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具有本征约瑟夫森结的高温超导体的时空晶体序。

Space-time crystalline order of a high-critical-temperature superconductor with intrinsic Josephson junctions.

作者信息

Kleiner Reinhold, Zhou Xianjing, Dorsch Eric, Zhang Xufeng, Koelle Dieter, Jin Dafei

机构信息

Physikalisches Institut, Center for Quantum Science (CQ) and LISA+, Universität Tübingen, Tübingen, Germany.

Center for Nanoscale Materials, Argonne National Laboratory, Argonne, IL, USA.

出版信息

Nat Commun. 2021 Oct 15;12(1):6038. doi: 10.1038/s41467-021-26132-y.

DOI:10.1038/s41467-021-26132-y
PMID:34654801
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8520017/
Abstract

We theoretically demonstrate that the high-critical-temperature (high-T) superconductor BiSrCaCuO (BSCCO) is a natural candidate for the recently envisioned classical space-time crystal. BSCCO intrinsically forms a stack of Josephson junctions. Under a periodic parametric modulation of the Josephson critical current density, the Josephson currents develop coupled space-time crystalline order, breaking the continuous translational symmetry in both space and time. The modulation frequency and amplitude span a (nonequilibrium) phase diagram for a so-defined spatiotemporal order parameter, which displays rigid pattern formation within a particular region of the phase diagram. Based on our calculations using representative material properties, we propose a laser-modulation experiment to realize the predicted space-time crystalline behavior. Our findings bring new insight into the nature of space-time crystals and, more generally, into nonequilibrium driven condensed matter systems.

摘要

我们从理论上证明,高临界温度(高温)超导体BiSrCaCuO(BSCCO)是最近设想的经典时空晶体的天然候选者。BSCCO本质上形成了约瑟夫森结的堆叠。在约瑟夫森临界电流密度的周期性参数调制下,约瑟夫森电流发展出耦合的时空晶体序,打破了空间和时间上的连续平移对称性。调制频率和幅度跨越了一个针对如此定义的时空序参量的(非平衡)相图,该相图在相图的特定区域内显示出刚性图案形成。基于我们使用代表性材料特性进行的计算,我们提出了一个激光调制实验来实现预测的时空晶体行为。我们的发现为时空晶体的本质,更一般地说,为非平衡驱动的凝聚态系统带来了新的见解。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/13ed1150f1c8/41467_2021_26132_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/ab8c2d4b9d69/41467_2021_26132_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/67df0823eb65/41467_2021_26132_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/dad348fffc95/41467_2021_26132_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/92021681d1b8/41467_2021_26132_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/131645659fae/41467_2021_26132_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/469217c2ddb8/41467_2021_26132_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/13ed1150f1c8/41467_2021_26132_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/ab8c2d4b9d69/41467_2021_26132_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/67df0823eb65/41467_2021_26132_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/dad348fffc95/41467_2021_26132_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/92021681d1b8/41467_2021_26132_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/131645659fae/41467_2021_26132_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/469217c2ddb8/41467_2021_26132_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1b68/8520017/13ed1150f1c8/41467_2021_26132_Fig7_HTML.jpg

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