Impurity Effect on the In-plane Penetration Depth of the Organic Superconductors $κ$-(BEDT-TTF)$_2X$ ($X$ = Cu(NCS)$_2$ and Cu[N(CN)$_2$]Br)

N. Yoneyama; A. Higashihara; T. Sasaki; T. Nojima; N. Kobayashi

doi:10.1143/JPSJ.73.1290

paper

Impurity Effect on the In-plane Penetration Depth of the Organic Superconductors $κ$ -(BEDT-TTF) $_{2} X$ ( $X$ = Cu(NCS) $_{2}$ and Cu[N(CN) $_{2}$ ]Br)

arXiv:cond-mat/0311300 · doi:10.1143/JPSJ.73.1290

Abstract

We report the in-plane penetration depth $λ_{∥}$ of single crystals $κ$ -(BEDT-TTF) $_{2} X$ ( $X =$ Cu(NCS) $_{2}$ and Cu[N(CN) $_{2}$ ]Br) by means of the reversible magnetization measurements under the control of cooling-rate. In $X$ = Cu(NCS) $_{2}$ , $λ_{∥} (0)$ as an extrapolation toward $T$ = 0 K does not change by the cooling-rate within the experimental accuracy, while $T_{c}$ is slightly reduced. On the other hand, in $X$ = Cu[N(CN) $_{2}$ ]Br, $λ_{∥} (0)$ indicates a distinct increase by cooling faster. The different behavior of $λ_{∥} (0)$ on cooling-rate between the two salts is quantitatively explained in terms of the local-clean approximation (London model), considering that the former salt belongs to the very clean system and the later the moderate clean one. The good agreement with this model demonstrates that disorders of ethylene-group in BEDT-TTF introduced by cooling faster increase the electron(quasiparticle)-scattering, resulting in shorter mean free path.

8 pages, 9 figures

Impurity Effect on the In-plane Penetration Depth of the Organic Superconductors κ-(BEDT-TTF)2​X (X = Cu(NCS)2​ and Cu[N(CN)2​]Br)

Abstract

Impurity Effect on the In-plane Penetration Depth of the Organic Superconductors $κ$ -(BEDT-TTF) $_{2} X$ ( $X$ = Cu(NCS) $_{2}$ and Cu[N(CN) $_{2}$ ]Br)