2016
DOI: 10.1016/j.physb.2015.10.015
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De Haas-van Alphen effect of a two-dimensional ultracold atomic gas

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Cited by 7 publications
(9 citation statements)
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“…When the filling number is of the order of unity, we expect the atomic gas to exhibit an oscillatory dependence on physical observables as a function of field strength at low temperature. Generally known as "quantum magnetic oscillations", these effects could be observed for example, for the atomic analog of the magnetization (de Haas-van Alphen oscillations) [35,36], the resistivity (Shubnikov-de Haas oscillations) [37], the Hall resistance [38], or the specific heat [39].…”
Section: Landau Levels For λ-Type Neutral Atomsmentioning
confidence: 99%
“…When the filling number is of the order of unity, we expect the atomic gas to exhibit an oscillatory dependence on physical observables as a function of field strength at low temperature. Generally known as "quantum magnetic oscillations", these effects could be observed for example, for the atomic analog of the magnetization (de Haas-van Alphen oscillations) [35,36], the resistivity (Shubnikov-de Haas oscillations) [37], the Hall resistance [38], or the specific heat [39].…”
Section: Landau Levels For λ-Type Neutral Atomsmentioning
confidence: 99%
“…On the other hand, in our system we consider the particles confined in a 2D atomic cloud which implies that the value of r is limited. In this case, we can obtain the analytical solution (12), in the limit of [12,[19][20][21]…”
Section: Landau-aharonov-casher Quantizationmentioning
confidence: 99%
“…In [18], Grenier et al have explored the possibility of observing like-dHvA oscillations for a non-interacting gas of fermionic atoms, either by putting the gas in rotation or by using artificial gauge fields. In another recent work we propose an experimental scheme for the realization of the dHvA effect in a 2D ultracold atomic cloud which uses the coupling between the internal states of tripod-type atoms and an appropriate spatially varying laser field arrangement [19].…”
Section: Introductionmentioning
confidence: 99%
“…However, the elementary aspects of the artificial magnetism, such as artificial Landau diamagnetism [13] and artificial de Haas-van Alphen effect [14], have not been observed in trapped gas of neutral fermionic atoms [23,24] exposed to an artificial magnetic field. A few such elementary aspects, on the other hand, were theoretically explored for both the 2D Fermi system [25] and the 3D Fermi system [26,27] for low temperatures and weak & strong fields. However, unification of the artificial Landau diamagnetism and the artificial de Haas-van Alphen effect have not been even theoretically achieved for all temperatures and all strengths of the field.…”
Section: Introductionmentioning
confidence: 99%