ライフサイエンスコーパス: electronic state

1 osecond lifetime of the virtual intermediate electronic state.

2 structural evolution of CNCbl in the excited electronic state.

3 ng an absence of interlayer coherency of the electronic state.

4 hat prevents deexcitation back to the ground electronic state.

5 oxide [IBr-(CO2)] on the second excited (A') electronic state.

6 tion after the wheel is reduced to its final electronic state.

7 makes the triplet state the computed ground electronic state.

8 g reactions, suggesting they are of the same electronic state.

9 tic shielding around these molecules in each electronic state.

10 a material in a magnetic field reflects its electronic state.

11 tifying how quantum interactions modify bare electronic states.

12 on between oxygen 2p and transition metal 3d electronic states.

13 arious dissociation pathways along different electronic states.

14 at its surface may form two-dimensional (2D) electronic states.

15 ctrum that are associated with each of these electronic states.

16 ansient energy level matching among multiple electronic states.

17 reflect the discreteness of their localized electronic states.

18 s origin in vibronic coupling with low-lying electronic states.

19 s of the ground and highly excited (Rydberg) electronic states.

20 denced both in the ground and in the excited electronic states.

21 l singlet, triplet, and closed-shell singlet electronic states.

22 ectrodes correlate with the local density of electronic states.

23 batic transitions within the manifold of the electronic states.

24 arkably different energetic orderings of its electronic states.

25 tic simulations of a four-state model of the electronic states.

26 ting that the two phenomena involve the same electronic states.

27 have been found to be useful probes of their electronic states.

28 and can reversibly interconvert between two electronic states.

29 antum mechanical mixtures of vibrational and electronic states.

30 entrating on reactions which occur on ground electronic states.

31 different rules of aromaticity in different electronic states.

32 ral features to transitions between specific electronic states.

33 ersections connecting the excited and ground electronic states.

34 ry, as long as one performs a sum over final electronic states.

35 urface states without interference from bulk electronic states.

36 e transfer (MLCT) character of the low-lying electronic states (641, 732, and 735 nm) observed for CP

37 tem to pass through at least three different electronic states, a process that is remarkably complex

38 ntermediates which originated from different electronic states accessed by electron transfer.

39 addition, the heterojunctions show distinct electronic states across the interface, as revealed by K

40 lations, we show that grain-boundary-induced electronic states act as acceptors, resulting in a negat

41 n strain fields, segregation of defects, and electronic states, adding a new dimension to understandi

42 relatively insensitive to differences in the electronic states along the Cu-O bond directions.

43 ts on the evolution of the low-lying singlet electronic states along the OO bond suggest that SiH2OO

44 cal evolution of quantum discord between the electronic state and the vibrational degrees of freedom

45 The interplay and coupling between the electronic state and vibrational manifold is fundamental

46 the different routes available to tune their electronic states and active sites.

47 We discuss the generation of excited electronic states and electron-hole pairs (excitons) at

48 ture becomes central only for non-stationary electronic states and has profound consequences for time

49 from its large energy window for Dirac-like electronic states and have been explored for application

50 ides, particularly on the formation of novel electronic states and manifested metal-insulator transit

51 , delocatization properties of participating electronic states and non-adiabatic coupling strengths.

52 o prepare lattice band populations, internal electronic states and quasi-momenta, and to produce spin

53 rly complete band gap between full and empty electronic states and stable compounds; we can thus pres

54 do not show instability in their respective electronic states and that the higher energy configurati

55 iffer in how they access the vibrational and electronic states and the frequency of their output sign

56 r two conditions: one is the symmetry of the electronic states and the other is their relative phase.

57 ed states report on the interactions between electronic states and their environment.

58 ound, direct experimental probes of relevant electronic states and their hybridization are limited.

