ライフサイエンスコーパス: phosphorescence

1 DF), whereas compound 2 shows a pure, yellow phosphorescence.

2 states can be monitored by room-temperature phosphorescence.

3 energy toward triplet states, enhancing the phosphorescence.

4 o produce surprisingly efficient solid-state phosphorescence.

5 ient and reversible quenching of the (3)MLCT phosphorescence.

6 xial ligands most conducive to near-infrared phosphorescence.

7 e cortex (pCO2) was measured by quenching of phosphorescence.

8 croM), whereas Ca2+ showed no effect on Tb3+ phosphorescence.

9 to downward, resulting in the suppression of phosphorescence.

10 thermally activated delayed fluorescence and phosphorescence.

11 1,3]thiadiazoles and why they are capable of phosphorescence.

12 ily access and emit from its T1 state with a phosphorescence (3)(7a)* lifetime of tauP = 395 mus at 7

13 ganometallic systems, where ligand-localized phosphorescence ((3) pi-pi*) is mediated by ligand-to-me

14 Long-lived phosphorescence (4 s at 77 K) was recorded, and quantum-

15 can subsequently be detected by its 1270 nm phosphorescence (a(1)Delta(g) --> X(3)Sigma(g)(-)) with

16 molecular materials with aggregation-induced phosphorescence (AIP) is designed, which exhibits two di

17 sistent with expectations from the theory of phosphorescence, an inverse correlation between out-of-p

18 Phosphorescence analyzer that measured dissolved O2 as f

19 culations corroborate that the emissions are phosphorescence and arise from charge transfer (LML'CT)

20 stable palladium complexes that exhibit both phosphorescence and delayed fluorescence are developed.

21 d whole waters with singlet oxygen ((1)O(2)) phosphorescence and determined the triplet energy of HDA

22 g red metal-to-ligand-charge-transfer (MLCT) phosphorescence and electrophosphorescence.

23 SC rate modulates the intensity ratio of the phosphorescence and fluorescence emission bands, with po

24 -monolayer NaCl film atop Ag(111) shows both phosphorescence and fluorescence signals at high applied

25 Phosphorescence and optical detection of magnetic resona

26 t(II) metallacage with oxygen-responsive red phosphorescence and steady fluorescence for in vivo hypo

27 The phosphorescence and zero field optically detected magnet

28 extended (3)MLCT lifetime (160 ps), (3)MLCT phosphorescence, and ambient environment stability.

29 effects, experiments utilizing endoperoxide, phosphorescence, and chemiluminescence quenching studies

30 Photophysical studies such as fluorescence, phosphorescence, and laser flash photolysis in addition

31 element has been studied using fluorescence, phosphorescence, and optically detected magnetic resonan

32 o F-actin at Cys-374 and performed transient phosphorescence anisotropy (TPA) experiments.

33 We have used time-resolved phosphorescence anisotropy (TPA) of actin to evaluate do

34 We have used transient phosphorescence anisotropy (TPA) to detect changes in ac

35 We have used time-resolved phosphorescence anisotropy (TPA) to probe rotational dyn

36 dynamics of actin, detected by time-resolved phosphorescence anisotropy (TPA).

37 d to C374 on actin, as detected by transient phosphorescence anisotropy (TPA).

38 in-iodoacetemide (ErIA), using time-resolved phosphorescence anisotropy (TPA).

39 Time-resolved phosphorescence anisotropy and fluorescence resonance en

40 ecrease in the correlation time of transient phosphorescence anisotropy decays.

41 Time-resolved phosphorescence anisotropy experiments demonstrated that

42 We used transient phosphorescence anisotropy to detect the microsecond rot

43 We have used time-resolved phosphorescence anisotropy to investigate the effects of

44 We have used transient phosphorescence anisotropy to monitor the microsecond ro

45 Here, using time-resolved phosphorescence anisotropy, electron cryomicroscopy, and

46 We have used optical spectroscopy (transient phosphorescence anisotropy, TPA, and fluorescence resona

47 /- 9 degrees as determined from steady-state phosphorescence anisotropy.

