Spin-helix Larmor mode
Abstract A two-dimensional electron gas (2DEG) with equal-strength Rashba and Dresselhaus spin-orbit coupling sustains persistent helical spin-wave states, which have remarkably long lifetimes. In the presence of an in-plane magnetic field, there exist single-particle excitations that have the chara...
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Nature Portfolio
2018
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oai:doaj.org-article:e9b7547702eb43b4b38a36159c1576a42021-12-02T11:41:24ZSpin-helix Larmor mode10.1038/s41598-018-21818-82045-2322https://doaj.org/article/e9b7547702eb43b4b38a36159c1576a42018-02-01T00:00:00Zhttps://doi.org/10.1038/s41598-018-21818-8https://doaj.org/toc/2045-2322Abstract A two-dimensional electron gas (2DEG) with equal-strength Rashba and Dresselhaus spin-orbit coupling sustains persistent helical spin-wave states, which have remarkably long lifetimes. In the presence of an in-plane magnetic field, there exist single-particle excitations that have the character of propagating helical spin waves. For magnon-like collective excitations, the spin-helix texture reemerges as a robust feature, giving rise to a decoupling of spin-orbit and electronic many-body effects. We prove that the resulting spin-flip wave dispersion is the same as in a magnetized 2DEG without spin-orbit coupling, apart from a shift by the spin-helix wave vector. The precessional mode about the persistent spin-helix state is shown to have an energy given by the bare Zeeman splitting, in analogy with Larmor’s theorem. We also discuss ways to observe the spin-helix Larmor mode experimentally.Shahrzad KarimiCarsten A. UllrichIrene D’AmicoFlorent PerezNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 8, Iss 1, Pp 1-10 (2018) |
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Medicine R Science Q Shahrzad Karimi Carsten A. Ullrich Irene D’Amico Florent Perez Spin-helix Larmor mode |
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Abstract A two-dimensional electron gas (2DEG) with equal-strength Rashba and Dresselhaus spin-orbit coupling sustains persistent helical spin-wave states, which have remarkably long lifetimes. In the presence of an in-plane magnetic field, there exist single-particle excitations that have the character of propagating helical spin waves. For magnon-like collective excitations, the spin-helix texture reemerges as a robust feature, giving rise to a decoupling of spin-orbit and electronic many-body effects. We prove that the resulting spin-flip wave dispersion is the same as in a magnetized 2DEG without spin-orbit coupling, apart from a shift by the spin-helix wave vector. The precessional mode about the persistent spin-helix state is shown to have an energy given by the bare Zeeman splitting, in analogy with Larmor’s theorem. We also discuss ways to observe the spin-helix Larmor mode experimentally. |
format |
article |
author |
Shahrzad Karimi Carsten A. Ullrich Irene D’Amico Florent Perez |
author_facet |
Shahrzad Karimi Carsten A. Ullrich Irene D’Amico Florent Perez |
author_sort |
Shahrzad Karimi |
title |
Spin-helix Larmor mode |
title_short |
Spin-helix Larmor mode |
title_full |
Spin-helix Larmor mode |
title_fullStr |
Spin-helix Larmor mode |
title_full_unstemmed |
Spin-helix Larmor mode |
title_sort |
spin-helix larmor mode |
publisher |
Nature Portfolio |
publishDate |
2018 |
url |
https://doaj.org/article/e9b7547702eb43b4b38a36159c1576a4 |
work_keys_str_mv |
AT shahrzadkarimi spinhelixlarmormode AT carstenaullrich spinhelixlarmormode AT irenedamico spinhelixlarmormode AT florentperez spinhelixlarmormode |
_version_ |
1718395434078044160 |