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1 ven on nanosecond times following an intense photoexcitation.
2 lly long-lived excited state is formed after photoexcitation.
3 ia a dark surface prereduction step prior to photoexcitation.
4 ion reactions under conditions of continuous photoexcitation.
5 d defect and trap states after above-bandgap photoexcitation.
6 uctural phase progression in a VO2 film upon photoexcitation.
7 cence and its dependence on the intensity of photoexcitation.
8 ewis acidity of MV(2+) is indeed enhanced by photoexcitation.
9 and tetracene within the first 500 fs after photoexcitation.
10 ases the transcriptional repressor PpsR upon photoexcitation.
11 lection of carriers from plasmons and direct photoexcitation.
12 mal change of interaxial lattice angles upon photoexcitation.
13 es taking place in the ground state and upon photoexcitation.
14 resonance-Raman spectrum following ultrafast photoexcitation.
15 vealed rapid demagnetization within 90 fs of photoexcitation.
16 calization of the excitonic states following photoexcitation.
17 -trans-retinal from photoreceptors following photoexcitation.
18 d throughout the early time scales following photoexcitation.
19 ergy to the fullerene inside the cavity upon photoexcitation.
20 ow how dibenzoyldiethylgermane 1 reacts upon photoexcitation.
21 ta on ring A show no rotation of ring A upon photoexcitation.
22 ated electrons adjacent to the diamond after photoexcitation.
23 s of the products formed via its ultraviolet photoexcitation.
24 protein matrix senses and responds to flavin photoexcitation.
25 ge generation primarily occurs 2-10 ns after photoexcitation.
26 the optical constants following femtosecond photoexcitation.
27 PYP is under direct experimental control by photoexcitation.
28 the sensitizers necessary for singlet state photoexcitation.
29 'off' intermittently, even under continuous photoexcitation.
30 upling and a high reorganization energy upon photoexcitation.
31 l stimuli including electrostatic gating and photoexcitation.
32 thiophenone molecules following ultraviolet photoexcitation.
33 ng to efficient energy transfer (>85 %) upon photoexcitation.
34 lution to the conical intersection following photoexcitation.
35 ution of multi-exciton populations following photoexcitation.
36 zation mechanism for the formation of 2 upon photoexcitation.
37 fast charge-transfer process within 20 ps of photoexcitation.
38 unds become weakened (and strengthened) upon photoexcitation.
39 induced by microwave, mm-wave, and terahertz photoexcitation.
40 expression) BLUF domain before and following photoexcitation.
41 an intramolecular charge-transfer event upon photoexcitation.
42 ymer interface, both mediated by the polymer photoexcitation.
43 induced bleaching rises abruptly 20 fs after photoexcitation.
44 open new relaxation channels for high-energy photoexcitations.
46 the generation of reactive intermediates by photoexcitation, [1,3]-dipolar cycloaddition chemistry,
49 ion is observed at early times following the photoexcitation, accompanied by faster motions of vanadi
50 External stimuli, such as electric field and photoexcitation, also play an important role in controll
52 arises within 60 +/- 20 fs after ultraviolet photoexcitation and decays with a time constant of 110 +
53 s are generated almost instantaneously after photoexcitation and dissociate in 2 ps forming highly mo
54 surements have been used to demonstrate that photoexcitation and electron injection by the MLCT excit
55 rge build-up within protein multilayers upon photoexcitation and external injection is obtained by Ke
58 e existence of an intermediate state between photoexcitation and proton transfer that lives for 3 ps.
60 oseconds at the above-threshold-level (~20%) photoexcitations and the distinct dynamics in diffusive
61 ntiaromatic excited state during the initial photoexcitation, and by the subsequent relief of this an
62 cesses immediately following charge transfer photoexcitation, and highlights the molecular features n
63 lled intermolecular processes directly after photoexcitation, and their proper description gives acce
64 scale, and the structural changes caused by photoexcitation are being probed by vibrational spectros
65 H, CH3, CH2CH3, CH2CH2CH3) nanoclusters upon photoexcitation are discussed using time-dependent densi
67 t the hot carriers in Cu-THQ generated after photoexcitation are highly mobile and undergo fast local
68 st at about the microsecond time scale after photoexcitation are key to the photocathode behavior obs
70 otoprotective mechanisms to dissipate excess photoexcitation as heat in a process called nonphotochem
74 ed and the spin-split VB gap is reduced upon photoexcitation before relaxing to equilibrium as the ca
75 it undergoes ligand release and doming upon photoexcitation, but its ferric form does not release th
76 ible for photosensitization of aryl iodides (photoexcitation by 254 nm UV light) with blue LED light
77 the merging of the dinuclear gold catalyst (photoexcitation by 315-400 nm UVA light) with Na(2)CO(3)
79 sting complex 2 of purple bacteria following photoexcitation by creating a chiral two-dimensional map
81 Short-term lattice instability caused by photoexcitation can be effective in driving a photochemi
83 cle-molecule hybrid systems by near-infrared photoexcitation can undergo efficient upconversion via a
