Difference between revisions of "Theory"
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− | An asymmetry <math>\triangle R_{np} ^{\pi^+ + \pi^-} = \frac {\triangle\sigma_p^{\pi^+ + \pi^-} - \triangle\sigma_n^{\pi^+ + \pi^-}} {\sigma_p^{\pi^+ + \pi^-} - \sigma_n^{\pi^+ + \pi^-}} </math> | + | An asymmetry <math>\triangle R_{np} ^{\pi^+ + \pi^-} = \frac {\triangle\sigma_p^{\pi^+ + \pi^-} - \triangle\sigma_n^{\pi^+ + \pi^-}} {\sigma_p^{\pi^+ + \pi^-} - \sigma_n^{\pi^+ + \pi^-}} = \frac {g_1^p - g_1^n} {F_1^p - F_1^n} </math> |
Revision as of 18:28, 18 July 2007
Inclusive Scattering
W
Semi-Inclusive Scattering
Quark distribution Functions
describe
and hereUnpolarized
Polarized
The inclusive double polarization asymmetries
can be written in terms of polarized and unpolarized valence quark distributions,
I =
I =
The semi-inclusive pion electro-production asymmetries can be written in terms of the valence quark distributions
=
=
where
where is the measured difference of the yield from oppositely charged pions.
The semi - inclusive asymmetry can be expressed in the following way
where
An asymmetry