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Exact spectral gaps of the asymmetric exclusion process with open boundaries

FREE ARTICLE Topical articles on The 75th Anniversary of the Bethe Ansatz

Jan de Gier1 and Fabian H L Essler2

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Part of Topical articles on The 75th Anniversary of the Bethe Ansatz

We derive the Bethe ansatz equations describing the complete spectrum of the transition matrix of the partially asymmetric exclusion process with the most general open boundary conditions. By analysing these equations in detail for the cases of totally asymmetric and symmetric diffusion, we calculate the finite-size scaling of the spectral gap, which characterizes the approach to stationarity at large times. In the totally asymmetric case we observe boundary induced crossovers between massive, diffusive and KPZ (Kardar–Parisi–Zhang) scaling regimes. We further study higher excitations, and demonstrate the absence of oscillatory behaviour at large times on the 'coexistence line', which separates the massive low and high density phases. In the maximum current phase, oscillations are present on the KPZ scale t\propto
L^{-3/2} . While independent of the boundary parameters, the spectral gap as well as the oscillation frequency in the maximum current phase have different values compared to the totally asymmetric exclusion process with periodic boundary conditions. We discuss a possible interpretation of our results in terms of an effective domain wall theory.


Keywords

exact results

driven diffusive systems (theory)

integrable spin chains (vertex models)

quantum integrability (Bethe ansatz)

PACS

75.10.Jm Quantized spin models

75.10.Pq Spin chain models

MSC

82Cxx Time-dependent statistical mechanics (dynamic and nonequilibrium)

Subjects

Condensed matter: electrical, magnetic and optical

Dates

Issue 12 (December 2006)

Received 25 September 2006, accepted for publication 18 November 2006

Published 14 December 2006



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