Propagation of Hadrons Through the Nuclear Medium

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First direct search for color transparency Transparency in A(p,2p) Reaction from BNL PRL 87, 212301 (2001) PRL 81, 5085 (1998) PRL 61, 1698 (1988) Solid line is fit to 1/oscillation in p-p scattering data Shaded band Glauber calculation Results inconsistent with CT only. But can be explained by including additional mechanisms such as nuclear filtering or charm resonance states.
Current Status of CT (Search for the onset of CT ) A(e,e'p) results Q 2 dependence consistent with standard nuclear physics calculations Solid Pts – JLab Open Pts -- other Constant value fit for Q 2 > 2 (GeV/c) 2 has χ 2 / df ~ 1 (‏‎1994‎‏)‏ N. C. R. Makins et al. PRL 72, 1986 (‏‎1992‎‏)‏ G. Garino et al. PRC 45, 780 (‏‎1998‎‏)‏ D. Abbott et al. PRL 80, 5072 (‏‎2002‎‏)‏ K. Garrow et al. PRC 66, 044613
Page 1 and 2: Hadron Propagation Through The Nucl
Page 3 and 4: Introduction We know QCD works, but
Page 5 and 6: How Transparent is Your Nucleus? Ra
Page 7 and 8: Nuclear Transparency Traditional nu
Page 9 and 10: Color Transparency:a color coherenc
Page 11: CT & Factorization Factorization th
Page 15 and 16: qqq vs qq systems There is no unam
Page 17 and 18: Pion Transparency: Q 2 Dependence 1
Page 19 and 20: Pion Transparency: 'A’ Dependence
Page 21 and 22: JLab Experiments conclusively find
Page 23 and 24: Kaon Transparency: Q 2 Dependence p
Page 25 and 26: Hadron Propagation in Nuclear Mediu
Page 27 and 28: Hadron Propagation in Nuclear Mediu
Page 29 and 30: Summary • These 11 GeV experiment
Page 36 and 37: Kaskulov, Galmiester & Mosel, PRC 7
Page 38 and 39: Need Both Electro and Photo Pions F
Page 40 and 41: Connecting GPDs & CT Connections be
Page 42: Introduction We know QCD works, but

Propagation of Hadrons Through the Nuclear Medium

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