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DVCS at 6/12 GeV, and ideas for the EIC

DVCS at 6/12 GeV, and ideas for the EIC

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Introduction Initial results Dedic<strong>at</strong>ed experiments Future 6 <strong>GeV</strong> <strong>12</strong> <strong>GeV</strong> <strong>EIC</strong> Conclusion<br />

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Hall B E1-<strong>DVCS</strong><br />

BSA in a large kinem<strong>at</strong>ic domain (Hall B)<br />

0.3 0.10 < x < 0.15<br />

B<br />

)<br />

2<br />

(<strong>GeV</strong><br />

2<br />

α(t)<br />

0.2<br />

0.1<br />

Q<br />

0<br />

4<br />

0 0.5 1 1.5 2<br />

|t| (<strong>GeV</strong> )<br />

3<br />

A =<br />

→<br />

σ −<br />

←<br />

σ<br />

→<br />

σ +<br />

←<br />

σ<br />

≈<br />

α sin φ<br />

1 + β cos φ<br />

2<br />

Simple models do not<br />

reproduce <strong>the</strong> d<strong>at</strong>a<br />

1<br />

0.1 0.2 0.3 0.4 0.5<br />

x B<br />

Carlos Muñoz Camacho<br />

Analysis of cross sections underway<br />

LPC Clermont-Ferr<strong>and</strong>, CNRS/IN2P3<br />

<strong>DVCS</strong> <strong>at</strong> 6/<strong>12</strong> <strong>GeV</strong> <strong>and</strong> <strong>ideas</strong> <strong>for</strong> <strong>EIC</strong> 15

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