Please use this identifier to cite or link to this item: https://hdl.handle.net/10356/79925
Title: Néel to spin-Peierls transition in a quasi-one-dimensional Heisenberg model coupled to bond phonons
Authors: Pillay, Jason Cornelius
Wierschem, Keola
Sengupta, Pinaki
Keywords: DRNTU::Science::Physics
Issue Date: 2013
Source: Pillay, J. C., Wierschem, K., & Sengupta, P. (2013). Néel to spin-Peierls transition in a quasi-one-dimensional Heisenberg model coupled to bond phonons. Physical review B - condensed matter and materials physics, 88(5), 054416-.
Series/Report no.: Physical review B - condensed matter and materials physics
Abstract: The zero and finite temperature spin-Peierls transitions in a quasi-one-dimensional spin- 1/ 2 Heisenberg model coupled to adiabatic bond phonons is investigated using the stochastic series expansion (SSE) quantum Monte Carlo (QMC) method. The quantum phase transition from a gapless Neel state to a spin-gapped Peierls state is studied in the parameter space spanned by spatial anisotropy, interchain coupling strength, and spin-lattice coupling strength. It is found that for any finite interchain coupling, the transition to a dimerized Peierls ground state only occurs when the spin-lattice coupling exceeds a finite, nonzero critical value. This is in contrast to the pure 1D model (zero interchain coupling), where adiabatic/classical phonons lead to a dimerized ground state for any nonzero spin-phonon interaction. The phase diagram in the parameter space shows that for a strong interchain coupling, the relation between the interchain coupling and the critical value of the spin-phonon interaction is linear whereas for weak interchain coupling, this behavior is found to have a natural logarithmlike relation. No region was found to have a long range magnetic order and dimerization occurring simultaneously. Instead, the Neel state order vanishes simultaneously with the setting in of the spin-Peierls state. For the thermal phase transition, a continuous heat capacity with a peak at the critical temperature Tc shows a second order phase transition. The variation of the equilibrium bond length distortion δeq with temperature showed a power law relation which decayed to zero as the temperature was increased to Tc, indicating a continuous transition from the dimerized phase to a paramagnetic phase with uniform bond length and zero antiferromagnetic susceptibility.
URI: https://hdl.handle.net/10356/79925
http://hdl.handle.net/10220/18712
DOI: 10.1103/PhysRevB.88.054416
Schools: School of Physical and Mathematical Sciences 
Rights: © 2013 American Physical Society. This paper was published in Physical Review B - Condensed Matter and Materials Physics and is made available as an electronic reprint (preprint) with permission of American Physical Society. The paper can be found at the following official DOI: [http://dx.doi.org/10.1103/PhysRevB.88.054416]. One print or electronic copy may be made for personal use only. Systematic or multiple reproduction, distribution to multiple locations via electronic or other means, duplication of any material in this paper for a fee or for commercial purposes, or modification of the content of the paper is prohibited and is subject to penalties under law.
Fulltext Permission: open
Fulltext Availability: With Fulltext
Appears in Collections:SPMS Journal Articles

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