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PIONS in DIS Bogdan Povh Max-Planck-Institut fuer Kernphysik
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Pion signature in experiment: Gottfried Sum rule Polarized structure function Forward neutrons in DIS
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DIS on Proton and Deuteron
Gottfried sum rule Spin structure function
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Pion signature NMC detector at CERN
Deep inelastic scattering of muons off protons and deuterons
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Pion signature Gottfried sum rule for flavour symmetric sea
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Pion signature
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SU(2) chiral model Eichten, Hinchliffe, Quigg Phys.Rev.D 45 1992
Baumgaertner, Pirner, Koenigsmann, P. ZP A Pirner Prog. Part. Nucl. Phys
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Pion signature SU(2) chiral model:pion is a short cut for the quark-antiquark pair of the constituent quark From GSR
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Spin Structure function
“Theoretical predictions using SU(3) Flavor model”:(Cabibbo, Nucl.Phys.B69,1974) F+D=g_A, F-D=-0.34 and the experiment disagree:1/3 of the prediction New value: quark carries 1/3 of the spin of the constituent quark
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SU(2) chiral model from g_A
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Pion signature SU(2) chiral model
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Forward Neutron Calorimeters at H1 and ZEUS at DESY
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FNC – design specifications
The size and weight of FNC is defined by the space available in HERA tunnel position– 105m from the interaction point, size ~ 70 x 70 x 200cm3 , weight <10t geometrical acceptance is limited by beam-line elements <0.8mrad should work in high radiation environment A.Bunyatyan “Physics with FNC”
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Pion signature H1 detector at HERA collider
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A.Bunyatyan “Physics with FNC”
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Neutron and photon energy spectrum measured in H1
-cluster in Preshower = photon, -cluster in main calorimeter and/or Preshower = neutron A.Bunyatyan “Physics with FNC”
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Different pion fluxes used in analysis (different form factors)
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Pion signature Estimation of the probability of the p→n+p+ in DIS from the neutron rate in DIS extrapolating to the full energy range (for 2 different pion fluxes} (Bunyatyan, Povh, EPJ A27,2006), Absorption (D’Alesio&Pirner EPJ A7 2000)
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Only one U quark contribute
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The spin-flavor function symmetric
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Conclusions
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In the first order the nucleon is composed of three quarks and one
quark-antiquark pair. One quarter of the quark-antiquark pair shows up as a pion of the nucleon
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Conclusions The constituent quarks are a superposition of the massive quarks and pions
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Spontaneous breaking of the chiral symmetry and fossil pions
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Microscopic view of the chiral symmetry breaking
Conclusions Microscopic view of the chiral symmetry breaking d u The interaction that is responsible for giving the mass to quarks binds quark-antiquark to a pion
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Chiral symmetry breaking
Peak of valence quarks
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Chiral symmetry breaking
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Chiral symmetry breaking
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Chiral symmetry breaking
Nambu-Jona-Lasinio Model
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Chiral symmetry breaking
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Nambu-Jona-Lasinio Model in Cartoons
Chiral symmetry breaking Nambu-Jona-Lasinio Model in Cartoons
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