ライフサイエンスコーパス: quantum yield

1 fects, causing an 80-fold enhancement of the quantum yield.

2 erved while retaining high photoluminescence quantum yield.

3 lar luminescence without suffering losses in quantum yield.

4 e(N)Cl(2) in 47% spectroscopic yield and 11% quantum yield.

5 sion rate, far-field emission intensity, and quantum yield.

6 old increase in its off-to-on photoswitching quantum yield.

7 t in the presence of changes in fluorescence quantum yield.

8 a momentary downregulation of photosynthetic quantum yield.

9 ents, wide effective Stokes shifts, and high quantum yields.

10 f-states collectively control photoswitching quantum yields.

11 ith the experimentally measured fluorescence quantum yields.

12 time for samples with high photoluminescence quantum yields.

13 lution for the determination of luminescence quantum yields.

14 g the temperature dependence of fluorescence quantum yields.

15 ganic solvents demonstrate high fluorescence quantum yields.

16 ovalent bonds and near-unity phosphorescence quantum yields.

17 06-707 nm), but also the lowest fluorescence quantum yields.

18 ut are also known to suffer from low optical quantum yields.

19 se complexes are yellow emitters with modest quantum yields.

20 s; yet, their inefficient photoluminescence (quantum yield ~1%) drives requirements for sizeable exci

21 These complexes had lower quantum yields (10% and non-emissive, respectively) due

22 esults, including unprecedented fluorescence quantum yields (2.3-9.6 %) from the S(2) states in the n

23 ls emit multicolor and white light with high quantum yields (~2-14%), high color-rendering indices (>

24 maximum at 530 nm with low chemiluminescent quantum yield [(2.1 +/- 0.1) x 10(-7) E mol(-1)].

25 e FAD(*-)/Y(373)(*) pair is formed with high quantum yield (~60%); its intrinsic decay by recombinati

26 long fluorescence lifetimes (17-20 ns), high quantum yields (~60%), and high photostabilities.

27 or all compounds, we observed a very high PL quantum yield (79-89%) and formation of stable radical i

28 Their high photoluminescence quantum yields along with the small DeltaE(ST) suggest t

29 es were found to possess the highest (1)O(2) quantum yields, an interesting result given that these f

30 65 acceptors, shows efficient FRET with >20% quantum yield and a signal amplification (antenna effect

31 ned reactivity at a ~15-fold increase in the quantum yield and a ~3-fold increase in the faradaic yie

32 opper, aluminum, zinc, and sulfur with ~20 % quantum yield and an attractive PL maximum of 450 nm.

33 flow are autonomously synthesized, and their quantum yield and composition polydispersity at target b

34 di-tert-butyl-4-methyl-pyridine enhances the quantum yield and efficiency of the cross-coupling react

35 ity, tunable bandgap, high photoluminescence quantum yield and facile chemical synthesis.

36 complexes, particularly the phosphorescence quantum yield and lifetime.

37 reveal the scaling laws of photoluminescence quantum yield and radiative lifetime with respect to the

38 In this study, we improved the quantum yield and sensitivity of the photoactivation exp

39 orption coefficient than the apparent/innate quantum yield and the lower photosensitivity was mainly

40 we found that both chlorophyll fluorescence quantum yields and fluorescence lifetimes clearly indica

41 ed strongly fluorescent properties with high quantum yields and MegaStokes shifts.

42 rganic glass monoliths provided fluorescence quantum yields and radiation detection properties exceed

43 azines (MgPzs) having similar singlet oxygen quantum yields and side groups with different electron-w

44 tes that exhibit 97 +/- 3% photoluminescence quantum yields and stabilities that exceed 300 h upon co

45 n and lower singlet oxygen and triplet-state quantum yields and steady state concentrations.

46 metallacycles that exhibit high fluorescence quantum yields and tunable fluorescence wavelengths thro

47 nstruct discrete SCCs with high fluorescence quantum yields and tunable fluorescence wavelengths.

