Difference between revisions of "MainPage:Nuclear:ChargeDistribution"
Jump to navigation
Jump to search
Line 1: | Line 1: | ||
__NOTOC__ | __NOTOC__ | ||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
{|border="1" cellpadding="2" cellspacing="0" style="background-color:lightgray" | {|border="1" cellpadding="2" cellspacing="0" style="background-color:lightgray" | ||
Line 13: | Line 7: | ||
<br> | <br> | ||
− | == Charge Distribution of Hadrons == | + | == Transverse Charge Distribution of Hadrons == |
This work is done by the Nuclear Physics Group at the CUA, together with [http://www.phys.washington.edu/~miller/ Dr. Gerald A. Miller], from the University of Washington. | This work is done by the Nuclear Physics Group at the CUA, together with [http://www.phys.washington.edu/~miller/ Dr. Gerald A. Miller], from the University of Washington. | ||
− | + | According to [http://arxiv.org/abs/1010.3629 Siddharth Venkat, 2010], having the form factor F(Q^2) of a particle it is possible to simplify the calculation of its two-dimensional transverse density using the finite radius approximation. | |
+ | |||
+ | In this work we are going to calculate the | ||
+ | |||
+ | <math> | ||
+ | \frac{1}{2} | ||
+ | </math> |
Revision as of 09:02, 31 July 2012
⇐ Back to the Main_Page |
Transverse Charge Distribution of Hadrons
This work is done by the Nuclear Physics Group at the CUA, together with Dr. Gerald A. Miller, from the University of Washington.
According to Siddharth Venkat, 2010, having the form factor F(Q^2) of a particle it is possible to simplify the calculation of its two-dimensional transverse density using the finite radius approximation.
In this work we are going to calculate the
<math> \frac{1}{2} </math>