Difference between revisions of "Determining Momentum Components After Collision in CM Frame"
Jump to navigation
Jump to search
| Line 23: | Line 23: | ||
<center><math>\textbf{\underline{Navigation}}</math> | <center><math>\textbf{\underline{Navigation}}</math> | ||
| − | [[ | + | [[Phase_space_Limiting_Particles|<math>\vartriangleleft </math>]] |
| − | [[VanWasshenova_Thesis# | + | [[VanWasshenova_Thesis#Weighted_Isotropic_Distribution_in_Lab_Frame|<math>\triangle </math>]] |
| − | [[ | + | [[Theta_Dependent_Components|<math>\vartriangleright </math>]] |
</center> | </center> | ||
Latest revision as of 14:59, 30 May 2017
4.1.3 Determining Momentum Components After Collision in CM Frame
The energy and total momentum of the Moller and scattered electron remain the same under a rotation in any frame of reference. After the collision, these quantities remain the same, but the x, y, z components change.
In this frame, we can cycle through values of theta from 90 to 180 degrees which physically correspond to a stationary electron being impinged by an electron.