48 cture, a 1.6-fold enhanced photoluminescence quantum yield, and a longer emission lifetime than the s

49 ysis of the absorption (color), fluorescence quantum yield, and energy barriers to ground- and excite

50 the visible region, fluorescence with a high quantum yield, and excellent photostability.

51 sensor with high extinction coefficient, low quantum yield, and high photobleaching resistance.

52 e of their narrow emission bands, near-unity quantum yield, and low fabrication cost, metal halide pe

53 the NIR region with large Stokes shift, high quantum yield, and strong solvatochromism.

54 of deep trap states, high photoluminescence quantum yield, and wide color tunability.

55 s, by determining fluoride production rates, quantum yields, and half-lives, and found that strong el

56 he large Stokes shifts, tuneable fluorescent quantum yields, and high photostability reveal promise i

57 d by changes in spectral profiles, increased quantum yields, and lifetime dynamics expected for excit

58 Each presents high brightness, quantum yields, and lifetimes.

59 NO(2) groups improved the photoisomerization quantum yields, and the extremely long thermal half-live

60 esized phenalenones exhibit low fluorescence quantum yields, and the fluorescence decay was studied i

61 photophysical properties (conversion rates, quantum yields, and thermal half-lives) are largely reta

62 idth at half-maximum (fwhm), relatively high quantum yields, and utility in immunofluorescence staini

63 le-range absorption, near-unity fluorescence quantum yields, and, to our knowledge, the most facile e

64 Furthermore, the quantum yield approaches that of commercial silicon phot

65 /g-C3 N4 PHJ, achieving an enhanced apparent quantum yield (AQY) of 27% at 440 nm over PCzF/g-C3 N4 .

66 culty of determining photobleaching apparent quantum yields (AQYs) that capture the dual spectral dep

67 fficiency of (3)DOM* formation (the apparent quantum yield, AQYT).

68 Fluorescence quantum yields are as high as 0.93 in nonpolar solvents,

69 Moreover, release quantum yields are dramatically improved by boron alkyla

70 In general, the observed emission quantum yields are high in nonpolar media (Phi(F) ca. 0.

71 emission wavelengths are red-shifted and the quantum yields are higher.

72 We show that quantum yields are highly affected by light gradients an

73 In contrast, (*)OH quantum yields are lowest downstream and correlate with

74 The RQD ORF cross-sections and quantum yields are significantly higher than their respe

75 ese materials demonstrated photoluminescence quantum yields as high as 0.89 in toluene, with emission

76 Very high quantum yields (as much as 58%) have been observed with

77 formation rates, but negatively with triplet quantum yields, as waters enriched in highly aromatic fo

78 trong photophysical profile including a 0.92 quantum yield ascribed to intramolecular charge transfer

79 The abrupt increase in photoluminescence quantum yield at excitation energy above twice band gap

80 nd fabrication techniques to increase the UC quantum yield at low excitation intensity.

81 increased retention of dark-adapted maximum quantum yields at higher temperatures.

82 etic pathways tested improved photosynthetic quantum yield by 20%.

83 vskite films with improved photoluminescence quantum yield by introducing trifluoroacetate anions to

84 effects explains the increase in the (1)O(2) quantum yield by one order of magnitude upon exposure to

85 a and are characterized by high fluorescence quantum yields (ca. 0.5-0.7) and brightness (ca. 35000-4

86 well as by isotopic labeling experiments and quantum yield calculations to evaluate the effect of lig

87 The differences in quantum yields can be explained by a twist in the chromo

88 erature (from 20 to 25 degrees C), where the quantum yield changes by -0.45% per Celsius degree.

89 (3)DOM quantum yield coefficients and (1)O(2) quantum yields in

90 The high chemical and quantum yields combined with the outstanding absorption

91 b720, with red-shifted spectra and increased quantum yield compared to iRFP.

