ライフサイエンスコーパス: electric dipole

1 olecular cations that arises from frustrated electric dipoles.

2 logues of magnets, electrets possess ordered electric dipoles.

3 in turn generates molecular distortions and electric dipoles.

4 c excitation, distinct from the magnetic and electric dipoles.

5 (antiferroelectric) collinear alignments of electric dipoles.

6 electric fields generated by their permanent electric dipoles.

7 ce acoustic phonons and qubit states with an electric dipole, a potential source of decoherence durin

8 We find electromagnon excitations and electric dipole active two-magnon excitations in the mag

9 hose containing polar molecules having their electric dipoles aligned parallel to such surfaces.

10 a are found to be dominated by iron np to 1s electric dipole allowed transitions, with pronounced sen

11 In contrast, nonlinear techniques probing electric-dipole-allowed effects have been used for sensi

12 ith approximately equal contributions of the electric dipole (alpha), quadrupole (A), and magnetic di

13 injection barriers are dependent both on the electric dipole and magnetic spin moment, we have been a

14 nchiral cubic structure to an incommensurate electric dipole and orbital helix via an intermediate de

15 patible with metallicity due to screening of electric dipoles and external electric fields by itinera

16 on to optical activity in which the sense of electric dipoles and magnetic dipoles become uncoupled w

17 olarization that is accompanied by radiative electric dipoles and weak, slowly-rotating in-plane magn

18 e resolves the apparent inconsistency of the electric dipole approximation's validity for photoioniza

19 expectedly, this approximation, known as the electric dipole approximation, is still valid for the io

20 d attention thanks to their existence in the electric dipole approximation, without relying on the we

21 dichroism, methods that are forbidden in the electric dipole approximation.

22 chiral light-matter interactions within the electric-dipole approximation (avoiding weak magnetic-di

23 interlayer excitons possess an out-of-plane electric dipole as well as an unusually large oscillator

24 static field in the catalytic site turns the electric dipole associated with the carbonyl group of th

25 interlayer excitons with static out-of-plane electric dipoles, at the expense of the strength of the

26 Simple vortex-like, electric-dipole-based topological structures have been o

27 vation of incommensurate helical ordering of electric dipoles by light hole doping of the quadruple p

28 While the electric dipole can be understood as a pair of opposite

29 For both BR variants, we derive a moderate electric dipole change of 5 [Formula: see text] 1 Debye,

30 erahertz (THz) Stark spectroscopy to measure electric dipole changes of wild-type BR and a BR D85T mu

31 tile electrostatic environment to create new electric dipole configurations.

32 ese chiral signals are mainly contributed by electric dipole contributions, which can dominate the ch

33 olecular charge-transfer occurs with forming electric dipoles (D(+*) ->A(-*) ), providing the ionic p

34 Two-qubit gates exploit a second-order electric dipole-dipole interaction, allowing selective c

35 n quenching mechanism was verified to be the electric dipole-dipole interaction.

36 report on the direct observation of resonant electric dipole-dipole interactions in a cubic array of

37 Due to the induction of an electric dipole, DNA molecules are pulled by a gradient

38 ultra-low loss lithium niobate piezoelectric electric dipole driven at acoustic resonance that radiat

39 nsity modulation, particularly enhancing the electric dipole (ED), magnetic dipole (MD), and electric

40 To date, the electric dipole equivalent of ordered magnetic spin latt

41 The spontaneous electric dipoles formed by Cu(+) ions displaced from the

42 he critical size limit of voltage-switchable electric dipoles has extensive implications for energy-e

43 BiMn(7)O(12) In analogy with magnetism, the electric dipole helicoidal texture is stabilized by comp

44 The electric dipole in the Janus heterobilayers leads to cha

45 The possible quantum liquids of electric dipoles in frustrated dielectrics open up a fre

46 The coupling between the magnetic and electric dipoles in multiferroic and magnetoelectric mat

47 ginate from the coupling between photons and electric dipoles in phonons.

48 opic symmetric exchange interactions between electric dipoles in this material.

