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W-D. Nowak - INFN

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Wolf-Dieter <strong>Nowak</strong>, Perspectives in Hadronic Physics, May 15, 2008 – p. 5<br />

DIS: Kinematics, Cross Sections, Asymmetry<br />

e<br />

N<br />

(E, p)<br />

γ *<br />

(E,<br />

’<br />

p ’)<br />

u<br />

q<br />

u<br />

d<br />

h<br />

h<br />

π<br />

Virtual-photon kinematics:<br />

Q 2 = −q 2 ν = E − E ′<br />

Fraction of nucleon momentum<br />

carried by struck quark: x = Q2<br />

2Mν<br />

fraction of virtual-photon energy<br />

carried by produced hadron h: z = E h<br />

ν<br />

π +<br />

Hadron transverse momentum: P h⊥<br />

Unpolarized cross section: σ UU ≡ 1 2 (σ →⇐ + σ →⇒ )<br />

Cross section (helicity) difference: σ LL ≡ 1 2 (σ →⇐ − σ →⇒ )<br />

Double-spin asymmetry: A || ≡ σ LL<br />

σ UU<br />

≃ g 1<br />

F 1<br />

(neglecting small g 2 contribution)<br />

Measured asymmetry: A || =<br />

1<br />

〈P B 〉〈P T 〉<br />

( N L ) → ⇐−( N<br />

L ) → ⇒<br />

( N L ) → ⇐+( N<br />

L ) → ⇒<br />

with P B (P T ) : longitudinal beam (target) polarization

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