ライフサイエンスコーパス: photoexcited

1 of 300 ps lived charge separated states once photoexcited.

2 n to yield the sensitizer that was initially photoexcited.

3 ized and the attached free base porphyrin is photoexcited.

4 rature dependence of the yield of CT between photoexcited 2-aminopurine (Ap) and G through DNA bridge

5 DNA duplexes and DNA:RNA hybrids containing photoexcited 2-aminopurine (Ap).

6 In these systems, the photoexcited acceptor state is predominantly deactivated

7 netostrictive, and photostrictive actuators; photoexcited actuators; electrostatic actuators; and pne

8 tor states, localized in the vicinity of the photoexcited adsorbate, and delocalized states extended

9 We demonstrated that photoexcited aliphatic ketones, such as acetone and diac

10 quential hydride and proton transfers in the photoexcited and ground states, respectively, and is an

11 intermediate, formed by the collision of one photoexcited and one ground-state TIPS-pentacene molecul

12 Electron solvation dynamics in photoexcited anion clusters of I-(D2O)n=4-6 and I-(H2O)4

13 Photoexcited Ap is used as a dual reporter of variations

14 ce, and with the same driving force, HT from photoexcited Ap to G in the 5' to 3' direction is more e

15 Here we show that photoexcited Arabidopsis cryptochrome 2 (CRY2) is phosph

16 Plasmons are launched from a photoexcited array of nanocavities and their propagation

17 mmetry-breaking charge separation (SB-CS) in photoexcited assemblies of organic chromophores is a pot

18 cattering to measure the lattice dynamics of photoexcited BaFe2As2.

19 long debated pathway for the deactivation of photoexcited base pairs, with possible implications for

20 uents like these have electrons to feed into photoexcited BODIPYs, quenching their fluorescence, ther

21 uctural dynamics of the all-trans retinal in photoexcited bR to a highly twisted 13-cis conformation.

22 and vibrational spectroscopic signatures of photoexcited breathers are predicted, and generalization

23 er between CdS and TiO2 when the CdS QDs are photoexcited by wavelengths shorter than 525 nm.

24 copy was used for temporal resolution of the photoexcited carrier dynamics between the QDs and ligand

25 The photoexcited carrier lifetime demonstrates that the opti

26 plications is often attributed to their long photoexcited carrier lifetimes, which has led to charge-

27 Our work demonstrates electrical control of photoexcited carrier transfer across the van der Waals i

28 We find evidence that photoexcited carriers acquire spin-polarization from the

29 ers with Al(2)O(3), the recombination of the photoexcited carriers at the surfaces is mostly eliminat

30 is responsible for the ultrafast trapping of photoexcited carriers in haematite (alpha-Fe2O3).

31 show a coverage-dependent energy transfer of photoexcited carriers in hydrogenated graphene, giving r

32 Recombination of photoexcited carriers in most two-dimensional metal dich

33 numerical model based on charge transport of photoexcited carriers in the substrate.

34 ments indicate that the critical process for photoexcited carriers is the escape of holes from trap s

35 The majority of photoexcited carriers near the band-edge are seen to rec

36 graphene is a promising detection mechanism; photoexcited carriers rapidly thermalize due to strong e

37 from the escape of either one or both of the photoexcited carriers to the nanocrystal surface.

38 ractions lead to ultrafast relaxation of the photoexcited carriers, and the energy of the incident in

39 section and ultrafast recombination rates of photoexcited carriers.

40 aphene layers enhances the collection of the photoexcited carriers.

41 calculations support a mechanism in which a photoexcited catalyst/substrate complex triggers an intr

42 ed to determine the lifetime and activity of photoexcited catalysts.

43 results establish the initial steps for how photoexcited CdS delivers electrons into the MoFe protei

44 ibe the charge transfer interactions between photoexcited CdS nanorods and mononuclear water oxidatio

45 g the rate and quantum efficiency of ET from photoexcited CdS NRs to CaI using transient absorption s

46 Electron and energy transfer rates from photoexcited CdSe colloidal quantum dots (QDs) to graphe

47 he relative hole transfer rate constant from photoexcited CdSe/CdS core/shell QDs to tethered ferroce

48 the monolayer MoS2 in the process of ET from photoexcited CdSe/ZnS nanocrystals.

