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1 n to yield the sensitizer that was initially photoexcited.
2 ized and the attached free base porphyrin is photoexcited.
3 of 300 ps lived charge separated states once 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 cattering to measure the lattice dynamics of photoexcited BaFe2As2.
18 long debated pathway for the deactivation of photoexcited base pairs, with possible implications for
19 uents like these have electrons to feed into photoexcited BODIPYs, quenching their fluorescence, ther
20  and vibrational spectroscopic signatures of photoexcited breathers are predicted, and generalization
21  light can cause phosphorylation of not only photoexcited but also non-excited rhodopsin in rod photo
22 er between CdS and TiO2 when the CdS QDs are photoexcited by wavelengths shorter than 525 nm.
23 copy was used for temporal resolution of the photoexcited carrier dynamics between the QDs and ligand
24                        We find evidence that photoexcited carriers acquire spin-polarization from the
25 is responsible for the ultrafast trapping of photoexcited carriers in haematite (alpha-Fe2O3).
26 show a coverage-dependent energy transfer of photoexcited carriers in hydrogenated graphene, giving r
27                             Recombination of photoexcited carriers in most two-dimensional metal dich
28 numerical model based on charge transport of photoexcited carriers in the substrate.
29 graphene is a promising detection mechanism; photoexcited carriers rapidly thermalize due to strong e
30 from the escape of either one or both of the photoexcited carriers to the nanocrystal surface.
31 ractions lead to ultrafast relaxation of the photoexcited carriers, and the energy of the incident in
32 aphene layers enhances the collection of the photoexcited carriers.
33 section and ultrafast recombination rates of photoexcited carriers.
34 ed to determine the lifetime and activity of photoexcited catalysts.
35 ibe the charge transfer interactions between photoexcited CdS nanorods and mononuclear water oxidatio
36 g the rate and quantum efficiency of ET from photoexcited CdS NRs to CaI using transient absorption s
37      Electron and energy transfer rates from photoexcited CdSe colloidal quantum dots (QDs) to graphe
38 he relative hole transfer rate constant from photoexcited CdSe/CdS core/shell QDs to tethered ferroce
39 the monolayer MoS2 in the process of ET from photoexcited CdSe/ZnS nanocrystals.
40       Computational modelling indicates that photoexcited charge carriers accumulated at the surface
41 lts help to explain the robust separation of photoexcited charge carriers between the two phases and
42 nement of sp(2) domains, and the trapping of photoexcited charge carriers in the localized states in
43 rimarily due to an energy gain involving the photoexcited charge carriers that are transiently popula
44 force microscopy (EFM) as a means to measure photoexcited charge in polymer films with a resolution o
45 lfide (MoS2 ) monolayers induce an effective photoexcited charge transfer at the interface.
46                                          The photoexcited charge transfer state of DMJ-An acts as a h
47 tion, the photoresponse due to the different photoexcited-charge-carrier trapping times in sp(2) and
48 Imaging the microchannel flows carrying thus photoexcited chelates of lanthanide ions allowed us to e
49 upled electronic states corresponding to the photoexcited chlorophyll special pair (donor), the reduc
50 namics of a three-spin system representing a photoexcited chromophore coupled to a stable radical spe
51 d structural rearrangement at the level of a photoexcited chromophore is known to occur in the femtos
52 ization of the molecular choreography of the photoexcited chromophore requires a spectroscopic techni
53 s studies have shown that the collision of a photoexcited chromophore with a ground-state chromophore
54                                Relaxation of photoexcited chromophores is a key factor determining di
55                             As a result, the photoexcited coumarin did not show any of the typical re
56 ults are consistent with the hypothesis that photoexcited CRY2 disengages its C-terminal domain from
57 clear bodies may result from accumulation of photoexcited CRY2-GFP waiting to be degraded.
58 ike kinases) interact with and phosphorylate photoexcited CRY2.
