L - Florence Theory Group - Infn

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Ω = α∆ 2 + β 2 ∆ 4 + γ 3 ∆ 6 + ⋅⋅⋅ (for regular crystalline structures all the ∆q are equal) The coefficients can be determined microscopically for the different structures (Bowers ( Bowers and Rajagopal (2002)) (2002)
Gap equation Propagator expansion Insert in the gap equation
Page 1 and 2: QCD@Work 2003 International Worksho
Page 3: Introduction mu, , md , ms s
Page 6 and 7: Relevant scales in CS δ (cutoff)
Page 8 and 9: Physics near the Fermi surface (see
Page 10 and 11: S = S E −1 = Dispersion relation
Page 12 and 13: For T T 0 1 G 2 At weak coupling d
Page 14 and 15: The inhomogeneous phase (LOFF) In m
Page 16 and 17: 2 2 comm comm ∆Ω ≈ 2∑ µ (
Page 18 and 19: µ ≠ µ or paramagnetic impuritie
Page 20 and 21: Simple plane wave: energy shift r r
Page 24 and 25: We get the equation α∆ + β∆ 3
Page 26 and 27: Results of Leibovich, Rajagopal &
Page 28 and 29: General analysis (Bowers Bowers and
Page 30 and 31: L phonon 2 2 2 ⎡1 ⎛ ∂ φ ∂
Page 32 and 33: Using the symmetry group of the cub
Page 34 and 35: LOFF phase in CSO Why the interest
Page 36 and 37: ρ n.m. .m.is is the saturation nuc
Page 38: Outlook Theoretical problems: prob

L - Florence Theory Group - Infn

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