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1 ng of nearly independent and quasi-classical magnetic dipoles.
2    Electrons have an intrinsic, indivisible, magnetic dipole aligned with their internal angular mome
3 t are closely interlocked and a noncollinear magnetic-dipole alignment is induced by antiferroic elec
4  strong SHG nonlinearity majorly result from magnetic dipole and electric quadrupole clearly provides
5                                              Magnetic dipole and nanocrystalline orientations of magn
6                                  The nuclear magnetic dipole and nuclear electric quadrupole hyperfin
7 ses because of the weak coupling between the magnetic dipole and the electromagnetic field.
8 dea, we introduce lithographically patterned magnetic dipoles and an applied magnetic field to drive
9 try) is triply forbidden by the electric and magnetic dipoles and the electric quadrupole.
10  selection rule because electric quadrupole, magnetic dipole, and coupled electric dipole-magnetic di
11 rial neutral sheet, where the effects of the magnetic dipole are absent.
12 rstood as a pair of opposite charges and the magnetic dipole as a current loop, the toroidal dipole c
13 ce coupling between the induced electric and magnetic dipoles associated with enantiomers and chiral
14 y in which the sense of electric dipoles and magnetic dipoles become uncoupled when electrons can cir
15 th the strong, pronouncedly-tilted, rotating magnetic dipoles characteristic on the nano-entities, wh
16     As meta-atoms can have both electric and magnetic dipole characteristics (and hence radiation pro
17 ggested that the effect resulted from strong magnetic-dipole contributions to the nanostructure's opt
18                                              Magnetic dipole coupling between the colloidal superpara
19 agnet and the free layer e.g., utilizing the magnetic dipole coupling between them can circumvent thi
20 Ta(2)NiSe(5) mediated by electric quadrupole/magnetic dipole coupling produces helicity-dependent DC
21 n of a chemical force (hydrogen bonding) and magnetic dipole coupling to assemble polymer-brush coate
22 e consider additional factors including AuNC magnetic dipoles, density of excited-states, dephasing t
23 at is a consequence of a competition between magnetic dipole-dipole and ligand interactions.
24                      There is no evidence of magnetic dipole-dipole coupling between the product trip
25                              Measurements of magnetic dipole-dipole couplings among (13)C nuclei in a
26                  Measurements of (13)C-(13)C magnetic dipole-dipole couplings among (13)C-labeled Ile
27 , traditionally derived from measurements of magnetic dipole-dipole couplings between protein nuclei,
28 peptide backbone at G33; (3) measurements of magnetic dipole-dipole couplings between the side chain
29  Measurements of 13C-13C and 15N-13C nuclear magnetic dipole-dipole couplings in isotopically labeled
30  Data include measurements of intermolecular magnetic dipole-dipole couplings in samples that are 13C
31 ements of intermolecular (13)C-(13)C nuclear magnetic dipole-dipole couplings indicate that Ure2p(10)
32 explained by a wavy chain model based on the magnetic dipole-dipole interaction and demagnetizing fac
33 ncorrelated spins is generated by the native magnetic dipole-dipole interaction between nitrogen-vaca
34 t the atoms are predominantly coupled by the magnetic dipole-dipole interaction, which, according to
35                                              Magnetic dipole-dipole interactions between the spins ar
36                                              Magnetic dipole-dipole interactions between the spins we
37 field splitting (ZFS) tensors describing the magnetic dipole-dipole interactions of the component spi
38  of the magnetic fields' abilities to induce magnetic dipole-dipole interactions or control the orien
39 rmined by the interplay of van der Waals and magnetic dipole-dipole interactions, Zeeman coupling, an
40 ure coherent spin state, under the effect of magnetic dipole-dipole interactions.
41 olar Lorentz force exerted on a photoinduced magnetic dipole excited by the magnetic component of lig
42 due to the interference between electric and magnetic dipoles excited in each nanoparticle, enabling
43 he force-torque wrench induced by a rotating magnetic dipole field on a solid conductive sphere (whic
44 nerated on a conductive sphere in a rotating magnetic dipole field.
45  nonmagnetic objects using multiple rotating magnetic dipole fields, utilizing an empirical model of
46 jects is possible by using multiple rotating magnetic dipole fields.
47  to conduct electric currents as feedback of magnetic dipole fluctuation in superparamagnetic grains.
48 electric dipole (alpha), quadrupole (A), and magnetic dipole (G') polarizabilities, only the electric
49 ns of magnetosomes that comprise a permanent magnetic dipole in each cell.
50                       Long-range ordering of magnetic dipoles in bulk materials gives rise to a broad
51 d support broader re-examination of rotating magnetic dipoles in producing non-thermal quiescent radi
52 8O4 prevents these nanorods from spontaneous magnetic-dipole-induced aggregation, while their magneti
53 ed results, the energy competition among the magnetic dipole interaction energy, magnetic potential e
54 ouble electron-electron resonance to measure magnetic dipole interactions between spin ensembles in i
55            Typically, it is the interplay of magnetic dipole interactions, spin anisotropy, and geome
56 e to the competition of the exchange and the magnetic dipole interactions, the minimum-energy magnon
57 electric-dipole approximation (avoiding weak magnetic-dipole interactions), yielding huge chiral sign
58 hich are compounds with electric rather than magnetic dipoles) is basically unknown.
