Difference between revisions of "Total Energy in CM Frame"
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where
is the angle between the particles in the Lab frame.
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where <math>E_{1}=\sqrt{p_{1}^2+m^2}\approx 11000 MeV</math> | where <math>E_{1}=\sqrt{p_{1}^2+m^2}\approx 11000 MeV</math> | ||
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+ | ---- | ||
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+ | <center><math>\textbf{\underline{Navigation}}</math> | ||
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+ | [[Special_Case_of_Equal_Mass_Particles|<math>\vartriangleleft </math>]] | ||
+ | [[VanWasshenova_Thesis#Initial_4-momentum_Components|<math>\triangle </math>]] | ||
+ | [[Scattered_and_Moller_Electron_Energies_in_CM_Frame|<math>\vartriangleright </math>]] | ||
+ | |||
+ | </center> |
Revision as of 01:08, 16 June 2017
Total Energy in CM Frame
Setting the lengths of the 4-momenta equal to each other,
we can use this for the collision of two particles of mass m. Since the total momentum is zero in the Center of Mass frame, we can express total energy in the center of mass frame as
Using the relations
In the frame where one particle (p2) is at rest
which implies,
where