1963
DOI: 10.1016/0003-4916(63)90066-6
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Binary mixtures of dilute bose gases with repulsive interactions at low temperature

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Cited by 75 publications
(61 citation statements)
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“…where n 0 = n ↑ + n ↓ and E kin , E trap , E MF and E LHY denote the kinetic, potential, mean-field and quantum fluctuation (Lee-Huang-Yang) contributions to the energy density of the mixture, respectively. Furthermore, V trap = 1 2 mω 2 r 2 corresponds to the harmonic confinement of the optical waveguide and f (x, y) = ± 1 + y ± (1 − y) 2 + 4xy 5/2 /4 √ 2 [42]. This en-ergy functional results in the extended Gross-Pitaevskii equation given in the main text…”
Section: B Theoretical Analysismentioning
confidence: 90%
“…where n 0 = n ↑ + n ↓ and E kin , E trap , E MF and E LHY denote the kinetic, potential, mean-field and quantum fluctuation (Lee-Huang-Yang) contributions to the energy density of the mixture, respectively. Furthermore, V trap = 1 2 mω 2 r 2 corresponds to the harmonic confinement of the optical waveguide and f (x, y) = ± 1 + y ± (1 − y) 2 + 4xy 5/2 /4 √ 2 [42]. This en-ergy functional results in the extended Gross-Pitaevskii equation given in the main text…”
Section: B Theoretical Analysismentioning
confidence: 90%
“…The leading correction to the MF energy for identical bosons with hard-sphere interactions was later obtained by Lee-Huang-Yang (LHY) [2] in the homogeneous case. These results were then extended to the case of twocomponent bosons by D. Larsen [3].…”
Section: Introductionmentioning
confidence: 91%
“…After summarizing known results to set the notation, we review the analytic LHY energy known for the special case of a mixture with largely imbalanced densities, with the majority component being the lighter species, i.e. the case of heavy impurities [3]. Then, we propose our approximated formula for the LHY energy and we show its limits of applicability by comparing it with the exact numerical results of the LHY integral.…”
Section: Introductionmentioning
confidence: 99%
“…The validity condition for this approximation is simply na 3 ≪ 1 (here and after for qualitative estimates we omit subscripts assuming that the masses are of the same order of magnitude, m 1 ∼ m 2 ∼ m, and the same holds for the densities, n 1 ∼ n 2 ∼ n, and scattering lengths, a 11 ∼ a 22 ∼ |a 12 | ∼ a). The equations of motion δL/δΨ ′ * i = 0 and δL/δΨ ′ i = 0 give two Bogoliubov excitation branches [14,15] …”
mentioning
confidence: 99%