ライフサイエンスコーパス: electronic transition

1 he subscript indicates the wavelength of the electronic transition).

2 ystem as well as vibrational coupling to the electronic transition.

3 data without considering the effects of the electronic transition.

4 ute polarizability is allowed to change with electronic transition.

5 n about the degree of charge transfer in the electronic transition.

6 ionic excited state is the lowest-accessible electronic transition.

7 vided further insight into the nature of the electronic transitions.

8 h absorption spectra reveals four low-energy electronic transitions.

9 arge-transfer) formulation of donor/acceptor electronic transitions.

10 unds and carotenoids by their characteristic electronic transitions.

11 , so-called J/H-aggregates, leads to shifted electronic transitions.

12 on states are strongly detuned from the bare electronic transitions.

13 aterial density on emissive and non-emissive electronic transitions.

14 calized and element-specific nature of X-ray electronic transitions.

15 lation of the energy and localization of the electronic transitions.

16 formation of new interlocked-state-specific electronic transitions.

17 the lanthanide signal and assign underlying electronic transitions.

18 rs the intensity borrowing from spin-allowed electronic transitions.

19 erved when activated vibrations overlap with electronic transitions.

20 energy dependence, which could be caused by electronic transitions.

21 otoexcited wave function due to nonadiabatic electronic transitions.

22 ed phosphors involves multiple mechanisms of electronic transitions.

23 edium via their rotational, infrared, and/or electronic transitions.

24 elopment of the low- and high-spin intersite electronic transitions.

25 isotope shift of approximately 15 pm for the electronic transition 2(2)P 2(2)S at around the waveleng

26 citon dynamics are dominated by spin-related electronic transitions ((4)T(1) -> (6)A(1)) with long li

27 in a systematic blue shift in the low-energy electronic transitions (7, 523 nm; 8, 505 nm; 9, 445 nm

28 ated coherent phonon couples strongly to the electronic transition above the bandgap in the van der W

29 vealed well-resolved first- and second-order electronic transitions accompanied by prominent sideband

30 mplete and direct microscopic picture of the electronic transition across the YBCO/LCMO interfaces, w

31 The electronic transition affords modulation of the opto-ele

32 The convergence of these electronic transitions agrees with theoretical treatment

33 nd that during both heating and cooling, the electronic transition always precedes the structural Pei

34 luorescent properties, and molecular orbital electronic transition analysis establish that its fluore

35 sive coupling occurs only with the above-gap electronic transition and is absent in the valence band

36 om the synergy of the mid-gap traps assisted electronic transition and local Ge-Ge chain growth as we

37 For complex III, the slightly red-shifted electronic transition and the stoichiometry are most con

38 oseconds, as well as associated photoinduced electronic transitions and charge transfer processes.

39 these regions, we observe symmetry-breaking electronic transitions and doping-dependent band-structu

40 The interaction between molecular electronic transitions and electromagnetic fields can be

41 velength range that cannot be used to excite electronic transitions and generate electricity.

42 However, the low-energy electronic transitions and resonance Raman features attr

43 dings and provided detailed insight into the electronic transitions and spectroscopic properties of t

44 molecule-like properties, including discrete electronic transitions and strong fluorescence.

45 The blue shifts in the electronic transitions and the bisignate shape of the ci

46 ,0 band is composed of two nearly degenerate electronic transitions and the split is due to the asymm

47 ) excited within the peptide bond pi --> pi* electronic transitions and within the aromatic amino aci

48 ured and revealed a strong dependence of the electronic transitions and, therefore, the colors upon t

49 nability (allowing selectivity in addressing electronic transitions) and higher photon flux (permitti

50 ctions, high thermal stabilities, low energy electronic transitions, and amphoteric redox behavior.

51 ) and of valence-to-core (Kss(2,5) emission) electronic transitions, and of Kalpha RIXS data, which w

52 mission wavelengths, to suppress undesirable electronic transitions, and to sensitize absorption of l

53 DOS is analogous to Fermi's Golden Rule for electronic transitions, and we denote the finding here,

54 even in isotropic samples when well-defined electronic transitions are excited.

