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ANAPOLE

Anapole

System of currents that do not radiate into the far field

anapole (from Greek ἀνά (ana) 'above' and πόλος (polos) 'pole') is a system of currents that does not radiate into the far field. The term "anapole"

Anapole

Toroidal moment

Type of electromagnetic dipole

arrangements whereas a polar (or magnetic) toroidal dipole (also called an anapole) corresponds to the field of a solenoid bent into a torus. A complex expression

Toroidal moment

Toroidal_moment

Dynamic toroidal dipole

toroidal dipole introduced by Zeldovich in 1957 under the name of static anapole. The dynamic toroidal multipoles were theoretically introduced in the 1970s

Dynamic toroidal dipole

Dynamic_toroidal_dipole

Electron electric dipole moment

Quantity relating an electron's potential energy to electric field strength

factor F 4 ( q 2 ) {\displaystyle F_{4}(q^{2})} would, if nonzero, be the anapole moment. Electron EDMs are usually not measured on free electrons, but instead

Electron electric dipole moment

Electron_electric_dipole_moment

Electron magnetic moment

Spin of an electron

factor F 4 ( q 2 ) {\displaystyle F_{4}(q^{2})} would, if non zero, be the anapole moment. The spin magnetic moment is intrinsic for an electron. It is μ

Electron magnetic moment

Electron_magnetic_moment

Majorana fermion

Fermion that is its own antiparticle

1016/S0370-2693(00)00358-0. S2CID 14251522. Ho, Chiu Man; Scherrer, Robert J. (2013). "Anapole Dark Matter". Physics Letters B. 722 (8): 341–346. arXiv:1211.0503. Bibcode:2013PhLB

Majorana fermion

Majorana_fermion

Refugio Reyes Rivas

Mexican architect (1862–1943)

laborer and assistant in the decoration of the "Templo y la Capilla de Anapoles" (sic) —Chapel of Naples—, when he was sixteen years old. Among his papers

Refugio Reyes Rivas

Refugio_Reyes_Rivas

Mie scattering

Scattering of an electromagnetic plane wave by a sphere

{\displaystyle \pi } ) are called multipole resonances, and zeros can be called anapoles. The dependence of the scattering cross-section on the wavelength and the

Mie scattering

Mie_scattering

Dmitry Budker

Russian-American physicist

constraints on the hypothetical "neutron skin" in heavy nuclei and for testing anapole moments predicted by the Standard Model. In 2010, Budker's group conducted

Dmitry Budker

Dmitry_Budker

Nikolay Zheludev

British scientist

observation of the fundamental electromagnetic toroidal moment electromagnetic anapole and toroidal light pulses, propagating counterparts of localized toroidal

Nikolay Zheludev

Nikolay_Zheludev

CP violating moments

factor F 4 ( q 2 ) {\displaystyle F_{4}(q^{2})} would, if nonzero, be the anapole moment. Electron EDMs are usually not measured on free electrons, but instead

CP violating moments

CP_violating_moments