Limits based on Mandelstam Variables

$\textbf{\underline{Navigation}}$

$\vartriangleleft$ $\triangle$ $\vartriangleright$

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:

$s+t+u=(4(m^2+ p \ ^{*2}))+(-2 p \ ^{*2}(1-cos\ \theta))+(-2 p \ ^{*2}(1+cos\ \theta))$

$s+t+u \equiv 4m^2$

Since

$s \equiv 4(m^2+\vec p \ ^{*2})$

This implies

$s \ge 4m^2$

In turn, this implies

$t \le 0 \qquad u \le 0$

At the condition both t and u are equal to zero, we find

$t = 0 \qquad u = 0$

$-2 p \ ^{*2}(1-cos\ \theta) = 0 \qquad -2 p \ ^{*2}(1+cos\ \theta) = 0$

$(-2 p \ ^{*2}+2 p \ ^{*2}cos\ \theta) = 0 \qquad (-2 p \ ^{*2}-2 p \ ^{*2}cos\ \theta) = 0$

$2 p \ ^{*2}cos\ \theta = 2 p \ ^{*2} \qquad -2 p \ ^{*2}cos\ \theta = 2 p \ ^{*2}$

$cos\ \theta = 1 \qquad cos\ \theta = -1$

$|Rightarrow \theta_{t=0} = arccos \ 1=0^{\circ} \qquad \theta_{u=0} = arccos \ -1=180^{\circ}$