W-D. Nowak - INFN
W-D. Nowak - INFN
W-D. Nowak - INFN
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Wolf-Dieter <strong>Nowak</strong>, Perspectives in Hadronic Physics, May 15, 2008 – p. 3<br />
3-dimensional Picture of the Proton<br />
Nucleon momentum in Infinite Momentum Frame: (p γ<br />
∗ + p nucl ) z → ∞<br />
• Form factor<br />
y<br />
• Parton density<br />
δ z<br />
⊥<br />
xp<br />
y<br />
• Generalized parton<br />
distribution at =0<br />
δ z<br />
⊥<br />
xp<br />
y<br />
b ⊥<br />
z<br />
b ⊥<br />
x<br />
z<br />
x<br />
z<br />
x<br />
f ( x)<br />
f ( x, b )<br />
⊥<br />
ρ( b ⊥<br />
)<br />
0<br />
b ⊥<br />
x<br />
1<br />
0<br />
x<br />
1<br />
0<br />
b ⊥<br />
Nucleon’s transv.<br />
charge distribution<br />
given by 2-dim.<br />
Fourier transform<br />
of Form Factor:<br />
⇒ Parton’s<br />
transverse<br />
localization b ⊥<br />
Probability density to<br />
find partons of given<br />
long. mom. fraction x<br />
at resol. scale 1/Q 2<br />
(no transv. inform.)<br />
⇒ Parton’s longitudinal<br />
momentum distribution<br />
function (PDF) f(x)<br />
Generalized Parton Distrib. s<br />
(GPDs) probe simultaneously<br />
transverse localization b ⊥<br />
for a given longitudinal<br />
momentum fraction x.<br />
2nd moment by Ji relation:<br />
J q,g = 1 2 lim t→0<br />
R<br />
x dx<br />
[H q,g (x, ξ, t) + E q,g (x, ξ, t)]