49 Computational modelling indicates that photoexcited charge carriers accumulated at the surface

50 obe the electronic structure and dynamics of photoexcited charge carriers at the Cu(2)O surface as we

51 lts help to explain the robust separation of photoexcited charge carriers between the two phases and

52 nement of sp(2) domains, and the trapping of photoexcited charge carriers in the localized states in

53 rimarily due to an energy gain involving the photoexcited charge carriers that are transiently popula

54 force microscopy (EFM) as a means to measure photoexcited charge in polymer films with a resolution o

55 lfide (MoS2 ) monolayers induce an effective photoexcited charge transfer at the interface.

56 The photoexcited charge transfer state of DMJ-An acts as a h

57 tion, the photoresponse due to the different photoexcited-charge-carrier trapping times in sp(2) and

58 d photoluminescence measurements reveal that photoexcited charges efficiently transfer to the passiva

59 Imaging the microchannel flows carrying thus photoexcited chelates of lanthanide ions allowed us to e

60 -bonding network and structural motions, the photoexcited chromophore could increase the photoswitchi

61 namics of a three-spin system representing a photoexcited chromophore coupled to a stable radical spe

62 d structural rearrangement at the level of a photoexcited chromophore is known to occur in the femtos

63 ization of the molecular choreography of the photoexcited chromophore requires a spectroscopic techni

64 s studies have shown that the collision of a photoexcited chromophore with a ground-state chromophore

65 Relaxation of photoexcited chromophores is a key factor determining di

66 uction mechanism involving delocalization of photoexcited conduction electrons wave function of gold

67 As a result, the photoexcited coumarin did not show any of the typical re

68 ults are consistent with the hypothesis that photoexcited CRY2 disengages its C-terminal domain from

69 clear bodies may result from accumulation of photoexcited CRY2-GFP waiting to be degraded.

70 ike kinases) interact with and phosphorylate photoexcited CRY2.

71 We have determined the steady state, photoexcited crystal structure of a flavin-bound LOV dom

72 The singlet fluorescence dynamics of photoexcited [Cu(I)(dmp)(2)](+) were measured in the coo

73 onal energy relaxation and redistribution in photoexcited cycloparaphenylene carbon nanorings with in

74 ergy transfer phenomenon that occurs between photoexcited D-/L-Trp enantiomers and rGO/gamma-CD givin

75 , demonstrating that both hole transfer from photoexcited DBFI-T to PSEHTT and electron transfer from

76 According to our analysis, 30% of the photoexcited diazo precursor molecules are eventually pr

77 Photoexcited dihydronicotinamides like NADH and analogue

78 ch liberates only trace hydrogen levels when photoexcited directly, does not appear to independently

79 One major decay channel of photoexcited DNA leads to reactive charge transfer state

80 ium(III) acceptor, a substantial fraction of photoexcited donor exhibits fast oxidative quenching (>3

81 xcited-state relaxation and injection as the photoexcited dye relaxes through the (3)MLCT manifold to

82 le electron transfer from the analyte to the photoexcited dye.

83 adsorbed O2 for receiving electrons from the photoexcited dyes.

84 Here we explore the photoexcited dynamics of molecules by an interaction wit

85 that the P cluster can function as a site of photoexcited electron delivery from CdS to MoFe protein.

86 Evolution of the time-dependent photoexcited electron during the initial 5 fs after inst

87 photo-induced resonant tunneling in which a photoexcited electron in the STM tip is transferred to t

88 and short-circuit the cell by accepting the photoexcited electron on a subpicosecond time scale.

89 t absorption (TA) spectroscopy revealed that photoexcited electron transfer rates increase with incre

90 le electron transfer (SET) event involving a photoexcited electron-donor-acceptor complex between an

91 tite (alpha-Fe2 O3) is engineered to improve photoexcited electron-hole pair separation by synthesizi

92 nce time-domain simulations, suggesting that photoexcited electron-hole pairs in the silicon waveguid

93 [H] or [D] and isotope alkanol-oxidation by photoexcited electron-hole pairs on a polymeric semicond

94 First, a shallow energy level traps a photoexcited electron.

95 Although the relaxation from the photoexcited electronic state during the ring-opening ha

96 Together this nano-architecture lets photoexcited electrons and holes dissociate instantaneou

97 dependent of electric field, indicating that photoexcited electrons and holes form excitons.

98 The ability to effectively transfer photoexcited electrons and holes is an important endeavo

99 results imply that the recombination of the photoexcited electrons and holes is suppressed by the sc

100 pathways for rapid and balanced transport of photoexcited electrons and holes, respectively, while mi

101 Photoexcited electrons are transferred to the metal and

102 ncident light was related to the trapping of photoexcited electrons by the WO(x) component.

