2011
DOI: 10.1103/physreva.83.052111
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Atomic states in optical traps near a planar surface

Abstract: In this work we discuss the atomic states in a vertical optical lattice in proximity of a surface. We study the modifications to the ordinary Wannier-Stark states in presence of a surface and we characterize the energy shifts produced by the Casimir-Polder interaction between atom and mirror. In this context, we introduce an effective model describing the finite size of the atom in order to regularize the energy corrections. In addition, the modifications to the energy levels due to a hypothetical non-Newtonia… Show more

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Cited by 11 publications
(15 citation statements)
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“…As we have shown in a recent paper [5], these energy levels can be strongly modified by the proximity of a surface. This arises from the intrinsic modification of atomic wave functions due to the presence of a boundary condition and to the interaction between the atoms and the quantized electromagnetic field, known as Casimir-Polder interaction [6,7], in the presence of the surface.…”
Section: Introductionmentioning
confidence: 55%
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“…As we have shown in a recent paper [5], these energy levels can be strongly modified by the proximity of a surface. This arises from the intrinsic modification of atomic wave functions due to the presence of a boundary condition and to the interaction between the atoms and the quantized electromagnetic field, known as Casimir-Polder interaction [6,7], in the presence of the surface.…”
Section: Introductionmentioning
confidence: 55%
“…[5], the resolution of the time-independent Schrödinger equation for H 0 leads to a class of states similar to the well-known Wannier-Stark states [10], with a modification due to the presence of the surface. These states, noted with ϕ m (z) (where m = 1,2, .…”
Section: Physical Systemmentioning
confidence: 94%
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“…The spread of the atomic wave function |W m depends on the lattice depth [43]. In the case of a shallow depth (U 0 < 5E r , where E r is the recoil energy defined by E r /h =hk 2 l /2m a = 2π × 8 kHz), the wave function can extend across a significant number of wells [43,44].…”
Section: Theoretical Simulationmentioning
confidence: 99%