48 Fluorescence and phosphorescence are clearly discriminated using a picose

49 )dbm(I)PLA with weak fluorescence and strong phosphorescence are promising as 'turn on' sensors for a

50 complex mer-[V(ddpd)(2)][PF(6)](3) yielding phosphorescence around 1100 nm in valeronitrile glass at

51 e melt and provides evidence of the value of phosphorescence as a probe of dynamic site heterogeneity

52 ed by two methods: direct measurement of its phosphorescence at 1275 nm and chemical trapping using u

53 of fluorescence and appearance of structured phosphorescence at 77 K are attributed to nitrophenyl-lo

54 target molecule, allowing the observation of phosphorescence at room temperature and alleviating cons

55 The phosphorescence band is blue-shifted ca. 20 nm in the ag

56 RT) and coarse- and fine-tuning to multiple phosphorescence bands across the visible spectrum via lu

57 ned, which exhibits two distinctly different phosphorescence bands and an absolute solid-state room-t

58 application by integrating the sensors of a phosphorescence based CGM system into a standard insulin

59 The integrated phosphorescence-based oxygen biosensor employs the quenc

60 eral reaction scheme to the development of a phosphorescence-based sensing system for cyanogen halide

61 Heavy-atom substitution alone increases phosphorescence by a given, not variable amount.

62 energy transfer, minimized quenching of the phosphorescence by electron transfer and increased signa

63 Here we report bright room temperature phosphorescence by embedding a purely organic phosphor i

64 e the theory and principles of computational phosphorescence by highlighting studies of classical exa

65 it is shown that both chemiluminescence and phosphorescence can also be observed in a highly directi

66 studies reveal that bright room temperature phosphorescence can be realized in purely organic crysta

67 r (IPr --> AuM2) and interligand (IPr --> E) phosphorescence character, as revealed by time-dependent

68 The bias voltage dependence of the phosphorescence, combined with differential conductance

69 Phosphorescence data are consistent with heavy-atom assi

70 ed experiments, monitoring the 1270 nm (1)O2 phosphorescence decay generated upon laser irradiation a

71 The rates of phosphorescence decay of 4,7-dimethylindanone (2), 6,9-d

72 determined by observing their effect on the phosphorescence decay of the triplet state of rose benga

73 s a substrate, with [O(2)] obtained from the phosphorescence decay rate of a palladium phosphor.

74 Phosphorescence decay times were found to be around ~5 u

75 dentical lifetimes to those observed for the phosphorescence decays when measured under identical exp

76 n designed to couple the aggregation induced phosphorescence, displayed by the core in the solid stat

77 It was found that the phosphorescence efficiency depends on the orientation of

78 onless transitions and hence greatly enhance phosphorescence efficiency of metal-free organic materia

79 erature triplet emitters are correlated with phosphorescence efficiency.

80 dence for this comes from a fast rise in the phosphorescence emission and measurements of a correspon

81 Data on the phosphorescence emission energy and lifetime from erythr

82 Single molecules are detected through the phosphorescence emission of their triplet states.

83 studies together with fluorescence and (1)O2 phosphorescence emission quantum yields collected on Br2

84 Phosphorescence emission spectra are resolved and shift

85 radiative decay, which in turn boosts (1)O2 phosphorescence emission to a greater extent.

86 was projected at an angle on the retina, and phosphorescence emission was imaged after intravitreal i

87 onal temperature sensing agents, (ii) bright phosphorescence emission, (iii) a reversible thermal res

88 energy transfer, solid-state solvation, and phosphorescence enables 10-fold increases in the power o

89 al excimer geometry and the magnitude of the phosphorescence energy lowering in going from the monome

90 erligand distances around 3.5-3.8 A, lead to phosphorescence energy lowerings with respect to the mon

91 We describe the red phosphorescence exhibited by a class of structurally sim

92 The absorption, steady-state fluorescence, phosphorescence, fluorescence lifetime, and phosphoresce

93 eport a strategy for modulating fluorescence/phosphorescence for a single-component, dual-emissive, i

94 tive materials that exhibit room temperature phosphorescence for technologies including bio-imaging,

95 locene (Cp)(2)Ti(NCS)(2) exhibits an intense phosphorescence from a ligand-to-metal charge transfer t

96 ons were monitored by measuring the decay of phosphorescence from a Pd phosphor in solution; the deca

97 de polymer is water soluble, and it exhibits phosphorescence from a triplet pi,pi exciton based on th

98 This study illustrates that phosphorescence from erythrosin B is sensitive both to l

99 resulting in lattice contraction as well as phosphorescence from five unpaired electrons.