103 HMe2(+)), which were capable of transferring photoexcited electrons directly to the negatively charge

104 e protein and ATP and provides low-potential photoexcited electrons for photocatalytic N(2) reduction

105 he device is based on thermionic emission of photoexcited electrons from a semiconductor cathode at h

106 Photoexcited electrons from cadmium sulfide nanorods (Cd

107 electron microscopy, we imaged the motion of photoexcited electrons from high-energy to low-energy st

108 a reduction step could occur by transfer of photoexcited electrons from the p-GaP photocathode and w

109 takes advantage of the reducing potential of photoexcited electrons in the conduction band of CdS and

110 (-) species is generated by the reaction of photoexcited electrons in the perovskite and molecular o

111 The photoexcited electrons of CZTS can be readily transporte

112 mechanism involving the coupling between the photoexcited electrons of the nanoparticles and the gold

113 mionic emission relies on vacuum emission of photoexcited electrons that are in thermal equilibrium w

114 It is found that both the transfer of photoexcited electrons to pyridinium and pyridinium adso

115 electrodes that can reduce water to H2 using photoexcited electrons.

116 Hole injection by photoexcited ethidium followed by radical migration to o

117 Absorption of X-ray photons generates photoexcited Fe(II)(LS) domains whose size rapidly grows

118 tion triggered by electron transfer from the photoexcited flavin cofactor to the dimer.

119 -radiative energy transfer occurring between photoexcited fluorophores (donors) and GO (acceptor), we

120 rface, without changes in the others, as the photoexcited fraction is increased.

121 The evolution from the photoexcited Franck-Condon MLCT state to the thermally e

122 The enhanced phonon scattering by photoexcited free carriers results in a substantial redu

123 y act as electron acceptors, whereas for the photoexcited fullerenes, SWCNTs act as electron donors.

124 The photoexcited GNRs enhanced the spin-spin and spin-lattic

125 s of the dynamics of hot electron cooling in photoexcited gold nanoparticles (Au NPs) with diameters

126 Our result suggests that photoexcited graphene transfers a hot electron to benzoy

127 y to accept an electron through space from a photoexcited guest.

128 ure change leading to proton transfer on the photoexcited half of the 7-azaindole dimer.

129 Photoexcited heptanal is believed to undergo rapid inter

130 we use a metallointercalator to introduce a photoexcited hole into the DNA pi-stack at a specific si

131 tion-band electron following transfer of the photoexcited hole to Ag(+).

132 It is not the presence of photoexcited holes and electrons, but a rise in temperat

133 In CdS nanocrystals, photoexcited holes rapidly become trapped at the particl

134 Under optical illumination, photoexcited hot carriers generated in the top layer tun

135 s owing to differences in decay channels for photoexcited hybrid plasmon-phonons and electrons.

136 The relaxation dynamics of the photoexcited hydrated electron have been subject to conf

137 In a spin: the dynamics of photoexcited ICN(-) (Ar)(0-5) are presented.

138 mploys the N-centered radical character of a photoexcited imine to facilitate the homolytic fragmenta

139 Photoexcited intramolecular charge transfer (CT) states

140 G and CPC is promoted efficiently by HT from photoexcited Ir(III) when the modified bases are positio

141 Mechanistic investigations suggest that the photoexcited iridium catalyst facilitated the nickel act

142 Here, the fragmentation of photoexcited iso-propyl iodide and tert-butyl iodide mol

143 The dynamics of photoexcited lead-free perovskite films, CH3NH3SnI3, wer

144 ill significantly lower than that induced by photoexcited lipofuscin.

145 methionine bioconjugation protocol that uses photoexcited lumiflavin to generate open-shell intermedi

146 ging by detecting the acoustic response of a photoexcited material.

147 In contrast to lipofuscin, photoexcited melanosomes did not substantially increase

148 The molecular structure and dynamics of the photoexcited metal-to-ligand-charge-transfer (MLCT) stat

149 The photoexcited metastable triplet state of Mg(2+)-mesoporp

150 ET quenching of both the singlet and triplet photoexcited MMb states, the direction of flow being det

151 rafast motion of electrons and nuclei of the photoexcited molecule presents a challenge to current sp

152 The electronic character of photoexcited molecules can abruptly change at avoided cr

153 vibrational, and vibronic couplings used by photoexcited molecules to transfer energy efficiently is

154 For photoexcited molecules, the nuclear dynamics determine t

155 tronic states often dictate the chemistry of photoexcited molecules.

