Influence of internal disorder on the superconducting state in the organic layered superconductor κ−(BEDT−TTF)2Cu[N(CN)2]Br
M. Pinterić, S. Tomić, M. Prester, Đ. Drobac, K. Maki
DOI 10.1103/PhysRevB.66.174521 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
We report high-sensitivity ac susceptibility measurements of the penetration depth in the Meissner state of the layered organic superconductor κ−(BEDT−TTF)2Cu[N(CN)2]Br. We have studied nominally pure single crystals from the two different syntheses and employed controlled cooling procedures in order to minimize intrinsic remnant disorder at low temperatures associated with the glass transition, caused by ordering of the ethylene moieties in BEDT-TTF molecule at TG=75K. We find that the optimal cooling procedures (slow cooling of −0.2K/h or annealing for 3 days in the region of TG) needed to establish the ground state depend critically on the sample origin, indicating different relaxation times of terminal ethylene groups. We show that, in the ground state, the behavior observed for nominally pure single crystals from both syntheses is consistent with unconventional d-wave order parameter. The in-plane penetration depth λin(T) is strongly linear, whereas the out-of-plane component λout(T) varies as T2. In contrast, the behavior of single crystals with long relaxation times observed after slow (−0.2K/h) cooling is as expected for a d-wave superconductor with impurities [i.e., λin(T)∝λout(T)∝T2] or might be also reasonably well described by the s-wave model. Our results might reconcile the contradictory findings previously reported by different authors.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| (BEDT-TTF)2Cu[N(CN)2]Br Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| (BEDT-TTF)2Cu[N(CN)2]Cl Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| (BEDT-TTF)2Cu(NCS)2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Magnetothermal instability in the organic layered superconductor κ−(BEDT-TTF)2Cu(NCS)2
similarity 0.97T. Konoike et al.
Source status unknown — claims are unverified
Effects of randomness on the critical temperature in quasi-two-dimensional organic superconductors
similarity 0.96Enver Nakhmedov et al.
Source status unknown — claims are unverified
In-plane superfluid density and microwave conductivity of the organic superconductor κ-(BEDT-TTF)2Cu[N(CN)2]Br: Evidence for d-wave pairing and resilient quasiparticles
similarity 0.96S. Milbradt et al.
Source status unknown — claims are unverified
Superconductivity and fluctuating magnetism in quasi-two-dimensional κ-(BEDT-TTF)2Cu[N(CN)2]Br probed with implanted muons
similarity 0.96T. Lancaster et al.
Source status unknown — claims are unverified
Interlayer magnetoresistance in the organic superconductor κ−(BEDT−TTF)2Cu[N(CN)2]Br near the superconducting transition
similarity 0.96F. Zuo et al.
Source status unknown — claims are unverified
Critical fields and mixed-state properties of the layered organic superconductor κ-(BEDT−TTF)2I3
similarity 0.96S. Wanka et al.
Source status unknown — claims are unverified