59         We have determined the steady state, photoexcited crystal structure of a flavin-bound LOV dom
60         The singlet fluorescence dynamics of photoexcited [Cu(I)(dmp)(2)](+) were measured in the coo
61 onal energy relaxation and redistribution in photoexcited cycloparaphenylene carbon nanorings with in
62 ergy transfer phenomenon that occurs between photoexcited D-/L-Trp enantiomers and rGO/gamma-CD givin
63 , demonstrating that both hole transfer from photoexcited DBFI-T to PSEHTT and electron transfer from
64        According to our analysis, 30% of the photoexcited diazo precursor molecules are eventually pr
65 ch liberates only trace hydrogen levels when photoexcited directly, does not appear to independently
66                   One major decay channel of photoexcited DNA leads to reactive charge transfer state
67 ium(III) acceptor, a substantial fraction of photoexcited donor exhibits fast oxidative quenching (>3
68 xcited-state relaxation and injection as the photoexcited dye relaxes through the (3)MLCT manifold to
69 adsorbed O2 for receiving electrons from the photoexcited dyes.
70                          Here we explore the photoexcited dynamics of molecules by an interaction wit
71              Evolution of the time-dependent photoexcited electron during the initial 5 fs after inst
72  photo-induced resonant tunneling in which a photoexcited electron in the STM tip is transferred to t
73  and short-circuit the cell by accepting the photoexcited electron on a subpicosecond time scale.
74 t absorption (TA) spectroscopy revealed that photoexcited electron transfer rates increase with incre
75 tite (alpha-Fe2 O3) is engineered to improve photoexcited electron-hole pair separation by synthesizi
76 nce time-domain simulations, suggesting that photoexcited electron-hole pairs in the silicon waveguid
77         Together this nano-architecture lets photoexcited electrons and holes dissociate instantaneou
78  results imply that the recombination of the photoexcited electrons and holes is suppressed by the sc
79 pathways for rapid and balanced transport of photoexcited electrons and holes, respectively, while mi
80                                              Photoexcited electrons are transferred to the metal and
81 HMe2(+)), which were capable of transferring photoexcited electrons directly to the negatively charge
82 he device is based on thermionic emission of photoexcited electrons from a semiconductor cathode at h
83 electron microscopy, we imaged the motion of photoexcited electrons from high-energy to low-energy st
84  a reduction step could occur by transfer of photoexcited electrons from the p-GaP photocathode and w
85 takes advantage of the reducing potential of photoexcited electrons in the conduction band of CdS and
86  (-) species is generated by the reaction of photoexcited electrons in the perovskite and molecular o
87                                          The photoexcited electrons of CZTS can be readily transporte
88 mechanism involving the coupling between the photoexcited electrons of the nanoparticles and the gold
89 mionic emission relies on vacuum emission of photoexcited electrons that are in thermal equilibrium w
90        It is found that both the transfer of photoexcited electrons to pyridinium and pyridinium adso
91 electrodes that can reduce water to H2 using photoexcited electrons.
92                            Hole injection by photoexcited ethidium followed by radical migration to o
93        Absorption of X-ray photons generates photoexcited Fe(II)(LS) domains whose size rapidly grows
94 tion triggered by electron transfer from the photoexcited flavin cofactor to the dimer.
95 rface, without changes in the others, as the photoexcited fraction is increased.
96                       The evolution from the photoexcited Franck-Condon MLCT state to the thermally e
97 y act as electron acceptors, whereas for the photoexcited fullerenes, SWCNTs act as electron donors.
98                                          The photoexcited GNRs enhanced the spin-spin and spin-lattic
99 s of the dynamics of hot electron cooling in photoexcited gold nanoparticles (Au NPs) with diameters
100                     Our result suggests that photoexcited graphene transfers a hot electron to benzoy
101 y to accept an electron through space from a photoexcited guest.
102 ure change leading to proton transfer on the photoexcited half of the 7-azaindole dimer.
103                                              Photoexcited heptanal is believed to undergo rapid inter
104  we use a metallointercalator to introduce a photoexcited hole into the DNA pi-stack at a specific si
105 tion-band electron following transfer of the photoexcited hole to Ag(+).