55 Both the longitudinal and transverse optical electronic transitions are measured, and the SW-CNT chir

56 centrations of stoichiometric VO(2) and that electronic transitions are regulated by the interplay be

57 Topology-driven, reversible electronic transitions are relevant across a broad range

58 ot one but two nearly orientation-degenerate electronic transitions are required to explain the 340-5

59 yet, Electronic Circular Dichroism that uses electronic transitions as a probe has by far been the me

60 ly at 440 gigapascals might be related to an electronic transition associated with pressure-induced i

61 These unique pressure-driven magnetic and electronic transitions, associated with the dome-shaped

62 empts to explain this coupled structural and electronic transition begin with two alternative startin

63 de were observed with strong, characteristic electronic transitions between 400 and 600 nm.

64 onantly absorb electromagnetic radiation via electronic transitions between Landau levels(1).

65 le conical intersection is implicated in the electronic transition but the excited state reaction lea

66 two-component atomic hydrogen may consist of electronic transitions caused by a highly distorted hcp

67 n PcoA, binds one Cu(II) and exhibits a weak electronic transition characteristic of a type II copper

68 Faraday rotation in the region of the Q-band electronic transition common to porphyrin and phthalocya

69 e observe spectral bleaching of the nanotube electronic transitions consistent with an electron-trans

70 ich is converted to vibrational energy after electronic transitions could lead to athermal hot ground

71 temperature dependence of the MBCT and MMCT electronic transitions defines the mixed valence complex

72 taking into account the distribution of the electronic transition densities in the dots and using th

73 flect the real-space phase modulation of the electronic transition density during the nonadiabatic pa

74 due to resonance with new optically allowed electronic transitions, determined by the relative orien

75 In the dyad, the electronic transition dipole moment of the electron dono

76 obtain information on the directions of the electronic transition dipole moments ((-->)m) of the chr

77 ive angle and separation between interacting electronic transition dipole moments and thus provide a

78 ically determined the relative angle between electronic transition dipole moments of its chlorophyll

79 orption bands of the triarylamines (pai,pai* electronic transitions) displayed bathochromic shifts as

80 rovskite and intergrowth layers leads to new electronic transitions distributed across both sublattic

81 how that increasing density causes a 3s->3pd electronic transition due to Pauli repulsion between the

82 Robin-Day Class II localized valency or even electronic transitions due to d-d metal-metal bonding.

83 vestigation of the dependence of the allowed electronic transition energies (electronic origins) on c

84 We have also calculated vertical electronic transition energies and determined the nature

85 c experiments have permitted us to determine electronic transition energies and polarizations, as wel

86 H) MCD spectroscopies were used to determine electronic transition energies and to obtain an estimate

87 ure MCD spectra reveal significant shifts in electronic transition energies that are correlated to di

88 te zero-field splitting (ZFS) parameters and electronic transition energies, intensities, and polariz

89 ne ground-state spin Hamiltonian parameters, electronic transition energies, oscillator strengths, an

90 mall despite large changes in the calculated electronic transition energies.

91 l, and acetonitrile cause blue shifts in the electronic transition energy of the bare m-nitrophenolat

92 tions incorporating heavy Br atoms optimized electronic transitions, enhancing TPA cross sections and

93 nstrate that this nonequilibrium topological electronic transition finds its microscopic origin in th

94 ared-vibrational absorption to a fluorescent electronic transition (fluorescence-encoded infrared (FE

95 The electronic transitions for solid Mo(4)PFT (lowest at 410

96 structural lattice distortion followed by an electronic transition from a semiconducting to metallic

97 We observe the predicted strongest electronic transition from the ground state, which is ne

98 density toward the cation with a subsequent electronic transition from the HOMO-2 to the HOMO.

99 his effect suitable for the determination of electronic transitions from a specific nucleus in a larg

100 lectronic structure of materials, separating electronic transitions from the composition of the corre

101 ctors for the lowest energy molecular nature electronic transition have been calculated and the origi

102 cules should display alternatively forbidden electronic transitions; however, for organic fluorophore

103 or absence of a Cooper pair in a long-lived electronic transition in (88)Sr atoms coupled to an opti

104 so reproduces the switching of the nature of electronic transition in higher homologues of (R2N)PPn(+

105 eity but identified a new, to our knowledge, electronic transition in the absorption profile at 644 n

106 c) resurgence to a possible pressure-induced electronic transition in the cuprate compounds due to a

107 iton Cotton effects in the region of (1)B(b) electronic transition in the naphthalene chromophores.

108 egion, although in some cases characteristic electronic transition in the near-IR region may appear.

109 We investigate the assignment of electronic transitions in alkyl peroxy radicals.

110 based magnetometer, employing spin-dependent electronic transitions in an organic diode, which combin

111 Electronic transitions in aromatic side chains are respo

112 lly superconducting phases and the nature of electronic transitions in high-pressure hydrides.

