ライフサイエンスコーパス: phosphorescence

1 energy toward triplet states, enhancing the phosphorescence.

2 o produce surprisingly efficient solid-state phosphorescence.

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

4 to downward, resulting in the suppression of phosphorescence.

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

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

7 decreases in flexibility, as measured by Trp phosphorescence.

8 esterases were investigated using tryptophan phosphorescence.

9 1,3]thiadiazoles and why they are capable of phosphorescence.

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

11 states can be monitored by room-temperature phosphorescence.

12 omplex formation produces a red-shift of the phosphorescence 0, 0-band (DeltaE0,0) of Trp37 as well a

13 nucleic acids results in a red-shift of the phosphorescence 0,0-band (delta E(0,0)) of the aromatic

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

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

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

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

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

19 Phosphorescence analyzer that measured dissolved O2 as f

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

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

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 These results are in general agreement with phosphorescence and ODMR measurements monitoring W.

25 Phosphorescence and optical detection of magnetic resona

26 oly(I), and rG(8)] have been investigated by phosphorescence and optically detected magnetic resonanc

27 Phosphorescence and optically detected magnetic resonanc

28 Phosphorescence and optically detected magnetic resonanc

29 and polynucleotides has been investigated by phosphorescence and optically detected magnetic resonanc

30 ose agreement between the quenching of donor phosphorescence and the efficiency of resonance energy t

31 The phosphorescence and zero field optically detected magnet

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

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

34 Fluorescence, phosphorescence, and optical detection of triplet state

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

36 states was estimated from the time-resolved phosphorescence anisotropy (TPA) decay of SR in which Ca

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

38 Time-resolved phosphorescence anisotropy (TPA) of ErIA and steady-stat

39 otion of actin was measured by time-resolved phosphorescence anisotropy (TPA) of erythrosin iodoaceta

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

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

42 We have used time-resolved phosphorescence anisotropy (TPA) to study the rotational

43 Time-resolved phosphorescence anisotropy (TPA) was used to determine c

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

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

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

47 Time-resolved phosphorescence anisotropy and fluorescence resonance en

48 tional mobility of IL-1 RI was assessed with phosphorescence anisotropy decay measurements using eryt

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

50 Time-resolved phosphorescence anisotropy experiments demonstrated that

51 Complementary measurements using phosphorescence anisotropy of erythrosin isothiocyanate

52 A strong positive correlation between the phosphorescence anisotropy of F-actin under specific con

53 The steady-state phosphorescence anisotropy of skeletal tropomyosin on F-

54 We used transient phosphorescence anisotropy to detect the microsecond rot

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

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

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

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

59 /- 9 degrees as determined from steady-state phosphorescence anisotropy.

60 Fluorescence and phosphorescence are clearly discriminated using a picose

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

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

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

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

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

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

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

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

69 Phosphorescence-based measurements can be used to determ

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

71 In this study, the authors developed a phosphorescence-based technique for measuring corneal O2

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

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

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

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

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

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

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

79 Phosphorescence data also suggest that the N- and C-term

80 Phosphorescence data are consistent with heavy-atom assi

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

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

83 ge ODMR and of short-lived components in the phosphorescence decay of the complex of R6WGR6 with poly

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

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

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

87 This discovery opens up the use of phosphorescence-detected hydrogen exchange as a sensitiv

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

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

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

91 erature triplet emitters are correlated with phosphorescence efficiency.

