Phase-slip residual-order spin state in FeSe

Fuente: arXiv
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Autori principali: Liu, Zhixin, Fan, Jiyu, Zhang, Lei, Chunlan, Ma, Ji, Yanda, Yang, Zhongqin, Zhu, Yan
Natura: Preprint
Pubblicazione: 2026
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author Liu, Zhixin
Fan, Jiyu
Zhang, Lei
Chunlan, Ma
Ji, Yanda
Yang, Zhongqin
Zhu, Yan
author_facet Liu, Zhixin
Fan, Jiyu
Zhang, Lei
Chunlan, Ma
Ji, Yanda
Yang, Zhongqin
Zhu, Yan
contents Clarifying the magnetic ground state is essential for analysing unconventional superconductivity, because microscopic magnetic order provides one of the basic starting assumptions for spin-fluctuation pairing theories. FeSe exhibits pronounced stripe- and Neel-type spin fluctuations yet lacks static long-range order, posing a long-standing puzzle. By combining PBE and r2SCAN mixed exchange-correlation calculations with spectrally weighted simulations of the static spin structure factor S(q), we show that FeSe is not governed by a single magnetic configuration but by a nearly degenerate manifold of phase-slip defects embedded in a stripe background. We term this state a residual-order spin state (ROSS): a spin state that retains local stripe-like antiferromagnetic correlations but loses long-range phase coherence because of phase slips. Multiple slip configurations are compressed into an exceptionally narrow energy window. Non-local magneto-elastic coupling redistributes domain-wall formation energy through the lattice, whereas competing magnetic interactions truncate the real-space coherence length to an optimal scale of about ten moments. Weighted superpositions of these slip states reproduce the momentum-space line shapes of both stripe- and Neel-type spin fluctuations observed by inelastic neutron scattering, providing a microscopic basis for superconductivity models built on spin fluctuations.
format Preprint
id arxiv_https___arxiv_org_abs_2605_12293
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Phase-slip residual-order spin state in FeSe
Liu, Zhixin
Fan, Jiyu
Zhang, Lei
Chunlan, Ma
Ji, Yanda
Yang, Zhongqin
Zhu, Yan
Superconductivity
Strongly Correlated Electrons
Clarifying the magnetic ground state is essential for analysing unconventional superconductivity, because microscopic magnetic order provides one of the basic starting assumptions for spin-fluctuation pairing theories. FeSe exhibits pronounced stripe- and Neel-type spin fluctuations yet lacks static long-range order, posing a long-standing puzzle. By combining PBE and r2SCAN mixed exchange-correlation calculations with spectrally weighted simulations of the static spin structure factor S(q), we show that FeSe is not governed by a single magnetic configuration but by a nearly degenerate manifold of phase-slip defects embedded in a stripe background. We term this state a residual-order spin state (ROSS): a spin state that retains local stripe-like antiferromagnetic correlations but loses long-range phase coherence because of phase slips. Multiple slip configurations are compressed into an exceptionally narrow energy window. Non-local magneto-elastic coupling redistributes domain-wall formation energy through the lattice, whereas competing magnetic interactions truncate the real-space coherence length to an optimal scale of about ten moments. Weighted superpositions of these slip states reproduce the momentum-space line shapes of both stripe- and Neel-type spin fluctuations observed by inelastic neutron scattering, providing a microscopic basis for superconductivity models built on spin fluctuations.
title Phase-slip residual-order spin state in FeSe
topic Superconductivity
Strongly Correlated Electrons
url https://arxiv.org/abs/2605.12293