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Zeeman-Driven Phase Transition within the Superconducting State of κ−(BEDT−TTF)2Cu(NCS)2

J. A. Wright, E. Green, P. Kuhns, A. Reyes, J. Brooks, J. Schlueter, R. Kato, H. Yamamoto, M. Kobayashi, S. E. Brown

DOI 10.1103/PhysRevLett.107.087002 · Physical Review Letters

T1

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Abstract

C13 nuclear magnetic resonance measurements were performed on κ−(BEDT−TTF)2Cu(NCS)2, with the external field placed parallel to the quasi-2D conducting layers. The absorption spectrum is used to determine the electronic spin polarization Ms as a function of external field H at a temperature T=0.35 K. A discontinuity in the derivative dMs/dH at an applied field of Hs=213±3 kOe is taken as evidence for a Zeeman-driven transition within the superconducting state and stabilization of inhomogeneous superconductivity.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
κ-(BEDT-TTF)2Cu(NCS)2

Archive — visibility unverified

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9.5Pressure not reportedonset
CeCoIn5

Archive — visibility unverified

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

—Pressure not reportedunknown

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