156 observation of ultrafast charge transfer in photoexcited MoS2/WS2 heterostructures using both photol

157 Energy transfer from photoexcited nanoparticles to their surroundings was stu

158 The relaxation of photoexcited nanosystems is a fundamental process of lig

159 ansfer (ET) contributed to the relaxation of photoexcited nc-CdTe relative to the intrinsic radiative

160 Photoexcited (NCN)CNx in the presence of an organic subs

161 ate of hole-capture by the host polymer from photoexcited NCs.

162 diminishes, and blue emission from a trapped photoexcited neutral chromophore dominates because ESPT

163 Photoexcited Nickel(II) tetramesitylporphyrin (NiTMP), l

164 ithin approximately 10 ps, ligand binding to photoexcited NiDPP is progressively longer in pyridine,

165 led by Hund's physics in strongly correlated photoexcited NiO.

166 ibited intramolecular charge-transfer within photoexcited NOM, leading to substantially increased rem

167 IR detection shows that photoexcited o-phenylene thioxocarbonate (2) and 2-chlor

168 ited-state energy transfer prevails from the photoexcited oligofluorene to the energy accepting fulle

169 arized intersubband absorption features when photoexcited or under applied bias, which can be tuned b

170 The improved hole mobility in photoexcited p-type arrays leads to a pronounced enhance

171 n data indicate that electron injection from photoexcited PbS QDs to PCBM occurs within our temporal

172 dence is given for an electron transfer from photoexcited Pc1 to the electron-accepting C60A that aff

173 rom photoexcited polymer, hole transfer from photoexcited PCBM, prompt (<100 fs) charge generation in

174 for simulating the nonadiabatic dynamics of photoexcited PCET are discussed.

175 the mechanisms of these new methods based on photoexcited Pd complexes usually operate through transf

176 derstanding the fundamental spin dynamics of photoexcited pentacene derivatives is important in order

177 inally, we show that after relaxation of the photoexcited peptides toward the minimum of the differen

178 The electron injection dynamics from the photoexcited perovskite layers to the neighboring film s

179 ight perylenes per porphyrin in toluene, the photoexcited perylene-monoimide dye (PMI) decays rapidly

180 observe more than a 200-fold increase in the photoexcited phosphorescent emission of PtOEP (2,3,7,8,1

181 en shown to quench the catalytic activity of photoexcited, phosphorylated rhodopsin in a reconstitute

182 nhancing electron transfer rates between the photoexcited photoredox catalyst and the substrate.

183 g at two well-separated energies in a highly photoexcited planar microcavity at room temperature.

184 efficient excitation energy transfer from a photoexcited polymer layer to the underlying perovskite.

185 These include electron transfer from photoexcited polymer, hole transfer from photoexcited PC

186 o determine the interspin distance between a photoexcited porphyrin triplet state (S = 1) and a nitro

187 For example, with respect to the photoexcited porphyrins and phthalocyanines, SWCNTs usua

188 In the triple mutant, the decay of the photoexcited primary electron donor (P) occurs with a ti

189 ations are triggered by reorientation of the photoexcited protein.

190 DBFI-T to PSEHTT and electron transfer from photoexcited PSEHTT to DBFI-T contribute substantially t

191 tween electronic and nuclear dynamics of the photoexcited pyridine molecule.

192 Approximately 10-50% of all photoexcited pyrimidine bases decay via the (1)npi* stat

193 oxidation is initiated by hole transfer from photoexcited QD to surface DTO and that these substrates

194 Photoexcited QDs could be used in the study of the effec

195 this process, in particular, whether or not photoexcited QDs play a direct role in the photoinduced

196 Transient EPR spectroscopy shows that the photoexcited QDs strongly spin polarize the NDI radical

197 work serves as an initial step toward using photoexcited QDs to strongly spin polarize organic radic

198 The electron transfer dynamics from photoexcited QDs to the appended NDI ligands is explored

199 ates in the energy transfer process from the photoexcited QDs to the molecular energy acceptor.

200 ination kinetics of the electron and hole of photoexcited QDs.

