Quantum Lifshitz points in an altermagnetic superconductor

Abstract We predict the existence of two tri-critical quantum Lifshitz points in recently discovered d -wave altermagnetic metals subjected to an external magnetic field. These points connect a spatially modulated Fulde–Ferrell–Larkin–Ovchinnikov (FFLO) phase, a uniform polarized Bardeen–Cooper–Schrieffer (BCS) superconducting phase, and the normal metallic phase in a nontrivial manner. Depending on whether the FFLO state is primarily induced by the magnetic field or by d -wave altermagnetism, we classify the corresponding Lifshitz points as field-driven or altermagnetism-driven, respectively. Notably, the two types exhibit distinct behaviors: the transition from the FFLO phase to the polarized BCS phase is first-order near the field-driven Lifshitz point, as might be expected, whereas it becomes continuous near the altermagnetism-driven Lifshitz point. We further explore the effects of finite temperature and find that the altermagnetism-driven Lifshitz point is significantly more sensitive to thermal fluctuations.

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Publication Details

Journal
AAPPS bulletin
Published
2025-12-02
DOI
https://doi.org/10.1007/s43673-025-00178-2
Primary Topic
Physics of Superconductivity and Magnetism
Type
article
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article

Quantum Lifshitz points in an altermagnetic superconductor

Xia-Ji Liu, Hui Hu
AAPPS bulletin
Physics of Superconductivity and Magnetism
article

Quantum Lifshitz points in an altermagnetic superconductor

Xia-Ji Liu, Hui Hu
article en

Abstract

Abstract We predict the existence of two tri-critical quantum Lifshitz points in recently discovered d -wave altermagnetic metals subjected to an external magnetic field. These points connect a spatially modulated Fulde–Ferrell–Larkin–Ovchinnikov (FFLO) phase, a uniform polarized Bardeen–Cooper–Schrieffer (BCS) superconducting phase, and the normal metallic phase in a nontrivial manner. Depending on whether the FFLO state is primarily induced by the magnetic field or by d -wave altermagnetism, we classify the corresponding Lifshitz points as field-driven or altermagnetism-driven, respectively. Notably, the two types exhibit distinct behaviors: the transition from the FFLO phase to the polarized BCS phase is first-order near the field-driven Lifshitz point, as might be expected, whereas it becomes continuous near the altermagnetism-driven Lifshitz point. We further explore the effects of finite temperature and find that the altermagnetism-driven Lifshitz point is significantly more sensitive to thermal fluctuations.

AAPPS bulletinVol. 35(1)
Quantum (Australia) (AU), Swinburne University of Technology (AU)
Openalex Percentile: Top 76%
Physics of Superconductivity and Magnetism
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