59 d to lift the degeneracy of partially filled electronic states and to open a HOMO-LUMO gap, the Jahn-

60 In the present paper, the nature of electronic states and transport properties of nanostruct

61 erties of MHPs, including crystal structure, electronic states, and charge transport, is provided fir

62 for modification of either ground or excited electronic states, and longer-lived charge separated sta

63 a transient close to a picosecond (ps), new electronic states appear in the O K-edge x-ray absorptio

64 Highly excited electronic states are challenging to explore experimenta

65 In polyatomic molecules, however, the electronic states are closer together, leading to more c

66 Moreover, strongly anisotropic or 1D electronic states are formed in Pb films as modulated by

67 Their low-lying electronic states are key to their remarkable reactivity

68 copically coexisting itinerant and localized electronic states are natural candidates for the pairing

69 suggestion that chemically generated excited electronic states are relevant to mammalian biology.

70 nterlayer thermal transport, even though all electronic states are strongly confined within individua

71 Unusual electronic states arise at ferroelectric domain walls du

72 itive charge states in dramatically distinct electronic states around the Fermi energy and formation

73 r2 IrO4 induces distinct 1D quantum-confined electronic states, as observed from optical spectroscopy

74 The ground electronic state assignments based on ion reactivity are

75 pectra of an essentially unexplored class of electronic states associated with double inner-shell vac

76 nal boundary is expected to possess peculiar electronic states associated with edge states of graphen

77 femtosecond control of spin-polarization for electronic states at around the Dirac cone.

78 ers detailed information on the evolution of electronic states at different electrochemical stages.

79 Electronic states at domain walls in bilayer graphene ar

80 th coexisting Dirac-fermions and pseudogaped electronic states at low energies.

81 ntum dots (CQDs) feature a low degeneracy of electronic states at the band edges compared with the co

82 ) structure, with a linear dispersion of the electronic states at the corners of the Brillouin zone (

83 The ability to control electronic states at the nanoscale has contributed to ou

84 new approach for tuning the energies of the electronic states based on the unusual strength of the C

85 Upon photoexcitation to the higher singlet electronic state (Bb) the structure of tryptophan is dis

86 s in dissociation are explained by different electronic states being accessed upon electron transfer

87 l points due to the decreasing occupation of electronic states below the Fermi level (EF) with increa

88 decompose the spectra into contributions of electronic state blocking and photo-induced band shifts

89 ed class of materials having insulating bulk electronic states but conducting boundary states disting

90 in-polarized hybridization between 5f and 6d electronic states by means of X-ray magnetic circular di

91 in momentum-space (k-space) generates exotic electronic states called 'heavy fermions'.

92 However, whether the competing electronic state can be suppressed to enhance T(c) in HT

93 This dramatic switch in favored electronic states can be ascribed to changes in ring aro

94 rtheless, understanding how their correlated electronic states can be manipulated at the nanoscale re

95 -femtosecond-laser-excited coherence between electronic states can switch magnetic order by 'suddenly

96 nce of quasicrystalline order, the ways that electronic states change remain a mystery.

97 Fe-based moieties experience structural and electronic-state changes.

98 re the [Fe{H2 B(pz)2 }2 (bipy)] moiety to an electronic state characteristic of the high spin state a

99 The model consists of six electronic states characterized by the number of electro

100 detailed origins of photocurrent generating electronic state coherence pathways.

101 idence for roaming pathways in two different electronic states, corresponding to both previously docu

102 determined by complex dynamics involving key electronic states coupled to particular nuclear motions.

103 osphorus, arising from the strong interlayer electronic-state coupling.

104 Excited electronic states created by UV excitation of the diribo

105 g ponderomotive interaction, dressing of the electronic states, creation of coherent phonon pairs, an

106 ages of mixed-valence para-Fe2 show that the electronic state density remains symmetric.

107 alence meta-Fe2 show pronounced asymmetry in electronic state density, despite the structural symmetr

108 In contrast, the delocalized electronic states detectable by quasiparticle interferen

109 to highly coherent domains with delocalized electronic states displaying metallic behavior.

