Dynamics of Large Boson Systems with Attractive Interaction and a Derivation of the Cubic Focusing NLS in
arXiv:1608.01615
Abstract
We consider a system of bosons where the particles experience a short range two-body interaction given by where , without a definite sign on . We extend the results of M. Grillakis and M. Machedon, Comm. Math. Phys., , 601(2013) and E. Kuz, Differ. Integral Equ., , 1613(2015) regarding the second-order correction to the mean-field evolution of systems with repulsive interaction to systems with attractive interaction for . Our extension allows for a more general set of initial data which includes coherent states. Inspired by the works of X. Chen and J. Holmer, Arch. Ration. Mech. Anal., , 631(2016) and Int. Math. Res. Not., , 4173(2017), and P. T. Nam and M. Napiórkowski, Adv. Theor. Math. Phys., , 683(2017), we also provide both a derivation of the focusing nonlinear Schrödinger equation (NLS) in D from the many-body system and its rate of convergence toward mean-field for . In particular, we give two derivations of the focusing NLS, one based on the -norm approximation given in the work of Nam and Napiórkowski and the other via a method introduced in P. Pickl, J. Stat. Phys., , 76(2010). The techniques used in this article are standard in the literature of dispersive PDEs. Nevertheless, the derivation of the focusing NLS had only previously been studied for the 1D \& 2D cases and conditionally answered for the 3D case for .
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- Derivation of the time-dependent Gross-Pitaevskii equation for the dipolar gases
- On the emergence of quantum Boltzmann fluctuation dynamics near a Bose-Einstein Condensate