Difference between revisions of "Limit of Energy in Lab Frame"
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<center><math>t \equiv \left({\mathbf P_1^*}- {\mathbf P_1^{'*}}\right)^2=\left({\mathbf P_2^{*}}- {\mathbf P_2^{'*}}\right)^2</math></center> | <center><math>t \equiv \left({\mathbf P_1^*}- {\mathbf P_1^{'*}}\right)^2=\left({\mathbf P_2^{*}}- {\mathbf P_2^{'*}}\right)^2</math></center> | ||
− | + | =In the CM Frame= | |
<center><math>{\mathbf P_1^{*}}=-{\mathbf P_2^{*}}</math></center> | <center><math>{\mathbf P_1^{*}}=-{\mathbf P_2^{*}}</math></center> | ||
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− | + | =In the Lab Frame= | |
<center><math>t={\mathbf P_1^{2}}+ {\mathbf P_1^{'2}}-2 {\mathbf P_1} {\mathbf P_1^{'}}</math></center> | <center><math>t={\mathbf P_1^{2}}+ {\mathbf P_1^{'2}}-2 {\mathbf P_1} {\mathbf P_1^{'}}</math></center> | ||
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− | <center><math>=2m^2-2E_1E_1^'+2 p_1 p_1^'=2m^2-2E_2E_2^'+2 p_2 p_2^'</math></center> | + | <center><math>t=2m^2-2E_1E_1^{'}+2 \vec p_1 \vec p_1^{'}=2m^2-2E_2E_2^{'}+2 p_2^ p_2^{'}</math></center> |
+ | |||
Revision as of 15:42, 15 March 2018
The t quantity is known as the square of the 4-momentum transfer
In the CM Frame
where and is the angle between the before and after momentum in the CM frame
Using the relativistic relation this reduces to
The maximum momentum is transfered at 90 degrees, i.e.
This can be rewritten again using the relativistic energy relation
In the Lab Frame
with
and