110 New electronic states emerge as a result of multiple copies

111 tron interaction are the most prominent, the electronic states exhibit a diverging spatial correlatio

112 Theorists have recently proposed that novel electronic states exist at these boundaries, but very li

113 porphyrins, relaxes rapidly through multiple electronic states following an initial porphyrin-based e

114 ified zone-folding scheme that generates the electronic states for all FLG materials from that of the

115 ysical properties of silicon provide surface electronic states for dynamic nuclear polarization, extr

116 We study highly excited diskoid-like electronic states formed in the vicinity of charged and

117 -body interactions are enhanced, driving the electronic states from a ferromagnetic polaronic metal t

118 iding a possible route to obtaining metallic electronic states from the parent insulating states in t

119 tical and experimental studies of the ground electronic state (GES), redox potentials, and C-H aminat

120 roscopy, one of the most sensitive probes of electronic states, has been mainly limited to ex situ ex

121 uired for the creation of the red phase, its electronic states have a predominant intrachain characte

122 We report the observation of a related electronic state in a noncuprate material, strontium iri

123 al conductivities to probe the nature of the electronic state in PrBa(2)Cu(4)O(8) as a function of te

124 ere, the authors demonstrate the coupling of electronic states in a double quantum dot to form Andree

125 le spectral function measures the density of electronic states in a material as a function of both mo

126 nfluenced by the density and distribution of electronic states in band gap and architectures of the s

127 It has recently been shown that electronic states in bulk gapless HgCdTe offer another r

128 e been shown to generate unusual interfacial electronic states in complex oxides.

129 freedom produces multiple nearly degenerate electronic states in correlated electron materials.

130 erful tool in the search for broken symmetry electronic states in cuprates, as well as in other mater

131 Electronic states in disordered conductors on the verge

132 d scanning tunneling microscopy to visualize electronic states in Ga(1-x)Mn(x)As samples close to thi

133 tructural quality can introduce well-defined electronic states in graphene and modify its electronic

134 yer separation is sufficient to decouple the electronic states in individual layers, leading to a tra

135 n alloys are related to the formation of new electronic states in response to alloying rather than to

136 e the generation of highly desired localized electronic states in the 2D surface.

137 tal angular momentum components of the bound electronic states in the atom are then compared with pho

138 rallel to the surface respectively, and form electronic states in the band gap of SrTiO3.

139 sion relations (energy versus wavevector) of electronic states in the copper oxides at binding energi

140 by the presence of localized, nonconductive electronic states in the optical gap.

141 follow the potential-dependent occupancy of electronic states in the polymer.

142 c and nuclear structure for critical excited electronic states in the relaxation pathway characterize

143 when the band lineup between the ambient and electronic states in the semiconductor is appropriate.

144 tions show that the spatial distributions of electronic states in the system are similar in character

145 ch as frontier orbital density take only the electronic state into account.

146 ssical model that classifies all the channel electronic states into four groups based on the sign of

147 define an experimental tool for identifying electronic states involved in spin-dependent exchange in

148 and determine the energy profiles of the two electronic states involved in the electron transfer (ET)

149 lue is only 0.10, suggesting that its ground electronic state is best described as a H2C=O(delta+)-O(

150 ter to the templating molecule itself, their electronic state is highly susceptible to thermal fluctu

151 ution of nuclear wavepackets across multiple electronic states is a general means for studying the st

152 rization time on acetylene dication in lower electronic states is not possible and point to misinterp

153 acy of the active orbitals in both competing electronic states; it is thus a purely electronic transi

154 s have a strongly spin-orbital coupled (SOC) electronic state, J eff = (1/2), that defines the electr

155 e properties of hydrogenic, diffuse, excited electronic states, known as superatom molecular orbitals

156 The competition between these degenerate electronic states largely determines the functionalities

157 of these materials, in which the topology of electronic states leads to robust surface states and ele

