Gauging non-compact lie groups

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SUMMARY

The discussion focuses on the challenges of gauging non-compact Lie groups, specifically addressing the limitations of using a kinetic term of the form Tr(F^{\mu \nu} F_{\mu \nu}) due to the absence of a positive definite Hamiltonian. Participants highlight that non-compact Lie groups can be gauged using a different kinetic term, Q_{\alpha \beta} F^{\alpha}_{\mu \nu} F^{\beta}_{\eta \rho} \epsilon^{\mu \nu \eta \rho}, with a carefully chosen constant matrix Q. The conversation also raises questions about the mathematical motivations behind this choice and the conditions required for Q to ensure a non-topological term and a positive definite Hamiltonian.

PREREQUISITES
  • Understanding of Lie group theory
  • Familiarity with Hamiltonian mechanics
  • Knowledge of gauge theories
  • Proficiency in tensor calculus
NEXT STEPS
  • Research the properties of non-compact Lie groups in gauge theories
  • Study the Einstein-Hilbert action and its derivation from the Lorentz group
  • Explore the role of the constant matrix Q in gauge theories
  • Investigate conditions for positive definiteness in Hamiltonians
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The discussion is beneficial for theoretical physicists, mathematicians specializing in gauge theories, and researchers interested in the mathematical foundations of non-compact Lie groups.

jarod765
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I know that gauging a lie-goup with a kinetic term of the form:

\begin{equation}
\Tr{F^{\mu \nu} F_{\mu \nu} }
\end{equation}

Is not allowed for a non-compact lie group because it does not lead to a positive definite Hamiltonian. I was wondering if anyone knew of a general way to gauge non-compac lie groups. I know there must be a way since the Lorentz group can be gauged to give the Einstein Hilbert action.
 
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I have been reading a little about this and it seems that people can gauge non-compact lie groups with a kinetic term of the form:

\begin{equation}
Q_{\alpha \beta} F^{\alpha}_{\mu \nu} F^{\beta}_{\eta \rho} \epsilon^{\mu \nu \eta \rho}
\end{equation}

with a specific choice of constant matrix Q. My question now is, 1) what mathematically motivates the choice above and 2) what conditions on the matrix Q is there to obtain a non-topological term *and* a positive definite hamiltonian?
 

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