100 Long-lived room temperature phosphorescence from organic molecular crystals attracts

101 The phosphorescence from Pt-p is quenched by viologens with

102 lar interactions to enhance room-temperature phosphorescence from purely organic materials in amorpho

103 e the fluorescence from S(2) excited states (phosphorescence from T(2) excited states).

104 Phosphorescence from the excited PS was quenched by the

105 for the direct signature of singlet fission, phosphorescence from the triplet state, in a model polym

106 ade use of direct time-resolved detection of phosphorescence, having the ability to efficiently rejec

107 A previously developed optical section phosphorescence imaging system was used to measure P(O2)

108 Achieving highly efficient phosphorescence in purely organic luminophors at room te

109 display highly efficient blue or blue-green phosphorescence in solution (Phi = 0.41-0.87) and the so

110 ment complexes, and room-temperature near-IR phosphorescence in the case of several 5d metal complexe

111 i-diboryne compounds (n = 2, 3) show intense phosphorescence in the red to near-IR region from their

112 nds responsible for pre-edge fluorescence or phosphorescence in the visible.

113 The strongly allowed phosphorescence in these complexes is the result of sign

114 be challenging to vary relative fluorescence/phosphorescence intensities for practical sensing applic

115 eight polymer with balanced fluorescence and phosphorescence intensities serve as ratiometric tumour

116 The phosphorescence intensity (lifetime), emission energy, a

117 f small or large intestine fragments, robust phosphorescence intensity and lifetime signals were prod

118 The phosphorescence intensity decay of PdOEP in the polymer

119 The cofilin concentration-dependence of the phosphorescence intensity is sigmoidal, consistent with

120 Cofilin quenches the phosphorescence intensity of actin-bound ErIA, indicatin

121 rate was obtained by fitting the tail of the phosphorescence intensity profile to an exponential.

122 onstruct exhibits concomitant changes in its phosphorescence intensity ratio and phosphorescence life

123 In contrast to the reduction in phosphorescence intensity, the changes in the rates of r

124 Phosphorescence is a phenomenon of delayed luminescence

125 Oxygen-dependent quenching of phosphorescence is a useful and essentially noninvasive

126 Phosphorescence is among the many functional features th

127 The bridging of the spin prohibition in phosphorescence is commonly analyzed by perturbation the

128 k deoxygenation system for measuring protein phosphorescence is described.

129 Because the phosphorescence is effectively quenched by molecular oxy

130 Ir(III) corrole phosphorescence is observed at ambient temperature at wa

131 Phosphorescence is observed from these clusters in glass

132 Phosphorescence is the simplest physical process which p

133 The single molecule phosphorescence is very sensitive to molecular oxygen.

134 loss of triplets, a key process to achieving phosphorescence, is difficult without heavy metal atoms.

135 riplets and exhibits efficient near-infrared phosphorescence (lambda(em) = 772 nm, Phi = 0.26).

136 Phosphorescence lifetime and blood flow imaging were per

137 The long phosphorescence lifetime and high (1) O(2) quantum yield

138 The large decrease in the phosphorescence lifetime and intensity of the porphyrin

139 Retinal PO2 maps were computed from phosphorescence lifetime images, and oxygen profiles thr

140 ension was measured in retinal vessels using phosphorescence lifetime imaging and converted to arteri

141 a melanoma tumour spheroid using one-photon phosphorescence lifetime imaging microscopy (PLIM) and a

142 An optical section phosphorescence lifetime imaging system was developed fo

143 ing our previously developed optical section phosphorescence lifetime imaging system.

144 n innovative optical system for dual oxyphor phosphorescence lifetime imaging to near-simultaneously

145 Phosphorescence lifetime imaging was used to measure eac

146 Phosphorescence lifetime imaging was used to measure flu

147 ield optical microscopy, including 2D and 3D phosphorescence lifetime imaging.

148 ot only simple lifetime measurement but also phosphorescence lifetime imaging.

149 s in its phosphorescence intensity ratio and phosphorescence lifetime in response to copper(II) ion.

150 g polarography, spectroscopy, and two-photon phosphorescence lifetime measurements of oxygen sensors.

151 phosphorescence, fluorescence lifetime, and phosphorescence lifetime measurements were carried out.

