<html><head><meta http-equiv="Content-Type" content="text/html charset=iso-8859-1"></head><body style="word-wrap: break-word; -webkit-nbsp-mode: space; -webkit-line-break: after-white-space;"><div>Dear all, <div>you are invited to the special seminars of the winners of the JSA/HUGS Fellowship,</div><div>who are visiting the Theory Center until Saturday.</div><div><br></div><div><br></div><b>JSA/HUGS Fellowships Seminars</b><br>Wed., June 22, 2016<br>2:00 p.m. (coffee at 1:45 p.m.)<br>CEBAF Center, Room L102<br><font color="#0f61c8"><br><br></font><b>Rajesh Sangem</b><br>Indian Institute of Technology <br>Bombay, India<br><font color="#0f61c8"><br></font><b>Linearly Polarized Gluons in J/\psi and \Upsilon
Production</b><br><font color="#0f61c8"><br></font>In this talk, I would discuss the effect of linearly polarized
gluons on transverse momentum and rapidity <br>spectrum of J/psi and Upsilon in unpolarized proton-proton
collision. I will start with a brief introduction<br>to gluon TMDs and quarkonium models. I will show that quarkonium
production spectra can be modulated <br>due to the presence of linearly polarized gluons inside an
unpolarized proton.<br><font color="#0f61c8"><br></font>--------------<br><font color="#0f61c8"><br></font><b>S. Bineta L. Amar</b><br>Cheikh Anta Diop University<br>Dakar, Senegal<br><font color="#0f61c8"><br></font><b>Meson Photo-production in GEANT4 for E_gamma = 0.15 - 3
GeV</b><br>Theoretical models implemented in the version 9.6.p02 of the
Geant4 Monte Carlo simulation toolkit for the <br>total and differential cross sections for pion photo-production
were validated against experimental data.<br>This presentation reports on the gamma p -> pi0
p reaction. Two models were studied: the Chiral Invariant <br>Phase Space (CHIPS) and Bertini (BERT). The experimental data
are from the CEBAF Large Acceptance <br>Spectrometer (CLAS detector) of Jefferson Lab,the Scattering
Analysis Interactive Dial-in (SAID) and the <br>world data (only for sigma_tot). The CHIPS model is the only one
that can adequately reproduce the main <br>resonances for the reaction channel with a
corrective coefficient needed to perform the result.<br><blockquote type="cite">
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