84 hat enone and ketone functional groups, upon photoexcitation, can direct site-selective sp(3) C-H flu
85 of unconventional PCs operates via a single photoexcitation/catalytic cycle, where the TM complex pl
87 d-type cells and behavioral mutants prior to photoexcitation, comparison of their absorption spectra,
90 l excitons produce a dominant blue-shift for photoexcitation detuned from resonance by less than the
92 nd excited-state dynamics following resonant photoexcitation enable the selective deformation of N-H
93 calculations to produce probes with tunable photoexcitation energies and excited states possessing c
98 ail in wide-stretched conformations and upon photoexcitation exhibit symmetry-breaking charge separat
99 of the triplets appearing within 1 ps after photoexcitation followed by a slower phase of triplet gr
100 ion (internal photoemission versus interband photoexcitation followed by electron transfer) are explo
106 acts and observed that charge extraction for photoexcitation >50 micrometers away from the contacts a
107 sport and recombination under a steady-state photoexcitation has been an important goal of organic el
110 ion of a phenylalanine residue after near-UV photoexcitation have been investigated in an isolated pe
111 tes in the octahedral sheet within 0.6 ps of photoexcitation; (ii) Mn(III) migration into the interla
112 ast response of self-energy to near-infrared photoexcitation in high-temperature cuprate superconduct
113 Experiments have established that intense photoexcitation in several metallic ferromagnets leads t
114 ap states with continuous-wave (CW) infrared photoexcitation in solution-processing quasi-2D perovski
116 and length scales of electrical response to photoexcitation in van der Waals materials, which is ess
118 of excess excitation energy on the nature of photoexcitations in donor-acceptor pi-conjugated materia
119 Feedback mechanisms that dissipate excess photoexcitations in light-harvesting complexes (LHCs) ar
120 al semiconductors, studies of above-band-gap photoexcitations in strongly correlated materials are st
122 mission bands and ultrafast dynamics of spin photoexcitations in two newly synthesized pi-conjugated
123 nes, the rates of charge recombination after photoexcitation increase with increasing electron donor-
124 a reduction in bond-length alternation upon photoexcitation, indicating significant cumulenic charac
125 sed to probe the ultrafast coherent decay of photoexcitations into charge-producing states in a polym
126 complexes accomplish the rapid conversion of photoexcitations into spatially separated electrons and
130 l behavior of luminescent nanomaterials upon photoexcitation is necessary to expand photocatalytic an
132 wn that the mirror-image process of acceptor photoexcitation leading to hole transfer to the donor is
134 uron activity, via either photoinhibition or photoexcitation, led to a decrease in the power of choli
135 ased optical gain thresholds, demanding high photoexcitation levels to achieve population inversion (
137 tion via i.v. injection, recharged by 400-nm photoexcitation light in superficial blood vessels durin
138 g lived ligand-to-metal charge transfer upon photoexcitation, making this material suitable for photo
139 and provide further evidence that rhodopsin photoexcitation may trigger signaling events alternative
140 upon illumination and suggest that rhodopsin photoexcitation may trigger signaling events alternative
141 elucidated the cellular mechanisms for HerGa photoexcitation-mediated cell damage using fluorescence
142 ents reveal that the structural changes upon photoexcitation occur mainly in the axial direction, whe
143 as studied in a pump-probe geometry in which photoexcitation occurred by counter-propagating the expa
147 etric and electronic changes that occur upon photoexcitation of [Cu(I)(dmp)(dppe)](+) in crystalline
149 vidence suggests this species is accessed by photoexcitation of a charge-transfer complex that forms
150 istent with a coupling pathway that includes photoexcitation of a copper-amidate complex, followed by
153 d triplet generation by singlet fission upon photoexcitation of a new aggregate of the carotenoid all
155 in a magnetic field using a microwave pulse, photoexcitation of A results in the formation of an enta
156 e have explored the dynamics occurring after photoexcitation of a trinuclear u(3)-oxo-bridged Mn(III)
157 ted by these bisretinoids have revealed that photoexcitation of A2E by wavelengths in the visible spe
160 offer a promising alternative and show that photoexcitation of alpha-sexithiophene (alpha-6T) films
161 rmediate, a radical ion pair, generated from photoexcitation of an initially formed charge-transfer c
163 ir (RP), (1)(G(+*)-PDI(-*)), while selective photoexcitation of Aq at 355 nm generates the correspond
165 , 100, and 500 micros after room-temperature photoexcitation of bovine rhodopsin in a lauryl maltosid
166 e made at delays from 1 micros to 2 ms after photoexcitation of bovine rhodopsin in hypotonically was
167 typically low and some studies suggest that photoexcitation of carbon nanotube excitonic transitions
169 etramers in toluene shows that the selective photoexcitation of Chl results in intramolecular electro
171 y sensitive chemical intermediates formed by photoexcitation of cryptochrome proteins in the retina.
