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Письма в Журнал экспериментальной и теоретической физики  / №5-6 2017

CHIRAL VORTICAL EffECT GENERATED BY CHIRAL ANOMALY IN VORTEX-SKYRMIONS (200,00 руб.)

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Первый авторVolovik
Страниц2
ID597389
АннотацияThe problems with Weyl materials – Weyl semimetals and Weyl superconductors (see latest reviews in Ref. [1] and Ref. [2] correspondingly) – is that at first glance they should possess any type of a bulk response that exists in conventional non-Weyl materials with the same symmetry [3, 4]. The task is to resolve the contribution of the Weyl physics from that based on symmetry consideration. Here we consider the situation when the effect is fully determined by chiral anomaly. This is the chiral vortical effect (CVE) – the type of the parity violating effects [5–7] when there is the current along the vortex axis concentrated in the vortex core
Volovik, G.E. CHIRAL VORTICAL EffECT GENERATED BY CHIRAL ANOMALY IN VORTEX-SKYRMIONS / G.E. Volovik // Письма в Журнал экспериментальной и теоретической физики .— 2017 .— №5-6 .— С. 26-27 .— URL: https://rucont.ru/efd/597389 (дата обращения: 27.04.2024)

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Pis’ma v ZhETF, vol. 105, iss. 5, pp. 282 – 283  2017 March 10 c Chiral vortical effect generated by chiral anomaly in vortex-skyrmions G.E.Volovik1) Low Temperature Laboratory, Aalto University, School of Science and Technology, P.O. Box 15100, FI-00076 AALTO, Finland Landau Institute for Theoretical Physics RAS, 119334 Moscow, Russia Submitted 12 January 2017 DOI: 10.7868/S0370274X1705006X The problems with Weyl materials –Weyl semimetals and Weyl superconductors (see latest reviews in Ref. [1] and Ref. [2] correspondingly) – is that at first glance they should possess any type of a bulk response that exists in conventional non-Weyl materials with the same symmetry [3, 4]. <...> The task is to resolve the contribution of theWeyl physics fromthat based on symmetry consideration. <...> Here we consider the situation when the effect is fully determined by chiral anomaly. <...> This is the chiral vortical effect (CVE) – the type of the parity violating effects [5–7] when there is the current along the vortex axis concentrated in the vortex core. <...> We consider the vortex-skyrmion in Weyl superfluids – the continuous (non-singular) texture in Fig. 1. <...> Instead we use the trick, which has been used for the calculation of the angular momentum of the texture in chiral Weyl superfluids [9] (see also Refs. [10, 11]), and for calculation of different manifestations of the chiral magnetic effect (CME) [12]. <...> We calculate the current generated by deformation of the order parameter within the skyrmion, when it is deformed from the state obeying the space inversion P to the state with the violated space inversion symmetry. <...> In the initial state there is no current along the axis of the skyrmion, since it is forbidden by the P-symmetry. <...> If the texture has no dependence on the coordinate Fig. 1. (Color online) Right: Neel-type vortex skyrmion, which is symmetric under the combined symmetry PTOx,π, which forbids the current along the vortex axis, since Jz = PTOxJz = −Jz. <...> Left: Bloch-type skyrmion, which is symmetric under the combined symmetry TOx,π. <...> The broken P-symmetry allows the current along the vortex axis – the chiral vortical effect. <...> The main difference from the Neel and Bloch skyrmions <...>