Difference between revisions of "Theory"
Jump to navigation
Jump to search
Line 10: | Line 10: | ||
<math>A_{1, p}</math> = <math>\frac {4\triangle u_v (x) + \triangle d_v (x)} {4 u_v (x) + d_v (x)} </math> <br> | <math>A_{1, p}</math> = <math>\frac {4\triangle u_v (x) + \triangle d_v (x)} {4 u_v (x) + d_v (x)} </math> <br> | ||
<math>A_{1, n}</math> = <math>\frac {\triangle u_v (x) + 4\triangle d_v (x)} {u_v (x) + 4d_v (x)} </math> <br> | <math>A_{1, n}</math> = <math>\frac {\triangle u_v (x) + 4\triangle d_v (x)} {u_v (x) + 4d_v (x)} </math> <br> | ||
+ | |||
+ | |||
+ | The semi-inclusive pion electro-production asymmetries can be written in terms of the valence quark distributions <br> |
Revision as of 23:55, 17 July 2007
Inclusive Scattering
W
Semi-Inclusive Scattering
Quark distribution Functions
Unpolarized
Polarized
The inclusive double polarization asymmetries
can be written in terms of polarized and unpolarized valence quark distributions,
=
=
The semi-inclusive pion electro-production asymmetries can be written in terms of the valence quark distributions