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arXiv 2605.07656cond-mat.supr-concond-mat.str-el
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二维d波铁磁体中有限温度配对密度波超导性

Finite temperature pair density wave superconductivity in $d$-wave altermagnets

SRM Institute of Science and Technology(SRM理工学院)

Amrutha N Madhusuthanan, Madhuparna Karmakar

AI总结:

研究通过非微扰静态路径近似蒙特卡罗方法,揭示d波铁磁体在有限温度下稳定有限动量超导的机制,发现配对密度波相在强热波动下仍具鲁棒性,提供实验验证的特征谱学和实空间信号。

摘要:

我们证明铁磁性提供了一种无场机制,用于在二维中稳定有限动量超导性。利用非微扰静态路径近似蒙特卡罗方法,我们展示d波铁磁体支持一种鲁棒的配对密度波(PDW)相,其在有限温度窗口内持续存在,尽管存在强热波动。其机制源于动量依赖的自旋分裂,这有效增强了有限质心动量下的配对不稳定性,而无需Zeeman场。我们识别出与相相干、能隙闭合和伪能隙形成相关的不同热尺度,并建立了PDW相的特征谱学和实空间信号。我们的结果揭示铁磁性作为热稳定有限动量超导性的稳健途径,并为铁磁性材料提供了实验可检验的特征信号。

英文摘要:

We demonstrate that altermagnetism provides a field-free mechanism for stabilizing finite-momentum superconductivity in two dimensions. Using a non-perturbative static path approximation Monte Carlo approach, we show that a d-wave altermagnet supports a robust pair-density-wave (PDW) phase that persists over a finite temperature window despite strong thermal fluctuations. The underlying mechanism originates from momentum-dependent spin splitting, which effectively enhances pairing instabilities at finite center-of-mass momentum without Zeeman fields. We identify distinct thermal scales associated with phase coherence, gap closing, and pseudogap formation, and establish characteristic spectroscopic and real-space signatures of the PDW state. Our results reveal altermagnetism as a robust route to thermally stable finite-momentum superconductivity and provide experimentally testable signatures for altermagnetic materials.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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