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场驱动量子系统的热化。

Thermalization of field driven quantum systems.

机构信息

Department of Physics, Georgetown University, 37th and O Sts. NW, Washington, DC 20057 USA.

出版信息

Sci Rep. 2014 Apr 16;4:4699. doi: 10.1038/srep04699.

DOI:10.1038/srep04699
PMID:24736404
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3988485/
Abstract

There is much interest in how quantum systems thermalize after a sudden change, because unitary evolution should preclude thermalization. The eigenstate thermalization hypothesis resolves this because all observables for quantum states in a small energy window have essentially the same value; it is violated for integrable systems due to the infinite number of conserved quantities. Here, we show that when a system is driven by a DC electric field there are five generic behaviors: (i) monotonic or (ii) oscillatory approach to an infinite-temperature steady state; (iii) monotonic or (iv) oscillatory approach to a nonthermal steady state; or (v) evolution to an oscillatory state. Examining the Hubbard model (which thermalizes under a quench) and the Falicov-Kimball model (which does not), we find both exhibit scenarios (i-iv), while only Hubbard shows scenario (v). This shows richer behavior than in interaction quenches and integrability in the absence of a field plays no role.

摘要

人们对量子系统在突然变化后如何热化非常感兴趣,因为幺正演化应该排除热化。本征态热化假说解决了这个问题,因为在小能量窗口中量子态的所有可观测量具有基本相同的值;对于可积系统来说,由于存在无限数量的守恒量,这一假说被违反。在这里,我们表明,当系统受到直流电场驱动时,存在五种通用行为:(i)单调或(ii)振荡到无限温度稳态;(iii)单调或(iv)振荡到非热稳态;或(v)演化到振荡状态。通过检查哈伯模型(在淬火下热化)和法利科夫-金博尔模型(不热化),我们发现这两个模型都表现出了情况(i-iv),而只有哈伯模型表现出了情况(v)。这表明了比相互作用淬火更丰富的行为,并且在没有场的情况下,可积性没有作用。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/ff030b104c95/srep04699-f8.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/aa8b8a6d3f46/srep04699-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/092e83f60a71/srep04699-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/9d1b9356c5ee/srep04699-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/ca66d9bd85ef/srep04699-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/ff030b104c95/srep04699-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/10d327cdfd3d/srep04699-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/fb5fb307e2ad/srep04699-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/94cb283b51c1/srep04699-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/aa8b8a6d3f46/srep04699-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/092e83f60a71/srep04699-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/9d1b9356c5ee/srep04699-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/ca66d9bd85ef/srep04699-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1c5f/3988485/ff030b104c95/srep04699-f8.jpg

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