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口頭

Non-Hermitian effective Hamiltonian for low-energy quasiparticles

永井 佑紀; Qi, Y.*; 磯部 大樹*; Kozii, V.*; Fu, L.*

no journal, , 

物質をトポロジーで分類することで、トポロジカル絶縁体やトポロジカル超伝導体など、格子欠陥や不純物に強いデバイスが提案されてきた。本ポスターにおいては、重元素化合物などの重い電子系や銅酸化物高温超伝導体などの強相関電子系と呼ばれる物質群において適用できる、新しいトポロジー理論を提案する。この理論では、従来の固体物理学では現れなかった非エルミート有効ハミルトニアンを用いることで、強相関電子系における強い電子間相互作用が誘起する現象を予言することができる。本講演では、近藤半金属というカテゴリーに属する重元素化合物において、角度分解光電子分光実験で測定できる「バルクフェルミアーク」という現象が現れることを予言した。本研究によって、重い電子系の物性の理解に、トポロジーというこれまでとは全く異なった視点を用いることができることが示された。

口頭

Spin-to-charge conversion on the edge of quantum spin Hall insulator

荒木 康史; 三澤 貴宏*; 野村 健太郎*

no journal, , 

We present our theoretical work on dynamical spin-to-charge conversion at the edge of a quantum spin Hall insulator (QSHI), namely a two-dimensional topological insulator with helical edge states. Interconversion between spin- and charge-related quantities has been a key idea in making use of magnetic materials, especially in the context of spintronics. QSHI is a typical system showing a universal charge-to-spin conversion behavior, namely the quantum spin Hall effect, whereas the spin-to-charge conversion therein is still not clearly understood. At a lateral heterojunction of a ferromagnet (FM) and a QSHI, it has been theoretically demonstrated that magnetization dynamics induces a charge current along the edge of QSHI; however, its mechanism from the viewpoint of spin-to-charge conversion still remains to be clarified. In order to understand the spin transfer and the spin-to-charge conversion mechanism in QSHI, we investigate the many-body dynamics of the electrons under the magnetization dynamics at the QSHI-FM junction. We analytically treat the electron dynamics in terms of the Floquet-Keldysh formalism, and compare two physical quantities present on the edge: the spin injection rate from the FM into the QSHI, and the charge current induced along the edge. Whereas the edge current seen in the previous works is reproduced, we find that it is not proportional to the spin injection rate, especially when the exchange interaction at the junction is strong enough. This relation implies that the spin-to-charge conversion in this system cannot be considered as the inverse spin Hall effect, while it can be rather seen as the inverse Edelstein effect, in which an electron spin accumulation at the junction is converted to a charge current. We also focus on the energy transfer at the junction, and interpret this phenomenon in terms of magnon exchange.

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