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Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)

Inverse problem for stationary state of a Bose-Einstein condensate

Yu. V. Likhanova, С. Б. Медведев, М. П. Федорук, P. L. Chapovsky

Published Jun 1, 2017• 0 citations
Publisher

Abstract

The Bose-Einstein condensate is generally described by the three-dimensional equations. However, the two-dimensional case is of great interest too. First, these results can be directly used to study the planar condensates. Second, it serves as a test version for numerical calculations and as a quasi-two-dimensional approximation for the complete three-dimensional problem. An additional advantage of the two-dimensional case is that with the help of variational approach one can obtain analytical results for the stationary state and for the expansion of the condensate. In this paper, we propose a new approach for investigation of the Bose condensate in harmonic potential based on the variational method. We consider the inverse problem of reconstructing coefficients of the two-dimensional Gross-Pitaevskii equation with harmonic potential under the initially given condensate parameters (particle number, interatomic interaction, cloud widths). In particular, we solve the stationary problem in the framework of three trial functions, i.e., the Gaussian, the super-Gaussian and the Thomas-Fermi functions. In addition to that, the virial relation valid for arbitrary trial functions is obtained. We introduce the concept of special nonlinearity parameter in order to differentiate various degrees of the interatomic interaction. We perform comparison the variational solutions for the problem with the results of numerical calculations at the various levels of nonlinearity. For example, the relative differences between the condensate widths (Q1 and Q2) obtained by the variational method and the results of the direct numerical simulation is presented. It can be seen that the Gaussian and the super-Gaussian approximate the widths of the condensate with the accuracy better than 5% at various levels of nonlinearity. We demonstrate that the suggested approach allows one to solve the inverse problem of reconstructing all the equation parameters under the initially given condensate parameters. The joint use of the variational approach to the problem together with the numerical calculations allows one efficiently link the characteristics of the Bose condensate with the parameters of the Gross-Pitaevskii equation. Moreover, the proposed analytical-numerical approach can be used for broader class of problems than we discuss in the paper, for example, for investigating the self-focusing electromagnetic waves.

