2-body scattering and Mandelstam Variables

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SUMMARY

The discussion focuses on the application of Mandelstam variables in 2-body scattering events, specifically the relationship between the total center of mass (CM) energy and the variable s. The variables are defined as s ≡ −(PA + PB)², t ≡ −(PA − PC)², and u ≡ −(PA − PD)², where PA, PB, PC, and PD represent the 4-momenta of particles A, B, C, and D, respectively. The discussion highlights the importance of the metric signature used in calculations, noting that the common convention among particle physicists is the +--- signature. The participant expresses confusion regarding the negative signs in the definitions of the Mandelstam variables and their implications for deriving the relationship √s = EA + EB.

PREREQUISITES
  • Understanding of 4-momenta in particle physics
  • Familiarity with Lorentz transformations
  • Knowledge of scalar products in Minkowski space
  • Basic principles of scattering theory
NEXT STEPS
  • Study the derivation of Mandelstam variables in different metric signatures
  • Learn about the implications of the +--- and -+++ metric conventions
  • Explore the relationship between Mandelstam variables and conservation laws in scattering
  • Investigate the applications of Mandelstam variables in various particle physics calculations
USEFUL FOR

This discussion is beneficial for particle physicists, students studying quantum field theory, and anyone interested in the mathematical foundations of scattering processes.

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Homework Statement


In a 2-body scattering event, A + B → C + D, it is convenient to introduce the Mandelstam variables,
s ≡ −(PA + PB)2 ,
t ≡ −(PA − PC) 2 ,
u ≡ −(PA − PD) 2 ,
where PA,...,D are the 4-momenta of the particles A, . . . , D respectively, (· · ·) 2 = (· · ·) · (· · ·) denotes a scalar product, and we are using natural units in this problem. The Mandelstam variables are useful in theoretical calculations because they are invariant under Lorentz transformation.

Demonstrate that in the centre of mass frame of A and B, the total CM energy, i.e., Etotal ≡ EA +EB = EC + ED , is equal to √ s.

Homework Equations


s + t + u = mA2 + mB2 + mC2 + mD2 (I had to show this before which I did, not sure if its relevant or not).
PA = -PB (due to being in a CM frame)

The Attempt at a Solution


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Using the scalar product notation for s, I managed to reduce s to -(EA + EB) however I still can't take the square root to show √ s = EA + EB due to the pesky negative sign.

Apart from me doing something wrong with my algebra, I was wondering if the given Mandelstam variables are correct. From all the secondary sources I've looked at none give them with the negative signs.
 
Physics news on Phys.org
This depends on whether or not you use a +--- or -+++ signature on your metric. Most particle physicists use +--- and it seems like your source does not. Check what convention is used.
 

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