute quantum efficiency of nano phosphors, normally a difficu

226 r first devices already exhibit an extrinsic quantum efficiency of nearly 10% and the emission can be

227 ng [Co4(H2O)2(PW9O34)2](10-) (1-P2), and the quantum efficiency of O2 formation at 6.0 muM 1-V2 reach

228 hotovoltaic devices has achieved an external quantum efficiency of over 100% and demonstrated signifi

229 On the other hand, D1-D170E lowers the quantum efficiency of photoactivation compared to the wi

230 The low quantum efficiency of photoactivation in D1-D170E is due

231 We report the quantum efficiency of photoluminescence processes of Er

232 less energy-efficient pathways, lowering the quantum efficiency of photosynthesis.

233 revealed a transient COR-induced decrease in quantum efficiency of photosystem II at dawn of the day

234 cence images showed dramatic declines in the quantum efficiency of photosystem II electron transport

235 ultures of O. tauri in parallel with maximum quantum efficiency of photosystem II photochemistry (Fv

236 ) s(-1)), as shown by the decline in maximum quantum efficiency of photosystem II photochemistry.

237 genes but was not associated with a reduced quantum efficiency of photosystem II.

238 n substantial and significant impacts on the quantum efficiency of PSI and PSII, electron transport,

239 ansport and oxygen evolution rates and lower quantum efficiency of PSII compared with the wild type,

240 stem II (PSII), indicated by reduced maximum quantum efficiency of PSII, and severe photobleaching.

241 The quantum efficiency of quantum dots is as high as 95%.

242 S-CdS quantum dots enhance the peak external quantum efficiency of shortwave-infrared light-emitting

243 ecombination is consistent with the internal quantum efficiency of the corresponding solar cell.

244 Total photoluminescence quantum efficiency of the dual emitting bands reached as

245 The quantum efficiency of the PICTT process was high (>24%),

246 The quantum efficiency of this photoconversion is similar to

247 The quantum efficiency of this system for photosynthetic ace

248 etane decomposition as well as with the high quantum efficiency of this transformation.

249 state has already been shown to enhance the quantum efficiency of transfer in theoretical models of

250 um brightness of 133 cd/m(2) and an external quantum efficiency of up to 0.07% in ambient air.

251 of approximately 6 V and a maximum external quantum efficiency of up to 1.2%, suggesting their poten

252 Finally, with a PL quantum efficiency of up to 36% and an enhanced PL stabi

253 ibit a detectivitiy>10(9) Jones, an external quantum efficiency of ~100%, a linear dynamic range of 8

254 semiconductor photocatalysts, photocatalytic quantum efficiencies on plasmonic metallic nanostructure

255 External quantum efficiencies over 20% are achieved and stable de

256 lectrodes can significantly mitigate the low-quantum efficiency performance of photoconductive terahe

257 2) assimilation rates, photosystem II (PSII) quantum efficiencies (PhiPSII), and reduction levels of

258 ia quinone methides (QMs), with methanolysis quantum efficiencies PhiR = 0.02-0.3.

259 before radiating with >11% photoluminescence quantum efficiency (PLQE) at low temperatures.

260 f H(2) was also a function of the nc-CdTe PL quantum efficiency (PLQE), with higher-PLQE nanocrystals

261 ght emitters with improved photoluminescence quantum efficiencies (PLQEs).

262 utilizing the solar resource at the maximum quantum efficiency possible in living cells.

263 O/CH3 NH3 PbBr3 /Au, with near 100% internal quantum efficiency, promising power conversion efficienc

264 The quantum efficiencies (Q(u)) of the amino and sulfhydryl

265 tomic level, with 2-10% Eu2+ giving the peak quantum efficiency (QE = 0.32).

266 rit of specific device characteristics, e.g. quantum efficiency (QE) in grating-based metallic photoc

267 e showed that the steady-state H2 generation quantum efficiencies (QEs) depended sensitively on the e

268 rcuit voltage of 0.7 V, and a broad external quantum efficiency ranging from 350 to 920 nm with a max

269 ation and result in the highest out of batch quantum efficiency reported to date of 15% prior to chem

270 t implied in reported conventional detective quantum efficiency results from the same systems.

271 that maser photons were produced with Carnot quantum efficiency (see Fig. 1A).

272 To increase the multiexcitonic quantum efficiency, several groups have explored plasmon

273 By comparing the external quantum efficiency spectra of the polymer solar cells fa

274 was investigated by J-V curves and external quantum efficiency spectra.

275 The external quantum efficiency spectrum of PSEHTT:DBFI-T devices had

276 olecule fluorescence from emitters with high quantum efficiencies such as organic dye molecules can e

277 Determination of the quantum efficiencies suggests distinct differences in th

278 results indicate that this strategy promotes quantum efficiency, temporal resolution, and fidelity of

279 broad, red-shifted emission, and have lower quantum efficiencies than their facial counterparts.

280 ester produces singlet carbene with greater quantum efficiency than the ketone analogue due to compe

281 ing a palette of chemical dyes with improved quantum efficiencies that spans the UV and visible range

282 ns to create a charge-separated state with a quantum efficiency that approaches 1.0.

283 ed solar cells, as manifested by an external quantum efficiency (the spectrally resolved ratio of col

284 rating point based on the PV cell's external quantum efficiency, the skin's transmission spectrum, an

285 have the potential for 100 per cent internal quantum efficiency: the phosphorescent molecules harness

286 We estimate internal quantum efficiencies to exceed 150% at relatively low en

287 The quantum efficiency to Q(B) via the B-branch Phi(B) range

288 0.71 ms (Er/Hg) and with the Er/Cd radiative quantum efficiency twice that of the Er/Hg compound.

289 negligible hysteresis and up to 80% external quantum efficiency under select monochromatic excitation

290 ocurrent from triplets, and achieve external quantum efficiencies up to 80%, and power conversion eff

291 ight photocatalytic activity and an apparent quantum efficiency up to 12.77%, which is 50 times highe

292 umental for sustained O(2) productivity with quantum efficiency up to 80% at lambda > 400 nm, thus op

293 ernal quantum efficiency of 55% and internal quantum efficiency up to 85%.

294 e copper doping into CQWs enables near-unity quantum efficiencies (up to approximately 97%), accompan

295 al relationship of BRET efficiency and donor quantum efficiency, we report generation of a novel BRET

296 The devices combine high (78-83%) external quantum efficiency with high (0.91-0.95 V) photovoltages

297 fully controllable synthesis as well as high quantum efficiency with improved thermal stability, make

298 y (~100-200 ms) refractory, thereby reducing quantum efficiency with increasing intensity.

299 is emitter achieves (31.1 +/- 0.1)% external quantum efficiency without any out-coupling, which shows

300 of green FP (bfloGFPa1) with perfect (100%) quantum efficiency yielding to unprecedentedly-high brig