152 A frequency-domain approach was used for phosphorescence lifetime measurements.

153 s of metalloporphyrins, including two-photon phosphorescence lifetime microscopy (2PLM) and two-photo

154 Recent development of two-photon phosphorescence lifetime microscopy (2PLM) of oxygen ena

155 rain of awake mice, by performing two-photon phosphorescence lifetime microscopy at micrometer resolu

156 Using two-photon phosphorescence lifetime microscopy, we determined the a

157 mercial time-resolved fluorescence reader in phosphorescence lifetime mode.

158 isoforms also differ in their effects on the phosphorescence lifetime of the actin-bound erythrosin i

159 to O2 (RSD at 21 KPa 1.9%), and reproducible phosphorescence lifetime readings.

160 luctuations on the picosecond time scale and phosphorescence lifetime was observed.

161 excitation and systematic variations in the phosphorescence lifetime with wavelength indicated that

162 The phosphorescence lifetime-based measurement circumvents t

163 scular P(O2) was measured by determining the phosphorescence lifetime.

164 n characteristics, notably strongly enhanced phosphorescence lifetimes (reaching 0.7 ms) and increase

165 et lifetimes were confirmed by measuring the phosphorescence lifetimes and with the help of diffusion

166 CT state increase from 4 to 12 ps, while the phosphorescence lifetimes are approximately 80 micros.

167 The phosphorescence lifetimes are shorter by an order of mag

168 Their long phosphorescence lifetimes in living cancer cells give ri

169 Phosphorescence lifetimes of 2 ms for N-acetyl-L-tryptop

170 the system was demonstrated by measuring the phosphorescence lifetimes of N-acetyl-L-tryptophanamide,

171 examined in detail, and compared with Trp102 phosphorescence lifetimes that were previously measured.

172 uced Cherenkov light to excite and image the phosphorescence lifetimes within the tissue.

173 hotoluminescence and excitation spectra, and phosphorescence lifetimes, are presented.

174 The homogeneous phosphorescence line width, which can be measured in sin

175 We describe the Madison laser-induced phosphorescence (LIP) instrument, an instrument based on

176 TP), emits a highly resolved low-temperature phosphorescence (LTP) spectrum and has the narrowest ODM

177 er, it is hard to achieve a room temperature phosphorescence material with simultaneous long lifetime

178 ed and fabricated, enabling room temperature phosphorescence material with simultaneous ultralong lif

179 Room temperature phosphorescence materials have inspired extensive attent

180 egy to construct metal-free room temperature phosphorescence materials with ultralong lifetime, high

181 minutes of eye closure, using a time-domain phosphorescence measurement system.

182 the effect of scavengers, the chlorothalonil phosphorescence measurement, and varying irradiation con

183 Low-temperature phosphorescence measurements determined the triplet ener

184 Electrochemistry and phosphorescence measurements of this complex indicate a

185 Time-resolved (1)O(2) phosphorescence measurements yielded different HDA quenc

186 detection of analytes through time-resolved phosphorescence measurements.

187 bulins have been quantified by time-resolved phosphorescence measurements.

188 Near-infrared confocal phosphorescence microscopy was used to demonstrate the a

189 fluorescence microscopy) or P(iO(2)) (n= 7; phosphorescence microscopy) was measured continuously.

190 ed, with particular emphasis on the quenched-phosphorescence O2 sensing technique.

191 In contrast, only phosphorescence occurs at low applied voltage, indicatin

192 ated based on the quenching by oxygen of the phosphorescence of an intravenously injected palladium p

193 The (3)MLCT phosphorescence of each of the three coordination polyme

194 is study used steady-state and time-resolved phosphorescence of erythrosin B to monitor mobility in t

195 The phosphorescence of Ir1-HSA was enhanced significantly co

196 The quenching mechanism of phosphorescence of Mn-doped ZnS QDs by IDA is a combined

197 tion of [1PtOEP] leads to an increase in the phosphorescence of PtOEP under ambient conditions.

198 In this study, the time-resolved phosphorescence of singlet oxygen produced by the sensit

199 The sensitization of phosphorescence of Tb3+ bound to factor VIII subunits wa

200 Mn2+ inhibited the phosphorescence of Tb3+ bound to HC and LC, as well as t

201 sion observed for 2 and 3 corresponds to the phosphorescence of the aromatic substrate and suggests t

202 Consistently, the phosphorescence of the benzophenone units and the fluore

203 Upon Mg(2+) complexation in THF solution, phosphorescence of the hexathiobenzene core is turned on

204 th the purpose of amplifying the 2PA induced phosphorescence of the metalloporphyrin.