113 ing superconducting phases and understanding electronic transitions in high-pressure synthesized mate

114 There is a great interest in electronic transitions in hydrogen-rich materials under

115 ence weak spin-orbit interaction can control electronic transitions in molecular and solid-state syst

116 applications, including the spectroscopy of electronic transitions in molecules, experimental tests

117 we identify the optically allowed molecular electronic transitions in nanometric PSbs as potential f

118 ray spectroscopic methods offer a new set of electronic transitions in probing the oxidation states,

119 tuning the energy difference between the two electronic transitions in the dimer to match a vibration

120 es of radical ligands can exhibit low-energy electronic transitions in the near-infrared (NIR) spectr

121 akened charge transfer (CT) character of the electronic transitions in the reduced state.

122 Urocanic acid, UCA, is characterized by two electronic transitions in the UV-B (280-320 nm) which co

123 he W-L complexes, to simulate and assign the electronic transitions in the UV-vis spectra, to determi

124 and HOMO-1-LUMO transitions are the primary electronic transitions in the UV-Visible spectra of the

125 ocesses of proteins harboring cofactors with electronic transitions in the visible range, such as ret

126 tion symmetries display absorptive 4f --> 5d electronic transitions in the visible region.

127 previously unidentified types of topological electronic transitions in Zintl compounds.

128 ded in the bulk of their hosts, making their electronic transitions inaccessible to surface modificat

129 ng potential, permitting coherent control of electronic transitions independent of the atomic center-

130 provided insights into reactivity trends and electronic transitions involved in optical properties, s

131 ltimate efficiencies by the type of emissive electronic transitions involved.

132 esponse theory allowed identification of the electronic transitions involved.

133 ethyl-THF glass) in the UV-vis region to (1) electronic transitions involving the four-center orbital

134 f the excited state is a triplet because the electronic transition is 'dark' with a vanishing oscilla

135 This electronic transition is accompanied by a dramatic struc

136 The electronic transition is attributed to the electric-fiel

137 A high-frequency (3300-2600 cm(-1)) electronic transition is observed for all PS I particles

138 beam spectroscopy, involving vibrational and electronic transitions, is a powerful tool allowing to r

139 e existence of a universal alignment for the electronic transition level of hydrogen in semiconductor

140 very interesting temperature-induced quantum electronic transition (Lifshitz transition), which is ma

141 ctroelectrochemical data with the calculated electronic transitions makes it possible to both evidenc

142 Electronic transition moments and circular dichroism ten

143 a. 12% of the absorbed intensity for the two electronic transitions most influenced by the spin-orbit

144 behaviour originates from the suppression of electronic transitions near the Weyl points due to the d

145 upling between an infrared-active phonon and electronic transitions near the Weyl points through the

146 investigation has gleaned novel insight into electronic transitions occurring on the time scales of v

147 Trp496 is shown to affect the electronic transition of PCB and to be essential for the

148 The most bathochromic electronic transition of the chromophores essentially ex

149 les act as hydrogen bond donors to alter the electronic transition of the molecular keto form from nn

150 The low-energy electronic transition of the PP(2)-PP(7) cation radicals

151 Raman spectra relate the electronic transition of this precursor state predominan

152 Raman spectra relate the electronic transition of this precursor state predominan

153 -1)) associated with the (2)F(5/2) (2)F(7/2) electronic transition of Yb(III).

154 theory calculations, which placed the major electronic transitions of (3)1N at 367 nm (f = 0.0407) a

155 rmed to analyze the orbitals involved in the electronic transitions of 4, 6, and 7.

156 ientations and intensities of the low-energy electronic transitions of 6-MI reported here should be u

157 or a particular size n, the measured valence electronic transitions of all these systems fall into ei

158 deration of the vibrational structure of the electronic transitions of aromatic side chains.

159 spectroscopy to atomic clocks by addressing electronic transitions of atoms and molecules.

