Generalized group for quantum mechanics

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SUMMARY

The discussion centers on the symmetry group relevant to relativistic quantum mechanics in the context of arbitrary Einstein metrics. The Poincare group governs translations, rotations, and boosts in flat space-time. For non-Minkowski spaces, the group of projective transformations is proposed as the relevant Lie group due to its geodesic-preserving properties. The infinite-dimensional Lie group described by the vector field ξμ(x) = x'μ - xμ resembles an infinite product of Lorentz groups, indicating its role as the gauge group for quantum gravity.

PREREQUISITES
  • Understanding of the Poincare group in quantum mechanics
  • Familiarity with Einstein metrics and their implications in physics
  • Knowledge of Lie groups and their applications in relativity
  • Concept of gauge groups in quantum gravity
NEXT STEPS
  • Research the properties of projective transformations in general relativity
  • Study the role of infinite-dimensional Lie groups in quantum field theory
  • Explore the concept of diffeomorphisms and their applications in gravitational theories
  • Investigate the relationship between gauge groups and particle transformations in quantum gravity
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The discussion is beneficial for theoretical physicists, researchers in quantum gravity, and students studying advanced concepts in general relativity and quantum mechanics.

jfy4
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Hi,

In flat space-time, the Poincare group, is the symmetry group responsible for translations, rotations, and boosts for relativistic quantum mechanics.

For an arbitrary Einstein metric (not Minkowski space), what Lie group is responsible for coordinate transformations in relativistic quantum mechanics?

Would it be the group of projective transformations, for their geodesic preserving properties?
 
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The group of coordinate transformations is an infinite-dimensional Lie group. It is described by a vector field ξμ(x) = x'μ - xμ, but its action resembles an infinite product of Lorentz groups, since it induces a Lorentz transformation ∂xμ/∂x'ν at each point. It is the gauge group for quantum gravity
 
Are you talking about the group of diffeomorphisms?

Why is it that the group of transformations for the gravitational field is the same transformation group for particles in a gravitational field?
 

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