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Condensed Matter > Statistical Mechanics

Title: The complete set of ground states of the ferromagnetic XXZ chains

Abstract: We show that the well-known translation invariant ground states and the recently discovered kink and antikink ground states are the complete set of pure infinite-volume ground states (in the sense of local stability) of the spin-S ferromagnetic XXZ chains with Hamiltonian H=-sum_x [ S^1_x S^1_{x+1} + S^2_x S^2_{x+1} + Delta S^3_x S^3_{x+1} ], for all Delta >1, and all S=1/2,1,3/2,.... For the isotropic model (Delta =1) we show that all ground states are translation invariant.
For the proof of these statements we propose a strategy for demonstrating completeness of the list of the pure infinite-volume ground states of a quantum many-body system, of which the present results for the XXX and XXZ chains can be seen as an example. The result for Delta>1 can also be proved by an easy extension to general $S$ of the method used in [T. Matsui, Lett. Math. Phys. 37 (1996) 397] for the spin-1/2 ferromagnetic XXZ chain with $\Delta>1$. However, our proof is different and does not rely on the existence of a spectral gap. In particular, it also works to prove absence of non-translationally invariant ground states for the isotropic chains (Delta=1), which have a gapless excitation spectrum.
Our results show that, while any small amount of the anisotropy is enough to stabilize the domain walls against the quantum fluctuations, no boundary condition exists that would stabilize a domain wall in the isotropic model (Delta=1).
Comments: 23 pages (LaTeX), typos corrected, references updated
Subjects: Statistical Mechanics (cond-mat.stat-mech); Mathematical Physics (math-ph)
Journal reference: Adv.Theor.Math.Phys.2:533-558,1998
Report number: KN-09-97
Cite as: arXiv:cond-mat/9709208 [cond-mat.stat-mech]
  (or arXiv:cond-mat/9709208v2 [cond-mat.stat-mech] for this version)

Submission history

From: Bruno Nachtergaele [view email]
[v1] Thu, 18 Sep 1997 19:12:59 GMT (20kb)
[v2] Mon, 13 Apr 1998 20:09:37 GMT (20kb)