92 et DOM ((3)DOM) and singlet oxygen ((1)O(2)) quantum yields, contradictory evidence exists for hydrox

93 rameters of the probe such as photobleaching quantum yield, count rate per molecule, and intensity of

94 mperature in acetonitrile with 1.8 x 10(-4)% quantum yield (ddpd = N,N'-dimethyl-N,N'-dipyridine-2-yl

95 on single particle brightness, upconversion quantum yield, decay lifetimes, and FRET coupling.

96 h eliminates a number of potential errors in quantum yield determination protocol and provides higher

97 n be avoided using a method for fluorescence quantum yield determination that relies on simultaneous

98 When the quantum yield deviates from unity by significantly less

99 ergy, self-assembled quantum wells, and high quantum yield draw attention for optoelectronic device a

100 Such molecules have been devised as high quantum yield emitters in modern organic light-emitting

101 ion results in an up to 10-fold fluorescence quantum yield enhancement.

102 peak emission wavelengths near 900 nm and a quantum yield exceeding 16% for 4,6-bis(2-thienyl)thieno

103 ations to cause decrease in the fluorescence quantum yield for a system with higher helicity.

104 ude water solubility, biocompatibility, high quantum yield for catalyst release, and responsiveness t

105 equilibrium constant of each complex and the quantum yield for each photochemical process.

106 a rationale for this apparent depletion; the quantum yield for forming SH(X) products, Gamma, decreas

107 The observed quantum yield for free chlorine loss actually decreased

108 e chains exhibits a record photoluminescence quantum yield for hybrid lead halides.

109 The quantum yield for photochemical conversion of 3 is ~0.03

110 large temperature dependence of fluorescence quantum yield for quinine in 0.05 M sulfuric acid.

111 ction of hydrogen from water with an overall quantum yield for solar energy conversion to hydrogen ga

112 pH and temperatures, maintaining their high quantum yields for > 110 days immersing in water.

113 attached BV showed the highest fluorescence quantum yield (FQY) of 16.6% reported for NIR FPs, where

114 While, WPI reduced its photodegradation quantum yield from 0.03 to 0.012 compared to 0.017 obtai

115 e primary driver for the 10-fold increase in quantum yield from 4.2% to 40%.

116 Singlet oxygen ((1)O(2)) generation quantum yields from chromophoric dissolved organic matte

117 n recruitment kinetics to GPCRs using a high quantum yield, genetically encoded fluorescent biosensor

118 while maintaining the high photoluminescence quantum yields (>50%), sharp absorption features, and na

119 tendency to keep increasing, as fluorescence quantum yield has a relatively muted sensitivity to ligh

120 l effect on the Nile red sensor fluorescence quantum yields, hereby defining the sensing detection li

121 n, easily observable even by naked eye, with quantum yield higher than the standard 9,10-diphenylanth

122 shows very strong blue fluorescence with 2% quantum yield in acetonitrile at room temperature.

123 The high, relatively sequence-independent quantum yield in duplexes makes 2CNqA promising as a nuc

124 Moreover, the 2CNqA fluorophore has a quantum yield in single-stranded and duplex DNA ranging

125 ) at resonance, as well as photoluminescence quantum yield in the range of 60-100%.

126 olymers, the VIR-QD spectral series has high quantum yield in the SWIR (14-33%), compact size (13 nm

127 The quantum yield in water is 500 times greater than that of

128 cular charge transfer, moderate fluorescence quantum yields in both solutions and thin films, and ext

129 aintaining similar fluorescence profiles and quantum yields in both states.

130 nzofuran and pyrene derivatives display high quantum yields in non-aqueous solvents and solvatochromi

131 monstrate how measured distributions of PSII quantum yields in plant tissue change under natural tiss

132 possess partially high relative fluorescence quantum yields in solution and fluoresce strongly in the

133 phospholes display quantitative luminescence quantum yields in solution and reversible reduction feat

134 is required to have reasonable fluorescence quantum yields in solution and that rigidification enhan

135 te-strength aqueous aerosol, with comparable quantum yields in solution and viscous films (10(-5)-10(

136 Although the molecules displayed low quantum yields in solution, higher quantum yields were o

137 able via the shell thickness with associated quantum yields in the 4.4-16.0% range.

