The inclusive double polarization asymmetries [math]A_N[/math] can be written in terms of polarized [math]\triangle q_v (x)[/math] and unpolarized [math]q_v (x)[/math] valence quark distributions,
[math]A_{1,p}[/math]=[math]\frac{\lt math\gt \triangle u_v (x)[/math] + [math]\triangle d_v (x)[/math]}{[math]4u_v (x)[/math] + [math]d_v (x)[/math]}</math>
[math]A_{1,p}[/math] = [math]4\triangle u_v (x)[/math] + [math]\triangle d_v (x)[/math]
[math]4 u_v (x)[/math] + [math]d_v (x)[/math]
[math]\frac{\lt math\gt 4\triangle u_v (x)[/math] + [math]\triangle d_v (x)[/math]}{[math]4 u_v (x)[/math] + [math]d_v (x)[/math]}</math>