Source: Ann. Appl. Probab. Volume 13, Number 2
(2003), 691-721.
Motivated by an exact mapping between anisotropic half integer spin
quantum Heisenberg models and asymmetric diffusions on the lattice, we
consider an anisotropic simple exclusion process with $N$ particles in a
rectangle of $\bbZ^2$. Every particle at row $h$ tries to jump to an
arbitrary empty site at row $h\pm 1$ with rate $q^{+ 1}$, where $q\in
(0,1)$ is a measure of the drift driving the particles toward the
bottom of the rectangle. We prove that the spectral gap
of the generator is uniformly positive in $N$ and in the size of the
rectangle. The proof is inspired by a recent interesting technique
envisioned by E. Carlen, M. C. Carvalho and M. Loss to analyze the Kac
model for the nonlinear Boltzmann equation. We then apply the result
to prove precise upper and lower bounds on the energy gap for the
spin-$S$, $S\in \ov2\bbN$,
$\mbox{\textit{{XXZ}}}$ chain and for the 111 interface
of the spin-$S$ $\mbox{\textit{{XXZ}}}$\vspace{-1pt}
Heisenberg model, thus generalizing previous
results valid only for spin $\ov2$.
References
[1] ALCARAZ, F. C. (1994). Exact steady states of asy mmetric diffusion and two-species annihilation with back reaction from the ground state of quantum spin models. Internat. J. Modern Phy s. B 8 3449-3461.
[2] ALCARAZ, F. C., SALINAS, S. R. and WRESZINSKI, W. F. (1995). Anisotropic ferromagnetic quantum domains. Phy s. Rev. Lett. 75 930-933.
[3] BENJAMINI, I., BERGER, N., HOFFMAN, C. and MOSSEL, E. (2002). Mixing time for biased shuffling card. Preprint.
[4] BOLINA, O., CONTUCCI, P., NACHTERGAELE, B. and STARR, S. (2000). Finite volume excitations of the 111 interface in the quantum XXZ model. Comm. Math. Phy s. 212 63-91.
[5] BRAMSON, M. and GRIFFEATH, D. (1980). Clustering and dispersion rates for some interacting particle sy stems on Z. Ann. Probab. 8.
[6] BRAMSON, M. and LEBOWITZ, J. (2001). Spatial structure in low dimensions for diffusion limited two-particle reactions. Ann. Appl. Probab. 11 121-181.
[7] CAPUTO, P. and MARTINELLI, F. (2002). Asy mmetric diffusion and the energy gap above the 111 ground state of the quantum XXZ model. Comm. Math. Phy s. 226 323-375.
[8] CARLEN, E., CARVALHO, M. C. and LOSS, M. (2001). Many-body aspects of approach to equilibrium. Seminaire: Equations aux derives partielles, 2000-2001. Exp. XIX, Semin. Equ. Deriv. Partielles. Ecole Poly tech., Palaiseau.
[9] DIACONIS, P. and SALOFF-COSTE, L. (1996). Logarithmic Sobolev inequalities for finite Markov chains. Ann. Appl. Probab. 6 695-750.
[10] DIACONIS, P. and SHAHSHAHANI, M. (1987). Time to reach stationarity in the Bernoulli- Laplace diffusion model. SIAM J. Math. Anal. 18 208-218.
[11] KOMA, T. and NACHTERGAELE, B. (1997). The spectral gap of the ferromagnetic XXZ chain. Lett. Math. Phy s. 40 1-16.
[12] KOMA, T., NACHTERGAELE, B. and STARR, S. (2001). The spectral gap for the ferromagnetic spin-J XXZ chain. Preprint. Available at front.math.ucdavis.edu/math-ph/0110017.
[13] LU, S. T. and YAU, H.-T. (1993). Spectral gap and logarithmic Sobolev inequality for Kawasaki and Glauber dy namics. Comm. Math. Phy s. 156 399-433.
[14] NACHTERGAELE, B. (2000). Interfaces and droplets in quantum lattice models. Preprint. Available at arxiv.org/abs/math-ph/0009027.
[15] STARR, S. (2001). Some properties of the low lying spectrum of the ferromagnetic, quantum XXZ Heisenberg model. Ph.D. dissertation, Univ. California, Davis. Available at front.math.ucdavis.edu/math-ph/0106024.