Route to thermalization in the α-Fermi-Pasta-Ulam system

被引:119
作者
Onorato, Miguel [1 ,2 ]
Vozella, Lara [1 ,2 ]
Proment, Davide [3 ]
Lvov, Yuri V. [4 ]
机构
[1] Univ Turin, Dipartimento Fis, I-10125 Turin, Italy
[2] Ist Nazl Fis Nucl, Sez Torino, I-10125 Turin, Italy
[3] Univ E Anglia, Sch Math, Norwich NR4 7TJ, Norfolk, England
[4] Rensselaer Polytech Inst, Dept Math Sci, Troy, NY 12180 USA
关键词
alpha-Fermi-Pasta-Ulam chain; thermalization; wave-wave interactions; FPU recurrence; resonant interactions; SURFACE; EQUIPARTITION; CHAIN; LIMIT;
D O I
10.1073/pnas.1404397112
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
We study the original alpha-Fermi-Pasta-Ulam (FPU) system with N = 16, 32, and 64 masses connected by a nonlinear quadratic spring. Our approach is based on resonant wave-wave interaction theory; i.e., we assume that, in the weakly nonlinear regime (the one in which Fermi was originally interested), the large time dynamics is ruled by exact resonances. After a detailed analysis of the alpha-FPU equation of motion, we find that the first nontrivial resonances correspond to six-wave interactions. Those are precisely the interactions responsible for the thermalization of the energy in the spectrum. We predict that, for small-amplitude random waves, the timescale of such interactions is extremely large and it is of the order of 1/is an element of(8), where is an element of is the small parameter in the system. The wave-wave interaction theory is not based on any threshold: Equipartition is predicted for arbitrary small nonlinearity. Our results are supported by extensive numerical simulations. A key role in our finding is played by the Umklapp (flipover) resonant interactions, typical of discrete systems. The thermodynamic limit is also briefly discussed.
引用
收藏
页码:4208 / 4213
页数:6
相关论文
共 33 条
[1]  
Arnold V. I., 1963, Russian Mathematical Surveys, V18, P85, DOI [10.1070/RM1963v018n06ABEH001143, DOI 10.1070/RM1963V018N06ABEH001143]
[2]   The Fermi-Pasta-Ulam Problem and Its Underlying Integrable Dynamics [J].
Benettin, G. ;
Christodoulidi, H. ;
Ponno, A. .
JOURNAL OF STATISTICAL PHYSICS, 2013, 152 (02) :195-212
[3]   The Fermi-Pasta-Ulam problem: Fifty years of progress [J].
Berman, GP ;
Izrailev, FM .
CHAOS, 2005, 15 (01)
[4]   The Fermi-Pasta-Ulam problem as a challenge for the foundations of physics [J].
Carati, A ;
Galgani, L ;
Giorgilli, A .
CHAOS, 2005, 15 (01)
[5]   The Fermi-Pasta-Ulam problem revisited: Stochasticity thresholds in nonlinear Hamiltonian systems [J].
Casetti, L ;
CerrutiSola, M ;
Pettini, M ;
Cohen, EGD .
PHYSICAL REVIEW E, 1997, 55 (06) :6566-6574
[6]   Localization and equipartition of energy in the β-FPU chain:: Chaotic breathers [J].
Cretegny, T ;
Dauxois, T ;
Ruffo, S ;
Torcini, A .
PHYSICA D, 1998, 121 (1-2) :109-126
[7]   On the nonintegrability of the free surface hydrodynamics [J].
Dyachenko, A. I. ;
Kachulin, D. I. ;
Zakharov, V. E. .
JETP LETTERS, 2013, 98 (01) :43-47
[8]   5-WAVE INTERACTION ON THE SURFACE OF DEEP FLUID [J].
DYACHENKO, AI ;
LVOV, YV ;
ZAKHAROV, VE .
PHYSICA D, 1995, 87 (1-4) :233-261
[9]   NON-LINEAR NORMAL-MODES FOR THE TODA CHAIN [J].
FERGUSON, WE ;
FLASCHKA, H ;
MCLAUGHLIN, DW .
JOURNAL OF COMPUTATIONAL PHYSICS, 1982, 45 (02) :157-209
[10]  
Fermi E., 1955, Tech. Rep.