DVCS at 6/12 GeV, and ideas for the EIC
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 />
Hall A E03-106<br />
<strong>DVCS</strong> on <strong>the</strong> neutron: experiment E03-106 <strong>at</strong> JLab<br />
I exp<br />
)<br />
n<br />
Im(C<br />
3<br />
2<br />
1<br />
0<br />
-1<br />
-2<br />
-3<br />
-4<br />
LD 2 target (F2 n(t) ≫ F 1 n(t) !) J u=-0.4<br />
J d=-0.6<br />
J u=0.3<br />
J d=0.2<br />
J u=0.6<br />
J d=0.8<br />
2<br />
t (<strong>GeV</strong> )<br />
σ → − σ ← = Γ(A sin ϕ + . . . )<br />
-0.5 -0.45 -0.4 -0.35 -0.3 -0.25 -0.2 -0.15 -0.1<br />
Charged particle veto<br />
in front of scintill<strong>at</strong>or array<br />
A = F 1 (t)H +<br />
Carlos Muñoz Camacho<br />
x B<br />
[F 1 (t) + F 2 (t)]<br />
2 − x ˜H t<br />
−<br />
B 4M 2 · F 2(t) · E<br />
} {{ }<br />
Main contribution <strong>for</strong> neutron<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> 14