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tions of the normal modes. 2. Quarks at MF + Mesons at RPA in NJL considering all possible channels in the bubble summation 0000 0 0 0 00 ,01 2 ( ) 2 ( ) 2 ( ) 2 ( )2 ( ) 1 2 ( ) 2 ( ) 2 ( )de t2 ( ) 2 ( ) 1 2 ( ) 2 ( )2 ( ) 2 ( ) 2 ( ) 1 2 ( )mk M kG k G k G k G kG k G k G k G kG k G k G k G kG k G k G k G k? ? ? ? ? ? ? ?? ? ? ? ? ? ? ?? ? ? ? ? ? ? ?? ? ? ? ? ? ? ???? ? ? ? ? ?? ? ? ? ? ??? ??? ? ? ? ? ? ? ?????? ? ? ? ? ? ? ??? ? ? ? ? ? ? ?? ? ? ? ? ? ? ???0,? ? ???mM,? ? ???MqqgDHENP 20220701 ATHIC, 2022, Seoul 5 3. Homogeneous and Inhomogeneous Pion Superfluid IB??? chiral and pion condensates at in NJL parison with Linear Sigma Model and Chiral Perturbation Theory analytic result: critical isospin chemical potential for pion superfluidity is exactly the pion mass in the vacuum: 0BTq?? ? ?cI m?? ?()BBn?I? pion superfluidity phase diagram in plane at T=0 : average Fermi surface : surface mismatch homogeneous (Sarma, ) and inhomogeneous pion superfluid (