2006
DOI: 10.1103/physreva.73.033602
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Elastic scattering losses from colliding Bose-Einstein condensates

Abstract: Bragg diffraction divides a Bose-Einstein condensate into two overlapping components, moving with respect to each other with high momentum. Elastic collisions between atoms from distinct wave packets can significantly deplete the condensate. Recently, Ziń et al. ͓Phys. Rev. Lett. 94, 200401 ͑2005͔͒ introduced a model of two counterpropagating atomic Gaussian wave packets incorporating the dynamics of the incoherent scattering processes. Here we study the properties of this model in detail, including the nature… Show more

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Cited by 32 publications
(50 citation statements)
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“…The search for efficient non-classical atomic sources is therefore both natural and desirable. There have been many proposals concerning atom pairs, especially the production and observation of individual entangled pairs of atoms through atomic collisions or the breakup of diatomic molecules (Band et al, 2000;Deuar and Drummond, 2007;Duan et al, 2000;Kheruntsyan and Drummond, 2002;Naidon and Masnou-Seeuws, 2006;Norrie et al, 2006;Opatrný and Kurizki, 2001;Pu and Meystre, 2000;Savage et al, 2006;Ziń et al, 2006Ziń et al, , 2005. As emphasized in Duan et al (2000), pair production can be studied in two limits.…”
Section: B Four-wave Mixing Of Matter Wavesmentioning
confidence: 99%
“…The search for efficient non-classical atomic sources is therefore both natural and desirable. There have been many proposals concerning atom pairs, especially the production and observation of individual entangled pairs of atoms through atomic collisions or the breakup of diatomic molecules (Band et al, 2000;Deuar and Drummond, 2007;Duan et al, 2000;Kheruntsyan and Drummond, 2002;Naidon and Masnou-Seeuws, 2006;Norrie et al, 2006;Opatrný and Kurizki, 2001;Pu and Meystre, 2000;Savage et al, 2006;Ziń et al, 2006Ziń et al, , 2005. As emphasized in Duan et al (2000), pair production can be studied in two limits.…”
Section: B Four-wave Mixing Of Matter Wavesmentioning
confidence: 99%
“…The Hamiltonian of the system in second quantization reads (see [6,7]) Ĥ ÿ Z d 3 r^ y r; t @ 2 r 2 2m^ r; t g 2 Z d 3 r^ y r; t^ y r; t^ r; t^ r; t; (1) where^ r; t is the bosonic field operator. Atoms interact via two-body contact interaction, determined by the single coupling constant g. As the system consists of two counterpropagating, highly occupied atomic wave packets and a ''sea'' of unoccupied modes, in the spirit of Bogoliubov approximation we decompose the field operator into a c-number condensate wave function Q r; t ÿQ r; t and the quantum field of scattered atomsr; t:…”
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confidence: 99%
“…[7]. We decompose the field operator into basis modes of a spherically symmetric harmonic oscillator [9] r; t X n;l;m R n;l rY lm ; b n;l;m t;…”
mentioning
confidence: 99%
“…An effective Hamiltonian governing the dynamics of the fluctuating component can then be found [36,37],…”
mentioning
confidence: 99%
“…Although it may appear crude, it has proven invaluable in simple analysis of condensate collisions and encapsulates many physical features of the full process. An effective Hamiltonian of the scattering process, in the Bogoliubov approximation, can be written in the form [36,37] H eff = d 3 r δ † (r, t) − 2 2m ∇ 2 δ (r, t) + 2U |ψ(r, t)| 2δ † (r, t)δ(r, t)…”
mentioning
confidence: 99%