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 ion layers exhibiting high photoluminescence quantum efficiency.

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

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

5 neous long lifetime and high phosphorescence quantum efficiency.

6 h released thymidine exclusively with higher quantum efficiency.

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

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

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

10 recently broken the 20% barrier for external quantum efficiency.

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

12 l thermal disturbance and the photodetection quantum efficiency.

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

14 examples nevertheless demonstrate near-unity quantum efficiency.

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

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

17 ding to simultaneously high color purity and quantum efficiency.

18 ts core antenna while achieving near perfect quantum efficiency.

19 r results in photocatalysts exhibiting a low quantum efficiency.

20 een emitting ZnO with significantly enhanced quantum efficiency.

21 environmental compatibility, and near-unity quantum efficiencies.

22 in photosynthesis are rapid events with high quantum efficiencies.

23 oalgal growth and outstanding photosynthetic quantum efficiencies.

24 ibit tunable emissions, as well as excellent quantum efficiencies.

25 erovskite single crystals with high external quantum efficiency (200%), ultralow dark current (10(-12

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

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

28 High quantum efficiencies (71 % and 55 % under 410 and 450 nm

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

30 Finally, in spite of a lower quantum efficiency, a blue fluorescent organic light-emi

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 t materials can well maintain their superior quantum efficiency after heating at a temperature over 1

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

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

36 brication into OLEDs/LECs with high external quantum efficiencies and stabilities.

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 nction of layer thickness, photoluminescence quantum efficiency and absorption coefficient of the org

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

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

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

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

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

48 ies that are deemed necessary to attain high quantum efficiency and high solar-to-hydrogen (STH) conv

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

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

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

52 y used extensively to calculate the internal quantum efficiency and its droop in the III-nitride LED.

53 ayer exhibit an improvement in both internal quantum efficiency and light output, which is similar to

54 hat can simultaneously achieve high external quantum efficiency and low voltage loss for OSC.

55 served changes in measured infrared external quantum efficiency and relative luminescence intensity i

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

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 ous ultralong lifetime, high phosphorescence quantum efficiency, and excellent stability.

61 ith ultralong lifetime, high phosphorescence quantum efficiency, and high stability for promising app

62 gy into electrical energy with close to 100% quantum efficiency, and there is increasing interest in

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

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

65 At 800 K, the spontaneous emission quantum efficiencies are around 40% for blue for lightin

66 Quantum efficiencies are dramatically higher than in pre

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

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

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

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

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

72 ht and demonstrate up to a 2000% increase in quantum efficiency as the power of the light is varied f

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 logy up to 2000 nm, given that high external quantum efficiencies can be maintained at these low phot

78 of the donor- and acceptor-material internal quantum efficiencies cancels this quantity.

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

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

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

82 te exhibits a ca. 16-fold enhancement in the quantum efficiency compared with the reported BiVO(4) na

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

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

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

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

87 The TET quantum efficiencies determined by ultrafast transient a

88 h 2D photovoltaic devices are limited by low quantum efficiencies due to the severe interface recombi

89 s a green emissive dopant have high external quantum efficiencies (EQE = 19.4%) and brightness of 54

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

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

92 green-emitting devices with a peak external quantum efficiency (EQE) of 14% at 1000 cd m(-2); their

93 iance of 2555 W sr(-1) m(-2) , peak external quantum efficiency (EQE) of 17%, considerably reduced EQ

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

95 ion-processed OLEDs achieves a high external quantum efficiency (EQE) of 30.8% with a very flat effic

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

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

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

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

100 as the emitter has achieved a high external quantum efficiency (EQE) up to 11.6%, far exceeding the

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

102 enges that limit the improvement of external quantum efficiency (EQE), making the search of alternati

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

104 Maximum external quantum efficiencies (EQEs) of 17.6% for Cs(0.2) FA(0.8)

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

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

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

108 The external quantum efficiency exceeds 80%.

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

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

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

112 erovskites, which enhances photoluminescence quantum efficiency from 1.1% to 19.8%.

113 e with a decrease in the photon upconversion quantum efficiency from 11.6% to 4.51% to 0.284%, as exp

114 eveal a significant leap in light-perception quantum efficiency from 35% to 73%.

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

116 diative recombination rates and luminescence quantum efficiencies >15% with high carrier mobilities e

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

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

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

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

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

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

123 ght emitting diode leads to a 72.5% external quantum efficiency improvement compared with the one wid

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

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

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

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

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

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

130 ming a major hurdle of low photoluminescence quantum efficiency in wide-bandgap perovskites.

131 4 and 5 phenylene units, photon upconversion quantum efficiencies increase again to 0.468% and 0.413%

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

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

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

135 This multistep process proceeds with low quantum efficiency, involves a molecular rearrangement b

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

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

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

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

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

143 he convention where the maximum upconversion quantum efficiency is 100%).

144 High quantum efficiency is achieved for some of these compoun

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

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

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

148 The extracted external quantum efficiency is ~0.1% and is comparable to recent

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

150 ncluding higher reliability and fluorescence quantum efficiency, larger diversity of subcellular targ

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

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

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

154 rs: 274 vs 17 mT) with high and low external quantum efficiency maximum, EQE(max) (21.05% vs 4.89%),

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

156 External quantum efficiency measurements show that PDPPTe2T produ

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

158 ency, electrochemical impedance and external quantum efficiency measurements.

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

160 123 mA cm(-2), giving external and internal quantum efficiencies of 0.1% and 0.4%, respectively.

