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Efficient density matrix renormalization group algorithm to study Y junctions with integer and half-integer spin

机译:高效的矩阵重归一化群算法研究整数和半整数自旋的Y结

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摘要

An efficient density matrix renormalization group (DMRG) algorithm is presented and applied to Y junctions, systems with three arms of n sites that meet at a central site. The accuracy is comparable to DMRG of chains. As in chains, new sites are always bonded to the most recently added sites and the superblock Hamiltonian contains only new or once renormalized operators. Junctions of up to N = 3n + 1 approximate to 500 sites are studied with antiferromagnetic (AF) Heisenberg exchange J between nearest-neighbor spins S or electron transfer t between nearest neighbors in half-filled Hubbard models. Exchange or electron transfer is exclusively between sites in two sublattices with N-A not equal N-B. The ground state (GS) and spin densities rho(r) = < S-r(z)> at site r are quite different for junctions with S = 1/2, 1, 3/2, and 2. The GS has finite total spin S-G = 2S(S) for even (odd) N and for M-G = S-G in the S-G spin manifold, rho(r) > 0(< 0) at sites of the larger (smaller) sublattice. S = 1/2 junctions have delocalized states and decreasing spin densities with increasing N. S = 1 junctions have four localized S-z = 1/2 states at the end of each arm and centered on the junction, consistent with localized states in S = 1 chains with finite Haldane gap. The GS of S = 3/2 or 2 junctions of up to 500 spins is a spin density wave with increased amplitude at the ends of arms or near the junction. Quantum fluctuations completely suppress AF order in S = 1/2 or 1 junctions, as well as in half-filled Hubbard junctions, but reduce rather than suppress AF order in S = 3/2 or 2 junctions.
机译:提出了一种有效的密度矩阵重归一化组(DMRG)算法,并将其应用于Y结,即具有在中心站点相遇的n个站点的三个分支的系统。精度可与链条的DMRG相媲美。与链式一样,新站点始终与最新添加的站点绑定,并且超级块哈密顿量仅包含新的或重新规范化的运算符。在半填充Hubbard模型中,使用近铁自旋S之间的反铁磁(AF)Heisenberg交换J或最近邻之间的电子转移t进行了反铁磁(AF)Heisenberg交换J的研究,研究了大约500个站点的N = 3n +1个结。交换或电子转移仅在N-A不等于N-B的两个子晶格中的位点之间进行。对于S = 1 / 2、1、3 / 2和2的结,基点(GS)和自旋密​​度rho(r)= 完全不同。在SG自旋歧管中,对于偶数(奇数)N SG = 2S(S),对于MG = SG,在较大(较小)子晶格的位置rho(r)> 0(<0)。 S = 1/2结具有离域状态,并且随着N的增加,自旋密度降低。S = 1结在每个臂的末端具有四个局部Sz = 1/2状态,并以结为中心,与S = 1中的局部状态一致Haldane间隙有限的链。 S = 3/2或2个结点的GS最多可旋转500次,这是一个自旋密度波,在臂的末端或结点附近振幅增加。量子涨落完全抑制了S = 1/2或1结以及半填充Hubbard结中的AF阶,但减小而不是抑制了S = 3/2或2结中的AF阶。

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