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Tomonaga-Luttinger liquid theory for one-dimensional attractive Fermi gases
The one-dimensional (1D) Yang-Gaudin model--an integrable $δ$-function interacting Fermi gas, serves as a paradigm in quantum many-body physics, encompassing phenomena from spin-charge separation to the Luther-Emery liquid. However, a consistent description of the Luther-Emery liquid and the Fulde-F
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