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

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

163 cur on a time scale of less than 100 fs with quantum efficiencies of 50 +/- 18% and 15 +/- 5%, respec

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

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

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

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

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

169 The quantum efficiencies of developed samples range from aro

170 Quantum efficiencies of organic-inorganic hybrid lead ha

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

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

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

174 mission from highly localized excitons, with quantum efficiencies of up to 75%, is observed in blue t

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

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

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

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

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

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

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

182 f 32.0 cd A(-1) corresponding to an external quantum efficiency of 10.5%.

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

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

185 000 cd m(-2) , while maintaining an external quantum efficiency of 15.3% at such high brightness, dem

186 ites, leading to PeLEDs with a peak external quantum efficiency of 17.3% and half-lifetime of approxi

187 We report blue devices with a peak external quantum efficiency of 17.3% in a host-free emitting laye

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

189 ly 100% selectivity to methanol and internal quantum efficiency of 2.1% in the visible region, furthe

190 ission peak of 456 nm and a maximum external quantum efficiency of 22.8% is achieved.

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

192 ltralong lifetime of 5.72 s, phosphorescence quantum efficiency of 26.36%, and exceptional stability

193 trix-protected CQDs show a photoluminescence quantum efficiency of 30 per cent for a CQD solid emitti

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 e simultaneously realizes a maximum external quantum efficiency of 32.5%, CIE(y) ~ 0.12, a full width

197 rrent density of 1.8 x 10(-10) A/cm(2) and a quantum efficiency of 40%, resulting in a detectivity of

198 y of 0.6 A/W at ~1.7 mum, corresponding to a quantum efficiency of 43% at zero bias under front-side

199 ield of photorelease of 3.8%, and an overall quantum efficiency of 4650 M(-1) cm(-1) at 680 nm.

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

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

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

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

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

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

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

207 Especially, a high external quantum efficiency of 71%, a record high power conversio

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

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

210 ited polaron pairs which has a markedly high quantum efficiency of about 97%.

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

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

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 fect white emission with a photoluminescence quantum efficiency of around 73 %.

216 the 50% indium composite having an external quantum efficiency of around 8%.

217 ts are possible as regards (a) the detective quantum efficiency of cameras at high resolution, (b) co

218 en-circuit voltage of 1.33 V and an external quantum efficiency of electroluminescence of 10(-4).

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 In an effort to improve the emission quantum efficiency of nanoscale 2D layered tin iodide pe

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

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

229 nversion efficiency of 22.7% and an external quantum efficiency of over 10% have been achieved for pe

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

231 The relatively low overall quantum efficiency of photoactivation is explained by th

232 , where the goal is to maximize the external quantum efficiency of photoelectric conversion.

233 We report the quantum efficiency of photoluminescence processes of Er

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

235 T78S mutation had reduced photosynthesis and quantum efficiency of photosystem II ( (PSII)) and reduc

236 The maximum quantum efficiency of photosystem II (F(v)/F(m)) was dec

237 we investigated the response of the maximum quantum efficiency of photosystem II (PSII) to rapidly i

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

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

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

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

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

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

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

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

246 ative efficiency, with the photoluminescence quantum efficiency of the film under solar excitation de

247 The dimerization constant of MB and the quantum efficiency of the monomer was determined.

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

249 The quantum efficiency of this photoconversion is similar to

250 The quantum efficiency of this system for photosynthetic ace

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

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

253 on peaked at 517 nm with a photoluminescence quantum efficiency of ~ 95%.

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

255 fficiency of ~102.0 cd A(-1) and an external quantum efficiency of ~28.5% ph/el, which agree well wit

256 The AlInN nanowires exhibit a high internal quantum efficiency of ~52% at room temperature for emiss

257 rvable EL is achieved with the high external quantum efficiency of ~6% at room temperature due to eff

258 semiconductor photocatalysts, photocatalytic quantum efficiencies on plasmonic metallic nanostructure

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

260 h intercalated graphene layers have superior quantum efficiency over single-bottom graphene/QD device

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

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

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

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

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

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

267 ities, a narrow range of absorption and poor quantum efficiencies (Q.E.) due to fast recombination of

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

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

270 The spontaneous emission quantum efficiency (QE) of blue, green, and red LED mate

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

272 unction organic solar cells with an external quantum efficiency reaching up to 44% and an open-circui

273 m the QDs was optimized to match the highest quantum efficiency region of the SiPMs.

274 o compensate for differences in the relative quantum efficiency (RQE) of each pixel.

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

276 in energy than the CT states in the external quantum efficiency spectra of a significant number of or

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

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

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

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

281 plast envelope, the C4 pathway having higher quantum efficiency than C3 for permeabilities below 300

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

283 This derivative has a quantum efficiency that is 50-fold higher than the best

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

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

286 e mixture further enhances photoluminescence quantum efficiency to 49.7%.

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

288 The compounds exhibit photoluminescent quantum efficiencies up to 100% in fluid solution and po

289 hibit tunable emissions as well as excellent quantum efficiency up to 0.96.

290 a thin film in prototype OLEDs with external quantum efficiency up to 11% and a narrow emission bandw

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

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

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

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

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

296 ing ratio [Phi(F)(3(+))/Phi(F)(3)] of 7.5 in quantum efficiency with oxidation state.

297 ibit significantly higher responsivities and quantum efficiencies, with similar dark currents, hence

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

299 nthesis achieves near unity light-harvesting quantum efficiency yet it remains unknown whether there

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