scholarly journals Mean-field regime and Thomas–Fermi approximations of trapped Bose–Einstein condensates with higher-order interactions in one and two dimensions

2016 ◽  
Vol 49 (12) ◽  
pp. 125304 ◽  
Author(s):  
Xinran Ruan ◽  
Yongyong Cai ◽  
Weizhu Bao
2010 ◽  
Vol 82 (4) ◽  
Author(s):  
Yongyong Cai ◽  
Matthias Rosenkranz ◽  
Zhen Lei ◽  
Weizhu Bao

2004 ◽  
Vol 18 (05n06) ◽  
pp. 173-202 ◽  
Author(s):  
P. G. KEVREKIDIS ◽  
D. J. FRANTZESKAKIS

In this short topical review, we revisit a number of works on the pattern-forming dynamical instabilities of Bose–Einstein condensates in one- and two-dimensional settings. In particular, we illustrate the trapping conditions that allow the reduction of the three-dimensional, mean field description of the condensates (through the Gross–Pitaevskii equation) to such lower dimensional settings, as well as to lattice settings. We then go on to study the modulational instability in one dimension and the snaking/transverse instability in two dimensions as typical examples of long-wavelength perturbations that can destabilize the condensates and lead to the formation of patterns of coherent structures in them. Trains of solitons in one dimension and vortex arrays in two dimensions are prototypical examples of the resulting nonlinear waveforms, upon which we briefly touch at the end of this review.


2018 ◽  
Vol 93 (12) ◽  
pp. 124004
Author(s):  
J Teske ◽  
M R Besbes ◽  
B Okhrimenko ◽  
R Walser

2021 ◽  
Vol 240 (1) ◽  
pp. 383-417
Author(s):  
Nikolai Leopold ◽  
David Mitrouskas ◽  
Robert Seiringer

AbstractWe consider the Fröhlich Hamiltonian in a mean-field limit where many bosonic particles weakly couple to the quantized phonon field. For large particle numbers and a suitably small coupling, we show that the dynamics of the system is approximately described by the Landau–Pekar equations. These describe a Bose–Einstein condensate interacting with a classical polarization field, whose dynamics is effected by the condensate, i.e., the back-reaction of the phonons that are created by the particles during the time evolution is of leading order.


Author(s):  
Phan Thành Nam ◽  
Marcin Napiórkowski

AbstractWe consider the homogeneous Bose gas on a unit torus in the mean-field regime when the interaction strength is proportional to the inverse of the particle number. In the limit when the number of particles becomes large, we derive a two-term expansion of the one-body density matrix of the ground state. The proof is based on a cubic correction to Bogoliubov’s approximation of the ground state energy and the ground state.


2019 ◽  
Vol 386-387 ◽  
pp. 38-48 ◽  
Author(s):  
Weizhu Bao ◽  
Yongyong Cai ◽  
Xinran Ruan

2001 ◽  
Vol 13 (36) ◽  
pp. L819-L824 ◽  
Author(s):  
S M M Virtanen ◽  
T P Simula ◽  
M M Salomaa

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