Graviton Propagator and energy-momentum tensor

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SUMMARY

The discussion centers on the relationship between graviton propagators and the energy-momentum tensor in particle scattering processes. It is established that the graviton propagator couples with the energy-momentum tensor of matter fields, leading to the conclusion that the vertex coupled with the graviton propagator can indeed be considered as the energy-momentum tensor. The participant highlights that the conservation of the energy-momentum tensor implies that when expressing graviton momentum as the sum of two incoming momenta, the contribution may vanish, particularly when analyzed in the context of harmonic gauge. The specific expression for the graviton propagator is provided, which leads to the Newtonian potential in the nonrelativistic limit.

PREREQUISITES
  • Understanding of graviton propagators in quantum field theory
  • Familiarity with energy-momentum tensor concepts
  • Knowledge of harmonic gauge in general relativity
  • Basic principles of particle scattering processes
NEXT STEPS
  • Study the derivation of the graviton propagator in quantum field theory
  • Explore the implications of energy-momentum tensor conservation in particle physics
  • Investigate the role of harmonic gauge in simplifying gravitational interactions
  • Review the Newtonian limit of gravitational theories as discussed in arXiv paper gr-qc/9512024
USEFUL FOR

The discussion is beneficial for theoretical physicists, particularly those specializing in quantum gravity, particle physicists analyzing scattering processes, and researchers interested in the mathematical formulation of graviton interactions.

Neitrino
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Dear PF,
I am a little bit confused could you pls help me ...

Suppose I a have a scatering or conversion of two particles via graviton propagator.
Graviton propagator couples with energy-momentum tensor of matter fields.

So can i assume that vertex to which graviton propagator is coupled is in fact energy-momentum tensor ?

Energy-momentum tensor is conserved and thus if i take graviton propagator in some general case where i have graviton momentum in numerator it should give me vanishing contribution.

But energy-momentum tensor (which I cast in this case as a vertxe +external lines) contains two different momentum: ingoing momentum p1 and ingoing momentum p2, so my propagator momentum will be q=p1+p2... so does it mean that when I express graviton momentum through p1+p2 and and couple it to a vertxe i will have identical zero...?

Thanks
 
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There are terms in the graviton propagator that do not have factors of the momentum in the numerator. For example, in harmonic gauge

D_{\mu\nu,\rho\sigma} = \frac{1}{q^2} \left( \eta_{\mu\rho}\eta_{\nu\sigma} + <br /> \eta_{\mu\sigma}\eta_{\nu\rho} - \eta_{\mu\nu}\eta_{\sigma\rho} \right).

This expression leads to the Newtonian potential in the nonrelativistic limit, as outlined for example, in section 4 of http://arxiv.org/abs/gr-qc/9512024.
 

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