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Thomas Bilitewski

 Thomas Bilitewski

Thomas Bilitewski

Member of Trinity College
PhD student in Prof Cooper's group

Office: 524 Mott Bld
Phone: +44(0)1223 3 37459
Email: tb494 @
ORCID: 0000-0002-9971-1835
Arxiv: Article list

TCM Group, Cavendish Laboratory
19 JJ Thomson Avenue,
Cambridge, CB3 0HE UK.

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I am working in the area of cold gas systems. My current project is motivated byrecent experimental developments, in particular the time-modulated tuning of system parameters in cold gas set-ups. It explores the novel aspects arising in these quantum many-body systems focussing on both time-dependent effects and collective many-body phases.

Most recently I've worked on the effects of interactions in time-periodically driven systems in the context of the generation of artificial gauge fields for cold atoms. The relevant framework for the treatment of time-periodic Hamiltonians is Floquet Theory. Due to the breaking of time-translation invariance energy is not conserved, but the time-periodicity of the Hamiltonian rather only ensures the conservation of quasi-energy.

I have explored the consequences of this in the case of specific model systems and for the experimentally relevant realisation of the Harper-Hofstadter Hamiltonian in terms of the competition between elastic scattering, required for correlated many-body phases, and inelastic scattering, leading to deleterious heating and particle loss.

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In Plain English

To deepen our understanding of various phenomena we often seek to find very controllable and clean model systems that should be able to capture the main physics of the relevant problem while allowing a theoretical description and a simple experimental realisation.

Cold gas systems are clouds of atoms that are cooled to extremely low temperatures such that their quantum nature becomes important. These systems allow very precise control and measurement of many of their properties and can be used to simulate a variety of physical systems.

One interesting approach is to expose these systems to time-varying light fields to be able to simulate the effect of magnetic (and more general) fields. In some sense this corresponds to “shaking” the atoms. Thus, one would expect that this procedure possibly injects energy into the system, heating it, or allows the atoms to be excited. Usually, one would like the system not to be heated up and to remain cool. Therefore, a theoretical understanding of these heating processes and prescriptions how to keep the good effects of the shaking while minimising the bad heating are required.