Feynman rules (vertecies) for graviton

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SUMMARY

The discussion focuses on the derivation of Feynman rules for gravitons, specifically graviton-scalar and graviton-graviton scattering. While a universally accepted theory of quantum gravity is lacking, perturbative quantum general relativity allows for effective calculations at low energies. Key references include "Quantum Gravity in Everyday Life: General Relativity as an Effective Field Theory" and "Weinberg's computation of gravitational bremsstrahlung," which provide insights into graviton interactions. The conversation emphasizes the challenges of deriving these rules and the potential use of string theory techniques.

PREREQUISITES
  • Understanding of perturbative quantum general relativity
  • Familiarity with effective field theory concepts
  • Knowledge of string theory mathematical techniques
  • Basic grasp of quantum field theory and Feynman diagrams
NEXT STEPS
  • Study "Calculation of Graviton Scattering Amplitudes using String-Based Methods"
  • Research "MHV-Vertices for Gravity Amplitudes"
  • Examine "Perturbative Quantum Gravity and its Relation to Gauge Theory"
  • Explore "Weinberg, S., Infrared Photons and Gravitons, Phys. Rev., 1965, 140, B516"
USEFUL FOR

Physicists, researchers in quantum gravity, and advanced students in theoretical physics seeking to understand graviton interactions and effective field theories.

Neitrino
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Hi,

Could u advise me please some references where the Feynman rules for graviton are derived I mean graviton-scalar graviton-graviton scattering ... in general graviton vertecies ...

Thank you
 
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Such rules would come from a theory of quantum gravity, and we don't have such a (generally accepted) theory yet, as far as I know.
 
I formally agree with jtbell, in the following manner : we do not know whether there is a graviton out there, so we can not calculate its "true" Feynman rules. However, I think this is not a very helpful observation.

The graviton is a well defined concept in perturbative quantum general relativity, which although non renormalizable, offers perfectly good effective calculations at low to moderate energies. The results we obtain in the low energy effective theory will be the same as whatever correct UV complete theory would give, in the low energy of course. In this well defined theory, we can in principle calculate the Feynman rules as we please. In practice this is hard. However, we can use insights from even other approaches to quantum gravity, such a string theory, use their mathematical technics in a different physical context. This is done for instance in
Calculation of Graviton Scattering Amplitudes using String-Based Methods
MHV-Vertices for Gravity Amplitudes
Perturbative Gravity and Twistor Space

Note that, they is not easy reading. I would recommend to start with
Quantum Gravity in Everyday Life: General Relativity as an Effective Field Theory
Perturbative Quantum Gravity and its Relation to Gauge Theory
 
OK, I gladly stand corrected!
 
Thanks Gents ...
 
Some classic papers... might be helpful...

Weinberg's computation of `gravitational bremsstrahlung': should give you the lepton-graviton vertex. Excellently written, as ever...
Weinberg, S., Infrared Photons and Gravitons,
Phys. Rev., 1965, 140, B516

Graviton self-coupling, and graviton-scalar... including proofs that the former is renormalizable at one loop, the latter is not. This is why @humanino refers to treating gravity as an 'effective field theory'.
't Hooft, G., One-Loop Divergencies in the Theory of Gravitation,
Ann. Inst. Henri Poincare A, 1974, 20, 69-94

Graviton-lepton again, same conclusion...
Deser, S. & van Nieuwenhuizen, P., Nonrenormalizability of the quantized Dirac-Einstein system,
Phys. Rev. D, 1974, 10, 411-420


Cheers,

Dave
 
These were calculated for KK gravitons in large extra dimensions in arXiv:hep-ph/9811350 . For normal gravitons just use the zero mode solutions.
 
A frankly adorable exercise is to quantized the Linearized Einstein field equations in the Lorentz Gauge.

\mathbf{\Box} g_{\alpha\beta}=0

This actually provides some insight into quantum gravity, just as the low energy limit quantization does.
 

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