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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Fulde-Ferrel-Larkin-Ovchinnikov inhomogeneous superconducting state and phase transitions induced by spin accumulation in a ferromagnet-d_(x~2-y~(2-))-wave superconductor-ferromagnet tunnel junction
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Fulde-Ferrel-Larkin-Ovchinnikov inhomogeneous superconducting state and phase transitions induced by spin accumulation in a ferromagnet-d_(x~2-y~(2-))-wave superconductor-ferromagnet tunnel junction

机译:铁磁体-d_(x〜2-y〜(2-))-波超导体-铁磁体隧道结中自旋积累引起的Fulde-Ferrel-Larkin-Ovchinnikov非均匀超导状态和相变

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摘要

Fulde-Ferrel-Larkin-Ovchinnikov (FFLO) inhomogeneous superconducting (SC) state, first- and second-order phase transitions, and quantum criticality induced by spin accumulation in a ferromagnet-d_(x~2-y~(2-))-wave superconductor-ferromagnet tunnel junction are theoretically predicted. A complex phase diagram in the temperature-bias voltage plane is determined. It is found that the phase transitions from the homogeneous BCS state to the inhomogeneous FFLO state, and from the FFLO state with the momentum q's azimuthal angle θ_q=0 to that with θ_q=π/4, are of the first order, whereas the transitions from all SC states to the normal state at critical voltages are of the second order. A Lifshitz point, a bicritical point, and a quantum critical point are identified.
机译:Fulde-Ferrel-Larkin-Ovchinnikov(FFLO)非均匀超导(SC)状态,一阶和二阶相变以及铁磁体d_(x〜2-y〜(2-))中自旋积累引起的量子临界性理论上预测了超波-铁磁体隧道结。确定了温度偏置电压平面中的复数相位图。发现从均相BCS状态到非均质FFLO状态以及从动量q方位角θ_q= 0的FFLO状态到θ_q=π/ 4的相位都处于一阶跃迁,而跃迁从所有SC状态到正常状态的临界电压均为二阶。鉴定了Lifshitz点,双临界点和量子临界点。

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