Position Space Interpretation for Generalized Parton Distributions
Position Space Interpretation for Generalized Parton Distributions
Position Space Interpretation for Generalized Parton Distributions
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(brief) Motivation<br />
generalization to p ′ ≠ p ⇒ <strong>Generalized</strong> <strong>Parton</strong> <strong>Distributions</strong><br />
GPD(x, ξ, t) ≡<br />
∫ dx<br />
−<br />
2π 〈p′ |q<br />
( ) ( )<br />
− x− x<br />
2 ,0 ⊥ γ + −<br />
q<br />
2 ,0 ⊥ |p〉 e ix− xP +<br />
with ∆ = p − p ′ , t = ∆ 2 , and ξ(p + + p +′ ) = −2∆ + .<br />
can be probed e.g. in Deeply Virtual Compton Scattering<br />
(DVCS) (HERMES, JLab@12GeV, eRHIC, ...)<br />
Interesting observation: X.Ji, PRL78,610(1997)<br />
〈J q 〉 = 1 2<br />
∫ 1<br />
0<br />
dxx[H q (x, 0, 0) + E q (x, 0, 0)]<br />
DVCS ⇔ GPDs ⇔ ⃗J q<br />
But: what other “physical in<strong>for</strong>mation” about the nucleon can<br />
we obtain by measuring/calculating GPDs<br />
<strong>Position</strong> <strong>Space</strong> <strong>Interpretation</strong> <strong>for</strong> <strong>Generalized</strong> <strong>Parton</strong> <strong>Distributions</strong> – p.3/55