Spin-Stripe Order Tied to the Pseudogap Phase in La1.8−xEu0.2SrxCuO4

IF 11.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY
Anne Missiaen, Hadrien Mayaffre, Steffen Krämer, Dan Zhao, Yanbing Zhou, Tao Wu, Xianhui Chen, Sunseng Pyon, Tomohiro Takayama, Hidenori Takagi, David LeBoeuf, Marc-Henri Julien
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In <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mrow><c:msub><c:mrow><c:mi>La</c:mi></c:mrow><c:mrow><c:mn>2</c:mn><c:mo>−</c:mo><c:mi>x</c:mi></c:mrow></c:msub><c:mrow><c:msub><c:mrow><c:mi>Sr</c:mi></c:mrow><c:mrow><c:mi>x</c:mi></c:mrow></c:msub></c:mrow><c:mrow><c:msub><c:mrow><c:mi>CuO</c:mi></c:mrow><c:mrow><c:mn>4</c:mn></c:mrow></c:msub></c:mrow></c:mrow></c:math> (LSCO) and in zero external magnetic field, static spin stripes are confined to a doping range well below <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:msup><e:mi>p</e:mi><e:mo>*</e:mo></e:msup></e:math>, the pseudogap boundary at zero temperature. However, when high fields suppress the competing effect of superconductivity, spin-stripe order is found to extend up to <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:msup><g:mi>p</g:mi><g:mo>*</g:mo></g:msup></g:math>. Here, we investigate <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mrow><i:msub><i:mrow><i:mi>La</i:mi></i:mrow><i:mrow><i:mn>1.8</i:mn><i:mo>−</i:mo><i:mi>x</i:mi></i:mrow></i:msub><i:mrow><i:msub><i:mrow><i:mi>Eu</i:mi></i:mrow><i:mrow><i:mn>0.2</i:mn></i:mrow></i:msub></i:mrow><i:mrow><i:msub><i:mrow><i:mi>Sr</i:mi></i:mrow><i:mrow><i:mi>x</i:mi></i:mrow></i:msub></i:mrow><i:mrow><i:msub><i:mrow><i:mi>CuO</i:mi></i:mrow><i:mrow><i:mn>4</i:mn></i:mrow></i:msub></i:mrow></i:mrow></i:math> (Eu-LSCO) using <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mrow><k:mmultiscripts><k:mrow><k:mi>La</k:mi></k:mrow><k:mprescripts/><k:none/><k:mrow><k:mn>139</k:mn></k:mrow></k:mmultiscripts></k:mrow></k:math> nuclear magnetic resonance and observe field-dependent spin fluctuations suggesting a similar competition between superconductivity and spin order as in LSCO. Nevertheless, we find that static spin stripes are present practically up to <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:msup><m:mi>p</m:mi><m:mo>*</m:mo></m:msup></m:math> irrespective of field strength: The stronger stripe order in Eu-LSCO prevents superconductivity from enforcing a nonmagnetic ground state, except very close to <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:msup><o:mi>p</o:mi><o:mo>*</o:mo></o:msup></o:math>. Thus, spin-stripe order is consistently bounded by <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><q:msup><q:mi>p</q:mi><q:mo>*</q:mo></q:msup></q:math> in both LSCO and Eu-LSCO, despite their differing balances between stripe order and superconductivity. This indicates that the canonical stripe order, where spins and charges are intertwined in a static pattern, is fundamentally tied to the pseudogap phase, though the exact nature of this connection has yet to be elucidated. Any stripe order beyond the pseudogap endpoint must then be of a different nature: Either spin and charge orders remain intertwined, but both fluctuating, or only spin order fluctuates while charge order remains static. 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引用次数: 0

