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| 001 | 904537 | ||
| 005 | 20240610120914.0 | ||
| 024 | 7 | _ | |a 10.1007/s10955-021-02709-1 |2 doi |
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| 037 | _ | _ | |a FZJ-2021-06107 |
| 082 | _ | _ | |a 530 |
| 100 | 1 | _ | |a Schmidt, J |0 P:(DE-HGF)0 |b 0 |e Corresponding author |
| 245 | _ | _ | |a A lattice Gas Model for Generic One-Dimensional Hamiltonian Systems |
| 260 | _ | _ | |a New York, NY [u.a.] |c 2021 |b Springer Science + Business Media B.V. |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 336 | 7 | _ | |a JOURNAL_ARTICLE |2 ORCID |
| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 520 | _ | _ | |a We present a three-lane exclusion process that exhibits the same universal fluctuation pattern as generic one-dimensional Hamiltonian dynamics with short-range interactions, viz., with two sound modes in the Kardar-Parisi-Zhang (KPZ) universality class (with dynamical exponent z=3/2 and symmetric Prähofer-Spohn scaling function) and a superdiffusive heat mode with dynamical exponent z=5/3 and symmetric Lévy scaling function. The lattice gas model is amenable to efficient numerical simulation. Our main findings, obtained from dynamical Monte-Carlo simulation, are: (i) The frequently observed numerical asymmetry of the sound modes is a finite time effect. (ii) The mode-coupling calculation of the scale factor for the 5/3-Lévy-mode gives at least the right order of magnitude. (iii) There are significant diffusive corrections which are non-universal. |
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| 700 | 1 | _ | |a Schütz, G. M. |0 P:(DE-Juel1)130966 |b 1 |
| 700 | 1 | _ | |a van Beijeren, H. |0 P:(DE-HGF)0 |b 2 |
| 773 | _ | _ | |a 10.1007/s10955-021-02709-1 |g Vol. 183, no. 1, p. 8 |0 PERI:(DE-600)2017302-7 |n 1 |p 8 |t Journal of statistical physics |v 183 |y 2021 |x 0022-4715 |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/904537/files/Schmidt2021_Article_ALatticeGasModelForGenericOne-.pdf |y OpenAccess |
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