Tailoring the Fulde-Ferrell-Larkin-Ovchinnikov state
Tailoring the Fulde-Ferrell-Larkin-Ovchinnikov state
复制标题
定制 Fulde-Ferrell-Larkin-Ovchinnikov 状态
DOI:
10.1002/andp.201200718
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发表时间:
2012
影响因子:
2.4
通讯作者:
Eschrig M
中科院分区:
文献类型:
--
作者:
Eschrig M
Imagine a piece of paper, 8 km long, 700 m wide, and 0.1 mm thick. Now scale that down by a factor of 105–to 80 mm times 7 mm, and correspondingly its thickness to 10 nm, and you have an idea about the precision and control necessary to create thin films in experiments like the one published recently in Annalen der Physik by Jan-Michael Kehrle and co-workers [1]. The motivation for creating such extraordinarily thin films over comparatively large areas was a prediction that if a thin layer of a conventional superconductor is sandwiched between two ferromagnetic films, then the superconducting transition temperature of this trilayer structure, after initially being suppressed, would show a reentrance behaviour when the thickness of one or both of the ferromagnetic layers is varied. The mechanism for such a reentrant behaviour of the superconducting critical temperature can ultimately be traced back to the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) effect. Peter Fulde and Richard Ferrell, working at the time at the University of Maryland, published their article in August 1964 in Physical Review B (Ref. 3 in [1]). Independently, working at the Moscow Physico-Technical Institute, Anatoly Larkin and Yuri Ovchinnikov published in September 1964 an article about similar effects in Zhurnal Eksperimental’noi i Teoricheskoi Fiziki (which appeared translated in March 1965 in Soviet Physics JETP)(Ref. 4 in [1]).