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Entropy

The Effect of a Long-Range Correlated-Hopping Interaction on Bariev Spin Chains

Tao Yang, Fa-Kai Wen, Kun Hao, Like Cao, Rui‐Hong Yue

Published Aug 28, 2015• 2 citations
Publisher

Abstract

We introduce a long-range particle and spin interaction into the standard Bariev model and show that this interaction is equivalent to a phase shift in the kinetic term of the Hamiltonian. When the particles circle around the chain and across the boundary, the accumulated phase shift acts as a twist boundary condition with respect to the normal periodic boundary condition. This boundary phase term depends on the total number of particles in the system and also the number of particles in different spin states, which relates to the spin fluctuations in the system. The model is solved exactly via a unitary transformation by the coordinate Bethe ansatz. We calculate the Bethe equations and work out the energy spectrum with varying number of particles and spins.

DOI
10.3390/e17096044

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We introduce a long-range particle and spin interaction into the standard Bariev model and show that this interaction is equivalent to a phase shift in the kinetic term of the Hamiltonian. When the particles circle around the chain and across the boundary, the accumulated phase shift acts as a twist boundary condition with respect to the normal periodic boundary condition. This boundary phase term depends on the total number of particles in the system and also the number of particles in different spin states, which relates to the spin fluctuations in the system. The model is solved exactly via a unitary transformation by the coordinate Bethe ansatz. We calculate the Bethe equations and work out the energy spectrum with varying number of particles and spins.
School of Physical Science and Technology, Yangzhou University, Yangzhou 225002, China* Authors to whom correspondence should be addressed; E-Mails: yangt@nwu.edu.cn (T.Y.);rhyue@yzu.edu.cn (R.Y.); Tel.: +86-29-88303513; Fax: +86-29-88302331.Academic Editors: Ignazio Licata and Sauro SucciReceived: 16 May 2015 / Accepted: 25 August 2015 / Published: 28 August 2015Abstract: We introduce a long-range particle and spin interaction into the standard Barievmodel and show that this interaction is equivalent to a phase shift in the kinetic term ofthe Hamiltonian. When the particles circle around the chain and across the boundary,the accumulated phase shift acts as a twist boundary condition with respect to the normalperiodic boundary condition. This boundary phase term depends on the total number ofparticles in the system and also the number of particles in different spin states, whichrelates to the spin fluctuations in the system. The model is solved exactly via a unitarytransformation by the coordinate Bethe ansatz. We calculate the Bethe equations and workout the energy spectrum with varying number of particles and spins.Keywords: Bariev model; long-range interaction; twist boundary condition; energyspectrum1. IntroductionOne dimensional (1D) (quasi-1D) systems exhibit some of the most diverse and intriguing physicalphenomena seen in all of condensed matter physics, such as charge (spin) density waves, quantumwires, quantum Hall bars, Josephson junction arrays, polymers and 1D Bose-Einstein condensates. Thecomplete description of a solid is a complex many body problem. The particles are strongly correlatedand cannot be understood by removing the interactions between them or by considering the effects of