205 can be measured in human subjects using the phosphorescence of the porphyrin-protein complex bound t

206 Phosphorescence of tryptophan can be seen from the prote

207 oxygen-sensitive molecular probe to generate phosphorescence optical section images.

208 , photostable fluorescence, oxygen-sensitive phosphorescence or dual emission for ratiometric sensing

209 of energy transfer via an emissive process (phosphorescence) or a nonemissive process (triplet-tripl

210 Delta E(0,0) is the shift of the tryptophan phosphorescence origin, provides a measure of aromatic s

211 orm are desirable, but when fluorescence and phosphorescence originate from the same dye, it can be c

212 -temperature dual emission, fluorescence and phosphorescence, originating mainly from (1)MLCT and (3)

213 therapy, using oxygen-dependent quenching of phosphorescence, oxygen probe Oxyphor PtG4 and the radio

214 tional aspects for the estimation of various phosphorescence parameters, like intensity, radiative ra

215 TADF path (62%) and one via the T1 state as phosphorescence path (38%).

216 Qualitative aspects of the phosphorescence phenomenon are discussed in terms of con

217 The solid-state quantum yields of phosphorescence (Phi) vary from 0.1% (1a) to 25% (1d), d

218 on spontaneous emission, and singlet-triplet phosphorescence processes--can occur on very short time

219 A sharp increase in phosphorescence quantum efficiency is observed in a vari

220 n dots exhibit ultralong lifetime of 5.72 s, phosphorescence quantum efficiency of 26.36%, and except

221 l with simultaneous ultralong lifetime, high phosphorescence quantum efficiency, and excellent stabil

222 ence materials with ultralong lifetime, high phosphorescence quantum efficiency, and high stability f

223 ial with simultaneous long lifetime and high phosphorescence quantum efficiency.

224 tophysics of the complexes, particularly the phosphorescence quantum yield and lifetime.

225 Disappointingly, the phosphorescence quantum yield invariably turned out to b

226 and an absolute solid-state room-temperature phosphorescence quantum yield up to 64%.

227 hibit rich photophysics combined with a high phosphorescence quantum yield, are employed in red and n

228 ovements include significant increase in the phosphorescence quantum yield, higher efficiency of the

229 d organic phosphors to achieve a bright 7.5% phosphorescence quantum yield.

230 Photophysical properties (2PA brightness and phosphorescence quantum yields and lifetimes) of the new

231 Triplet energies and phosphorescence quantum yields as well as quantum effici

232 Remarkably, the phosphorescence quantum yields of Pd and Pt TBPs reach a

233 te Cu(I)-Au(I) covalent bonds and near-unity phosphorescence quantum yields.

234 Among existing pO(2) measurement methods, phosphorescence quenching is optimally suited for the ta

235 We used the phosphorescence quenching method and a specially designe

236 Tissue pO(2) and pH were determined by phosphorescence quenching microscopy and ratio imaging m

237 Phosphorescence quenching microscopy provided PO(2) meas

238 tical microscopy, and O(2) distributions via phosphorescence quenching microscopy.

239 resolution can be made possible by combining phosphorescence quenching technique with multiphoton las

240 We adapted phosphorescence quenching techniques to determine the.Q(

241 To test this hypothesis, we utilized phosphorescence quenching techniques to measure mean mic

242 Radiolabelled microsphere and phosphorescence quenching techniques were used to measur

243 We measured thermal activation of tryptophan phosphorescence quenching to explore millisecond-range p

244 terstitial space oxygen pressures (PO(2) is; phosphorescence quenching) and convective and diffusive

245 O2 uptake (VO2) ratio) profile (assessed via phosphorescence quenching) compared to muscle of primari

246 flow (radiolabelled microspheres), PO(2)mv (phosphorescence quenching), and V(O(2)) (Fick calculatio

247 decline in diaphragm microvascular PO2 (via phosphorescence quenching).

248 tercalation with [d(CGACGTCG)](2) produces a phosphorescence redshift, while groove binding with [d(G

249 te was determined from the dependence of the phosphorescence relaxation rate on dye concentration in

250 As a general property of molecules, phosphorescence represents a cornerstone problem of chem

251 rely organic materials with room-temperature phosphorescence (RTP) are currently under intense invest

252 Although persistent room-temperature phosphorescence (RTP) emission has been observed for a f

253 anic materials that exhibit room-temperature phosphorescence (RTP) is a very attractive topic owing t

254 printed polymer (MIP)-based room temperature phosphorescence (RTP) probe by combining the RTP of Mn-d

255 zines (DA3 and DA6) exhibit room-temperature phosphorescence (RTP) properties.

