Koutroulakis G, Kühne H, Schlueter J A, Wosnitza J, Brown S E
Department of Physics and Astronomy, UCLA, Los Angeles, California 90095, USA.
Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany.
Phys Rev Lett. 2016 Feb 12;116(6):067003. doi: 10.1103/PhysRevLett.116.067003.
Quasi-two-dimensional superconductors with a sufficiently weak interlayer coupling allow magnetic flux to penetrate in the form of Josephson vortices for in-plane applied magnetic fields. A consequence is the dominance of the Zeeman interaction over orbital effects. In the clean limit, the normal state is favored over superconductivity for fields greater than the paramagnetic limiting field, unless an intermediate, inhomogeneous state is stabilized. Presented here are nuclear magnetic resonance (NMR) studies of the inhomogeneous Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) state for β''-(ET)2SF5CH2CF2SO3. The uniform superconductivity-FFLO transition is identified at an applied field value of 9.3(0.1) T at low temperature (T=130 mK), and evidence for a possible second transition between inhomogeneous states at ∼11 T is presented. The spin polarization distribution inferred from the NMR absorption spectrum compares favorably to a single-Q modulation of the superconducting order parameter.
对于层间耦合足够弱的准二维超导体,当施加面内磁场时,磁通量能够以约瑟夫森涡旋的形式穿透。结果是塞曼相互作用在轨道效应中占主导地位。在清洁极限下,对于大于顺磁极限场的磁场,正常态比超导态更受青睐,除非一种中间的非均匀态得以稳定。本文展示了对β''-(ET)2SF5CH2CF2SO3的非均匀富尔德 - 费雷尔 - 拉金 - 奥夫钦尼科夫(FFLO)态的核磁共振(NMR)研究。在低温(T = 130 mK)下,在9.3(0.1) T的外加场值处确定了均匀超导 - FFLO转变,并给出了在约11 T处非均匀态之间可能存在第二次转变的证据。从NMR吸收光谱推断出的自旋极化分布与超导序参量的单Q调制结果吻合良好。