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Homework 3



1) By working out explicitely the components of the hadronic tensor in the parton model:


\begin{displaymath}W_{\mu\nu}(P,q) = \sum_{i} \int d^4 k f_i(k,P) w_{\mu\nu}(q,k)
\delta \left( (k+q)^2 \right), \end{displaymath}

with


\begin{displaymath}w_{\mu\nu} = 2 k_\mu k_\nu + k_\mu q_\nu + q_\mu k_\nu - g_{\mu\nu} (kq) \end{displaymath}

,

we showed in class that the dimensionless structure function, $F_1$, can be written as:


\begin{displaymath}F_1(x) = \sum_i e_i^2 \left[ \frac{pi}{2} \int d^2 k_T f_i(k,P) \right] \end{displaymath}

.

Derive using a similar procedure an expression for the structure function $F_2$.

2) Within the Infinite Momentum Frame discussed in class, derive an expression for the constant $C$ in the cross section:


\begin{displaymath}d\sigma (\gamma^* k \rightarrow k^\prime) = C(x,Q^2) \delta(\xi-x), \end{displaymath}

where $\xi=k/P$, $k$ being the initial struck quark's momentum, $k^\prime$ being the quark's final momentum, $P$ being the proton's momentum, and $q$ the virtual photon momentum ($Q^2=-q^2$).





Simonetta Liuti 2005-02-12