DOI
10.1109/cleoe-eqec.2017.8087454

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The Bose-Einstein condensate is generally described by the three-dimensional equations. However, the two-dimensional case is of great interest too. First, these results can be directly used to study the planar condensates. Second, it serves as a test version for numerical calculations and as a quasi-two-dimensional approximation for the complete three-dimensional problem. An additional advantage of the two-dimensional case is that with the help of variational approach one can obtain analytical results for the stationary state and for the expansion of the condensate. In this paper, we propose a new approach for investigation of the Bose condensate in harmonic potential based on the variational method. We consider the inverse problem of reconstructing coefficients of the two-dimensional Gross-Pitaevskii equation with harmonic potential under the initially given condensate parameters (particle number, interatomic interaction, cloud widths). In particular, we solve the stationary problem in the framework of three trial functions, i.e., the Gaussian, the super-Gaussian and the Thomas-Fermi functions. In addition to that, the virial relation valid for arbitrary trial functions is obtained. We introduce the concept of special nonlinearity parameter in order to differentiate various degrees of the interatomic interaction. We perform comparison the variational solutions for the problem with the results of numerical calculations at the various levels of nonlinearity. For example, the relative differences between the condensate widths (Q1 and Q2) obtained by the variational method and the results of the direct numerical simulation is presented. It can be seen that the Gaussian and the super-Gaussian approximate the widths of the condensate with the accuracy better than 5% at various levels of nonlinearity. We demonstrate that the suggested approach allows one to solve the inverse problem of reconstructing all the equation parameters under the initially given condensate parameters. The joint use of the variational approach to the problem together with the numerical calculations allows one efficiently link the characteristics of the Bose condensate with the parameters of the Gross-Pitaevskii equation. Moreover, the proposed analytical-numerical approach can be used for broader class of problems than we discuss in the paper, for example, for investigating the self-focusing electromagnetic waves.
A variational technique is applied to solve the time-dependent nonlinear Schr\"odinger equation (Gross-Pitaevskii equation) with the goal to model the dynamics of dilute ultracold atom clouds in the Bose-Einstein condensed phase. We derive analytical predictions for the collapse, equilibrium widths, and evolution laws of the condensate parameters and find them to be in very good agreement with our numerical simulations of the nonlinear Schr\"odinger equation. It is found that not only the number of particles, but also both the initial width of the condensate and the effect of different perturbations to the condensate may play a crucial role in the collapse dynamics. The results are applicable when the shape of the condensate is sufficiently simple.
We show analytically that the profile of the Bose–Einstein condensate can evolve exact self-similarly when the time-dependent interatomic interaction and harmonic potential satisfy a certain condition for one-, two- and three-dimensional geometries, respectively. Based on the exact scaling laws for the amplitude and width of the condensate profile, we propose experimentally feasible ways to improve the accuracy in measuring the stationary-state profile of the condensate when its spatial size is so small that the direct measurement is not available, and to squeeze the condensate to high local particle density to check the validity of the Gross–Pitaevskii equation via the controllable exact self-similar evolution of the condensate profile.
We present a method for approximating the solution of the three-dimensional, time-dependent Gross-Pitaevskii equation (GPE) for Bose-Einstein-condensate systems where the confinement in one dimension is much tighter than in the other two. This method employs a hybrid Lagrangian variational technique whose trial wave function is the product of a completely unspecified function of the coordinates in the plane of weak confinement and a Gaussian in the strongly confined direction having a time-dependent width and quadratic phase. The hybrid Lagrangian variational method produces equations of motion that consist of (1) a two-dimensional (2D) effective GPE whose nonlinear coefficient contains the width of the Gaussian and (2) an equation of motion for the width that depends on the integral of the fourth power of the solution of the 2D effective GPE. We apply this method to the dynamics of Bose-Einstein condensates confined in ring-shaped potentials and compare the approximate solution to the numerical solution of the full 3D GPE.
The experimental discovery of dilute ultracold quantum gases in 1995 has instigated a broad interest in ultracold atoms and molecules, and paved the way for extensive studies of a wide range of both experimental and theoretical topics. Various theories were developed to describe Bose-Einstein condensates (BECs) for different ranges of temperature and interaction strengths. This thesis focuses on studying the mean-field theory of the Gross-Pitaevskii (GP) equation which provides a good description for the macroscopic wave function when both quantum and thermal fluctuations are negligible. This means that the range of validity is restricted to small interaction strengths at zero temperature. Within the GP theory we study analytically and numerically the nonlinear dynamics of BECs which are induced by a harmonic modulation of either the interaction strength or the harmonic trapping potential. At first a detailed numerical investigation reveals that solving the partial differential equation of Gross and Pitaevskii can be reduced to solving ordinary differential equations for the condensate widths within a Gaussian variational approach. Despite this tremendous simplification the prominent nonlinearity of the underlying GP equation is inherited by the variational equations, which thus allow to describe a rich variety of nonlinear phenomena in different experimental setups. In order to describe them analytically we transfer the Poincar\'e-Lindstedt method, which represents a well-established tool in the field of nonlinear dynamics, to the Gaussian variational approach. Modulation of some of the parameters of a BEC can give rise to prominent nonlinear features, such as shifts in the frequencies of collective oscillation modes, higher harmonics generation, and resonant mode coupling. As a first application we consider a recent Bose-Einstein condensate of Li-7, which has been excited experimentally by a harmonic modulation of the atomic s-wave scattering length with the help of a Feshbach resonance. Combining an analytical perturbative approach with extensive numerical simulations, we analyze the emerging nonlinear dynamics. In particular, we present the resulting shift of collective excitation spectra close to parametric resonances where the driving frequency coincides with a collective mode frequency. Another application of experimental importance is to study geometric resonances in BECs with two-body and three-body contact interactions, where changing the geometry of the trapping potential leads to commensurate collective excitation frequencies with emerging nonlinear effects such as frequency shifts and resonant mode coupling. In this context we also show that a small repulsive three-body interaction is able to extend the stability region of the condensate for an attractive two-body interaction as it increases the critical number of atoms in the trap. Apart from a periodic modulation of a system parameter the dipole mode frequency can be excited by introducing an abrupt change in the potential, where the center of mass oscillates according to the Kohn theorem back and forth in the trapping potential with the natural trap frequency irrespective of both the strength and the type of the two-particle interaction. To this end, we study the collective excitation modes of a Bose-Einstein condensate in a harmonic Ioffe- Pritchard in the vicinity of a Feshbach resonance for experimentally realistic parameters of a Rb-85 BEC, where the dipole mode is excited in z-direction. A linearization of the underlying equations of motions shows that the dipole mode frequency decreases when the bias magnetic field approaches the Feshbach resonance, so the Kohn theorem is violated. Finally within a variational approach we discuss the physical properties of a BEC in an axially-symmetric harmonic trap with a single vortex in the center. At first we analyze the equilibrium configuration and determine the vortex size as well as the Thomas- Fermi radii of the condensate in the Thomas-Fermi limit. Then we calculate the critical rotation frequency for the emergence of the vortex and compare our findings with the literature. Finally, we investigate how the presence of the vortex changes the collective excitation frequencies and we discuss the free expansion of the BEC. All these results indicate how nonlinear dynamics properties could be made clearly observable in future experiments on the basis of our results.
A Bose–Einstein condensate in a double-well potential is considered by using the Feynman path integral theory combined with a variational approach. The system consists of N interacting bosons confined in the double well which is taken as a harmonic potential with a Gaussian barrier. The calculation is carried out within the first cumulant approximation measured with respect to the harmonic action containing variational parameters. Assuming a separable expression for the trial action corresponds to the usual mean field approximation. Performing the variational calculations, we obtain analytical results for the ground state energy and its condensate wavefunction. Using a projection onto the odd contributions, the first excited state energy and condensate wavefunction are determined, too. We find very good agreement with a full numerical solution of the Gross–Pitaevskii equation over the full range of potential parameters.