Orphan high field superconductivity in non-superconducting uranium ditelluride.

Published

April 20, 2024

Author(s)

Corey Frank, Sylvia Lewin, Gicela Saucedo Salas, Peter Czajka, Ian Hayes, Hyeok Yoon, Tristin Metz, Johnpierre Paglione, John Singleton, Nicholas Butch

Abstract

Reentrant superconductivity is an uncommon phenomenon in which the destructive effects of magnetic field on superconductivity are mitigated, allowing a zero-resistance state to survive under conditions that would otherwise destroy it. Typically, the reentrant superconducting region derives from a zero-field parent superconducting phase. Here, we show that in UTe2 crystals extreme applied magnetic fields give rise to an unprecedented high-field superconductor that lacks a zero-field antecedent. This high-field orphan superconductivity exists at angles offset between 29 (deg.) and 42 (deg.) from the crystallographic b to c axes with applied fields between 37 T and 52 T. The stability of field-induced orphan superconductivity presented in this work defies both empirical precedent and theoretical explanation and demonstrates that high-field superconductivity can exist in an otherwise non-superconducting material.

Citation

Nature Communications

Volume

15

Pub Type

Journals

Download Paper

https://doi.org/10.1038/s41467-024-47090-1

Local Download

Keywords

Superconductivity, Topological Superconductors, Spin triplet superconductors, Heavy fermions

Citation

Frank, C. , Lewin, S. , Saucedo Salas, G. , Czajka, P. , Hayes, I. , Yoon, H. , Metz, T. , Paglione, J. , Singleton, J. and Butch, N. (2024), Orphan high field superconductivity in non-superconducting uranium ditelluride., Nature Communications, [online], https://doi.org/10.1038/s41467-024-47090-1, https://tsapps.nist.gov/publication/get_pdf.cfm?pub_id=936504 (Accessed July 17, 2024)