2014
DOI: 10.1007/s10946-014-9409-4
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Dynamics of Bec Mixtures Loaded into the Optical Lattice in the Presence of Linear Inter-Component Coupling

Abstract: We consider dynamics of a two-component Bose-Einstein condensate where the components correspond to different hyperfine states of the same sort of atoms. External microwave radiation leads to resonant transitions between the states. The condensate is loaded into the optical lattice. We invoke the tightbinding approximation and examine the interplay of spatial and internal dynamics of the mixture. It is shown that internal dynamics qualitatively depends on the intra-component interaction strength and the phase … Show more

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Cited by 5 publications
(18 citation statements)
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References 37 publications
(45 reference statements)
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“…As in Ref. [10], we assume that the interaction between atoms belonging to different hyperfine states is weak and can be neglected, g 12 = g 21 = 0. Indeed, both intra-species and inter-species scattering lengths can be readily tuned in experiments by means of the Feshbach resonance [16,17], that is, one has some freedom in choosing their values.…”
Section: Basic Equationsmentioning
confidence: 99%
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“…As in Ref. [10], we assume that the interaction between atoms belonging to different hyperfine states is weak and can be neglected, g 12 = g 21 = 0. Indeed, both intra-species and inter-species scattering lengths can be readily tuned in experiments by means of the Feshbach resonance [16,17], that is, one has some freedom in choosing their values.…”
Section: Basic Equationsmentioning
confidence: 99%
“…This suggest that such solitons should be well spatially separated (in order to reduce the kinetic energy) and consist of only one species (to reduce the Rabi energy). Results of [10] indicate that solitons of this kind can arise spontaneously, provided wavepacket spreading is weak.…”
Section: Basic Equationsmentioning
confidence: 99%
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“…The case of χ n = 0 (25) corresponds to onset of resonance in Eqs. (15), when c n1 = c n2 = −c n3 = c n4 = 1/2, therefore, α n and β n+l oscillate with frequency Ω/2.…”
Section: Noiseless Case -Analytical Solutionmentioning
confidence: 99%
“…Further we omit the subscript n. From Eq. (29) it is clear that quantityΩ stands for effective Rabi frequency taking into account momentum-dependent detuning from the resonance (25).…”
Section: Phase Space Representation Of Rabi Oscillationsmentioning
confidence: 99%