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arXiv 1803.04530cond-mat.stat-mechcond-mat.str-el
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混合自旋Ising-Heisenberg双层阻挫阶梯的相变和磁化强度

Phase transitions and magnetization of the mixed-spin Ising-Heisenberg double sawtooth frustrated ladder

Hamid Arian Zad, Nerses Ananikian

摘要:

用转移矩阵方法近似求解了含有自旋1和自旋1/2节原子混合物和自旋1/2间隙二聚体的混合自旋(1,1/2)Ising-Heisenberg双阶梯.在这里,我们详细研究了基态相图,以及双线性交换耦合的梯级和循环的四自旋交换相互作用在每个块的正方形元格中的磁化强度和磁化率在低温下的建议阶梯的影响。这样的双梯形可以在Shastry-Sutherland格型中找到。尽管奇块和偶块的自旋序是不同的,但由于不同块之间的对易关系,模型的相图、磁化行为和热力学性质对于奇块和偶块是相同的。我们表明,在低温下,这两个交换耦合可以改变磁化平台的质量和数量与磁场的变化。特别地,我们发现了一个新的磁化平台M/Ms = 5/6。此外,我们还详细地研究了该模型的磁化率和比热。证明了在低温下磁化强度和磁化率的行为是一致的。比热随温度的变化呈现多样性,在特定的温度区间内有一个肖特基峰。我们观察到,随着梯级上的双线性交换耦合的增加,第二峰值温度依赖性增长。

英文摘要:

The mixed spin-(1,1/2) Ising-Heisenberg double sawtooth ladder containing mixture of both spin-1 and spin-1/2 nodal atoms, and the spin-1/2 interstitial dimers is approximately solved by the transfer-matrix method. Here, we study in detail the ground-state phase diagrams, also influences of the bilinear exchange coupling on the rungs and cyclic four-spin exchange interaction in square plaquette of each block on the magnetization and magnetic susceptibility of the suggested ladder at low temperature. Such a double sawtooth ladder may be found in a Shastry-Sutherland Lattice-type. In spite of odd and even blocks spin ordering are different from each other, but due to the commutation relation between all different block Hamiltonians, phase diagrams, magnetization behavior and thermodynamic properties of the model are the same for odd and even blocks. We show that at low temperature, both exchange couplings can change the quality and quantity of the magnetization plateaus versus the magnetic field changes. Specially, we find a new magnetization plateau M/Ms = 5/6 for this model. Besides, we examine the magnetic susceptibility and specific heat of the model in detail. It is proven that behaviors of the magnetization and the magnetic susceptibility coincide at low temperature. The specific heat displays diverse temperature dependencies, which include a Schottky-type peak at a special temperature interval. We observe that with increase of the bilinear exchange coupling on the rungs, second peak temperature dependence grows.

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