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本文在具有Dzyaloshinsky-Moriya(DM)相互作用的一维XY自旋链中,以双自旋比特系统为研究对象,基于Jensen-Shannon熵,研究了量子相干分布(局域相干和集体相干)及其相变临界行为。研究发现,通过改变自旋-自旋耦合作用和DM相互作用,可以有效调控局域相干与集体相干之间的相互转化。此外,局域相干和集体相干能够通过局部极值或发散的临界行为准确地表征自旋链的一阶和二阶量子相变。当一阶量子相变的探测受到自旋-自旋耦合作用和DM相互作用的干扰时,集体相干比局域相干具有更加稳定的识别效果。最后,长距离自旋对的总体相干和集体相干在表征二阶量子相变上都具有显著优势。 相似文献
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基于矩阵乘积态表述的无限时间演化块算法,研究了具有x,y,z三个自旋方向的轨道自由度和轨道序竞争的量子罗盘自旋链模型.为了刻画该模型的量子相和相变,计算了基态能量、局域序参量、弦关联序参量、临界指数、冯诺依曼熵、有限纠缠标度和中心荷.结果表明:该量子基态相图由条纹反铁磁相、反铁磁相、单调奇数Haldane相和振荡奇数Haldane相构成.从条纹反铁磁相到反铁磁相,以及从单调奇数Haldane相到振荡奇数Haldane相发生了非连续相变;从振荡奇数Haldane相到条纹反铁磁相,以及从反铁磁相到单调奇数Haldane相发生了连续相变;连续相变线和非连续相变线的交点是多临界点.此外,连续相变点处的临界指数β=1/8和中心荷c=1/2表明连续相变的普适类属于Ising类.由此揭示了该模型量子基态相图的本性,对今后研究更高自旋以及更为复杂轨道序竞争的量子罗盘链模型的量子相与相变具有一定借鉴与参考意义. 相似文献
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对于无限大尺寸两腿自旋1/2的XXZ自旋梯子模型,通过运用基于随机行走的张量网络(TN)算法数值模拟出基态波函数,首次尝试研究自旋梯子模型的约化保真度、普适序参量、纠缠熵等物理观测量,并系统研究基态保真度的三维挤点与二维分叉、约化保真度的分叉、局域序参量、普适序参量、纠缠熵和量子相变之间存在的关联关系.基于张量网络表示的算法在任意随机选择初始状态时,可以得到两腿XXZ量子自旋梯子系统简并的对称破缺基态波函数,该基态波函数是由于Z2对称破缺引起的.本文期望所提供的方法可为进一步研究凝聚态物质中热力学极限下的强关联电子量子晶格自旋梯子系统的量子相变和量子临界现象提供一种更有效的强大的工具. 相似文献
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利用基于张量网络表示的矩阵乘积态算法以及无限虚时间演化块抽取方法,本文研究了一维无限格点自旋1的键交替反铁磁XXZ海森伯模型中的量子相变.分别计算了系统的von Neumann熵、单位格点保真度和序参量,从而得到了系统随键交替强度的变化从拓扑有序Néel相到局域有序二聚化相的量子相变点.我们用矩阵乘积态方法拟合出了相变的中心荷c?0.5,表明此相变属于二维经典的Ising普适类.另外,通过对拓扑Néel序的数值拟合,我们得到了相变点处的特征临界指数β′=0.236和γ′=0.838. 相似文献
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电子的量子自旋霍尔效应的发现推进了当今凝聚态物理学的发展,它是一种电子自旋依赖的具有量子行为的输运效应.近年来,大量的理论和实验研究表明,描述电磁波场运动规律的麦克斯韦方程组内禀了光的量子自旋霍尔效应,存在于界面的倏逝波表现出强烈的自旋与动量关联性.得益于新兴的光学材料:超构材料(metamaterials)的发展,不仅能够任意设定光学参数,同时也能引入很多复杂的自旋-轨道耦合机理,让我们能够更加清晰地了解和验证其中的物理机理.本文对超构材料中量子自旋霍尔效应做了简要的介绍,内容主要包括真空中光的量子自旋霍尔效应的物理本质、电单负和磁单负超构材料能带反转导致的不同拓扑相的界面态、拓扑电路系统中光量子自旋霍尔效应等. 相似文献
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绿宝石晶体自旋二重态对基态能级的影响及Jahn-Teller效应 总被引:5,自引:2,他引:5
应用不可约张量方法和群的理论构造了三角对称晶场中考虑自旋 轨道相互作用,自旋 自旋相互作用和自旋 其它轨道相互作用的3d3/3d7态离子的可完全对角化的120阶微扰哈密顿矩阵.利用该矩阵计算了绿宝石晶体的基态能级、零场分裂参量,研究了自旋二重态对基态能级的贡献.理论计算值与实验值相符合,证明二重态对基态的贡献是不可忽略的.在此基础上,进一步研究了自旋 自旋相互作用、自旋 其它轨道相互作用和自旋 轨道相互作用对绿宝石晶体的光谱精细结构和零场分裂参量的影响,发现自旋 自旋和自旋 其它轨道相互作用对绿宝石晶体基态能级和零场分裂参量的影响都是不可忽略的.从而通过理论计算值和实验值的比较,证实了在绿宝石晶体中Jahn Teller效应的存在,它能够对光谱精细结构的分裂提出一些更加合理的解释. 相似文献
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Ground-State Phase Diagram of Transverse Spin-2 Ising Model with Longitudinal Crystal-Field 总被引:2,自引:0,他引:2
The transverse spin-2 Ising ferromagnetic model with a longitudinal crystal-field is studied within the mean-field theory based on Bogoliubov inequality for the Gibbs free energy. The ground-state phase diagram and the tricritical point are obtained in the transverse field Ω/z J-longitudinal crystal D/zJ field plane. We find that there are the first order-order phase transitions in a very smallrange of D/zJ besides the usual first order-disorder phase transitions and the second order-disorder phase transitions. 相似文献
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The transverse spin-2 Ising ferromagnetic model with a longitudinal crystal field is studied within the mean-field theory. The phase diagrams and magnetization curves are obtained by diagonalizing the Hamiltonian Hi of the Ising system numerically, and the first order-order phase transitions, the first order-disorder phase transitions, and the second-order phase transitions are discussed in details. Reentrant phenomenaoccur when the value of the transverse field is not zero and the reentrantdiagram is given. 相似文献
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The transverse spin-2 Ising ferromagnetic model with a longitudinal crystal field is studied within the mean-field theory. The phase diagrams and magnetization curves are obtained by diagonalizing the Hamiltonian Hi of the Ising system numerically, and the first order-order phase transitions, the first order-disorder phase transitions, and the second-order phase transitions are discussed in details. Reentrant phenomena occur when the value of the transverse field is not zero and the reentrant diagram is given. 相似文献
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A sequence space model which describes the interplay of mutation and selection in molecular evolution is shown to be equivalent to an Ising quantum chain. Observable quantities tailored to match the biological situation are then employed to treat three fitness landscapes exactly. 相似文献
