1990
DOI: 10.1103/physrevb.41.4570
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Effect of lattice discreteness on the statistical mechanics of a dilute gas of kinks

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Cited by 29 publications
(11 citation statements)
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“…Thus a Klein-Gordon kink when boosted can only radiate some energy away and finally stop to become a static kink solution! In order to account for these effects a collective coordinate approach was developed [195], [165], [28], [194], [29], [193], [57], [30]. Within this approach one performs a canonical transformation to new coordinates some of whom are collective (nonlocal in the old coordinates).…”
Section: Movabilitymentioning
confidence: 99%
“…Thus a Klein-Gordon kink when boosted can only radiate some energy away and finally stop to become a static kink solution! In order to account for these effects a collective coordinate approach was developed [195], [165], [28], [194], [29], [193], [57], [30]. Within this approach one performs a canonical transformation to new coordinates some of whom are collective (nonlocal in the old coordinates).…”
Section: Movabilitymentioning
confidence: 99%
“…From fundamental physical interest, the idea of a discrete nature has considerably improved our understanding of the effect of discreteness on topological solitons [4][5][6][7][8] and nontopological solitons [9], classical thermodynamic properties [10][11][12][13], modulational instabilities [14][15][16], wave-collapse phenomena [17,18], intrinsic localized vibrational states [19][20][21], diffusion in discrete nonlinear dynamical systems [22], self-induced gap solitons [23,24].…”
Section: Introductionmentioning
confidence: 99%
“…The rank of the gyrocoupling matrix G is used to classify the excitations: In the case of vanishing G the excitations have an effective mass and exhibit Newtonian dynamics; in the case of regular G, the excitations behave like charged, massless particles in an external magnetic field, similar to the gyrotropic excitations defined in section 2.3. The above theory is a generalization of earlier work of Tomboulis [42], Boesch et al [43], and Willis et al [44], which applies only to "standard" Hamiltonians (i. e., consisting of the sum of kinetic and potential energy terms). This generalization is necessary, e. g., in the case of magnetic systems which cannot be modelled by standard Hamiltonians.…”
Section: An Alternative Approach: Coupling To Magnonsmentioning
confidence: 85%