201 Here, we show that photoexcited quantum dots (QDs) can kill a wide range of

202 Cu(I) oxidation by a photoexcited Re(I)-diimine at position 124 on a histidin

203 The analysis revealed that 30% of the photoexcited receptor molecules followed Cycle 1 through

204 , while CPG undergoes ring-opening both with photoexcited [Rh(phi)2(bpy)]3+ and with [Ru(phen)(dppz)(

205 A photoexcited rhodium intercalator, Rh(phi)2DMB3+ (phi =

206 mma and, as heterotrimeric proteins, bind to photoexcited rhodopsin (R*).

207 Gbetagamma(t) or activation of transducin by photoexcited rhodopsin (R*).

208 al rod cells, which controls the lifetime of photoexcited rhodopsin by inhibiting rhodopsin kinase.

209 In vertebrate photoreceptors, photoexcited rhodopsin interacts with the G protein tran

210 ydrolysis occurring over the period in which photoexcited rhodopsin is quenched.

211 ansducin and an increased activation rate by photoexcited rhodopsin or more efficient activation of c

212 GDP-bound x-ray structure of Gt reveals that photoexcited rhodopsin promotes the formation of a conti

213 well established that normal inactivation of photoexcited rhodopsin, the GPCR of rod phototransductio

214 restin molecules are available to quench the photoexcited rhodopsin.

215 ial first step in the prompt deactivation of photoexcited rhodopsin.

216 er effect spectroscopy while it was bound to photoexcited rhodopsin.

217 e-electron transfer process occurs between a photoexcited Ru(II) -cyclometalated complex and alkyl ha

218 ntermediates are generated upon quenching of photoexcited Ru*(bpz)3(2) with a variety of thiols.

219 The excited-state lifetime of photoexcited [Ru(bpy)(2)(pbnHH)](2+) is found to be abou

220 systems, electron-transfer occurred from the photoexcited ruthenium polypyridyl donor to the pentammi

221 nfrared (TRIR) spectroscopy was performed on photoexcited ruthenium polypyridyl-DNA crystals, the ato

222 odopsin in the native membrane suggested the photoexcited samples were heterogeneous.

223 Photoexcited semiconductor nanoparticles undergo charge

224 e pairs bound by the Coulomb attraction in a photoexcited semiconductor, has remained an elusive goal

225 c photocurrent results from reduction of the photoexcited sensitizer by free electrons in ITO.

226 sensitizer-acceptor design in which multiple photoexcited sensitizers resonantly and simultaneously t

227 receptor, in particular the lifetime of the photoexcited signaling states.

228 single-junction solar cells by splitting one photoexcited singlet exciton (S1) into two triplets (2T1

229 The reason is that photoexcited singlet oxygen is highly reactive, so the p

230 produces two triplet excited states from one photoexcited singlet state, is a means to circumvent the

231 Correspondingly, charge-separation ET from a photoexcited singlet zinc porphyrin incorporated within

232 neration of two spin triplet states from one photoexcited singlet.

233 experimental constraints on the reaction of photoexcited SO2 with atmospheric hydrocarbons.

234 e for the strongly oxidizing behavior of the photoexcited species is provided, while the stability of

235 of an applied external electric field on the photoexcited species of CH3NH3PbI3 thin films, both at r

236 t affects the nonradiative decay rate of the photoexcited species.

237 ent work, we demonstrate a method to harness photoexcited spin states in QDs to produce long-lived sp

238 y measuring an electromotive force driven by photoexcited spin-polarized electrons drifting through G

239 ith high reactivity with O(2) at the triplet photoexcited state and favorable redox potential and cou

240 , the role of small polaron formation in the photoexcited state and how this affects the photoconvers

241 eds through rapid internal conversion of the photoexcited state into a dark state of multi-exciton ch

242 presents a novel case in which the molecular photoexcited state is at the edge of the conduction band

243 In the system under investigation, the photoexcited state lies close to the bottom of the TiO 2

244 sion of (+)-2 into 14 by binding the triplet photoexcited state of 6 in proximity to (+)-2.

245 cter (triplet excitons) are generated from a photoexcited state of higher energy with singlet spin ch

246 chieving catalytic promiscuity that uses the photoexcited state of nicotinamide co-factors (molecules

247 n kinase and to modulate the lifetime of the photoexcited state of rhodopsin (Rh*), the visual pigmen

248 sistent with that of photolyase in which the photoexcited state of the purine donates an electron to

249 a silver nanocluster (AgNC), the reduced or photoexcited state of which is a powerful reductant.