59 ric dipole-like behaviour and the other with magnetic dipole-like behaviour.
60 s rare systems in which ordered electric and magnetic dipoles may reside on the same transition metal
61 icularly enhancing the electric dipole (ED), magnetic dipole (MD), and electric quadrupole (EQ) modes
62 ow-index quartz substrates, the electric and magnetic dipole modes are easily identifiable across a w
63 e pitch, the frequencies of the electric and magnetic dipole modes can be exchanged in frequency orde
64 lecules that possess a permanent electric or magnetic dipole moment can be manipulated using electric
65 inguished between an induced and a permanent magnetic dipole moment model of Europa's internal field.
66 e characterized by a quantized and unbounded magnetic dipole moment parallel to their propagation dir
67 ic and magnetic fields with stronger induced magnetic dipole moment upon excitation in comparison to
68 ambiguously showed that the large transition magnetic dipole moment |m| of 2 is responsible for its h
69 ntiferromagnets, which carry no net external magnetic dipole moment, yet have a periodic arrangement
70 rise to a quantized, small, but controllable magnetic dipole moment.
71 detect magnetic cells and to determine their magnetic dipole moment.
72  of magnetite, too small to hold a permanent magnetic dipole moment.
73  symmetric exchange interactions between two magnetic dipole moments - responsible for intriguing mag
74 e apply a pulsed magnetic field to align the magnetic dipole moments and use a high-transition temper
75                    In addition, electric and magnetic dipole moments are computed with the self-consi
76 ting from the good alignment of electric and magnetic dipole moments determined by the multilayer str
77 y selection rules governing the electric and magnetic dipole moments in chiral molecules.
78 sion minima, where alignment of electric and magnetic dipole moments occurs.
79 ed to high-finesse cavities(5,6), with large magnetic dipole moments(7-13), and spin-orbit-coupled, t
80 so demonstrate that the coupling between the magnetic dipole of a spin and the electromagnetic field
81                   For plasma confined by the magnetic dipole of LSR J1835 + 3259, we estimate 15 MeV
82 ganism in the case of some bacteria, but the magnetic dipoles of individual molecules are too small t
83 the third dimension induces net electric and magnetic dipoles of split-ring resonators parallel or an
84 ct of the cyt b(5) heme ring current-induced magnetic dipole on cyt c were used to discriminate betwe
85 c dipoles and weak, slowly-rotating in-plane magnetic dipoles on the nano-objects; where the outgoing
86 use lattice geometry suppresses conventional magnetic dipole order, potentially allowing "hidden" ord
87 eliospheric magnetic field originates from a magnetic dipole oriented nearly perpendicular to, instea
88 non was demonstrated, where the electric and magnetic dipoles overlap both spatially and spectrally.
89 servation is grounded in the electric dipole-magnetic dipole polarizability contribution to optical a
90 d, when suitably time-averaged, is that of a magnetic dipole positioned at the Earth's centre and ali
91                                 We find that magnetic dipoles randomly distributed in a solid matrix
92  reflectance modulation of up to 0.35 at the magnetic dipole resonance of the metasurfaces and a spec
93 al-insulator-metal structures to introduce a magnetic dipole resonance that allows increased tuning f
94 efficiency is attributed to the electric and magnetic dipole resonance, as illustrated through the el
95  terahertz emission arises from exciting the magnetic-dipole resonance of the split-ring resonators a
96 he destructive interference of electric- and magnetic-dipole responses of nanoparticle array with the
97                    The amplitudes, i.e., the magnetic dipole strengths of the SEFs were higher during
98 tic nanoparticles, that comprise a permanent magnetic dipole that causes the cells to align along mag
99 consist of panels with different patterns of magnetic dipoles that are capable of specific binding.
100 long-range order of atomic-scale electric or magnetic dipoles that can be switched by applying an app
101  at low rotation frequencies of the rotating magnetic dipole, that is substantially more intuitive, e
102 f neighbouring regions of oppositely aligned magnetic dipoles, their equivalent in optics have not be
103 ns that have been affected by a micron-scale magnetic dipole, thus establishing that our sorter can b
104 The large scalar product of the electric and magnetic dipole transition moments ([Formula: see text])
105 or these prism[4]arenes, due to electric and magnetic dipole transition moments both directed along t
106 guration of [9]HBNG between its electric and magnetic dipole transition moments.
107 his new class of clocks, based on an optical magnetic-dipole transition in Ar(13+).
108 magnetic dipole, and coupled electric dipole-magnetic dipole transitions are forbidden in a far field
109 be distinguished from electric multipole and magnetic dipole transitions.
110 age a pair of spectrally close electric- and magnetic-dipole transitions in trivalent europium to pro
111  resonances in the form of optical-frequency magnetic-dipole transitions.
112     In the present work, we study systems of magnetic dipoles where the dipoles are arranged on vario
113 dels, valid when two conditions are met: the magnetic dipole (which is assumed to be at the center of
114 agnetic scheme for the assembly and study of magnetic dipoles within designed confinement profiles th

 
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