138 with ca. 2700-8400 cm(-1) Stokes shifts and quantum yields in the 65-74% range in water and in the 4

139 3)DOM quantum yield coefficients and (1)O(2) quantum yields increase downstream and correlate strongl

140 As in DNA, we find a high quantum yield inside RNA duplexes (<PhiF> = 0.22) that i

141 Disappointingly, the phosphorescence quantum yield invariably turned out to be very low, abou

142 Photothermal threshold quantum yield is based on the quantization of light to m

143 respect to [8]cycloparaphenylene 1, and its quantum yield is higher; (ii) in the presence of an octa

144 mission at 1100-1350 nm and the fluorescence quantum yield is significantly increased by metal-atom d

145 on cross-sections and high photoluminescence quantum yields, lead halide perovskite quantum dots (PQD

146 reased below 22.1 GPa, thus enhancing the PL quantum yield leading to Sn (3) P1 --> (1) S0 photons tr

147 Full spectral profiles as well as quantum yields, lifetimes, and the crystal structures of

148 The combination of a high quantum yield, long fluorescence lifetime, and emission

149 We obtain a photothermal threshold quantum yield luminescence efficiency of 99.6 +/- 0.2%,

150 root and nodule biomass, predawn and midday quantum yields, maximum electron transport rates, water

151 equently, externally measured effective PSII quantum yields may be composed of signals derived from c

152 2'-Cl substituent was critical for the high quantum yield measured for triclosan and necessary for t

153 e quenching, deuterium labeling studies, and quantum yield measurements provide information about the

154 se in fluorescence, resulting in the highest quantum yield molecular fluorophore thus far.

155 ed switching wavelengths and remarkably high quantum yields (-NH-CH(2)- bridged diazocine: Phi(Z->E)

156 n irradiation at 254 nm was confirmed with a quantum yield of >0.8.

157 it pronounced optical properties with a high quantum yield of 0.23.

158 tautomer (480 nm) emissions with an overall quantum yield of 0.25.

159 ) exhibits a comparatively high fluorescence quantum yield of 0.31 in the solid state.

160 fective Stokes shift while retaining a large quantum yield of 0.59.

161 kable fluorescent intensity with a very good quantum yield of 0.85 and lifetime of 870ps.

162 ng to its favorable features: a fluorescence quantum yield of 0.98 and an extinction coefficient of 8

163 and manganite (gamma-MnOOH) with an apparent quantum yield of 1.37 x 10(-3) moles hydrogen per moles

164 A quantum yield of 200% is obtained on the early picosecon

165 XDPAdeCage photolyzes with a quantum yield of 27%, and binds Zn(2+) with 4.6 pM affin

166 a white light continuum with a fluorescence quantum yield of 29.9%.

167 up to 95% and a remarkably high fluorescence quantum yield of 30%, along with high stability.

168 -dots showed strong photoluminescence with a quantum yield of 4%.

169 elatively high solid-state photoluminescence quantum yield of 44%.

170 l)-2'-deoxyadenosine (8-TrzdA), exhibiting a quantum yield of 44%.

171 excited-state lifetime of 1.2 ms and a high quantum yield of 5.2% at room temperature in water.

172 p to 54+/-2 mmol H2 g(ZnSe) (-1) h(-1) and a quantum yield of 50+/-4 % (lambda=400 nm) under visible

173 ith an impressive external photoluminescence quantum yield of 75.4(9)%.

174 Measurements of the quantum yield of 8-DEA-tC mispaired with adenosine and,

175 The quantum yield of a photochemical reaction is one of the

176 sum competition of rates, improvement of the quantum yield of a photoreaction can be achieved either

177 0)(light) ratio of ~368 and a singlet oxygen quantum yield of about 20%.

