Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physics Today

Putting quantum gases under the microscope

Barbara Goss Levi

Published Sep 14, 2010• 0 citations
Publisher
DOI
10.1063/pt.4.0870

Related papers

Optical Microscope for Quantum Gases in a 2D Trap

Waseem Bakr, Jonathon I. Gillen, Amy Peng +2 more

Bulletin of the American Physical Society•May 23, 2009•0 citations

Quantum gas microscope

Jonathon I. Gillen, Waseem Bakr, Amy Peng +2 more

Bulletin of the American Physical Society•Mar 19, 2009•1 citation

Putting quantum gases under the microscope

Barbara Goss Levi

Microscopes with single-site resolution are vital for using ultracold atoms to simulate strongly correlated electrons in solids.

Physics Today•Oct 1, 2010•8 citations

Microscopic treatment of binary interactions in the nonequilibrium dynamics of partially Bose-condensed trapped gases

Nick P. Proukakis, K Burnett, HTC Stoof

In this paper we use microscopic arguments to derive a nonlinear Schrödinger equation for trapped Bose-condensed gases. This is made possible by considering the equations of motion of various anomalous averages. The resulting equation explicitly includes the effect of repeated binary interactions (in particular ladders) between the atoms. Moreover, under the conditions where dressing of the intermediate states of a collision can be ignored, this equation is shown to reduce to the conventional Gross-Pitaevskii equation in the pseudopotential limit. Extending the treatment, we show first how the occupation of excited (bare particle) states affects the collisions, and thus obtain the many-body T-matrix approximation in a trap. In addition, we discuss how the bare particle many-body T matrix gets dressed by mean fields due to condensed and excited atoms. We conclude that the most commonly used version of the Gross-Pitaevskii equation can only be put on a microscopic basis for a restrictive range of conditions. For partial condensation, we need to take account of interactions between condensed and excited atoms, which, in a consistent formulation, should also be expressed in terms of the many-body T matrix. This can be achieved by considering fluctuations around the condensate mean field beyond those included in the conventional finite temperature mean field, i.e., Hartree-Fock-Bogoliubov, theory.

•Feb 1, 1998•0 citations

Progress Towards a Quantum Gas Microscope

Amy Peng, Waseem Bakr, Jonathon I. Gillen +2 more

Bulletin of the American Physical Society•May 28, 2008•0 citations

Experiments with Atomic and Molecular Quantum Gas Microscopes

Sejal Aggarwal

•Jul 26, 2019•0 citations
In this paper we use microscopic arguments to derive a nonlinear Schrödinger equation for trapped Bose-condensed gases. This is made possible by considering the equations of motion of various anomalous averages. The resulting equation explicitly includes the effect of repeated binary interactions (in particular ladders) between the atoms. Moreover, under the conditions where dressing of the intermediate states of a collision can be ignored, this equation is shown to reduce to the conventional Gross-Pitaevskii equation in the pseudopotential limit. Extending the treatment, we show first how the occupation of excited (bare particle) states affects the collisions, and thus obtain the many-body T-matrix approximation in a trap. In addition, we discuss how the bare particle many-body T matrix gets dressed by mean fields due to condensed and excited atoms. We conclude that the most commonly used version of the Gross-Pitaevskii equation can only be put on a microscopic basis for a restrictive range of conditions. For partial condensation, we need to take account of interactions between condensed and excited atoms, which, in a consistent formulation, should also be expressed in terms of the many-body T matrix. This can be achieved by considering fluctuations around the condensate mean field beyond those included in the conventional finite temperature mean field, i.e., Hartree-Fock-Bogoliubov, theory.