49 eying local "ice rules," in analogy with the electric dipoles in water ice.

50 etion layer due to the presence of localized electric dipoles induced by adsorbed oxygen.

51 computational results show that the observed electric dipole-induced spin-dependent transport inversi

52 t is based on the existence of an "effective electric dipole" inspired by recent reported structures

53 ncreased by reduction of hydrogen bonding or electric dipole interaction ability.

54 rt on a remarkable phenomenon of interfacial electric dipole inversion coupled to changes in atomic s

55 The electric dipole is also expected to enhance exciton-exci

56 Inducing and controlling electric dipoles is hindered in the ultrathin limit by t

57 rolyte (PE) macromolecules, treating them as electric dipoles, is proposed.

58 linearly polarised resonant modes: one with electric dipole-like behaviour and the other with magnet

59 sents a promising candidate for the proposed electric-dipole liquid.

60 Here we propose that quantum electric-dipole liquids, analogues of quantum spin liqui

61 ation of this observation is grounded in the electric dipole-magnetic dipole polarizability contribut

62 ric quadrupole, magnetic dipole, and coupled electric dipole-magnetic dipole transitions are forbidde

63 t k satisfies [Formula: see text], the point electric dipole model becomes accurate.

64 eric, with a distortion characterized by the electric dipole moment (EDM), d(e).

65 ated a method for searching for the electron electric dipole moment (eEDM).

66 , in addition to possibly having a permanent electric dipole moment as a consequence of violation of

67 We report the observation of a permanent electric dipole moment in a homonuclear molecule in whic

68 spatially indirect excitons with a permanent electric dipole moment in heterobilayer crystals promise

69 ulation correlated with the component of the electric dipole moment in the aromatic ring, suggesting

70 ime-reversal invariance, develops an induced electric dipole moment in the presence of an external el

71 ea, or thiourea groups introduce a localized electric dipole moment into the SAM and change the polar

72 e direction of the purple-membrane permanent electric dipole moment is determined by the purple-membr

73 Their permanent electric dipole moment is expected to generate systems w

74 in dielectric constant is consistent with an electric dipole moment of 0.51+/-0.05 Debye for an encap

75 Furthermore, the large electric dipole moment of polar molecules can be tuned u

76 Our simulations show that the electric dipole moment of residues around heme a changes

77 ated with these new particles will induce an electric dipole moment of the electron (eEDM).

78 The electric dipole moment of the Schiff base in the S[Formu

79 Large differences in the electric dipole moment of the two tautomers, estimated f

80 ion of magnetic moment mu at a site of local electric dipole moment p, it is unknown to date whether

81 3) symmetry leads to a substantial molecular electric dipole moment that is directly connected to its

82 absorption can be affected by the permanent electric dipole moment which could be adjusted by modify

83 of the EI sustains an out-of-plane permanent electric dipole moment with an antiferroelectric texture

84 a steep power-law dependence on the induced electric dipole moment, and we show that this dependence

85 and, for biomolecules that lack a permanent electric dipole moment, provides a mechanism for orienti

86 The polar molecules have a permanent electric dipole moment, which we measure with Stark spec

87 ermine the PKa for reversal of the permanent electric dipole moment.

88 density and the non-observation of a neutron electric dipole moment.

89 ization, which originates from a microscopic electric dipole moment.

90 oscopy constrains the size of the electron's electric dipole moment.

91 the latter also possesses anomalously large electric dipole moment.

92 components, such as searches for the neutron electric dipole moment.

93 citons, which we accessed using their static electric dipole moment.

94 susceptibility and the time-averaged dynamic electric dipole moment.

95 , (ii) surface hydrophobicity, and (iii) the electric dipole moment.

96 general relativity or searches for electron electric dipole moment.

97 p) is first absorbed by excitations carrying electric dipole moment.

98 h could lead to an increase of its permanent electric dipole moment.

99 cience, including the search for an electron electric dipole moment.

100 of the radical pair: a transient, long-lived electric dipole moment.

101 surface, a molecule can migrate and carry an electric dipole moment.

