Limits based on Mandelstam Variables

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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(m2+p 2))+(2p 2(1cos θ))+(2p 2(1+cos θ))


s+t+u4m2


Since

s4(m2+p 2)


This implies

s4m2


In turn, this implies


t0u0


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


t=0u=0


2p 2(1cos θ)=02p 2(1+cos θ)=0


(2p 2+2p 2cos θ)=0(2p 22p 2cos θ)=0


2p 2cos θ=2p 22p 2cos θ=2p 2


cos θ=1cos θ=1


θt=0=arccos 1=0θu=0=arccos 1=180

Holding u constant at zero we can find the maximum of t


s+t4m2


t=4m2s


t=4m24m2+4p 2)


t=4p 2


2p 2(1cos θ)=4p 2


(1cos θ)=2


cos θ=3


θmaxarccos3


The domain of the arccos function is from −1 to +1 inclusive and the range is from 0 to π radians inclusive (or from 0° to 180°). This implies for arccos 3, the range will include imaginary numbers. Knowing that the range of the cosine function is -1 to +1 inclusive and the domain to be any angle


z=arccos3


cosz=cosarccos3


cosz=3


From Euler's formula


cosx=eiz+eiz2


eiz+eiz2=3


eiz+eiz=6


Multiply with eiz


e2iz+1=6eiz


Letting y=eiz


We get an quadratic equation:


y26y+1=0


y=(6±32)/2


y1=5.828427=eiz


y2=0.171573=eiz


Apply the natural log on both sides gives the solution for arccos 3:


z1=ln(5.828427)i=1.76275i


z2=ln(0.171573)i=1.76275i