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Meson production in proton-proton scattering within an eLSM. Khaled Teilab in collaboration with Susanna Gallas , Francesco Giacosa and Dirk H. Rischke. Outline. The eLSM in the baryonic sector Results pion-nucleon scattering length w production near threshold Summary Outlook.
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Meson production in proton-proton scattering within an eLSM Khaled Teilab in collaboration with Susanna Gallas, Francesco Giacosa and Dirk H. Rischke
Outline • The eLSM in the baryonic sector • Results • pion-nucleon scattering length • w production near threshold • Summary • Outlook
The eLSM in the baryonic sector for Nf =2 • The nucleon and its chiral partner • (pseudo-) scalar & (axial-) vector mesons • Chiral symmetry and dilatation invariance • mirror assignment • chirally symmetric mass term C. De Tar and T. Kunihiro, PRD 39 (1989) 2805)
The eLSM in the baryonic sector for Nf =2 Interaction of baryons with (pseudo-) scalar and (axial-) vector mesons Details in S. Gallas et al. Phys.Rev. D82 (2010) 014004
The mass of the nucleon parameterizes the contribution which does not stem from the quark condensate Details in S. Gallas, Francesco Giacosa and Dirk H. Rischke, Phys.Rev. D82 (2010) 014004
pion-nucleon scattering length large theoretical uncertainty due to the scalar-isoscalar sector Mirror assignment and vector mesons are important to obtain this agreement
Baryonic Lagrangian with physical fields NO RESONANCE
pp→ppw near threshold no resonance References for data points in: F. Balestra et al. Phys. Rev. C, Vol. 63, 024004
pp→ppw near threshold no resonance N(1535) N(1650)
pp→ppw near threshold mw=774 MeV mw=778 MeV mw=782 MeV mw=786 MeV mw=791 MeV NO RESONANCE
Summary • A chirally symmetric Lagrangian was developed with baryons and vector mesons • Only 5 more parameters in the baryonic sector • pion-nucleon scattering length in agreement with experiment • Good description of w production near threshold • Outlook …
pp→ppw away from threshold no resonance N(1535) N(1650)
pp→ppw away from threshold no resonance
pp→pph no resonance References for data points in: F. Balestra et al. Phys. Rev. C, Vol. 69, 064003
r & p mesons pp→ppr pp→ppp no resonance no resonance
Lagrangian in the baryon sector Interaction of baryons with (pseudo)scalar and (axial-)vector mesons
The eLSM with Nf =2 spontaneous breaking of chiral symmertry non-physical mixing terms appear Solution: shift of the axial vectors as: renormalize the pseudoscalars as:
pp→ppw near threshold Dependence on the resonance mass N(1535) N(1650) same parameters for both curves
pp→ppw near threshold Dependence on the parameters c1 and c2 c1=-3.0 c2=11 c1=-4.0 c2=13 c1=-5.0 c2=15 c2 fixed at 13 c1 fixed at -3.0 Large sensitivity to the parameters c1 and c2
Mass of the nucleon Details in S. Gallas, F. G., D. H. Rischke, Phys.Rev. D82 (2010) 014004, arXiv:0907.5084 parameterizes the contribution which does not stem from the quark condensate Crucial also at nonzero temperature and density also in the so-called quarkyonic phase: L. McLerran, R. Pisarski Nucl.Phys.A796:83-100,2007