Experimental and semiempirical method to determine the Pauli-limiting field in quasi-two-dimensional superconductors as applied to $\ensuremath{\kappa}$-(BEDT-TTF)${}_{2}$Cu(NCS)${}_{2}$: Strong evidence of a FFLO state

Experimental and semiempirical method to determine the Pauli-limiting field in quasi-two-dimensional superconductors as applied to $κ$ -(BEDT-TTF) $_{2}$ Cu(NCS) $_{2}$ : Strong evidence of a FFLO state

C. C. Agosta, Jing Jin, W. A. Coniglio, B. E. Smith, K. Cho, I. Stroe, C. Martin, S. W. Tozer, T. P. Murphy, E. C. Palm, J. A. Schlueter, and M. Kurmoo

Phys. Rev. B 85, 214514 – Published 15 June 2012

Abstract

We present upper critical field data for $κ$ -(BEDT-TTF) $_{2}$ Cu(NCS) $_{2}$ with the magnetic field close to parallel and parallel to the conducting layers. We show that we can eliminate the effect of vortex dynamics in these layered materials if the layers are oriented within 0.3 $^{\circ}$ of parallel to the applied magnetic field. Eliminating vortex effects leaves one remaining feature in the data that corresponds to the Pauli paramagnetic limit ( $H_{p}$ ). We propose a semiempirical method to calculate the $H_{p}$ in quasi-2D superconductors. This method takes into account the energy gap of each of the quasi-2D superconductors, which is calculated from specific-heat data, and the influence of many-body effects. The calculated Pauli paramagnetic limits are then compared to critical field data for the title compound and other organic conductors. Many of the examined quasi-2D superconductors, including the above organic superconductors and CeCoIn $_{5}$ , exhibit upper critical fields that exceed their calculated $H_{p}$ suggesting unconventional superconductivity. We show that the high-field low-temperature state in $κ$ -(BEDT-TTF) $_{2}$ Cu(NCS) $_{2}$ is consistent with the Fulde-Ferrell-Larkin-Ovchinnikov state.