158 interfaces and address interactions between electronic states, local electromagnetic fields (tip-ind

159 Here, we resolve the electronic states localized on domain walls in a Mott-ch

160 selection rules and appearance of low-energy electronic states localized on the acenes due to gradual

161 A two-electronic-state model was used to follow the dynamics,

162 ely studied, experimental work on the ground electronic state, most relevant to chemistry and biology

163 es and the characterization of four of their electronic states, namely 1) the ground state, 2) the ex

164 performed based on changes in the density of electronic states near the Fermi edge, which was used as

165 ensity, and consistent with the existence of electronic states near the spin-degenerate Dirac point o

166 The singlet diradical electronic state of 2 is 10 kcal mol(-1) higher than the

167 The nature of the electronic state of a metal depends strongly on its dime

168 ron-transfer theories is the coupling of the electronic state of a molecule to its structure.

169 surface composition, atomic arrangement, and electronic state of bimetallic catalysts could be differ

170 -growth step, (3) the probable oxidation and electronic state of Co during the polymerization, (4) th

171 esting that NMR may be a useful probe of the electronic state of copper sites in proteins.

172 Our results show that the ground electronic state of Fe(2+) at the critical pressure Pc o

173 onal potential energy surface for the ground electronic state of H2-CO with an estimated uncertainty

174 f NO2, which then recombines with the ground electronic state of IMD radical to form IMD-UR and N2O i

175 and the effects of compression on the ground electronic state of iron, electronic and magnetic states

176 lation of the Fe protein does not affect the electronic state of its metal cluster and prevents assoc

177 We propose that a narrow electronic state of significant oxygen 2p character near

178 olet absorption spectra for the lowest-lying electronic state of subcritical and supercritical water.

179 residue, which occurs from the ground ( X ) electronic state of the cation radical.

180 a reversible electrocatalyst, show that the electronic state of the electrode strongly biases the di

181 rily in terms of the local site geometry and electronic state of the Mn(III) ion, as best evidenced b

182 tential energy surface of the ground doublet electronic state of the peptide radicals provided rate c

183 n the potential energy surface of the ground electronic state of the radical.

184 mental limit (i.e. one unit-cell-thick), the electronic state of the SLs changed from a Mott insulato

185 opic and computational studies show that the electronic state of the {FeNO}(7) complex is best descri

186 ctric materials because the strain state and electronic state of these materials are strongly coupled

187 density functional theory the structure and electronic state of three porphyrinic moieties, CoN4C12,

188 a carbene-like triplet state similar to the electronic state of triplet phenyl cations.

189 g across a heterogeneous energy barrier, via electronic states of alanine and tryptophan, and by rela

190 h and polarization for the optical trap, two electronic states of an atom can experience the same tra

191 The reversible switching between electronic states of azobenzene can be controlled throug

192 sitions in which the electron is promoted to electronic states of different character, in some cases

193 ectronic structure of the two lowest excited electronic states of FAD and FADH(*) in folate-depleted

194 Here the electronic states of Gd atom trapped in open Fe corrals

195 We report detailed studies on two S = 2 electronic states of high-spin iron(II) porphyrinates.

196 ximizing the influence of this effect on the electronic states of interest remains a challenge.

197 tudy the competition between the cooperative electronic states of magnetic order and superconductivit

198 of the EDLTs demonstrate that the ambipolar electronic states of massless Dirac fermions with a high

199 can be a promising approach to engineer new electronic states of matter.

200 PE spectrum for formation of the four lowest electronic states of neutral MBQ from the (2)A2 state of

201 demonstrate that it is possible to alter the electronic states of non-ferromagnetic materials, such a

202 d here provide a unique insight into how the electronic states of oxyluciferin are altered by microen

203 weak van der Waals interlayer coupling, the electronic states of participating materials remain larg

204 The geometries and energies of the electronic states of phenyloxenium ion 1 (Ph-O(+)) were

205 pecific chemical reactions by modulating the electronic states of PLP through distinct active site en

206 promote various reactions by modulating the electronic states of PLP through weak interactions in th

207 the two-dimensional nature of the conducting electronic states of SmB6.