178 threne, which shows the highest fluorescence quantum yield of all nonsubstituted BN-phenanthrenes rep

179 This treatment improves the quantum yield of both freshly synthesized (PLQY approxim

180 six Arctic plant species and determined the quantum yield of CO(2) fixation ( CO2 ) and the convexit

181 Fluorescence quantum yield of each dyad in nonpolar solvent (toluene)

182 The quantum yield of fructosazine was two times less than th

183 ondary photoreactions; (iii) it enhances the quantum yield of intersystem crossing (ISC), i.e., it is

184 g phosphorescence lifetime and high (1) O(2) quantum yield of Ir1-HSA are highly favorable properties

185 ead of the dipole-forbidden npai* state, the quantum yield of isomerization from trans- to cis-azoben

186 slow charge recombination results in a high quantum yield of MV(2+) photoreduction, while the doping

187 while the doping drastically influences this quantum yield of MV(2+) radical.

188 on transport (ETRmax), and negative with the quantum yield of non-photochemical energy conversion in

189 ptimized D-A-D dye exhibits greatly improved quantum yield of organic D-A-D fluorophores in aqueous s

190 g experiments and kinetic modeling, accurate quantum yield of PAA under UV(254) (Phi = 0.88 +/- 0.04

191 strong red fluorescence with a fluorescence quantum yield of PhiF = 0.3.

192 otein surface that imparts an unusually high quantum yield of photoreduction.

193 nction coefficient of 124000 M(-1) cm(-1), a quantum yield of photorelease of 3.8%, and an overall qu

194 However, the increase in the apparent quantum yield of photosynthesis below the Kok break poin

195 fect is a well-known phenomenon in which the quantum yield of photosynthesis changes abruptly at low

196 ferences (p > 0.05) were observed, including quantum yield of photosystem II (PSII), effective quantu

197 elationship with the effective photochemical quantum yield of Photosystem II (Y(II)) and the maximum

198 raits enabling it to preserve a high maximal quantum yield of photosystem II photochemistry in extrem

199 ought in four genotypes of Brassica rapa The quantum yield of PSII ( (PSII) ) is here analyzed as an

200 um yield of photosystem II (PSII), effective quantum yield of PSII, photochemical quenching and non-p

201 In contrast, the fluorescence quantum yield of quinine in 0.1 M perchloric acid shows

202 etection efficiency of spectrometer, and low quantum yield of RIXS process, we find that less than 2%

203 he poor temperature tolerance and suboptimal quantum yield of the existing metal halide perovskites i

204 The absolute photoluminescence quantum yield of the PDS fabricated using these QDs exce

205 ular hydrogen bond favors an increase of the quantum yield of the photocyclization reaction.

206 d losses of rehydration capacity and maximum quantum yield of the photosystem II (F(v) /F(m) ) in the

207 h to -Ph results in a marked increase in the quantum yield of the scaffold as well as a moderate red-

208 The photolysis quantum yield of the virus outweighed the seasonal solar

209 ajor UV-induced lesions) in genomic DNA; the quantum yield of these dimers in TEL21/Na(+) is found to

210 The quantum yield of this process often plays an essential r

211 ff and shows an external electroluminescence quantum yield of up to 5.8%, more than the theoretical l

212 ceptor feed ratio in the preparation and the quantum yield of white light emission from the system wa

213 examined here display high photoluminescence quantum yields of 0.8-1.0.

214 The cages are highly emissive (luminescence quantum yields of 16(1) to 18(1)%) and exhibit impressiv

215 em) ~ 440 nm) upon excitation at 255 nm with quantum yields of 4% (3) and 30% ([3][GaCl(4)]) affordin

216 The quantum yields of all processes were found to depend str

217 re compact, electron-rich alpha-aryl groups, quantum yields of fluorescence decrease dramatically des

218 is quenched and the effect this has on their quantum yields of fluorescence.

219 to acquire steady-state emission spectra and quantum yields of highly absorbing samples is presented.

