nonlinear phenomena in degenerate quantum gases

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Physica D 238 (2009) 1289–1298 Contents lists available at ScienceDirect Physica D journal homepage: www.elsevier.com/locate/physd Preface Nonlinear phenomena in degenerate quantum gases Víctor M. Pérez-García a,* , Natalia G. Berloff b , Panayotis G. Kevrekidis c , Vladimir V. Konotop d,e , Boris A. Malomed f a Departamento de Matemáticas, E. T. S. I. Industriales and Instituto de Matemática Aplicada a la Ciencia y la Ingeniería, Edificio Politécnico, Avenida de Camilo José Cela, 3, Universidad de Castilla-La Mancha 13071 Ciudad Real, Spain b Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, CB3 0WA, United Kingdom c Department of Mathematics and Statistics, University of Massachusetts, Amherst, MA 01003-4515, USA d Centro de Física Teórica e Computacional, Universidade de Lisboa, Complexo Interdisciplinar, Avenida Professor Gama Pinto 2, Lisboa 1649-003, Portugal e Departamento de Física, Faculdade de Ciências, Universidade de Lisboa, Campo Grande, Ed. C8, Piso 6, Lisboa 1749-016, Portugal f Department of Physical Electronics, School of Electrical Engineering, Faculty of Engineering, Tel Aviv University, Tel Aviv 69978, Israel article info Article history: Available online 12 May 2009 PACS: 03.75.Lm 05.45.Yv Keywords: Nonlinear Schrödinger equations Gross–Pitaevskii equation Degenerate quantum gases Nonlinear phenomena Solitons Vortices Matter waves abstract In this introductory survey, we give an overview of the main physical problems and corresponding themes of research addressed in this Special Issue. We also briefly discuss some avenues of potential interest for future research in degenerate quantum gases. © 2009 Elsevier B.V. All rights reserved. 1. The background Fourteen years ago – a very long time, in terms of modern sci- ence– three experimental groups were able to cool down bosonic gases ( 87 Rb, 7 Li, and 23 Na, respectively) below the Bose–Einstein transition temperature [1–3]. These experiments provided the first direct demonstration of Bose–Einstein condensation, a phe- nomenon predicted almost a century ago [4,5]. These achieve- ments are now rightfully among the landmarks of modern physics. The creation of Bose–Einstein condensates (BECs) in ultracold alkali gases was not only the advent of a long-sought state of matter and the verification of a fundamental theoretical prediction. Actually, this event had ushered a new era in condensed-matter physics, since these media have proven to be a universal laboratory for the study of phenomena previously predicted but never clearly observed in many areas of Physics, ranging from quantum fluids to the theory of quantum phase transitions [6–8]. * Corresponding editor. Tel.: +34 926 295 435; fax: +34 92 629 5361. E-mail address: [email protected] (V.M. Pérez-García). While the original prediction of the BEC was made for noninter- acting and spatially uniform systems, ultracold atomic condensates feature, and indeed require in order to condense, collisional inter- actions between atoms. Moreover, they are spatially inhomoge- neous because of the effect of trapping fields. Typically, the atoms interact weakly enough for the condensate to remain as a dilute gas, but strongly enough to make nonlinear effects not only notice- able but even critical in the creation of the condensates and their dynamics. On the theoretical level, a fundamental mean-field theory for boson condensates was developed independently forty years ago by Pitaevskii [9] and Gross [10] (originally, this was done with the intention to apply the resultant equations, currently known as Gross-Pitaevskii equations (GPEs), to quasi-particles in liquid helium). One of the basic conclusions made in the early days of development of this field was the fact that the experimental observations concerning the shape, dynamical expansion, and collective excitations of trapped condensates [11–13], can be indeed explained by means of the GPEs, in virtually all physical situations, with a surprisingly accurate precision and without the use of any adjustable parameters [14–21]. These results confirmed the significance of nonlinearities in the dynamics 0167-2789/$ – see front matter © 2009 Elsevier B.V. All rights reserved. doi:10.1016/j.physd.2009.05.001

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Physica D 238 (2009) 1289–1298

