01.01.2015 Views

W-D. Nowak - INFN

W-D. Nowak - INFN

W-D. Nowak - INFN

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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)]

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!