106                    It is not the presence of photoexcited holes and electrons, but a rise in temperat
107                         In CdS nanocrystals, photoexcited holes rapidly become trapped at the particl
108                  Under optical illumination, photoexcited hot carriers generated in the top layer tun
109 s owing to differences in decay channels for photoexcited hybrid plasmon-phonons and electrons.
110               The relaxation dynamics of the photoexcited hydrated electron have been subject to conf
111                   In a spin: the dynamics of photoexcited ICN(-) (Ar)(0-5) are presented.
112                                              Photoexcited intramolecular charge transfer (CT) states
113 G and CPC is promoted efficiently by HT from photoexcited Ir(III) when the modified bases are positio
114  Mechanistic investigations suggest that the photoexcited iridium catalyst facilitated the nickel act
115                              The dynamics of photoexcited lead-free perovskite films, CH3NH3SnI3, wer
116 ill significantly lower than that induced by photoexcited lipofuscin.
117 ging by detecting the acoustic response of a photoexcited material.
118                   In contrast to lipofuscin, photoexcited melanosomes did not substantially increase
119  The molecular structure and dynamics of the photoexcited metal-to-ligand-charge-transfer (MLCT) stat
120                                          The photoexcited metastable triplet state of Mg(2+)-mesoporp
121 ET quenching of both the singlet and triplet photoexcited MMb states, the direction of flow being det
122 rafast motion of electrons and nuclei of the photoexcited molecule presents a challenge to current sp
123                                          For photoexcited molecules, the nuclear dynamics determine t
124  observation of ultrafast charge transfer in photoexcited MoS2/WS2 heterostructures using both photol
125                         Energy transfer from photoexcited nanoparticles to their surroundings was stu
126 ansfer (ET) contributed to the relaxation of photoexcited nc-CdTe relative to the intrinsic radiative
127                                              Photoexcited (NCN)CNx in the presence of an organic subs
128 ate of hole-capture by the host polymer from photoexcited NCs.
129 diminishes, and blue emission from a trapped photoexcited neutral chromophore dominates because ESPT
130                                              Photoexcited Nickel(II) tetramesitylporphyrin (NiTMP), l
131 ithin approximately 10 ps, ligand binding to photoexcited NiDPP is progressively longer in pyridine,
132 ibited intramolecular charge-transfer within photoexcited NOM, leading to substantially increased rem
133                      IR detection shows that photoexcited o-phenylene thioxocarbonate (2) and 2-chlor
134 ited-state energy transfer prevails from the photoexcited oligofluorene to the energy accepting fulle
135 n data indicate that electron injection from photoexcited PbS QDs to PCBM occurs within our temporal
136 dence is given for an electron transfer from photoexcited Pc1 to the electron-accepting C60A that aff
137 rom photoexcited polymer, hole transfer from photoexcited PCBM, prompt (<100 fs) charge generation in
138  for simulating the nonadiabatic dynamics of photoexcited PCET are discussed.
139 derstanding the fundamental spin dynamics of photoexcited pentacene derivatives is important in order
140     The electron injection dynamics from the photoexcited perovskite layers to the neighboring film s
141 ight perylenes per porphyrin in toluene, the photoexcited perylene-monoimide dye (PMI) decays rapidly
142 observe more than a 200-fold increase in the photoexcited phosphorescent emission of PtOEP (2,3,7,8,1
143 en shown to quench the catalytic activity of photoexcited, phosphorylated rhodopsin in a reconstitute
144 nhancing electron transfer rates between the photoexcited photoredox catalyst and the substrate.
145 g at two well-separated energies in a highly photoexcited planar microcavity at room temperature.
146         These include electron transfer from photoexcited polymer, hole transfer from photoexcited PC
147 o determine the interspin distance between a photoexcited porphyrin triplet state (S = 1) and a nitro
148             For example, with respect to the photoexcited porphyrins and phthalocyanines, SWCNTs usua
149       In the triple mutant, the decay of the photoexcited primary electron donor (P) occurs with a ti
150 ations are triggered by reorientation of the photoexcited protein.
