2004
DOI: 10.1103/physrevlett.93.080404
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Single-Atom Density of States of an Optical Lattice

Abstract: We consider a single atom in an optical lattice, subject to a harmonic trapping potential. The problem is treated in the tight-binding approximation, with an extra parameter kappa denoting the strength of the harmonic trap. It is shown that the kappa-->0 limit of this problem is singular, in the sense that the density of states for a very shallow trap (kappa-->0) is qualitatively different from that of a translationally invariant lattice (kappa=0). The physics of this difference is discussed, and densities of … Show more

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Cited by 59 publications
(94 citation statements)
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“…In the case of nonvanishing V T the single-particle eigenstates become qualitatively different [205][206][207][208]. They can be separated into two parts and some transient regime between those.…”
Section: Harmonic Trapmentioning
confidence: 98%
“…In the case of nonvanishing V T the single-particle eigenstates become qualitatively different [205][206][207][208]. They can be separated into two parts and some transient regime between those.…”
Section: Harmonic Trapmentioning
confidence: 98%
“…1. The pairs of degenerate states with indices k = 2|j| + 1 and k ′ = 2|j| + 2 are localised around sites j = ±|j| (|j| > j max ) equidistant from the center of the parabolic potential, the corresponding energies being given by E k,k ′ ≈ Ωj 2 [4,5]. For such states, the localization occurs because, for large enough |j|, the transitions |1 j → |1 j±1 effected by the last term of Hamiltonian (1) become non-resonant and the particle tunneling between neighboring lattice sites is suppressed.…”
Section: The Modelmentioning
confidence: 99%
“…Typically this condition is satisfied if the harmonic trapping frequency is small compared to the tunneling rate, ω c ≪ t. Second, we require that the two points in our correlation function, x and y, are separated by a distance much smaller than the size of the cloud. Thus there is an upper limit on the length scale over which we can measure D xy [12]. If D xy decays sufficiently rapidly, then we can completely characterize this function by experiments on a finite cloud.…”
Section: Introductionmentioning
confidence: 99%