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Absence of μSR evidence for magnetic order in the pseudogap phase of Bi_(2+x)Sr_(2-x)CaCu_2O_(8+δ)

机译:在Bi_(2 + x)sr_(2-x)cacu_2o_(8 +δ)的伪曲面阶段中磁场缺失μsr证据

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摘要

We present an extended zero-field muon spin relaxation (ZF-μSR) study of overdoped Bi_(2+x)Sr_(2-x)CaCu_2O_(8+δ) (Bi2212) single crystals, intended to elucidate the origin of weak quasistatic magnetism previously detected by μSR in the superconducting and normal states of optimally doped and overdoped samples. New results on heavily overdoped single crystals show a similar monotonically decreasing ZF-μSR relaxation rate with increasing temperature that persists above the pseudogap (PG) temperature T* and does not evolve with hole doping (p). Additional measurements using an ultralow-background apparatus confirm that this behavior is an intrinsic property of Bi2212, which cannot be due to magnetic order associated with the PG phase. Instead we show that the temperature-dependent relaxation rate is most likely caused by structural changes that modify the contribution of the nuclear dipole fields to the ZF-μSR signal. Our results for Bi2212 emphasize the importance of not assuming that the nuclear-dipole field contribution is independent of temperature in ZF-μSR studies of high-temperature (high-T_c) cuprate superconductors, and do not support a recent μSR study of YBa_2Cu_3O(6+x) that claims to detect magnetic order in the PG phase.
机译:我们介绍过零域μs旋转弛豫(ZF-μSR)研究的过载Bi_(2 + x)Sr_(2-x)Cacu_2O_(8 +δ)(Bi2212)单晶,旨在阐明弱Quasistatic的起源先前在最佳掺杂和过掺杂的样品的超导和正常状态下由μSR检测的磁力。在覆盖的单晶上的新结果显示出类似的单调减少ZF-μSR弛豫率,随着持续的温度(PG)温度T *而持续的温度,不与孔掺杂(P)的升高。使用超级背景装置的额外测量确认该行为是BI2212的内在属性,其不能由于与PG相相关的磁性顺序。相反,我们表明温度依赖性的弛豫率最有可能由结构变化来改变核偶极场对ZF-μSR信号的贡献。我们对BI2212的结果强调了不假设核 - 偶极场贡献与高温(高T_C)铜替代超导体ZF-μSR研究中的温度无关的重要性,并且不支持最近的YBA_2CU_3O的研究(6 + X)声称在PG阶段检测磁场。

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  • 来源
    《Physical review》 |2020年第18期|184511.1-184511.7|共7页
  • 作者单位

    Department of Physics Simon Fraser University Burnaby British Columbia Canada V5A IS6;

    Department of Physics Simon Fraser University Burnaby British Columbia Canada V5A IS6;

    Department of Physics Simon Fraser University Burnaby British Columbia Canada V5A IS6;

    Department of Physics Simon Fraser University Burnaby British Columbia Canada V5A IS6;

    Department of Physics Simon Fraser University Burnaby British Columbia Canada V5A IS6 Kwantlen Polytechnic University Richmond British Columbia Canada V6X 3X7;

    Department of Physics Simon Fraser University Burnaby British Columbia Canada V5A IS6 Centre for Molecular and Materials Science TRIUMF Vancouver British Columbia Canada V6T 2A3;

    Brookhaven National Laboratory Upton New York 11973 USA;

    Department of Physics Simon Fraser University Burnaby British Columbia Canada V5A IS6;

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