208 roperties of these complexes, excited by the electronic states of the chromophoric ligands, showed th

209 tal results and add insight into the various electronic states of the complex.

210 d/itinerant duality underlies the correlated electronic states of the high-Tc cuprate superconductors

211 -range migration of a hole through low-lying electronic states of the nucleobases.

212 surface and does not interact with the core electronic states of the QD.

213 electron spectroscopy to probe the first two electronic states of the radical cation, and resolve the

214 l potential of the electrons and perturb the electronic states of the reactants because of hybridizat

215 duction and phonon transport associated with electronic states of the rigid sulfur sublattice and sof

216 o differences in the electron density of the electronic states of the structurally different BODIPY c

217 l for the description of the coupling of the electronic states of the system to an external environme

218 "fingerprints" which are reproduced in other electronic states of the two molecules and allow classif

219 e is known about the interaction between the electronic states of these layered systems.

220 on and circular dichroism spectra to excited electronic states of this class of thiahelicene phosphor

221 However, investigating the electronic states of TI NWs is complicated, due to their

222 iguously show that we can switch the excited electronic state on attosecond timescales, coherently gu

223 ating of individual molecules with localized electronic states on the surface of a locally reactive 2

224 g nanomaterials can be tuned to couple other electronic states on the surface such as excitations of

225 epend on transition metal d-electron-derived electronic states, on which the vast majority of attenti

226 d II-VI nanostructures, introducing intragap electronic states optically coupled to the host conducti

227 ing electronics based on strongly correlated electronic states, or 'Mottronics', lies in finding an e

228 edient structures in which the two competing electronic states originate from separate structural com

229 rprisingly, the role in superconductivity of electronic states originating from simple free surfaces

230 Heavy electronic states originating from the f atomic orbitals

231 The time-dependent electronic state populations and the branching ratio of

232 superconductivity below this temperature for electronic states predominantly in the CuO2 plane.

233 The controllability over strongly correlated electronic states promises unique electronic devices.

234 reen fluorescent protein to study its ground-electronic-state proton-transport kinetics, revealing a

235 nal states provide spectral selectivity, and electronic states provide large signal enhancements.

236 t 1 is the first silylene to exhibit triplet electronic state reactivity.

237 indicate that the relative orderings of the electronic states remain largely unperturbed for these p

238 tacks of two-dimensional (2D) materials, the electronic states remain tightly confined within individ

239 mensurate/commensurate phases and associated electronic states remains enigmatic.

240 atively similar to those caused by competing electronic states, rendering a standard approach to thei

241 y through the in-plane d orbitals, localized electronic states resembling those of the free molecule

242 tate of MBQ, followed by the (1)B2 and (1)A1 electronic states, respectively 9.0 +/- 0.2 and 16.6 +/-

243 ent filament and to a renormalization of the electronic states responsible for transport.

244 nd azobenzene, with excitation to high-lying electronic states, reveal a rich diversity of photochemi

245 initio potential energy surfaces (PESs) for electronic states S(1), T(1), and S(0).

246 (1)) and subsequent relaxation to the ground electronic state (S(0)).

247 spectra of detachment to the radical ground electronic states show detailed structure, allowing assi

248 ve been used to probe the ground and excited electronic state structures of the dimer and radical pai

249 ariation of control parameters offers exotic electronic states such as anomalous and possibly high-tr

250 Strong spin-orbit coupling fosters exotic electronic states such as topological insulators and sup

251 n boundaries and the presence of a localized electronic state that acts like a barrier for exciton di

252 elated vibrational wavepackets on the ground electronic state that exhibit not only 2D spectroscopic

253 hen the metallic regime was tuned towards an electronic state that hosts unconventional superconducti

254 superconductivity in cuprates arises from an electronic state that remains poorly understood.