256 ohybrids were used as novel room temperature phosphorescence (RTP) sensor to detect double stranded d

257 ion and thus enables bright room-temperature phosphorescence (RTP) with quantum yields reaching 24%.

258 er work to be the source of room-temperature phosphorescence (RTP), emits a highly resolved low-tempe

259 elayed fluorescence (TADF), room-temperature phosphorescence (RTP), mechanoluminescence (ML), and dis

260 We devised a novel room-temperature-phosphorescence (RTP)-based oxygen detection platform by

261 In this study, a facile room-temperature phosphorescence sensor is developed to detect DA based o

262 l characteristics allowed differentiation of phosphorescence signals from the retinal vasculature and

263 Phosphorescence spectroscopy of mixed aggregate/gels con

264 R and optical (absorption, fluorescence, and phosphorescence) spectroscopy.

265 ecombine to form singlet excitons during the phosphorescence spectrum measurement.

266 (iii) The phosphorescence spectrum of Trp-151 is red-shifted in th

267 ombination of Solid Surface-Room Temperature Phosphorescence (SS-RTP) and nanotechnology has led to a

268 bre mat) with Solid Surface-Room Temperature Phosphorescence (SS-RTP) measurement for the determinati

269 The interpretation of room temperature phosphorescence studies of proteins requires an understa

270 rk is put in the context of room temperature phosphorescence studies of proteins.

271 resolved absorption, fluorescence, and (1)O2 phosphorescence studies together with fluorescence and (

272 tandards and corroborated by low-temperature phosphorescence studies, established cooperative assembl

273 efficient intersystem-crossing S1 --> Tn and phosphorescence T1 --> S0.

274 lymeric structure, sensitization of the core phosphorescence takes place with >90% efficiency.

275 reate purely organic materials demonstrating phosphorescence that can be turned on by incorporating h

276 We furthermore discuss modern studies of phosphorescence that cover topics of applied relevance,

277 The transduction of the sensor is phosphorescence; the covalently immobilized tryptamine i

278 ata formats in both the fluorescence and the phosphorescence time domains.

279 The spectrum taken in the phosphorescence time window at low temperature may conse

280 , ZnCl(2) Br(2) , ZnBr(4) ), from efficient phosphorescence to ultralong afterglow.

281 y water molecules produced unique reversible phosphorescence-to-fluorescence switching behavior.

282 Apart from enhanced red phosphorescence upon hypoxia, the ratio between red and

283 s, spin-orbit coupling is less efficient and phosphorescence usually cannot compete with radiationles

284 Combined with exceptionally bright phosphorescence (varphiphos = 0.45), strong 2PA makes Pt

285 arkable ratiometric changes of intensity for phosphorescence versus fluorescence that are excitation

286 tion, and a relatively strong and long-lived phosphorescence was observed in low-temperature glasses

287 A progressively red-shifted phosphorescence was observed with increasing atomic numb

288 for twisted systems unexpectedly long-lived phosphorescence was observed.

289 In this manuscript, time-resolved (1)O(2) phosphorescence was used to determine the (1)O(2) quantu

290 By using single tryptophan protein phosphorescence, we follow site-specific internal protei

291 eport of a highly efficient OLED(2) based on phosphorescence, which is produced by the decay of T(1)

292 hin a cylindrical capsule gives bright green phosphorescence, while irradiation of benzil and dimetho

293 und exhibits an additional highly structured phosphorescence with a vibronic structure corresponding

294 Finally, the AuNC displays phosphorescence with large Stokes shift and microsecond

295 phosphorescent nanoparticles exhibit strong phosphorescence with long lifetime and large Stoke shift

296 However, previous attempts to couple phosphorescence with two-photon laser scanning microscop

297 The latter display light-green phosphorescence with unusually long lifetimes and circul

298 species (fluorescence, chemiluminescence and phosphorescence) within a few hundred nanometers from th

299 The phosphorescence yield for protein and model indole compo

300 ere is not a consistent effect on triplet or phosphorescence yields.