One-Dimensional Classical Many-Body System Having a Normal Thermal Conductivity

1984 ◽  
Vol 53 (11) ◽  
pp. 1120-1120 ◽  
Author(s):  
Giulio Casati ◽  
Joseph Ford ◽  
Franco Vivaldi ◽  
William M. Visscher
1984 ◽  
Vol 52 (21) ◽  
pp. 1861-1864 ◽  
Author(s):  
Giulio Casati ◽  
Joseph Ford ◽  
Franco Vivaldi ◽  
William M. Visscher

Quantum ◽  
2021 ◽  
Vol 5 ◽  
pp. 486
Author(s):  
Thomás Fogarty ◽  
Miguel Ángel García-March ◽  
Lea F. Santos ◽  
Nathan L. Harshman

Interacting quantum systems in the chaotic domain are at the core of various ongoing studies of many-body physics, ranging from the scrambling of quantum information to the onset of thermalization. We propose a minimum model for chaos that can be experimentally realized with cold atoms trapped in one-dimensional multi-well potentials. We explore the emergence of chaos as the number of particles is increased, starting with as few as two, and as the number of wells is increased, ranging from a double well to a multi-well Kronig-Penney-like system. In this way, we illuminate the narrow boundary between integrability and chaos in a highly tunable few-body system. We show that the competition between the particle interactions and the periodic structure of the confining potential reveals subtle indications of quantum chaos for 3 particles, while for 4 particles stronger signatures are seen. The analysis is performed for bosonic particles and could also be extended to distinguishable fermions.


1994 ◽  
Vol 50 (2) ◽  
pp. 888-896 ◽  
Author(s):  
Bill Sutherland ◽  
Joel Campbell

1982 ◽  
Vol 23 (12) ◽  
pp. 2439-2444 ◽  
Author(s):  
V. C. Aguilera‐Navarro ◽  
E. Ley‐Koo ◽  
M. de Llano ◽  
S. M. Peltier ◽  
A. Plastino

1993 ◽  
Vol 71 (17) ◽  
pp. 2789-2792 ◽  
Author(s):  
Bill Sutherland ◽  
Rudolf A. Römer

Quantum ◽  
2018 ◽  
Vol 2 ◽  
pp. 42 ◽  
Author(s):  
Louis Villa ◽  
Gabriele De Chiara

We propose a method to experimentally measure the internal energy of a system of ultracold atoms trapped in optical lattices by coupling them to the fields of two optical cavities. We show that the tunnelling and self-interaction terms of the one-dimensional Bose-Hubbard Hamiltonian can be mapped to the field and photon number of each cavity, respectively. We compare the energy estimated using this method with numerical results obtained using the density matrix renormalisation group algorithm. Our method can be employed for the assessment of power and efficiency of thermal machines whose working substance is a strongly correlated many-body system.


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