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具有单轴单离子各向异性的混合自旋-(1/2)海森堡二聚体的二分纠缠的非常规热驱动和磁场驱动变化

Unconventional Thermal and Magnetic-Field-Driven Changes of a Bipartite Entanglement of a Mixed Spin-(1/2,) Heisenberg Dimer with an Uniaxial Single-Ion Anisotropy.

作者信息

Vargová Hana, Strečka Jozef

机构信息

Institute of Experimental Physics, Slovak Academy of Sciences, Watsonova 47, 040 01 Košice, Slovakia.

Department of Theoretical Physics and Astrophysics, Faculty of Science, P. J. Šafárik University, Park Angelinum 9, 040 01 Košice, Slovakia.

出版信息

Nanomaterials (Basel). 2021 Nov 16;11(11):3096. doi: 10.3390/nano11113096.

DOI:10.3390/nano11113096
PMID:34835860
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8623281/
Abstract

The concept of negativity is adapted in order to explore the quantum and thermal entanglement of the mixed spin-(1/2,) Heisenberg dimers in presence of an external magnetic field. The mutual interplay between the spin size , XXZ exchange and uniaxial single-ion anisotropy is thoroughly examined with a goal to tune the degree and thermal stability of the pairwise entanglement. It turns out that the antiferromagnetic spin-(1/2,) Heisenberg dimers exhibit higher degree of entanglement and higher threshold temperature in comparison with their ferromagnetic counterparts when assuming the same set of model parameters. The increasing spin magnitude accompanied with an easy-plane uniaxial single-ion anisotropy can enhance not only the thermal stability but simultaneously the degree of entanglement. It is additionally shown that the further enhancement of a bipartite entanglement can be achieved in the mixed spin-(1/2,) Heisenberg dimers, involving half-odd-integer spins . Under this condition the thermal negativity saturates at low-enough temperatures in its maximal value regardless of the magnitude of half-odd-integer spin . The magnetic field induces consecutive discontinuous phase transitions in the mixed spin-(1/2,) Heisenberg dimers with S>1, which are manifested in a surprising oscillating magnetic-field dependence of the negativity observed at low enough temperature.

摘要

为了探究在存在外部磁场的情况下混合自旋 -(1/2)海森堡二聚体的量子和热纠缠,我们采用了负性的概念。我们深入研究了自旋大小、XXZ 交换和单轴单离子各向异性之间的相互作用,目的是调节成对纠缠的程度和热稳定性。结果表明,在假设相同的一组模型参数时,反铁磁自旋 -(1/2)海森堡二聚体与其铁磁对应物相比,表现出更高程度的纠缠和更高的阈值温度。伴随着易平面单轴单离子各向异性的自旋大小增加,不仅可以提高热稳定性,同时还能提高纠缠程度。此外还表明,在涉及半奇数整数自旋的混合自旋 -(1/2)海森堡二聚体中,可以进一步增强二分纠缠。在这种情况下,无论半奇数整数自旋的大小如何,热负性在足够低的温度下都会饱和到其最大值。磁场在 S > 1 的混合自旋 -(1/2)海森堡二聚体中诱导连续的不连续相变,这在足够低的温度下观察到的负性的令人惊讶的振荡磁场依赖性中表现出来。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/8411c3590f16/nanomaterials-11-03096-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/250024359a96/nanomaterials-11-03096-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/4abfc8bcc4c0/nanomaterials-11-03096-g002a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/01d424698809/nanomaterials-11-03096-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/7fd099c570e0/nanomaterials-11-03096-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/338890126773/nanomaterials-11-03096-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/82891918fd96/nanomaterials-11-03096-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/8411c3590f16/nanomaterials-11-03096-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/250024359a96/nanomaterials-11-03096-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/4abfc8bcc4c0/nanomaterials-11-03096-g002a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/01d424698809/nanomaterials-11-03096-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/7fd099c570e0/nanomaterials-11-03096-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/338890126773/nanomaterials-11-03096-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/82891918fd96/nanomaterials-11-03096-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9f13/8623281/8411c3590f16/nanomaterials-11-03096-g007.jpg

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