000 02416nab a2200325 c 4500
001 koha000894747
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008 220524|2021 xxu s a eng d
024 7 _a10.1103/PhysRevB.103.024303
_2doi
035 _akoha000894747
040 _aRU-ToGU
_brus
_cRU-ToGU
245 1 0 _aElectron-phonon coupling in the magnetic Weyl semimetal ZrCo2Sn
_cI. Yu. Sklyadneva, R. Heid, P. M. Echenique, E. V. Chulkov
336 _aТекст
337 _aэлектронный
504 _aБиблиогр.: 36 назв.
520 3 _aElectron-phonon coupling in ZrCo2Sn is investigated within the density-functional theory and linear-response approach in the mixed-basis pseudopotential representation. Phonon-induced scattering is analyzed for excited electrons (holes) in two majority bands, which form the topological Weyl state. Although the electron-phonon coupling in the energy range under consideration demonstrates some dependence on the available phase space, the strength of the phonon-mediated scattering, lambda, changes rather weakly with the hole (electron) energy and momentum, varying between 0.1 and 0.3. The momentum-averaged value of lambda ranges from 0.25 to 0.45. The phonon-mediated scattering of electrons near the Weyl point is found to be weak enough to warrant well-defined quasiparticles. Most of the modes actively involved in electron scattering are middle- and high-frequency lattice vibrations, while the participation of low-energy acoustic phonons is significantly suppressed by electron-phonon matrix elements. Of the long-wavelength optical phonons, only the T-2g Raman active modes generated by opposite vibrations of Co atoms make a noticeable contribution to the scattering of electrons.
653 _aэлектрон-фононное взаимодействие
653 _aВейля магнитные полуметаллы
653 _aлинейный отклик
655 4 _aстатьи в журналах
_9805200
700 1 _aSklyadneva, Irina Yu.
_9117782
700 1 _aHeid, Rolf
_9117778
700 1 _aEchenique, Pedro Miguel
_9117781
700 1 _aChulkov, Evgueni V.
_989119
773 0 _tPhysical Review B
_d2021
_gVol. 103, № 2. P. 024303-1-024303-6
_x2469-9950
852 4 _aRU-ToGU
856 4 _uhttp://vital.lib.tsu.ru/vital/access/manager/Repository/koha:000894747
908 _aстатья
999 _c894747