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arXiv:0905.2157 · Condensed Matter Physics

Field-controlled spin current in frustrated spin chains

Alexei K. Kolezhuk, Ian P. McCulloch

Published Jan 1, 2009• 6 citations
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Abstract

We study states with spontaneous spin current, emerging in frustrated antiferromagnetic spin-S chains subject to a strong external magnetic field.As a numerical tool, we use a non-Abelian symmetry realization of the density matrix renormalization group.The field dependence of the order parameter and the critical exponents are presented for zigzag chains with S = 1/2, 1, 3/2, and 2.

DOI
10.5488/cmp.12.3.429

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A modified density matrix renormalization group (DMRG) algorithm is applied to the zigzag spin-12\frac{1}{2}21​ chain with frustrated antiferromagnetic exchange J1{J}_{1}J1​ and J2{J}_{2}J2​ between first and second neighbors. The modified algorithm yields accurate results up to ${J}_{2}/{J}_{1}\ensuremath{\approx}4$ for the magnetic gap $\ensuremath{\Delta}$ to the lowest triplet state, the amplitude BBB of the bond order wave phase, the wavelength $\ensuremath{\lambda}$ of the spiral phase, and the spin correlation length $\ensuremath{\xi}$. The J2/J1{J}_{2}/{J}_{1}J2​/J1​ dependences of $\ensuremath{\Delta}$, BBB, $\ensuremath{\lambda}$, and $\ensuremath{\xi}$ provide multiple comparisons to field theories of the zigzag chain. The twist angle of the spiral phase and the spin structure factor yield additional comparisons between DMRG and field theory. Attention is given to the numerical accuracy required to obtain exponentially small gaps or exponentially long correlations near a quantum phase transition.
We study thermodynamic behaviors of the antiferromagnetic zigzag spin chain in magnetic fields, using the density-matrix renormalization-group method for the quantum transfer matrix. We focus on the thermodynamics of the system near the critical fields in the ground-state magnetization process $(M\ensuremath{-}H$ curve): the saturation field, the lower critical field associated with excitation gap, and the field at the middle-field cusp singularity. We calculate magnetization, susceptibility, and specific heat of the zigzag chain in magnetic fields at finite temperatures, and then discuss how the calculated quantities reflect the low-lying excitations of the system related with the critical behaviors in the $M\ensuremath{-}H$ curve.