ライフサイエンスコーパス: electric dipole

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

2 electric fields generated by their permanent electric dipoles.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

45 general relativity or searches for electron electric dipole moment.

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

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

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

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

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

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

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

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

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

55 Permanent electric dipole moments are important for understanding

56 Permanent electric dipole moments in molecules require a breaking

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

58 The electric dipole moments of the GaN rods increased substa

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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