151  DBFI-T to PSEHTT and electron transfer from photoexcited PSEHTT to DBFI-T contribute substantially t
152                  Approximately 10-50% of all photoexcited pyrimidine bases decay via the (1)npi* stat
153 oxidation is initiated by hole transfer from photoexcited QD to surface DTO and that these substrates
154                                              Photoexcited QDs could be used in the study of the effec
155  this process, in particular, whether or not photoexcited QDs play a direct role in the photoinduced
156 ates in the energy transfer process from the photoexcited QDs to the molecular energy acceptor.
157 ination kinetics of the electron and hole of photoexcited QDs.
158                           Here, we show that photoexcited quantum dots (QDs) can kill a wide range of
159                         Cu(I) oxidation by a photoexcited Re(I)-diimine at position 124 on a histidin
160        The analysis revealed that 30% of the photoexcited receptor molecules followed Cycle 1 through
161 , while CPG undergoes ring-opening both with photoexcited [Rh(phi)2(bpy)]3+ and with [Ru(phen)(dppz)(
162                                            A photoexcited rhodium intercalator, Rh(phi)2DMB3+ (phi =
163 mma and, as heterotrimeric proteins, bind to photoexcited rhodopsin (R*).
164 Gbetagamma(t) or activation of transducin by photoexcited rhodopsin (R*).
165                                              Photoexcited rhodopsin activates an enzymatic cascade in
166 al rod cells, which controls the lifetime of photoexcited rhodopsin by inhibiting rhodopsin kinase.
167                In vertebrate photoreceptors, photoexcited rhodopsin interacts with the G protein tran
168 ydrolysis occurring over the period in which photoexcited rhodopsin is quenched.
169 ansducin and an increased activation rate by photoexcited rhodopsin or more efficient activation of c
170 GDP-bound x-ray structure of Gt reveals that photoexcited rhodopsin promotes the formation of a conti
171 well established that normal inactivation of photoexcited rhodopsin, the GPCR of rod phototransductio
172 restin molecules are available to quench the photoexcited rhodopsin.
173 ial first step in the prompt deactivation of photoexcited rhodopsin.
174 er effect spectroscopy while it was bound to photoexcited rhodopsin.
175 ntermediates are generated upon quenching of photoexcited Ru*(bpz)3(2) with a variety of thiols.
176                The excited-state lifetime of photoexcited [Ru(bpy)(2)(pbnHH)](2+) is found to be abou
177 systems, electron-transfer occurred from the photoexcited ruthenium polypyridyl donor to the pentammi
178 nfrared (TRIR) spectroscopy was performed on photoexcited ruthenium polypyridyl-DNA crystals, the ato
179 odopsin in the native membrane suggested the photoexcited samples were heterogeneous.
180                                              Photoexcited semiconductor nanoparticles undergo charge
181 c photocurrent results from reduction of the photoexcited sensitizer by free electrons in ITO.
182 sensitizer-acceptor design in which multiple photoexcited sensitizers resonantly and simultaneously t
183  receptor, in particular the lifetime of the photoexcited signaling states.
184 single-junction solar cells by splitting one photoexcited singlet exciton (S1) into two triplets (2T1
185                           The reason is that photoexcited singlet oxygen is highly reactive, so the p
186 produces two triplet excited states from one photoexcited singlet state, is a means to circumvent the
187 Correspondingly, charge-separation ET from a photoexcited singlet zinc porphyrin incorporated within
188 neration of two spin triplet states from one photoexcited singlet.
189  experimental constraints on the reaction of photoexcited SO2 with atmospheric hydrocarbons.
190 of an applied external electric field on the photoexcited species of CH3NH3PbI3 thin films, both at r
191 t affects the nonradiative decay rate of the photoexcited species.
192 y measuring an electromotive force driven by photoexcited spin-polarized electrons drifting through G
193 ith high reactivity with O(2) at the triplet photoexcited state and favorable redox potential and cou
194 , the role of small polaron formation in the photoexcited state and how this affects the photoconvers
195 eds through rapid internal conversion of the photoexcited state into a dark state of multi-exciton ch
196 presents a novel case in which the molecular photoexcited state is at the edge of the conduction band
197       In the system under investigation, the photoexcited state lies close to the bottom of the TiO 2
198 sion of (+)-2 into 14 by binding the triplet photoexcited state of 6 in proximity to (+)-2.
