Zhou Feng1, 2, Li Xiao1, 2, Ke Min2, 3, †, Wang Jin2, 3, Zhan Ming-Sheng1, 2, 3, ‡
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(color online) Potential distribution for 87Rb in the hyperfine states and . (a) Identical double-well potential created by static and fictitious magnetic fields: . (b) For hyperfine state , the MW repulsive potential increases the separation between the double-well OFMTs: . (c) For hyperfine state , the MW attractive potential merges the two OFMTs: .
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