Lorentz Generators, Srednicki eq. 2.13

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SUMMARY

The discussion focuses on proving equation 2.13 from Srednicki's work, specifically the relationship involving the Lorentz generators and the transformation properties of the unitary operator \( U(\Lambda) \). The key equation under scrutiny is \( \delta \omega _{\mu\nu}U(\Lambda)^{-1}M^{\mu\nu}U(\Lambda) = \delta \omega _{\mu\nu}\Lambda^\mu{}_{\rho}\Lambda^\nu{}_{\sigma}M^{\rho\sigma} \). The user expands the unitary operator and utilizes the antisymmetric property of \( \omega \) to derive an expression that leads to a near-solution. The discussion highlights the importance of understanding the transformation properties of \( U(\Lambda) \) and the implications of the linear term expansion.

PREREQUISITES
  • Understanding of Lorentz transformations and their properties
  • Familiarity with quantum mechanics, specifically unitary operators
  • Knowledge of antisymmetric tensors and their applications
  • Proficiency in mathematical physics, particularly in the context of Srednicki's formalism
NEXT STEPS
  • Study the derivation of unitary operators in quantum mechanics
  • Explore the properties of antisymmetric matrices and their physical significance
  • Investigate the implications of Lorentz transformations in quantum field theory
  • Review Srednicki's textbook, focusing on sections related to Lorentz generators and their applications
USEFUL FOR

This discussion is beneficial for theoretical physicists, graduate students in quantum mechanics, and researchers focusing on quantum field theory and Lorentz invariance. It provides insights into the mathematical framework necessary for understanding transformations in particle physics.

malawi_glenn
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Hello, I am trying to prove eq 2.13 in srednicki:

[tex]\delta \omega _{\mu\nu}U(\Lambda)^{-1}M^{\mu\nu}U(\Lambda) = \delta \omega _{\mu\nu}\Lambda^\mu{}_{\rho}\Lambda^\nu{}_{\sigma}M^{\rho\sigma}[/tex]

where we have expanded the following and comparing the linear term:

[tex]U(\Lambda)^{-1}U(\Lambda)^{*}U(\Lambda) = U(\Lambda^{-1}\Lambda ^{*}\Lambda)[/tex]

and

[tex]\Lambda^{*} = 1 +\omega[/tex]

(omega is of course antisymmetric)

and

[tex]U(1+ \delta \omega ) = I + \dfrac{i}{2}\delta \omega _{\mu\nu}M^{\mu\nu}[/tex]

Now I get something like:

[tex]\delta \omega _{\mu\nu}U(\Lambda)^{-1}M^{\mu\nu}U(\Lambda) = U(1+\Lambda^{-1}\delta \omega\Lambda )[/tex]

by just straightforward computation of
[tex]U(\Lambda^{-1}\Lambda ^{*}\Lambda)[/tex]

and now I am stuck badly :-(
 
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update: I am very close to solve it =D
 

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