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Robust ground state and artificial gauge in DQW exciton condensates under weak magnetic field

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Fig. 2. The same as Fig. 1 for n  a0. The upper and lower branches: (a) and (d) at B¼0, n x a 2 B ¼ 0:55 and n  ¼ 0; 0:12; 0:36; 0:51 (from top to bottom at k¼0); (b) and (e) at n x ¼1.5 and for n  a 2 B ¼ 0; 0:36; 0:72; 1:44 at B¼0 (from top to bottom
Fig. 3. The critical B-field with their positions k n a B as a function of the dimension- dimension-less exciton concentration n x a 2 B

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