255 exciton wave functions into the interfacial electronic states that are formed from interaction of th

256 ological surface states are a class of novel electronic states that are of potential interest in quan

257 of diatomic molecules, which typically have electronic states that are relatively well separated in

258 ng tunneling microscope to examine the novel electronic states that emerge from the uranium f states

259 itons to a high-energy manifold of fullerene electronic states that enables efficient charge generati

260 l to resolve the contributions of the chiral electronic states that have a phase difference between t

261 /dielectric interfaces, leading to localized electronic states that serve as a basis for electrically

262 y, layer uniformity, interface stability and electronic states that severely complicate fabrication a

263 The two lowest electronic states that undergo a conical intersection ha

264 We show that in the ground electronic state the structure representing the wild-typ

265 Due to a specific electronic state, the lattice undergoes a reversible non

266 quality of their surfaces, and the pristine electronic states they host.

267 that strain can be used to engineer graphene electronic states through the creation of a pseudo-magne

268 results in quasi-one dimensional (1D) Dirac electronic states throughout the SBZ that we argue are i

269 states transfers a discrete-variable unknown electronic state to a continuous-variable photonic cat s

270 he reduced model that shows almost identical electronic states to 32 free electrons in a jellium box.

271 s correlated with coherent superpositions of electronic states to initiate local ferromagnetic correl

272 graphene oxide, arising from the coupling of electronic states to the asymmetric stretch mode of a ye

273 nic decay from the initial optically excited electronic state towards the high spin state is distingu

274 ge transport measurement results indicate an electronic state transition happening simultaneously wit

275 surface hydrogen effect to modulate the pure electronic-state transition in perovskite Ca0.9 Yb0.1 Mn

276 ribe ultrafast proton transfer in the ground electronic state triggered by the use of shock waves cre

277 nstrating the formation of an incompressible electronic state under these resonant excitation conditi

278 an be driven by a coherent excitation of two electronic states under two conditions: one is the symme

279 ges in the frameworks' steric confinement or electronic state upon the recognition of small molecule

280 these systems' potential of realizing novel electronic states upon carrier doping.

281 NMe(2)) in their lowest singlet and triplet electronic states was investigated by computational mean

282 Its structure and electronic state were confirmed by EPR and XAS.

283 ion of the excited state to a stable "phane" electronic state which is responsible for emission.

284 nductivity is optimized by tailoring the key electronic state, which is not disturbed by further modi

285 t photons first excite a set of intermediate electronic states, which then generate crystal elementar

286 radical, singlet (formally Ti(III) enolates) electronic states, whose origin is to be basically found

287 g a quantum of energy and moving to a higher electronic state will adjust to the new state and emit a

288 fect led to the realization of a topological electronic state with dissipationless currents circulati

289 urements characterized the molecule's ground electronic state with sufficient resolution to distingui

290 ct both quantum amplitudes and phases of the electronic states with a resolution of ~100 attoseconds.

291 ctral overlap integrals (SOIs) of lanthanoid electronic states with aromatic C-(H/D) overtones are ev

292 n attributed to competing but never-observed electronic states with different bonding properties simi

293 odified by the site-dependent spin mixing of electronic states with different relative canting angles

294 ese molecular metals have sparsely organized electronic states with distinctive visible and near-infr

295 onetheless, because certain SiC defects have electronic states with sharp optical and spin transition

296 t low energies is due to transitions between electronic states with similar character on ions of the

297 en in the ground (4)S and first excited (2)D electronic states with simple hydrocarbons or hydrocarbo

298 bservations of the spatial reorganization of electronic states with the onset of the pseudogap state

299 ity of domain wall electronic properties.The electronic states within domain walls in an interacting

300 However, electronic states within domain walls themselves have no