Difference between revisions of "Limits based on Mandelstam Variables"
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<center><math>\Rightarrow \theta_{t=0} = \arccos \ 1=0^{\circ} \qquad \theta_{u=0} = \arccos \ -1=180^{\circ}</math></center> | <center><math>\Rightarrow \theta_{t=0} = \arccos \ 1=0^{\circ} \qquad \theta_{u=0} = \arccos \ -1=180^{\circ}</math></center> | ||
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+ | Holding u constant at zero we can find the maximum of t | ||
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+ | <center><math>s+t=4m^2</math></center> | ||
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+ | <center><math>t=4m^2-s</math></center> | ||
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+ | <center><math>t=4m^2-4m^2+ 4p \ ^{*2})</math></center> | ||
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+ | <center><math>t=4p \ ^{*2}</math></center> | ||
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+ | <center><math>-2 p \ ^{*2}(1-cos\ \theta)=4p \ ^{*2}</math></center> | ||
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+ | <center><math>(1-cos\ \theta)=-2p \ ^{*2}</math></center> |
Revision as of 00:05, 10 June 2017
Limits based on Mandelstam Variables
Since the Mandelstam variables are the scalar product of 4-momenta, which are invariants, they are invariants as well. The sum of these invariant variables must also be invariant as well. Find the sum of the 3 Mandelstam variables when the two particles have equal mass in the center of mass frame gives:
Since
This implies
In turn, this implies
At the condition both t and u are equal to zero, we find
Holding u constant at zero we can find the maximum of t