199 chieving catalytic promiscuity that uses the photoexcited state of nicotinamide co-factors (molecules
200 n kinase and to modulate the lifetime of the photoexcited state of rhodopsin (Rh*), the visual pigmen
201 sistent with that of photolyase in which the photoexcited state of the purine donates an electron to
202 ssion occurs directly from the initial 1B(u) photoexcited state on ultrafast time scales.
203                                          The photoexcited state Ru(II*) of Ru2Z is reduced to Ru(I) b
204 ays the electronic relaxation of the initial photoexcited state within 200 fs.
205 dy configurations within the lifetime of the photoexcited state.
206 m a particular C-O bond stretch in the pipi* photoexcited state.
207 s a result of changes in the distribution of photoexcited-state energies and, hence, in the density o
208 h in generating a nonuniform distribution of photoexcited states and in driving the ET process.
209  the broad emission comes from the transient photoexcited states generated by self-trapped excitons (
210 estigation of the dynamics and relaxation of photoexcited states in conjugated polyfluorenes, which a
211 at, like their dihydrophenazine analogs, the photoexcited states of phenoxazine photoredox catalysts
212            The singlet S(1) and triplet T(1) photoexcited states of the compounds containing MM quadr
213 ntal and computational studies show that the photoexcited states of the two complexes are very differ
214 fer, injection in particular, accelerate for photoexcited states that are delocalized between the two
215 he structure of transient molecules, such as photoexcited states, in disordered media (such as in sol
216 oflavin dimers do not interact in ground and photoexcited states.
217                                 The study of photoexcited strongly correlated materials is attracting
218    This fundamental insight into the role of photoexcited surface FLPs for catalytic CO2 reduction co
219               Our results also indicate that photoexcited SWCNTs can catalyze lipid peroxidation simi
220 ransfer states due to electron transfer from photoexcited tetracene to the lowest unoccupied molecula
221 e used, while in cage oxygen transfer to the photoexcited (thio)pyrylium derivatives have been charac
222 g on the interfacial charge transfer between photoexcited TiO2 and SWNTs as well as the mechanism of
223         Longer than 1 ns lifetimes for holes photoexcited to the lower valence subband offer a potent
224 ace and bulk transient carrier dynamics in a photoexcited topological insulator can control an essent
225 g the electronic and geometric structures of photoexcited transient species with high accuracy is cru
226 e singlet excited state, but does quench the photoexcited triplet excited state as a function of TEMP
227                    The delocalization of the photoexcited triplet state in a linear butadiyne-linked
228 lar oxygen via the presumed quenching of the photoexcited triplet state of 6.
229  temperature dependence and splitting of the photoexcited triplet state of myoglobin in which the iro
230 troscopic probe used in these studies is the photoexcited triplet state of Trp37, which is associated
231 phyrin oligomers lead to localization of the photoexcited triplet state on a single porphyrin unit, w
232 y acquired from the spin polarization of the photoexcited triplet state spectrum.
233                                          The photoexcited triplet states of a series of linear and cy
234             The transient EPR spectra of the photoexcited triplet states of the porphyrin monomer and
235 obins (Mb) the fluorescence quenching of the photoexcited tryptophan 14 (*Trp(14)) residue is in part
236 cond of the electron-transfer process in the photoexcited type-II heterostructure-a fundamental pheno
237                                              Photoexcited visual pigment activates the GTP-binding pr
238 anism involves the ultrafast collapse of the photoexcited wave function due to nonadiabatic electroni
239 ibit hole injection into surface states when photoexcited with visible light (lambda = 400-680 nm).
240 s when other bacteriorhodopsin molecules are photoexcited within the two-dimensional lattice of the p
241                       Electron transfer from photoexcited zinc porphyrin to C(60) is witnessed in the
242 the vesicle was capable of reacting with the photoexcited zinc porphyrin.

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