2012
DOI: 10.1103/physreva.86.013640
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Quantum kinetic theory model of a continuous atom laser

Abstract: We investigate the feasible limits for realizing a continuously evaporated atom laser with high-temperature sources. A plausible scheme for realizing a truly continuous atom laser is to outcouple atoms from a partially condensed Bose gas while continuously reloading the system with noncondensed thermal atoms and performing evaporative cooling. Here we use quantum kinetic theory to model this system and estimate feasible limits for the operation of such a scheme. For sufficiently high temperatures, the figure o… Show more

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Cited by 4 publications
(6 citation statements)
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“…The total atom number per site N for the condensate plus thermal cloud determined by absorption imaging (Fig. 13(a)) decays with a half-life t 1/2 ∼ 0.9 ± 0.3 s, which is consistent with the three-body decay half-life for a pure condensate, t 1/2 ∼ 0.6 ± 0.2, estimated using N c (t) = N c (0)[1 + αN c (0)t] −5/4 , where α = L 3 (mω/ ) 12/5 14×15 1/5 π 2 a 6/5 s [27], L 3 = (5.8 ± 1.9) × 10 −30 cm 6 s −1 [11], a s = 5.3 nm and ω/2π = 2.40 kHz. The above half-life, t 1/2 ∼ 0.9 ± 0.3 s, is also similar (within about 10%) to the three-body decay half-life for an ultracold thermal cloud in which the six-times larger L 3 coefficient [11] is approximately compensated by the much smaller peak atom density for the thermal cloud (Fig.…”
Section: Rf Spectra For Various Holding Timessupporting
confidence: 86%
“…The total atom number per site N for the condensate plus thermal cloud determined by absorption imaging (Fig. 13(a)) decays with a half-life t 1/2 ∼ 0.9 ± 0.3 s, which is consistent with the three-body decay half-life for a pure condensate, t 1/2 ∼ 0.6 ± 0.2, estimated using N c (t) = N c (0)[1 + αN c (0)t] −5/4 , where α = L 3 (mω/ ) 12/5 14×15 1/5 π 2 a 6/5 s [27], L 3 = (5.8 ± 1.9) × 10 −30 cm 6 s −1 [11], a s = 5.3 nm and ω/2π = 2.40 kHz. The above half-life, t 1/2 ∼ 0.9 ± 0.3 s, is also similar (within about 10%) to the three-body decay half-life for an ultracold thermal cloud in which the six-times larger L 3 coefficient [11] is approximately compensated by the much smaller peak atom density for the thermal cloud (Fig.…”
Section: Rf Spectra For Various Holding Timessupporting
confidence: 86%
“…A tantalizing prospect is to add an output coupler to extract a propagating matter-wave. This could be implemented by coherently transferring atoms to an untrapped state and would bring the long-sought CW atom laser finally within reach 15 , 45 . This prospect is especially compelling because our CW BEC is made of strontium, the element used in some of today’s best clocks 56 and the element of choice for future cutting-edge atom interferometers 20 24 , 57 , 58 .…”
Section: Discussionmentioning
confidence: 99%
“…The corresponding phase-space flux is (ref. 45 ), in which ħ is the reduced Planck constant, k B the Boltzmann constant and ω R i /2π are the reservoir trap frequencies.…”
Section: Methodsmentioning
confidence: 99%
“…We expect this is a reasonable approximation in steady state if we imagine that we can replenish thermal atoms at a constant rate while undergoing continuous cooling, e.g. [19,22]. The stationary incoherent region thus continuously replenishes the coherent region through Bose-stimulated collisions.…”
Section: Model Of a Continuously Pumped Atom Lasermentioning
confidence: 95%
“…Many theoretical proposals for continuously-pumped operation have been made, using either evaporative cooling [20][21][22] or spontaneous emission [23][24][25], A number of studies have already considered the properties of a CW atom laser at zero temperature [26][27][28][29][30][31][32][33][34][35][36]. However, one of the most likely experimental routes to a true CW atom laser will involve replenishing the BEC via cooling from a reservoir containing thermal atoms so that the condensate mode is maintained in a steady state via Bose-stimulated collisions, similar to the experiment of Stellmer et al [19].…”
Section: Introductionmentioning
confidence: 99%