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Critical behaviour at the transition by breaking of analyticity in the discrete Frenkel-Kontorova model

M Peyrard et al 1983 J. Phys. C: Solid State Phys. 16 1593-1608   doi: 10.1088/0022-3719/16/9/005  Help

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M Peyrard and S Aubry
Los Alamos Nat. Lab., Center for Nonlinear Studies, Los Alamos, NM, USA

Abstract. The authors study numerically the transition by breaking of analyticity which occurs in the incommensurate ground state of the Frenkel-Kontorova model (1938) when the amplitude lambda of its periodic-potential V(u) is increased beyond a critical value lambda c. A brief review of the properties of this transition and its connection with the standard map is given. They consider four quantities which are critical when lambda goes to lambda c from upper values: the gap in the phonon spectrum, the coherence length of the ground state, the Peierls-Nabarro barrier and the depinning force. The numerical method is discussed and the authors show in particular that the mapping method is unpracticable for lambda > lambda c. They observe the transition by breaking of analyticity and show that in the stochastic region ( lambda > lambda c) the ground state is never chaotic. Nevertheless in this region metastable chaotic states can be obtained. The numerical calculations, performed with a ratio of the atomic mean distance to the period of the potential V(u), l/2a=(3- square root 5)/2 equivalent to the golden mean, show that critical exponents can be defined for the four critical quantities studied. Their values reveal two scaling laws which are empirically explained.

Print publication: Issue 9 (30 March 1983)

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