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Understanding the FPU state in FPU-like models

  • Received: 05 March 2020 Accepted: 24 May 2020 Published: 23 July 2020
  • Many papers investigated, in a variety of ways, the so-called "FPU state" in the Fermi-Pasta-Ulam model, namely the state, intermediate between the initial state and equipartition, that the system soon reaches if initially one or a few long-wavelength normal modes are excited. The FPU state has been observed, in particular, to obey a few characterizing scalings laws. The aim of this paper is twofold: First, reviewing and commenting the literature on the FPU state, suggesting a possible way to organize it. Second, contributing to a better understanding of the FPU state by studying the similar state in the Toda model, which provides, as is known, the closest integrable approximation to FPU. As a new tool, we analyze the dimensionality of Toda invariant tori in states corresponding to the FPU state, and observe it obeys the main scaling law characterizing the FPU state.

    Citation: Giancarlo Benettin, Antonio Ponno. Understanding the FPU state in FPU-like models[J]. Mathematics in Engineering, 2021, 3(3): 1-22. doi: 10.3934/mine.2021025

    Related Papers:

  • Many papers investigated, in a variety of ways, the so-called "FPU state" in the Fermi-Pasta-Ulam model, namely the state, intermediate between the initial state and equipartition, that the system soon reaches if initially one or a few long-wavelength normal modes are excited. The FPU state has been observed, in particular, to obey a few characterizing scalings laws. The aim of this paper is twofold: First, reviewing and commenting the literature on the FPU state, suggesting a possible way to organize it. Second, contributing to a better understanding of the FPU state by studying the similar state in the Toda model, which provides, as is known, the closest integrable approximation to FPU. As a new tool, we analyze the dimensionality of Toda invariant tori in states corresponding to the FPU state, and observe it obeys the main scaling law characterizing the FPU state.


