2010
DOI: 10.1103/physreva.82.033609
|View full text |Cite
|
Sign up to set email alerts
|

Controlling phase separation of binary Bose-Einstein condensates via mixed-spin-channel Feshbach resonance

Abstract: We investigate controlled phase separation of a binary Bose-Einstein condensate (BEC) in the proximity of mixed-spin-channel Feshbach resonance in the |F = 1, mF = +1 and |F = 2, mF = −1 states of 87 Rb at a magnetic field of 9.10 G. Phase separation occurs on the lower magnetic-field side of the Feshbach resonance while the two components overlap on the higher magnetic-field side. The Feshbach resonance curve of the scattering length is obtained from the shape of the atomic cloud by comparison with the numeri… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
232
0
1

Year Published

2011
2011
2019
2019

Publication Types

Select...
5
5

Relationship

0
10

Authors

Journals

citations
Cited by 213 publications
(233 citation statements)
references
References 40 publications
0
232
0
1
Order By: Relevance
“…Such multicomponent BEC's can be realized when more than one hyperfine spin state is simultaneously populated or when more than one species of atoms are mixed. The s-wave scattering wave-length can be tuned via a Feshbach resonance [3][4][5]. Moreover, recent experimental achievement of a condensate of ytterbium offers condensations up to five components [6].…”
Section: Introductionmentioning
confidence: 99%
“…Such multicomponent BEC's can be realized when more than one hyperfine spin state is simultaneously populated or when more than one species of atoms are mixed. The s-wave scattering wave-length can be tuned via a Feshbach resonance [3][4][5]. Moreover, recent experimental achievement of a condensate of ytterbium offers condensations up to five components [6].…”
Section: Introductionmentioning
confidence: 99%
“…Resonant two-photon combined radio-frequency and microwave radiation coherently couples the two hyperfine states (a 11 , a 22 , a 12 ) = (95.0, 100.4, 97.7) a B [8] leading to a system close to the miscibility-immiscibiliy threshold a 2 12 = a 11 a 22 [16,17]. Utilizing a Feshbach resonance at B = 9.10 G [18,19] we tune a 12 into the miscible (B = 9.17 G, a 12 ≈ 94a B ) and immiscible regime (B = 9.03 G, a 12 ≈ 102a B ) [10]. Three-body recombination and spin relaxation losses in |2 result in a 1/e-lifetime of 310 ms for both magnetic field settings.…”
mentioning
confidence: 99%
“…This method of domain counting can easily be adopted experimentally by performing absorption imaging of the two components after Stern-Gerlach separation [54,55]. The mean number of formed domains N d versus the quench time τ Q is plotted in Fig.…”
Section: Homogeneous Bose-einstein Condensate In a Ring Trapmentioning
confidence: 99%