← Back to search

Unusual behavior in the upper critical magnetic fields of the ambient-pressure organic superconductor κ-(BEDT-TTF)2Cu[N(CN)2]Br [where BEDT-TTF represents bis(ethylenedithio)tetrathiofulvalene]

W. K. Kwok, U. Welp, K. D. Carlson, G. W. Crabtree, K. G. Vandervoort, H. H. Wang, A. M. Kini, J. M. Williams, D. L. Stupka, L. K. Montgomery, J. E. Thompson

DOI 10.1103/PhysRevB.42.8686 · Physical Review B

T1

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 a determination of the temperature dependence of the upper critical magnetic fields Hc2 for κ-(BEDT-TTF)2Cu[N(CN)2]Br, with the use of dc-magnetization measurements that show a well-defined diamagnetic onset. We find large slopes of -20 T/K and -2.2 T/K for H∥ac and H∥b, respectively, which lead to coherence lengths of 37 and 4 Å. There is unusual structure in the critical fields and a possible dimensional crossover at T/Tc∼0.97 for H∥ac. Neither the slopes nor the structure are observable in the superconducting transition measured by ac magnetoresistance, which exhibits strong magnetic-field broadening similar to that of the high-Tc copper oxide superconductor YBa2Cu3O7−δ. We find a strong depression of Tc, as large as 1.2 K, when the sample is rapidly cooled.

Source-reported materials — not catalogue approval

FormulaReported 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.

11.6Pressure unresolvedonset
(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.

10.8Pressure unresolvedunknown
(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.

9.6Pressure unresolvedunknown
(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.

12.5Pressure unresolvedonset
(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.

10.5Pressure unresolvedzero_resistance
YBa2Cu3O7-δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown
(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 reportedunknown

Similar papers