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Superconductivity in the regime of attractive interactions in the Tomonaga-Luttinger liquid

Ž. Gosar, N. Janša, T. Arh, P. Jeglič, M. Klanjšek, H. F. Zhai, B. Lv, D. Arčon

DOI 10.1103/PhysRevB.101.220508 · Physical Review B

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Abstract

While the vast majority of known physical realizations of the Tomonaga-Luttinger liquid (TLL) have repulsive interactions defined with the dimensionless interaction parameter Kc<1, we here report that Rb2Mo3As3 is in the opposite TLL regime of attractive interactions. This is concluded from a TLL-characteristic power-law temperature dependence of the Rb87 spin-lattice relaxation rates over a broad temperature range yielding the TLL interaction parameter for charge collective modes Kc=1.4. The TLL of the one-dimensional band can be traced almost down to Tc=10.4 K, where the bulk superconducting state is stabilized by the presence of a three-dimensional band and characterized by the Rb87 temperature-independent Knight shift and the absence of the Hebel-Slichter coherence peak in the relaxation rates. The small superconducting gap measured in high magnetic fields reflects either the importance of the vortex core relaxation or the uniqueness of the superconducting state stemming from the attractive interactions defining the precursor TLL.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Rb2Mo3As3

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10.4Pressure not reportedzero_resistance
Rb2Mo3As3

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10Pressure not reportedonset
K2Mo3As3

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10.4Pressure not reportedunknown
A2Cr3As3

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5Pressure not reportedunknown

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