160 bility to tune the emission is attributed to electronic transitions of mixed ligand-to-metal-metal-ch

161 arise from circular dichroism of the strong electronic transitions of photosynthetic absorption band

162 rational spectra and TDDFT simulation of the electronic transitions of potential photointermediates c

163 Furthermore, the electronic transitions of R6G on Ag surface were studied

164 The electronic transitions of several -C(5)- carbenes are co

165 The d-d electronic transitions of the Co(II)-substituted hexamer

166 velength-dependent character of the involved electronic transitions of the detected key intermediates

167 The major electronic transitions of the light-harvesting complex o

168 oupling in an optical microcavity to mix the electronic transitions of two J-aggregated molecular dye

169 vis region of the spectra are due to pi-pi* electronic transitions, of an intramolecular charge-tran

170 nesiowustite and the isolated effects of the electronic transitions on the elasticity of magnesiowust

171 Through direct determination of electronic transition orientations and analysis of domai

172 rescent ligands to be probed even when their electronic transitions overlap with those of the macromo

173 -positions of the macrocycles results in new electronic transitions polarized along the long axes of

174 for fundamental and overtone vibrational and electronic transitions-possibly all within the same mole

175 e further insight into the energy levels and electronic transitions present, computational studies of

176 -CNN(+), owing to a large enhancement of the electronic transition probability by vibronic coupling.

177 ctrical conductivity (0.02 S cm(-1) ), broad electronic transitions, promising thermoelectric behavio

178 Attosecond probing of core-level electronic transitions provides a sensitive tool for stu

179 s been analyzed to obtain information on the electronic transitions responsible for the linkage isome

180 increase in the average energy of the first electronic transition (S(1) -> S(0)) that was assessed u

181 t probably related to the two-photon allowed electronic transition S0-->S2.

182 at 50-1400 cm(-1) , which was attributed to electronic transitions, scattering, photoluminescent emi

183 In addition, the electronic transition state of graphene within the UV re

184 or studying elusive quantum effects in which electronic transitions strongly couple to phonons and vi

185 dicate that these divide into three types of electronic transitions; t(2) --> t(2) involving excitati

186 in the UV spectral region where the relevant electronic transitions take place, we have developed and

187 The accessible electronic transitions, term energies, and orbital angul

188 r UV-absorption spectra show a lowest energy electronic transition that decreases in energy (3.54 eV,

189 ength (457 nanometers) in the vicinity of an electronic transition that shows circular dichroism in b

190 , which is accomplished by targeting special electronic transitions that allows for a fast screening

191 understanding of the metal-metal bonding and electronic transitions that are responsible for their UV

192 line width is a result of multiple, discrete electronic transitions that couple to vibrations of the

193 y calculations to assign and analyze the two electronic transitions that create the blue color.

194 fundamental physical phenomena and quantized electronic transitions that have made solid-state laser-

195 tum chemical calculations, we identified six electronic transitions that occur within the 25,000-50,0

196 uires that the dipole moment of the resonant electronic transition, the change of the dipole moment u

197 ficant density change is observed across the electronic transition, the jump in the sound velocities

198 eting electronic states; it is thus a purely electronic transition to a superconducting state, with a

199 by coupling photons generated from interband electronic transition to phonon polariton modes on the s

200 ld enables us to control and manipulate this electronic transition to the extent that a p-n junction

201 emistry where the cavity is made resonant to electronic transitions to control molecular nonadiabatic

202 nd within the aromatic amino acid pi --> pi* electronic transitions to examine the temperature depend

203 ed species also shifts the near-IR interband electronic transitions to lower energy by more than 10%.

204 e apply a new algorithm for modeling protein electronic transitions to simulate two-dimensional UV ph

205 phenol, and indole that describe the valence electronic transitions to the (1)L(b), (1)L(a), (1)B(b),

206 ne hand, CID takes place via direct resonant electronic transitions to the lowest unoccupied molecula

207 With consumer electronics transitioning toward flexible products, ther

208 de is characterized on its first pai* <- pai electronic transition using a ground-state depletion met

209 re rationalized by correlation with computed electronic transitions using DFT methods.

210 candidate for inducing coupled magnetic and electronic transition via fast and reversible redox reac

211 conductor with light that resonates with its electronic transition, we find that halide-containing ar

212 h-spin diiron(II) complexes with distinctive electronic transitions were prepared by using 4-cyanopyr

213 ocalized exciton, including the S(2) <- S(1) electronic transition, whose energy reflects interbranch

214 e the bound dyes (with calf thymus DNA) have electronic transitions with lambda(max) = 514 nm (comple

215 ansition of the ABC-flavanone moiety and the electronic transition within the DEF-flavone moiety, whi

216 y and the DEF-flavone moiety, as well as the electronic transition within the DEF-flavone moiety.

217 th the excitation energy for the interfacial electronic transition within the Pt-CO bond.