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Density-matrix renormalization group study of the spin-Peierls instability in the antiferromagnetic Heisenberg ladder

机译:反铁磁海森堡阶梯中自旋Peierls不稳定性的密度矩阵重整化组研究

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摘要

The columnar dimerized antiferromagnetic S = 1/2 spin ladder is numerically studied by the density-matrix renormalization-group (DMRG) method. The elastic lattice with spin-phonon coupling α and lattice elastic force k is introduced into the system. Thus the S = 1/2 Heisenberg spin chain is unstable towards dimerization (the spin-Peierls transition). However, the dimerization should be suppressed if the rung coupling J⊥ is sufficiently large, and a Columnar dimer to Rung singlet phase transition takes place. After a self-consistent calculation of the dimerization, we determine the quantum phase diagram by numerically computing the singlet-triplet gap, the dimerization amplitude, the order parameters, the rung spin correlation and quantum entropies. Our results show that the phase boundary between the Columnar dimer phase and Rung singlet phase is approximately of the form J⊥t ~ (k/α~2)?5/4.
机译:柱状二聚反铁磁S = 1/2自旋阶梯通过密度矩阵重归一化群(DMRG)方法进行了数值研究。将具有自旋声子耦合α和晶格弹力k的弹性晶格引入系统。因此,S = 1/2海森堡自旋链对二聚化(自旋-Peierls跃迁)不稳定。但是,如果梯级偶合J 1足够大,则应抑制二聚化,并且发生柱状二聚体至Rung单线态的相变。经过二元化的自洽计算,我们通过数值计算单重态-三重态间隙,二聚化幅度,阶数参数,梯级自旋相关性和量子熵来确定量子相图。结果表明,柱状二聚体相与and单峰相的相界近似为J⊥t〜(k /α〜2)?5/4。

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