Calculating Centre of Mass Energy in Fixed Target Interactions with the LHC

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SUMMARY

The discussion focuses on calculating the centre of mass energy in fixed target interactions using the Large Hadron Collider (LHC) with a maximum colliding beam energy of 7 TeV per beam. To achieve the same centre of mass energy in a fixed target interaction, the required beam energy must be calculated using the formula \(\frac{2E^{2}_{c}}{M_{p}}\), where \(M_{p}\) is the proton mass. The key approach involves using Lorentz transformations and understanding the relationship between total energy, kinetic energy, and rest energy. The solution emphasizes the importance of working in both the centre of mass frame and the rest frame of one beam.

PREREQUISITES
  • Understanding of Lorentz transformations
  • Familiarity with relativistic energy equations (E=mc², E²=p²c² + (mc²)²)
  • Knowledge of centre of mass energy concepts
  • Basic principles of particle physics and proton mass (Mₚ)
NEXT STEPS
  • Study Lorentz transformations in detail
  • Learn about invariant mass and its applications in particle physics
  • Explore the concept of centre of mass energy in different collision scenarios
  • Review relativistic momentum and energy conservation laws
USEFUL FOR

This discussion is beneficial for physics students, particle physicists, and researchers involved in high-energy physics experiments, particularly those working with the LHC and fixed target interactions.

leoflindall
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Homework Statement



The proposed maximum colliding beam energy, Ec, in the Large Hadron Collider is 7TeV per beam (proton-proton collisions). By a Lorenz transformation, show clearly that to produce the same centre of mass energy in a 'fixed target' interaction, the beam energy woulr have to be \frac{2E^{2}_{c}}{M_{p}}, where mp is the proton mass and it is assumed that the beam energy is very much greater then MpC2.

Homework Equations



E=mc2

E=pc

E2=p2c2 + (mc2)2



The Attempt at a Solution




I don't think this is particularly hard but I can't see how to approach this problem. I though maybe take the total relativistic energy to be equal to the kinetic energy + the rest energy, and then rearrange for the required equation but I can't get it to work for me.

I would appreciate if anyone could tell em how to approach this problem?

Many Thanks

Leo
 
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The key thing to remember is that for any system with total energy E and momentum p, the quantity E2-c2p2 is a scalar (frame independent): the squared rest energy.

You need to work in two frames: the centre of mass frame, and the frame in which one beam is at rest. Equate the invariant rest energy for each single beam and for the whole system in each frame.
 


Cheers for the help! Worked it out now!

Many thanks

Leo
 

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