别列津斯基-科斯特利茨-索利斯相变

别列津斯基-科斯特利茨-索利斯相变（英语：Berezinskii–Kosterlitz–Thouless transition，又称BKT相变；科斯特利茨-索利斯相变及KT相变）是二维XY模型中的一种相变。它是指超过某一临界温度时，系统中的涡旋-反涡旋束缚态融化成为不成对的涡旋和反涡旋的相变。这种相变是以凝聚态物理学家瓦季姆·别列津斯基（英语：Vadim Berezinskii）、约翰·科斯特利茨和戴维·索利斯命名的。BKT相变在凝聚态物理学中多个可用XY模型作近似的系统中出现，例如约瑟夫森接面阵列和薄无序超导颗粒膜。这个词最近还被研究二维超导绝缘体相变的社群应用，用于把库珀对钉在绝缘区，能够这样做是因为超导中的这一相变与BKT相变有相似的地方。

对这种相变的研究使得索利斯和科斯特利茨于2016年与邓肯·霍尔丹一同获授诺贝尔物理学奖。

XY模型[编辑]

XY模型的哈密顿是

$H=-J\sum _{\langle i,j\rangle }\mathbf {S} _{i}\cdot \mathbf {S} _{j}=-J\sum _{\langle i,j\rangle }\cos(\theta _{i}-\theta _{j})$

${\boldsymbol {S}}_{i}=(\cos {\theta _{i}},\sin {\theta _{i}})$

格林函数（传播子）是

$G({\boldsymbol {r}}_{i}-{\boldsymbol {r}}_{j})=\langle {\boldsymbol {S}}_{i}\cdot {\boldsymbol {S}}_{j}\rangle =\langle \cos(\theta _{i}-\theta _{j})\rangle =\langle e^{i(\theta _{i}-\theta _{j})}\rangle$

$G({\boldsymbol {r}}_{i}-{\boldsymbol {r}}_{j})\sim \exp \left(-r\log {\frac {2}{\beta J}}\right)$

$G({\boldsymbol {r}}_{i}-{\boldsymbol {r}}_{j})\sim \left({\frac {1}{r}}\right)^{1/2\pi \beta J}$

动力学[编辑]

単独涡旋的能量[编辑]

$E\sim {\frac {J}{2}}\int {\mathrm {d} }^{2}r(\nabla \theta )^{2}={\frac {J}{2}}\int _{a}^{L}d^{2}r2\pi {\mathrm {d} }r{\frac {1}{r^{2}}}=\pi J\log \left({\frac {L}{a}}\right)$

$S=\log \left({\frac {L}{a}}\right)^{2}$

$F=E-TS=(\pi J-2T)\log \left({\frac {L}{a}}\right)$

$T_{BKT}={\frac {\pi J}{2}}$

一对涡旋的能量[编辑]

$E\sim -\pi J\sum _{i\neq j}n_{i}n_{j}\log \left|{\frac {{\boldsymbol {r}}_{i}-{\boldsymbol {r}}_{j}}{a}}\right|+\pi J\left(\sum _{i}n_{i}\right)^{2}\log \left({\frac {L}{a}}\right)$

$E\sim 2\pi J\log \left|{\frac {{\boldsymbol {r}}_{i}-{\boldsymbol {r}}_{j}}{a}}\right|$

参考资料[编辑]

Березинский, В. Л., Разрушение дальнего порядка в одномерных и двумерных системах с непрерывной группой симметрии I. Классические системы, ЖЭТФ, 1970, 59 (3): 907–920 （俄语） . Translation available: Berezinskii, V. L., Destruction of long-range order in one-dimensional and two-dimensional systems having a continuous symmetry group I. Classical systems (pdf), Sov. Phys. JETP, 1971, 32 (3): 493–500 [2016-10-04], Bibcode:1971JETP...32..493B, （原始内容存档 (PDF)于2019-07-13）
Березинский, В. Л., Разрушение дальнего порядка в одномерных и двумерных системах с непрерывной группой симметрии II. Квантовые системы, ЖЭТФ, 1971, 61 (3): 1144–1156 （俄语） . Translation available: Berezinskii, V. L., Destruction of long-range order in one-dimensional and two-dimensional systems having a continuous symmetry group II. Quantum systems (pdf), Sov. Phys. JETP, 1972, 34 (3): 610–616 [2016-10-04], Bibcode:1972JETP...34..610B, （原始内容存档 (PDF)于2019-07-13）
Kosterlitz, J. M.; Thouless, D. J., Ordering, metastability and phase transitions in two-dimensional systems, Journal of Physics C: Solid State Physics, 1973, 6: 1181–1203, Bibcode:1973JPhC....6.1181K, doi:10.1088/0022-3719/6/7/010
McBryan, O.; Spencer, T., On the decay of correlations in SO(n)-symmetric ferromagnets, Commun. Math. Phys., 1977, 53: 299, Bibcode:1977CMaPh..53..299M, doi:10.1007/BF01609854
B. I. Halperin, D. R. Nelson, Phys. Rev. Lett. 41, 121 (1978)
A. P. Young, Phys. Rev. B 19, 1855 (1979)
Resnick, D.J.; Garland, J.C.; Boyd, J.T.; Shoemaker, S.; Newrock, R.S., Kosterlitz Thouless Transition in Proximity Coupled Superconducting Arrays, Phys. Rev. Lett., 1981, 47: 1542, Bibcode:1981PhRvL..47.1542R, doi:10.1103/PhysRevLett.47.1542
Fröhlich, Jürg; Spencer, Thomas, The Kosterlitz–Thouless transition in two-dimensional abelian spin systems and the Coulomb gas, Comm. Math. Phys., 1981, 81 (4): 527–602, Bibcode:1981CMaPh..81..527F, doi:10.1007/bf01208273
Z. Hadzibabic; et al, Berezinskii–Kosterlitz–Thouless crossover in a trapped atomic gas, Nature, 2006, 41: 1118, Bibcode:2006Natur.441.1118H, arXiv:cond-mat/0605291 , doi:10.1038/nature04851

XY模型[编辑]

动力学[编辑]

単独涡旋的能量[编辑]

一对涡旋的能量[编辑]

参考资料[编辑]

相关书籍[编辑]