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Quantitative derivation of effective evolution equations for the dynamics of Bose-Einstein condensates.

机译:玻色-爱因斯坦凝聚物动力学的有效演化方程的定量推导。

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摘要

This thesis proves certain results concerning an important question in nonequilibrium quantum statistical mechanics which is the derivation of effective evolution equations approximating the dynamics of a system of large number of bosons initially at equilibrium (ground state at very low temperatures). The dynamics of such systems are governed by the time-dependent linear many-body Schrodinger equation from which it is typically difficult to extract useful information due to the number of particles being large. We will study quantitatively (i.e. with explicit bounds on the error) how a suitable one particle non-linear Schrodinger equation arises in the mean field limit as number of particles N → infinity and how the appropriate corrections to the mean field will provide better approximations of the exact dynamics.;In the first part of this thesis we consider the evolution of N bosons, where N is large, with two-body interactions of the form N3betaupsilon(Nbeta·), 0 ≤ beta ≤ 1. The parameter beta measures the strength and the range of interactions. We compare the exact evolution with an approximation which considers the evolution of a mean field coupled with an appropriate description of pair excitations, see [18,19] by Grillakis-Machedon-Margetis. We extend the results for 0 ≤ beta < 1/3 in [19,20] to the case of beta 0 and p( t) is a polynomial, which implies a specific rate of convergence as N → infinity.;In the second part, utilizing estimates of the type discussed in the first part, we compare the exact evolution with the mean field approximation in the sense of marginals. We prove that the exact evolution is close to the approximate in trace norm for times of the order o(1)√ N compared to log(o(1)N) as obtained in Chen-Lee-Schlein [6] for the Hartree evolution. Estimates of similar type are obtained for stronger interactions as well.;[6] L. Chen, J. O. Lee and B. Schlein, Rate of convergence towards Hartree dynamics, J. Stat. Phys. 144, 872--903 (2011).;[18] M. Grillakis, M. Machedon and D. Margetis, Second-order corrections to mean field evolution of weakly interacting Bosons. I, Commun. Math. Phys. 294, 273--301 (2010).;[19] M. Grillakis, M. Machedon and D. Margetis, Second-order corrections to mean field evolution of weakly interacting Bosons. II, Adv. in Math. 228, 1788--1815 (2011).;[20] M. Grillakis and M. Machedon, Pair excitations and the mean field approximation of interacting Bosons, I, Commun. Math. Phys. 324, 601--636 (2013).
机译:本文证明了有关非平衡量子统计力学中一个重要问题的某些结果,这是有效演化方程的推导,该方程近似于最初处于平衡状态(非常低温下的基态)的大量玻色子系统的动力学。这种系统的动力学受时间相关的线性多体薛定inger方程控制,由于粒子数量很大,通常很难从中提取有用的信息。我们将定量研究(即在误差上有明确的界限)当粒子数N→无穷大时,如何在平均场极限中出现合适的一个粒子非线性Schrodinger方程,以及对平均场的适当校正将如何提供更好的近似值。在本文的第一部分中,我们考虑了N个玻色子的演化,其中N大,形式为N3betaupsilon(Nbeta·),0≤beta≤1的两体相互作用。强度和相互作用的范围。我们将精确的演化与近似值进行比较,该近似值考虑了平均场的演化以及对对激发的适当描述,请参见Grillakis-Machedon-Margetis的[18,19]。我们将[19,20]中0≤beta <1/3的结果扩展到beta 0的情况,并且p(t)是多项式,这意味着特定的收敛速度为N→无穷大。 ,利用在第一部分中讨论的类型的估计,我们将精确的演化与在边际意义上的平均场近似进行比较。我们证明,与Chen-Lee-Schlein [6]中针对Hartree演化获得的log(o(1)N)相比,o(1)√N阶次的时间精确演化接近于迹范数的近似。 。 [6] L. Chen,J。O. Lee和B. Schlein,朝向Hartree动力学的收敛速度,J。Stat。物理144,872--903(2011)。; [18] M. Grillakis,M。Machedon和D.Margetis,对弱相互作用的玻色子的场演化进行二阶校正。我,Commun。数学。物理294,273--301(2010)。; [19] M. Grillakis,M。Machedon和D.Margetis,对弱相互作用的玻色子的场演化进行二阶校正。 II,高级在数学中。 228,1788--1815(2011)。[20] M. Grillakis和M. Machedon,对激发和相互作用的玻色子的平均场近似,I,Commun。数学。物理324,601--636(2013)。

著录项

  • 作者

    Kuz, Elif.;

  • 作者单位

    University of Maryland, College Park.;

  • 授予单位 University of Maryland, College Park.;
  • 学科 Mathematics.;Quantum physics.
  • 学位 Ph.D.
  • 年度 2016
  • 页码 134 p.
  • 总页数 134
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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