172 ny spontaneously reacting anion source using photoexcitation of CsPbX3 NCs as the triggering mechanis
182 we use the mid-infrared and terahertz (THz) photoexcitation of exclusive intraband transitions to en
184 dynamics of excitons following non-resonant photoexcitation of free electron-hole pairs have been ch
189 advanced theoretical simulations, show that photoexcitation of methyl azide by a 10-fs UV pulse at 8
190 H(2)PO(4)(-), Cl(-), etc.) often require the photoexcitation of moderately pi-acidic NDIs to generate
195 ensitivity to the Fe-NO binding after 532-nm photoexcitation of nitrosylmyoglobin (MbNO) in physiolog
203 scopy experiments demonstrate that selective photoexcitation of Re(I)-bpy results in electron transfe
204 R-XANES) measurements at the Eu L3 edge upon photoexcitation of several Eu(III)-based luminescent lan
207 ic processes, to directly participate in the photoexcitation of substrates either by forming a photoa
208 ic background reactions that occur by direct photoexcitation of substrates while unbound to catalyst.
209 -electron reduction of aryl halides upon the photoexcitation of tetrasulfide dianions (S(4)(2-)).
210 s in which photocurrent is generated through photoexcitation of the acceptor followed by hole transfe
212 dentity of the light-adapted state following photoexcitation of the bound flavin remains elusive.
215 t absorption spectroscopy confirm that after photoexcitation of the donor HBC a photoinduced electron
217 spectroscopic studies showed that, following photoexcitation of the electron acceptor, fast electron
219 t generation in organic solar cells involves photoexcitation of the electron donor, followed by elect
222 surface Cu atoms, which is brought about by photoexcitation of the localized surface plasmon resonan
223 od as a process which predominantly involves photoexcitation of the lower ionization potential specie
225 alysts for hydrogen evolution by synergistic photoexcitation of the MOF frameworks and electron injec
226 icrochannel provided a means for pulsed-like photoexcitation of the moieties carried by the fluid.
234 easurements corroborated that upon selective photoexcitation of the perylenediimides (1a/1b), an ener
237 through time-resolved emission studies that photoexcitation of the QDs is followed by energy transfe
239 p-coumaric acid carbonyl group following the photoexcitation of the R52Q mutant of photoactive yellow
240 d photoelectron imaging is used to show that photoexcitation of the S(1)(paipai*) state of the methyl
241 the conduction band in Bi2Se3 allows direct photoexcitation of the surface electrons in n-doped samp
245 ited-state spectral dynamics after simulated photoexcitation of this noncavity hydrated electron show
246 port a radical-based mechanism involving the photoexcitation of TiO(2) with 390 nm light in the prese
247 ol of the THz emission is achieved by tuning photoexcitation of ultrafast photocurrents via the photo
250 lectron must either be populated directly by photoexcitation or the state must lie in a band gap (or
252 lectrons from intrinsic defects, dopants and photoexcitation play a key role in many of the propertie
253 the bulk material in real time, follows the photoexcitation process in both the insulating and metal
254 limited by a well-defined T*neq(p) line, the photoexcitation process triggers the evolution of antino
255 ot interact in an intermolecular fashion and photoexcitation produces emission features characteristi
257 ence both electron and proton transfers upon photoexcitation, proving an amenable model system to stu
259 ent is proposed to be due to the accelerated photoexcitation rate of the M(412) (in the presence of t
261 first principles calculations, we find that photoexcitation reduces the Peierls-like electronic inst
263 , and their influence on the dynamics of the photoexcitations remain an open issue to be clarified.
264 now, the initial quantum dynamics following photoexcitation remains elusive in the hybrid perovskite
265 erated luminescence and charges from a local photoexcitation spot in thin films of lead tri-iodide pe
267 ous polarization of a nonpolar molecule upon photoexcitation (the sudden polarization effect) earlier
273 rom ZnPc to C60 occurs in about 150 fs after photoexcitation, the localization and energy relaxation
274 ility of geminate charge recombination, upon photoexcitation, thereby resulting in a long-lived charg
278 S1 state is spectroscopically dark, whereas photoexcitation to higher-lying singlet excited S2 and S
282 suggest the following decay mechanism: upon photoexcitation to the S(1) state, an ultrafast adiabati
284 d regime of fast diffusion immediately after photoexcitation, together with spontaneous electron-hole
287 roduct spectral intensities as a function of photoexcitation wavelength provides information on the w
288 ld for higher excess energies directly after photoexcitation when compared to the exciton population.
289 hromophores form charge-transfer states upon photoexcitation which relax with a moderate fluorescence
290 fluorene-alt-benzothiadiazole) polymer under photoexcitation, which is completely absent when microca
291 ge in which the Pt-Pt distance shortens upon photoexcitation, which leads to the formation of two dis
292 ers between these components were induced by photoexcitation, which led to the formation of hydrogen
293 lectron appears inside TiO2 immediately upon photoexcitation with a high probability (~50%), bypassin
295 tive to a benchmark cyanine dye (ICG) during photoexcitation with exceptional photostability from the
297 atures of the monomer and the foldamer after photoexcitation, with an additional time constant for th
298 of transient electric fields that form upon photoexcitation within bare p-GaInP2, p-GaInP2/platinum
300 ver that the Auger spectrum as a function of photoexcitation--X-ray-probe delay contains valuable inf