Contents lists available at ScienceDirect

Physica D

journal homepage: www.elsevier.com/locate/physd

Preface

Nonlinear phenomena in degenerate quantum gases

Víctor M. Pérez-García a,∗, Natalia G. Berloff b, Panayotis G. Kevrekidis c, Vladimir V. Konotop d,e,Boris A. Malomed fa Departamento de Matemáticas, E. T. S. I. Industriales and Instituto de Matemática Aplicada a la Ciencia y la Ingeniería, Edificio Politécnico, Avenida de Camilo José Cela, 3,Universidad de Castilla-La Mancha 13071 Ciudad Real, Spainb Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, CB3 0WA, United Kingdomc Department of Mathematics and Statistics, University of Massachusetts, Amherst, MA 01003-4515, USAd Centro de Física Teórica e Computacional, Universidade de Lisboa, Complexo Interdisciplinar, Avenida Professor Gama Pinto 2, Lisboa 1649-003, Portugale Departamento de Física, Faculdade de Ciências, Universidade de Lisboa, Campo Grande, Ed. C8, Piso 6, Lisboa 1749-016, Portugalf Department of Physical Electronics, School of Electrical Engineering, Faculty of Engineering, Tel Aviv University, Tel Aviv 69978, Israel

a r t i c l e i n f o

Article history:Available online 12 May 2009

PACS:03.75.Lm05.45.Yv

Keywords:Nonlinear Schrödinger equationsGross–Pitaevskii equationDegenerate quantum gasesNonlinear phenomenaSolitonsVorticesMatter waves

a b s t r a c t

In this introductory survey,we give an overviewof themain physical problems and corresponding themesof research addressed in this Special Issue. We also briefly discuss some avenues of potential interest forfuture research in degenerate quantum gases.

© 2009 Elsevier B.V. All rights reserved.

1. The background

Fourteen years ago – a very long time, in terms of modern sci-ence– three experimental groups were able to cool down bosonicgases (87Rb, 7Li, and 23Na, respectively) below the Bose–Einsteintransition temperature [1–3]. These experiments provided thefirst direct demonstration of Bose–Einstein condensation, a phe-nomenon predicted almost a century ago [4,5]. These achieve-ments are now rightfully among the landmarks of modern physics.The creation of Bose–Einstein condensates (BECs) in ultracold

alkali gases was not only the advent of a long-sought state ofmatter and the verification of a fundamental theoretical prediction.Actually, this event had ushered a new era in condensed-matterphysics, since thesemedia have proven to be a universal laboratoryfor the study of phenomena previously predicted but never clearlyobserved in many areas of Physics, ranging from quantum fluids tothe theory of quantum phase transitions [6–8].

∗ Corresponding editor. Tel.: +34 926 295 435; fax: +34 92 629 5361.E-mail address: [email protected] (V.M. Pérez-García).

While the original prediction of the BECwasmade for noninter-acting and spatially uniformsystems, ultracold atomic condensatesfeature, and indeed require in order to condense, collisional inter-actions between atoms. Moreover, they are spatially inhomoge-neous because of the effect of trapping fields. Typically, the atomsinteract weakly enough for the condensate to remain as a dilutegas, but strongly enough tomake nonlinear effects not only notice-able but even critical in the creation of the condensates and theirdynamics.On the theoretical level, a fundamental mean-field theory for

boson condensates was developed independently forty years agoby Pitaevskii [9] and Gross [10] (originally, this was done withthe intention to apply the resultant equations, currently knownas Gross-Pitaevskii equations (GPEs), to quasi-particles in liquidhelium). One of the basic conclusions made in the early daysof development of this field was the fact that the experimentalobservations concerning the shape, dynamical expansion, andcollective excitations of trapped condensates [11–13], can beindeed explained by means of the GPEs, in virtually all physicalsituations, with a surprisingly accurate precision and withoutthe use of any adjustable parameters [14–21]. These resultsconfirmed the significance of nonlinearities in the dynamics

0167-2789/$ – see front matter© 2009 Elsevier B.V. All rights reserved.doi:10.1016/j.physd.2009.05.001