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Thermodynamic properties and phase diagrams of a mixed spin-(1,2) Ising ferrimagnetic system with single ion anisotropy on hexagonal nanowire are studied by using effective-field theory with correlations. The susceptibility, internal energy and specific heat of the system are numerically examined and some interesting phenomena in these quantities are found. The effect of the Hamiltonian parameters on phase diagrams are examined in detail. Besides second-order phase transition, lines of first-order transition and tricritical points are found. In particular, we found that for some negative values of single-ion anisotropies, there exist first-order phase transitions. 相似文献
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LIU Wei-Jie XIN Zi-Hua HU Hong-Liang 《理论物理通讯》2007,47(5):955-960
Using the effective-field theory we studied the magnetic properties of a spin-1/2 Ising supedattice, which consist of three different ferromagnet materials. The magnetic behavior of this superlattice is examined. The critical temperature and the compensation temprature of the system are studied as a function of the exchange interactions between the nearest-neiboring spins across the interface and in the intraface. Temperature dependence of magenetizations is also given. 相似文献
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A transverse Ising spin system, in the presence of time-dependentlongitudinal field, is studied by the effective-field theory (EFT). Theeffective-field equations of motion of the average magnetization are givenfor the simple cubic lattice (Z = 6) and the honeycomb lattice (Z = 3).The Liapunov exponent λ is calculated for discussing the stability of the magnetization and it is used to determine the phase boundary. Thedynamic phase transition diagrams in h0/ ZJ -Γ/ZJ plane and in h0/ZJ-T/ZJ plane have been drawn, and there is no dynamical tricritical point on the dynamic phase transition boundary. The effect of the thermal fluctuations upon the dynamic phase boundary has been discussed. 相似文献
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The spin-3/2 Ising model is investigated for the case of
antiferromagnetic (AFM/AFM) interactions on the two-layer Bethe
lattice by using the exact recursion relations in the pairwise
approach for given coordination numbers q=3, 4 and 6 when the
layers are under the influences of equal external magnetic and equal
crystal fields. The ground state (GS) phase diagrams are obtained on
the different planes in detail and then the temperature-dependent
phase diagrams of the system are calculated accordingly. It is
observed that the system presents both second- and first-order phase
transitions for all q, therefore, tricritical points. It is also
found that the system exhibits double-critical end points and
isolated points. The model also presents two Néel temperatures,
TN, and the existence of which leads to the reentrant
behaviour. 相似文献
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We study the role of Franck-Condon (F-C) principle in the dynamics of a central spin system, which is coupled to an Ising chain in transverse field. The transition process of energy levels caused by the excited central spin is studied to manifest the quantum critical effect through the Franck-Condon principle. The super-sensitivity of this quantum critical system is demonstrated clearly from the properties of Franck-Condon factors. We analytically show how spin numbers, coupling strength and order parameter of the Ising chain sensitively effect on the energy level populations in dynamical evolution near the critical point. This super-sensitivity and criticality are explicitly displayed in absorption spectrum. 相似文献
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The ground states of the ultracold spin-1 atoms trapped in a deep one-dimensional double-well optical superlattice in a weak magnetic field are obtained. It is shown that the ground-state diagrams of the reduced double- well model are remarkably different for the antiferromagnetic and ferromagnetic condensates. The transition between the singlet state and nematic state is observed for the antiferromagnetic interaction atoms, which can be realized by modulating the tunneling parameter or the quadratic Zeeman energy. An experiment to distinguish the different spin states is suggested. 相似文献