220 Furthermore, ROS quantum yields of irradiated ambient PM(10) extracts wer

221 The photolysis effective quantum yields of PF-2M3P, PF-3M2B, and 2M3P were estima

222 In particular, we find that the quantum yields of photorelease are improved with derivat

223 aryl substitutions were found to improve the quantum yields of photorelease by excited state particip

224 805 nm and photophysical properties, such as quantum yields of singlet-oxygen formation, decompositio

225 ht of the spectrometer, and the ratio of the quantum yields of these processes is about 3.3.

226 The quantum yields of these processes vary significantly, fr

227 he NHC-capped QDs maintain photoluminescence quantum yields of up to 4.2 +/- 1.8% for shifts of the o

228 mation, were found to do so efficiently with quantum yields Phi((1)O(2)) = 0.71 and 0.38 for L = py a

229 in turnover number (TON(CO) = 100 +/- 4) and quantum yield (Phi(CO) = 23.3 +/- 0.8%) for CO formation

230 enching and a trade-off between fluorescence quantum yield (Phi(f) ) and absorption cross-section (si

231 We measure an average nitrite quantum yield (Phi(NO2(-))) of (1.1 +/- 0.2)% (313 nm, 5

232 (-1) cm(-1) at 630 nm), satisfactory triplet quantum yield (Phi(T) =52 %), and long-lived triplet sta

233 t properties of the CyHQ PPG, including high quantum yield (Phi(u)), low susceptibility to spontaneou

234 in singlet oxygen ((1)O(2)) and fluorescence quantum yields (Phi(1O2) and Phi(F)).

235 We quantified the apparent quantum yields (Phi(app,RI)) of photochemically produced

236 horescence was used to determine the (1)O(2) quantum yields (Phi(Delta)) of a variety of dissolved or

237 the most pronounced ICT rather high emission quantum yields (Phi(F) ca. 0.4) are observed for emissio

238 owed fluorescence with moderate fluorescence quantum yields (Phi(fl)).

239 tants (k') (210-2730 m(2) einstein(-1)), and quantum yields (Phi) (0.03-0.95 mol einstein(-1)).

240 tory measurements of [PPRI](ss) and apparent quantum yields (Phi) of three PPRIs ((3)DOM*, (1)O(2), a

241 50 nm, near-unity intersystem crossing (ISC) quantum yields (PhiISC), and triplet excited-state (T1)

242 ion rates, RRI) and intrinsic (to predict RI quantum yields, PhiRI) parameters.

243 ies, including outstanding photoluminescence quantum yield (PLQY) and tunable optical band gap.

244 s without compromising the photoluminescence quantum yield (PLQY) are reported.

245 Photoluminescence quantum yield (PLQY) measurements show that nonradiative

246 , we compute a theoretical photoluminescence quantum yield (PLQY) of 53%.

247 e range (145-415 K) with a photoluminescence quantum yield (PLQY) of at least 20.3% at RT.

248 e while maintaining a high photoluminescence quantum yield (PLQY) of the patterned QD layers.

249 l factors that dictate the photoluminescence quantum yield (PLQY) of these materials, we report five

250 s) featuring high absolute photoluminescence quantum yield (PLQY), low reabsorption, and high stabili

251 ications due to their high photoluminescence quantum yields (PLQY).

252 ght emission with improved photoluminescence quantum yields (PLQYs).

253 ll increase both the up- and down-conversion quantum yields, potentially exceeding the Shockley-Queis

254 r flanking G/C residues but its fluorescence quantum yield (QY) and lifetime values were almost indep

255 ell increases the linear photon upconversion quantum yield (QY) from 3.5 % for PbS QDs to 5.0 % for P

256 The Kok effect - an abrupt decline in quantum yield (QY) of net CO2 assimilation at low photos

257 bstantially lower the photoluminescence (PL) quantum yield (QY), a key metric of optoelectronic perfo

258 rimentally by a sizable decrease in emission quantum yield (QY), accompanied by a faster population d

259 ers (AuNCs) into NIR-II region with improved quantum yields (QY) could be achieved by engineering a p

260 The photoluminescence quantum yields range from 40 to 52%.

261 resulting fluoromodules exhibit fluorescence quantum yields ranging from 0.17 to 0.51 and excellent p

262 The donor, qAN1, has quantum yields reaching 21% and 11% in single- and doubl

263 emissive in solution, with photoluminescence quantum yields reaching 72%.