250 ssion occurs directly from the initial 1B(u) photoexcited state on ultrafast time scales.

251 ce of the increasingly heavy elements on the photoexcited state properties, which were correlated wit

252 The photoexcited state Ru(II*) of Ru2Z is reduced to Ru(I) b

253 These studies revealed that in its photoexcited state this iodonium is capable of facilitat

254 ays the electronic relaxation of the initial photoexcited state within 200 fs.

255 m a particular C-O bond stretch in the pipi* photoexcited state.

256 dy configurations within the lifetime of the photoexcited state.

257 s a result of changes in the distribution of photoexcited-state energies and, hence, in the density o

258 h in generating a nonuniform distribution of photoexcited states and in driving the ET process.

259 the broad emission comes from the transient photoexcited states generated by self-trapped excitons (

260 estigation of the dynamics and relaxation of photoexcited states in conjugated polyfluorenes, which a

261 at, like their dihydrophenazine analogs, the photoexcited states of phenoxazine photoredox catalysts

262 The singlet S(1) and triplet T(1) photoexcited states of the compounds containing MM quadr

263 ntal and computational studies show that the photoexcited states of the two complexes are very differ

264 fer, injection in particular, accelerate for photoexcited states that are delocalized between the two

265 ally excited states can be employed to steer photoexcited states toward useful, high-energy products

266 he structure of transient molecules, such as photoexcited states, in disordered media (such as in sol

267 oflavin dimers do not interact in ground and photoexcited states.

268 The study of photoexcited strongly correlated materials is attracting

269 n be omitted and the Ni(II) complex directly photoexcited suggests that the PC may perform energy tra

270 This fundamental insight into the role of photoexcited surface FLPs for catalytic CO2 reduction co

271 Our results also indicate that photoexcited SWCNTs can catalyze lipid peroxidation simi

272 tom transfer (HAT) from the substrate to the photoexcited TAC radical dication, thus demonstrating a

273 ransfer states due to electron transfer from photoexcited tetracene to the lowest unoccupied molecula

274 ic acid to absorb solar radiation and become photoexcited, then directly or indirectly oxidize a vola

275 e used, while in cage oxygen transfer to the photoexcited (thio)pyrylium derivatives have been charac

276 ation of these phototoxic effects, 1(4+) was photoexcited through TPA at a power of 60 mW, which was

277 g on the interfacial charge transfer between photoexcited TiO2 and SWNTs as well as the mechanism of

278 Longer than 1 ns lifetimes for holes photoexcited to the lower valence subband offer a potent

279 ace and bulk transient carrier dynamics in a photoexcited topological insulator can control an essent

280 g the electronic and geometric structures of photoexcited transient species with high accuracy is cru

281 stem crossing and subsequent relaxation of a photoexcited transition metal complex.

282 e singlet excited state, but does quench the photoexcited triplet excited state as a function of TEMP

283 The delocalization of the photoexcited triplet state in a linear butadiyne-linked

284 lar oxygen via the presumed quenching of the photoexcited triplet state of 6.

285 temperature dependence and splitting of the photoexcited triplet state of myoglobin in which the iro

286 troscopic probe used in these studies is the photoexcited triplet state of Trp37, which is associated

287 phyrin oligomers lead to localization of the photoexcited triplet state on a single porphyrin unit, w

288 y acquired from the spin polarization of the photoexcited triplet state spectrum.

289 The photoexcited triplet states of a series of linear and cy

290 The transient EPR spectra of the photoexcited triplet states of the porphyrin monomer and

291 obins (Mb) the fluorescence quenching of the photoexcited tryptophan 14 (*Trp(14)) residue is in part

292 cond of the electron-transfer process in the photoexcited type-II heterostructure-a fundamental pheno

293 It was confirmed that the complex is readily photoexcited using near-infrared, NIR, and light through

294 Photoexcited visual pigment activates the GTP-binding pr

295 anism involves the ultrafast collapse of the photoexcited wave function due to nonadiabatic electroni

296 both molecules, the sub-100 fs transfer of a photoexcited wave packet from the (3)Q(0) state into the

297 ibit hole injection into surface states when photoexcited with visible light (lambda = 400-680 nm).

298 s when other bacteriorhodopsin molecules are photoexcited within the two-dimensional lattice of the p

299 Electron transfer from photoexcited zinc porphyrin to C(60) is witnessed in the

300 the vesicle was capable of reacting with the photoexcited zinc porphyrin.