Abstract

Although spin and charge stripes in high-Tc cuprates have been extensively studied, the exact range of carrier concentration over which they form a static order remains uncertain, complicating efforts to understand their significance. The problem is challenging due to the combined effects of quenched disorder and competition with superconductivity—both significant in cuprates—which add to the inherent difficulty of determining phase boundaries. In La2xSrxCuO4 (LSCO) and in zero external magnetic field, static spin stripes are confined to a doping range well below p*, the pseudogap boundary at zero temperature. However, when high fields suppress the competing effect of superconductivity, spin-stripe order is found to extend up to p*. Here, we investigate La1.8xEu0.2SrxCuO4 (Eu-LSCO) using La139 nuclear magnetic resonance and observe field-dependent spin fluctuations suggesting a similar competition between superconductivity and spin order as in LSCO. Nevertheless, we find that static spin stripes are present practically up to p* irrespective of field strength: The stronger stripe order in Eu-LSCO prevents superconductivity from enforcing a nonmagnetic ground state, except very close to p*. Thus, spin-stripe order is consistently bounded by p* in both LSCO and Eu-LSCO, despite their differing balances between stripe order and superconductivity. This indicates that the canonical stripe order, where spins and charges are intertwined in a static pattern, is fundamentally tied to the pseudogap phase, though the exact nature of this connection has yet to be elucidated. Any stripe order beyond the pseudogap endpoint must then be of a different nature: Either spin and charge orders remain intertwined, but both fluctuating, or only spin order fluctuates while charge order remains static. The presence of spin-stripe order up to p* and the pervasive, slow, and field-dependent spin-stripe fluctuations, as well as the electronic inhomogeneity documented in this work, must all be carefully considered in discussions of Fermi surface transformations, putative quantum criticality, and strange metal behavior. Published by the American Physical Society 2025
La1.8−xEu0.2SrxCuO4中赝隙相的自旋条纹序
尽管高tc铜酸盐中的自旋和电荷条纹已被广泛研究,但它们形成静态顺序的载流子浓度的确切范围仍然不确定,这使理解其意义的努力复杂化。这个问题是具有挑战性的,因为在铜酸盐中,淬火无序和超导竞争的综合影响都很显著,这增加了确定相边界的固有困难。在La2−xSrxCuO4 (LSCO)中,在零外加磁场下,静态自旋条纹被限制在远低于p*(零温度下的赝隙边界)的掺杂范围内。然而,当高场抑制超导性的竞争效应时,发现自旋条纹顺序扩展到p*。在这里,我们使用La139核磁共振研究了La1.8−xEu0.2SrxCuO4 (Eu-LSCO),并观察到场相关的自旋涨落,表明超导性和自旋顺序之间存在类似于LSCO中的竞争。尽管如此,我们发现静态自旋条纹几乎在p*处存在,与场强无关:Eu-LSCO中较强的条纹顺序阻止了超导性强制非磁性基态,除非非常接近p*。因此,在LSCO和Eu-LSCO中,尽管条带顺序和超导性之间的平衡不同,但自旋-条带顺序始终以p*为界。这表明,自旋和电荷以静态模式交织在一起的规范条纹秩序从根本上与赝隙相联系在一起,尽管这种联系的确切性质尚未得到阐明。任何超出赝隙端点的条纹顺序必须具有不同的性质:自旋和电荷顺序仍然交织在一起,但都是波动的,或者只有自旋顺序波动而电荷顺序保持静态。在讨论费米表面变换、假定的量子临界性和奇怪的金属行为时,必须仔细考虑到高达p*的自旋条序和普遍的、缓慢的、场相关的自旋条波动,以及本工作中记录的电子不均匀性。2025年由美国物理学会出版
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Physical Review X
Physical Review X PHYSICS, MULTIDISCIPLINARY-
CiteScore
24.60
自引率
1.60%
发文量
197
审稿时长
3 months
期刊介绍: Physical Review X (PRX) stands as an exclusively online, fully open-access journal, emphasizing innovation, quality, and enduring impact in the scientific content it disseminates. Devoted to showcasing a curated selection of papers from pure, applied, and interdisciplinary physics, PRX aims to feature work with the potential to shape current and future research while leaving a lasting and profound impact in their respective fields. Encompassing the entire spectrum of physics subject areas, PRX places a special focus on groundbreaking interdisciplinary research with broad-reaching influence.
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