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1 Electrons have an intrinsic, indivisible, magnetic dipole aligned with their internal angular mome
3 selection rule because electric quadrupole, magnetic dipole, and coupled electric dipole-magnetic di
4 rstood as a pair of opposite charges and the magnetic dipole as a current loop, the toroidal dipole c
5 y in which the sense of electric dipoles and magnetic dipoles become uncoupled when electrons can cir
6 ggested that the effect resulted from strong magnetic-dipole contributions to the nanostructure's opt
7 agnet and the free layer e.g., utilizing the magnetic dipole coupling between them can circumvent thi
8 e consider additional factors including AuNC magnetic dipoles, density of excited-states, dephasing t
12 , traditionally derived from measurements of magnetic dipole-dipole couplings between protein nuclei,
13 peptide backbone at G33; (3) measurements of magnetic dipole-dipole couplings between the side chain
14 Measurements of 13C-13C and 15N-13C nuclear magnetic dipole-dipole couplings in isotopically labeled
15 Data include measurements of intermolecular magnetic dipole-dipole couplings in samples that are 13C
16 ements of intermolecular (13)C-(13)C nuclear magnetic dipole-dipole couplings indicate that Ure2p(10)
17 t the atoms are predominantly coupled by the magnetic dipole-dipole interaction, which, according to
20 field splitting (ZFS) tensors describing the magnetic dipole-dipole interactions of the component spi
21 of the magnetic fields' abilities to induce magnetic dipole-dipole interactions or control the orien
22 rmined by the interplay of van der Waals and magnetic dipole-dipole interactions, Zeeman coupling, an
23 due to the interference between electric and magnetic dipoles excited in each nanoparticle, enabling
24 electric dipole (alpha), quadrupole (A), and magnetic dipole (G') polarizabilities, only the electric
26 8O4 prevents these nanorods from spontaneous magnetic-dipole-induced aggregation, while their magneti
27 ouble electron-electron resonance to measure magnetic dipole interactions between spin ensembles in i
29 ow-index quartz substrates, the electric and magnetic dipole modes are easily identifiable across a w
30 lecules that possess a permanent electric or magnetic dipole moment can be manipulated using electric
31 inguished between an induced and a permanent magnetic dipole moment model of Europa's internal field.
32 e characterized by a quantized and unbounded magnetic dipole moment parallel to their propagation dir
33 ic and magnetic fields with stronger induced magnetic dipole moment upon excitation in comparison to
34 ntiferromagnets, which carry no net external magnetic dipole moment, yet have a periodic arrangement
37 e apply a pulsed magnetic field to align the magnetic dipole moments and use a high-transition temper
39 so demonstrate that the coupling between the magnetic dipole of a spin and the electromagnetic field
40 ganism in the case of some bacteria, but the magnetic dipoles of individual molecules are too small t
41 the third dimension induces net electric and magnetic dipoles of split-ring resonators parallel or an
42 ct of the cyt b(5) heme ring current-induced magnetic dipole on cyt c were used to discriminate betwe
43 use lattice geometry suppresses conventional magnetic dipole order, potentially allowing "hidden" ord
44 eliospheric magnetic field originates from a magnetic dipole oriented nearly perpendicular to, instea
45 servation is grounded in the electric dipole-magnetic dipole polarizability contribution to optical a
46 d, when suitably time-averaged, is that of a magnetic dipole positioned at the Earth's centre and ali
48 reflectance modulation of up to 0.35 at the magnetic dipole resonance of the metasurfaces and a spec
49 terahertz emission arises from exciting the magnetic-dipole resonance of the split-ring resonators a
50 he destructive interference of electric- and magnetic-dipole responses of nanoparticle array with the
52 tic nanoparticles, that comprise a permanent magnetic dipole that causes the cells to align along mag
53 long-range order of atomic-scale electric or magnetic dipoles that can be switched by applying an app
54 f neighbouring regions of oppositely aligned magnetic dipoles, their equivalent in optics have not be
55 ns that have been affected by a micron-scale magnetic dipole, thus establishing that our sorter can b
56 magnetic dipole, and coupled electric dipole-magnetic dipole transitions are forbidden in a far field
57 age a pair of spectrally close electric- and magnetic-dipole transitions in trivalent europium to pro
59 agnetic scheme for the assembly and study of magnetic dipoles within designed confinement profiles th
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