264 QD and dye PL intensities, when adjusted for quantum yields, reflected changes in the relative rate o

265 mentally and theoretically support, that the quantum yield remains large due to the lack of intramole

266 nine is by far the most popular fluorescence quantum yield standard used nowadays.

267 ion moments, as well as reduced fluorescence quantum yields, Stokes shifts, and fluorescence lifetime

268 Subsequently, we investigated the quantum yield temperature dependence of quinine solution

269 e B solutions, which have well characterized quantum yield temperature dependences.

270 s higher color purity, horizontal ratio, and quantum yield than 2DPyM-mDTC, which has a more flexible

271 ise to higher (5)(T(1)T(1))-to-(T(1) + T(1)) quantum yields than A and B, with a maximum value of 85%

272 n, A and B feature much higher (1)(T(1)T(1)) quantum yields than C and D, with a maximum value of 162

273 t efforts in improving the photoluminescence quantum yield, the chemical stability and the biocompati

274 stationary states (PSSs), photoisomerization quantum yields, thermal half-lives (tau(1/2)), and solut

275 citation and their influence on fluorescence quantum yields; they also provide background information

276 der optimized conditions, a leap in emission quantum yield to a record high 21% was accomplished for

277 method for the determination of fluorescence quantum yields to facilitate a fast characterization of

278 excellent photoluminescent properties: high quantum yield, tunable emission wavelengths (410-700 nm)

279 dependent emission, focusing on upconversion quantum yield (UCQY) and UV emission.

280 GDD), had a significant influence on initial quantum yield under direct but not diffuse light conditi

281 laying exceptional photophysical properties (quantum yield up to 31 % and |g(lum) | up to 0.240) by i

282 solid-state room-temperature phosphorescence quantum yield up to 64%.

283 highly polar solvent, exciplex fluorescence quantum yields up to 0.03 and lifetimes up to 17 ns were

284 Depending on ligand design, luminescence quantum yields up to 0.20 and microsecond excited state

285 The molecular crystals exhibit RTP quantum yields up to 20 % and lifetimes up to 520 ms.

286 ctive blue-emitting fluorophores, exhibiting quantum yields up to 98% and Stokes shifts up to 67 nm.

287 e delta(u) values (up to 2.64 GM), excellent quantum yields (up to 0.88), and high-yielding effector

288 water to oil (2000-fold) as well as its high quantum yields (up to 0.97) led us to investigate its ab

289 ld enhancement in the squaraine fluorescence quantum yield upon encapsulation as a rotaxane.

290 t up to 40-fold improvements in upconversion quantum yields using molecular engineering to selectivel

291 where, in the entire range, the luminescence quantum yield value remains constant and equal to 0.60 +

292 In general, the (1)O(2) quantum yield values in this study are in the middle, al

293 verall reduction of the Eu(III) luminescence quantum yield was found to be comparable and, in many ca

294 creased with increasing viscosity, while the quantum yield was increased.

295 -lives, photostationary states, fatigue, and quantum yields were determined.

296 layed low quantum yields in solution, higher quantum yields were observed in the solid state.

297 nanodots retain 80% of its initial emission quantum yield when immersed in water for 13 h, and a two

298 derivatives with higher intersystem crossing quantum yields, which can be promoted by core heavy atom

299 nts as compared with conventionally measured quantum yields with even exposure to actinic light.

300 quantified (1)O(2), OH radical, and H(2)O(2) quantum yields within photoirradiated solutions of labor