Changes

Jump to navigation Jump to search
Line 241: Line 241:  
\Gamma_L(m;m_0,\Gamma_0)=\Gamma_0 \frac{m_0}{m} \frac{q}{q_0} \frac{F^2_L(q)}{F^2_L(q_0)}  
 
\Gamma_L(m;m_0,\Gamma_0)=\Gamma_0 \frac{m_0}{m} \frac{q}{q_0} \frac{F^2_L(q)}{F^2_L(q_0)}  
 
</math>
 
</math>
where ''q'' is the breakup momentum of the daughter particles and ''q<sub>0</sub>'' is the same, evaluated at ''m<sub>0</sub>''.
+
where ''q'' is the breakup momentum of the daughter particles in the rest frame of the parent particle, and ''q<sub>0</sub>'' is the same, evaluated at ''m<sub>0</sub>''.
 
:<math>
 
:<math>
 
q(m) = \sqrt{\left(\frac{m^2+m_1^2-m_2^2}{2m}\right)^2-m_1^2}
 
q(m) = \sqrt{\left(\frac{m^2+m_1^2-m_2^2}{2m}\right)^2-m_1^2}
 
</math>
 
</math>
 +
The functions <math>F_L(q)</math> are the angular momentum barrier factors that are given in the literature.  ''The first few of these barrier factors should be listed explicitly here.''
    
===Describing s and t dependence===
 
===Describing s and t dependence===

Navigation menu