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

93 was monitored by measuring the steady-state phosphorescence emission anisotropy (rFA) of the triplet

94 filaments were monitored using steady-state phosphorescence emission anisotropy of the triplet probe

95 Data on the phosphorescence emission energy and lifetime from erythr

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

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

98 Phosphorescence emission spectra are resolved and shift

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

100 Bathochromic shifts in the phosphorescence emission upon exciting to the red in CT

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

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

103 anthraniloyl and further enhancement in the phosphorescence emitted by Tb3+ upon excitation at 320 n

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

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

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

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

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

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

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

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

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

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

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

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

116 Phosphorescence from the excited PS was quenched by the

117 Polarized phosphorescence from the triplet probe erythrosin-5-iodo

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

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

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

121 However, phosphorescence in organic molecules is rare at room tem

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

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

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

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

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

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

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

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

130 The phosphorescence intensity decay of PdOEP in the polymer

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

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

133 resolution, using the temperature-dependent phosphorescence intensity of the rare earth chelate Eu-T

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

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

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

137 Phosphorescence is a phenomenon of delayed luminescence

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

139 Phosphorescence is among the many functional features th

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

141 k deoxygenation system for measuring protein phosphorescence is described.

142 Because the phosphorescence is effectively quenched by molecular oxy

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

144 Phosphorescence is observed from these clusters in glass

145 Phosphorescence is the simplest physical process which p

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

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

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

149 Careful analysis of the phosphorescence lifetime distribution of Trp 109 in Esch

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

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

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

153 An optical section phosphorescence lifetime imaging system was developed fo

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

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

156 Phosphorescence lifetime imaging was used to measure eac

157 Phosphorescence lifetime imaging was used to measure flu

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

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

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

161 The room-temperature tryptophan (Trp) phosphorescence lifetime is sensitive to details of the

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

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

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

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

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

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

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

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

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

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

172 ameters D and E, and a significantly reduced phosphorescence lifetime, each consistent with aromatic

173 The phosphorescence lifetime-based measurement circumvents t

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

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

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

177 The phosphorescence lifetimes are shorter by an order of mag

178 Their long phosphorescence lifetimes in living cancer cells give ri

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

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

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

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

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

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

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

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

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

188 Frequency-domain phosphorescence measurements of the rotational dynamics

189 Electrochemistry and phosphorescence measurements of this complex indicate a

190 detection of analytes through time-resolved phosphorescence measurements.

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

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

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

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

195 s based on oxygen-dependent quenching of the phosphorescence of a Pt-porphyrin complex immobilized on

196 ninvasively by oxygen-dependent quenching of phosphorescence of an injected dye that is excited by li

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

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

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

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

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

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

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

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

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

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

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

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

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

210 Phosphorescence of tryptophan can be seen from the prote

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

230 Phosphorescence quenching and viscometric titrations ind

231 consumption impose limitations on the use of phosphorescence quenching in thick tissues.

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

233 We used the phosphorescence quenching method and a specially designe

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

235 Phosphorescence quenching microscopy provided PO(2) meas

236 eric arterioles in vivo by using noninvasive phosphorescence quenching microscopy.

237 ograft, using fluorescence ratio imaging and phosphorescence quenching microscopy.

238 Phosphorescence quenching of certain metalloporphyrins i

239 PO2 was measured, using the phosphorescence quenching of Pd-meso-tetra-(4-carboxyphe

240 eal oxygen consumption is measured using the phosphorescence quenching of Pd-meso-tetra-(4-carboxyphe

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

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

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

244 Radiolabelled microsphere and phosphorescence quenching techniques were used to measur

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

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

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

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

249 e nucleoprotein complex was characterized by phosphorescence, radiative decay lifetimes, and low-temp

250 Addition of poly(I) to p10 leads to a phosphorescence red shift, reduction in the zero-field s

251 (5-BrdU)7dT yields large phosphorescence red shifts in p10 and p10-ZF, and reduct

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

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

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

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

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

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

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

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

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

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

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

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

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

265 ips can be obtained between the solid-matrix phosphorescence (SMP) and the percent modification of be

266 ing correlation between the magnitude of the phosphorescence spectral shift, Deltanu(0-0), and the gu

267 Phosphorescence spectroscopy of mixed aggregate/gels con

268 me activation, we have used frequency-domain phosphorescence spectroscopy to measure the rotational d

269 Thus, we can use frequency-domain phosphorescence spectroscopy to measure the rotational d

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

292 ng ocular fluorometer was designed to excite phosphorescence with a brief flash of light and to measu

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.