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    [1] Fermi E, Pasta J, Ulam S (1955) Studies of Non Linear Problems, Los-Alamos Internal Report, Document LA-1940.
    [2] Lazarus RB, Voorhees EA, Wells MB, et al. (1978) Computing at LASL in the 1949s and 1950s, Los Alamos internal note LA-6943-H, part Ⅲ.
    [3] Tuck JL, Menzell MT (1972) The superperiod of the nonlinear weighted string (FPU) problem. Adv Math 9: 399-407.
    [4] Campbell DK, Rosenau P, Zaslavsky GM (2005) Introduction: The "Fermi-Pasta-Ulam" problem-the first 50 years. Chaos 15: 015101.
    [5] Gallavotti G (2008) The Fermi-Pasta-Ulam Problem: A Status Report, Berlin-Heidelberg: Springer.
    [6] Zabusky NJ, Kruskal MD (1965) Interaction of solitons in a collisionless plasma and the recurrence of initial states. Phys Rev Lett 15: 240-245.
    [7] Izrailev FM, Chirikov BV (1966) Statistical properties of a nonlinear string. Sov Phys Dokl 11: 30-34.
    [8] Manakov SV (1974) Complete integrability and stochastization of discrete dynamical systems. Sov Phys JEPT 40: 269-274.
    [9] Ferguson WE, Flaschka H, McLaughlin DW (1982) Nonlinear Toda modes for the Toda chain. J Comput Phys 45: 157-209.
    [10] Benettin G, Ponno A (2011) Time-scales to equipartition in the Fermi-Pasta-Ulam problem: Finite-size effects and thermodynamic limit. J Stat Phys 144: 793-812.
    [11] Fucito E, Marchesoni F, Marinari E, et al. (1982) Approach to equilibrium in a chain of nonlinear oscillators. J Phys 43: 707-713.
    [12] Livi R, Pettini M, Ruffo S, et al. (1983) Relaxation to different stationary states in the Fermi-PastaUlam model. Phys Rev A 28: 3544-3552.
    [13] Kramer PR, Biello JA, L'vov YV (2003) Application of weak turbulence theory to FPU model, In: Proceedings of the Fourth International Conference on Dynamical Systems and Differential Equations (May 24-27, 2002, Wilmington, NC, USA), AIMS Conference Publications, 482-491.
    [14] Berchialla L, Galgani L, Giorgilli A (2004) Localization of energy in FPU chains. Discrete Cont Dyn-A 11: 855-866.
    [15] Bambusi D, Ponno A (2006) On metastability in FPU. Commun Math Phys 264: 539-561.
    [16] Benettin G, Carati A, Galgani L, et al. The Fermi-Pasta-Ulam problem and the metastability perspective, In: The Fermi-Pasta-Ulam Problem, Berlin: Springer, 151-189.
    [17] Carati A, Galgani L, Giorgilli A, et al. (2007) FPU phenomenon for generic initial data. Phys Rev E 76: 022104/1-4.
    [18] Carati A, Galgani L, Giorgilli A (2004) The Fermi-Pasta-Ulam problem as a challenge for the foundations of physics. Chaos 15: 015105.
    [19] Benettin G, Christodoulidi H, Ponno A (2013), The Fermi-Pasta-Ulam problem and its underlying integrable dynamics. J Stat Phys 152: 195-212.
    [20] Biello JA, Kramer PR, L'vov YV (2003) Stages of energy transfer in the FPU model, In: Proceedings of the Fourth International Conference on Dynamical Systems and Differential Equations (May 24-27, 2002, Wilmington, NC, USA), AIMS Conference Publications, 113-122.
    [21] Shepelyansky DL (1997) Low-energy chaos in the Fermi-Pasta-Ulam Problem. Nonlinearity 10: 1331-1338.
    [22] Benettin G, Livi R, Ponno A (2009) The Fermi-Pasta-Ulam problem: scaling laws vs. initial conditions. J Stat Phys 135: 873-893.
    [23] Livi R, Pettini M, Ruffo S, et al. (1985) Equipartition threshold in nonlinear large Hamiltonian systems: The Fermi-Pasta-Ulam model. Phys Rev A 31: 1039-1045.
    [24] Gardner CS, Green JM, Kruskal MD (1967) Method for solving the Korteweg-de Vries equation. Phys Rev Lett 19: 1095-1097.
    [25] Lax PD (1968) Integrals of nonlinear equations of evolution and solitary waves. Commun Pure Appl Math 21: 467-490.
    [26] Miura RM, Gardner CS, Kruskal MD (1968) Korteweg-de Vries equation and generalization, Ⅱ. Existence of conservation laws and constants of motion. J Math Phys 9: 1204-1209.
    [27] Zakharov VE, Feddeev LD (1971) Korteweg-de Vries equation: A completely integrable Hamiltonian system. Funct Anal Appl 5: 280-286.
    [28] Zakharov VE (1973) On stochastization of one dimensional chains of nonlinear oscillators. Sov Phys JETP 38: 108-110.
    [29] Toda M (1967) Vibration of a chain with nonlinear interaction. J Phys Soc Jpn 22: 431-436.
    [30] Toda M (1967) Wave propagation in anharmonic lattices. J Phys Soc Jpn 23: 501-506.
    [31] Toda M (1969) Mechanics and statistical mechanics of nonlinear chains. J Phys Soc Jpn 26: 109-111.
    [32] Toda M (1970) Waves in nonlinear lattice. Prog Theor Phys 45: 174-200.
    [33] Hénon M (1974) Integrals of the Toda lattice. Phys Rev B 9: 1921-1923.
    [34] Flaschka H (1974) The Toda lattice. Ⅱ. existence of integrals. Phys Rev B 9: 1924-1925.
    [35] Cecchetto M (2015) Normal modes and actions in the Toda Model, Master thesis of University of Padua, Dept. of Mathematics "Tullio Levi-Civita".
    [36] Henrici A, Kappeler T (2008) Global action-angle variables for the periodic Toda lattice. Int Math Res Not 2008: 1-52.
    [37] Henrici A, Kappeler T (2008) Global Birkhoff coordinates for the periodic Toda lattice. Nonlinearity 21: 2731-2758.
    [38] Bambusi D, Maspero A (2016) Birkhoff coordinates for the Toda Lattice in the limit of infinitely many particles with an application to FPU. J Funct Anal 270: 1818-1887.
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