102 cs beyond the standard model; any measurable electric-dipole moment (a signature of the latter) is ex

103 s for the enhancement of a measurable atomic electric-dipole moment.

104 on via searches for effects due to permanent electric dipole moments and other CP-odd properties in l

105 However, large molecular permanent electric dipole moments are challenging to realize exper

106 Permanent electric dipole moments are important for understanding

107 Permanent electric dipole moments in molecules require a breaking

108 orting interlayer excitons with out-of-plane electric dipole moments in opposite directions.

109 The linear dichroism fixes the transition electric dipole moments in the aromatic plane with respe

110 The electric dipole moments of cyanide ions in Cd(CN)(2) ass

111 The electric dipole moments of the GaN rods increased substa

112 that the odd order and even order nonlinear electric dipole moments scale with the area and perimete

113 of ~100 nanometers and kilo-Debye permanent electric dipole moments that form when an ultracold grou

114 e, heteronuclear molecules possess permanent electric dipole moments that lead to long-range, tunable

115 n of molecules, particularly their permanent electric dipole moments, allow a broad array of applicat

116 ee-dimensional orientation of individual TLS electric dipole moments.

117 l (3AP) on the basis of differences in their electric dipole moments.

118 ttain an anomalous component with very large electric dipole moments.

119 phenomenon is important for measurements of electric-dipole moments of atoms, which would indicate C

120 andidates for experimental studies of atomic electric-dipole moments that might reveal extensions to

121 n, in which the interactions between induced electric dipoles of adjacent particles lead to particle

122 or estimating the direction of the intrinsic electric dipoles of these conjugates.

123 stabilize a ferrielectric-like non-collinear electric-dipole order in the final heterostructure while

124 it coupling between spontaneous magnetic and electric dipole ordering, have significant potential for

125 Specifically, we engineer the electric-dipole ordering in ferroelectric oxide heterost

126 Se-sublayer due to strong sublayer-localised electric dipoles orientated along the c-axis.

127 d spherulites present all orientations of an electric dipole oscillator in spatially localized region

128 e to map the enantiomer-dependent sign of an electric dipole Rabi frequency onto the phase of emitted

129 ropic symmetric exchange interaction between electric dipoles remains ambiguous.

130 lectrics where antiferroelectrically coupled electric dipoles reside on a triangular lattice.

131 ambda/lambda ~ 15%) mode shifting between an electric dipole resonance and an anapole state.

132 olor is determined by localized magnetic and electric dipole resonance of nanostructures, which are s

133 ehaviors were ascribed to pendular ions with electric dipoles reversibly locked by the strong field i

134 We leverage the surface sensitivity of electric dipole second harmonic generation (SHG) to reso

135 etween electronic levels are governed by the electric dipole selection rule because electric quadrupo

136 es cannot occur in atomic systems due to the electric-dipole selection rules.

137 g manifests as a shift and broadening of the electric dipole spin resonance (EDSR), respectively.

138 s remained controversial because of the poor electric dipole stability in single molecules.

139 lecule electret is the switching between two electric dipole states by an external electric field.

140 c materials are characterized by a permanent electric dipole that can be reversed through the applica

141 the polar B-P bond forms a stable permanent electric dipole that radially points inward in the nanoc

142 c bubbles are sub-10nm spherical vortices of electric dipoles that can spontaneously form in ultra-th

143 d by accounting for the interactions between electric dipoles that the particles in the aggregates in

144 udied the orientations and magnitudes of the electric dipole transition moments (EDTMs) of 6-methyl i

145 on, linear dichroism, and orientation of the electric dipole transition moments and to display them a

146 It is shown that electric dipole transitions can be enhanced near the foc

147 enhancement allows us to resolve Stark-split electric dipole transitions, which are typically only ob

148 to explore light-matter interactions beyond electric dipole transitions.

149 energies can be tuned due to their in-built electric dipole via the Stark effect.

150 anti-symmetric exchange interactions between electric dipoles was proved to exist (with materials hos

151 ctric materials show electrically switchable electric dipoles, which are usually formed by spatial se