Grand unified theories and quantum mechanics

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SUMMARY

The discussion centers on the challenges of unifying general relativity and quantum mechanics, specifically highlighting the properties of gravity quanta, which must be massless and possess spin 2. Participants reference the Weinberg-Witten theorem, which asserts that a Lorentz-invariant and renormalizable quantum field theory cannot be constructed under these conditions. Additionally, the existence of singularities in classical general relativity complicates the integration with quantum field theories that do not exhibit similar behaviors.

PREREQUISITES
  • Understanding of general relativity principles
  • Familiarity with quantum mechanics concepts
  • Knowledge of the Weinberg-Witten theorem
  • Basic grasp of quantum field theory
NEXT STEPS
  • Research the implications of the Weinberg-Witten theorem on quantum gravity theories
  • Explore the properties of gravitons and their role in quantum field theory
  • Study the behavior of singularities in general relativity
  • Investigate alternative approaches to unifying general relativity and quantum mechanics, such as string theory
USEFUL FOR

Physicists, theoretical researchers, and students interested in the intersection of general relativity and quantum mechanics, particularly those focused on quantum gravity and field theory challenges.

Vals509
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Why is it that general relativity and quantum mechanics are so different and that physicists are having difficulty combining them.

Please give me a simple answer. I scoured the whole net and each website has its own opinion.
 
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hehe and you do not think that people answering here will give his/her opinion? ;-)

To me, the most difficult thing is that the quanta of gravity must have spin 2 and be massless, and you can't construct a quantum field theory which is Lorentz-invariant and renormalizable. This is wienberg-witten theorem.
 
I agree with malawi_glenn, and another important reason is that classically the equations of General Relativity develop singularities (black holes) within a finite time. The classical analogues of our quantum fields for the color force, weak force, and e&m do not have this behavior.
 
Mass has not anti-mass in the same way as we have positive and negative charges etc.
 
To me, the most difficult thing is that the quanta of gravity must have spin 2 and be massless, and you can't construct a quantum field theory which is Lorentz-invariant and renormalizable. This is wienberg-witten theorem.

Could you put that clearer? Do you find it difficult that
- quanta of gravity must have spin 2 and be massless
and
- can't construct a quantum field theory which is Lorentz-invariant and renormalizable

If so, why do you find it difficult?
 
You can show that gravitons must have that property within the standard model and then the rest follows from Wienberg-Witten theorem.

The difficultly is that you can't construct a quantum field theory which is lorentz invariant and renormalizable with that property of the graviton.
 

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