Gamma as a Jacobian of Lorentz transformations

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SUMMARY

The Jacobian of a Lorentz transformation is definitively 1, indicating that in special relativistic field theories, the measure remains invariant and does not require adjustment for scalar densities. The presence of gamma in Lorentz transformations is intrinsic to the transformation itself, rather than being a component of the Jacobian. For general coordinate transformations, the measure is not invariant, necessitating the use of the square root of the determinant of the metric, which equals 1 for the Minkowski metric. This distinction is crucial for understanding the mathematical framework of relativistic physics.

PREREQUISITES
  • Understanding of Lorentz transformations
  • Familiarity with Jacobians in coordinate transformations
  • Knowledge of special relativistic field theories
  • Basic grasp of Minkowski metric properties
NEXT STEPS
  • Study the implications of Jacobians in general coordinate transformations
  • Explore the role of gamma in Lorentz transformations
  • Investigate the mathematical foundations of special relativistic field theories
  • Read "Light and Matter" by Benjamin Crowell for practical examples
USEFUL FOR

Physicists, mathematicians, and students of relativity who seek to deepen their understanding of coordinate transformations and their implications in relativistic frameworks.

wil3
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Hello. When one is converting between coordinate systems, the Jacobian arises as a necessary consequence of the conversion. Does this occur with transformations between relativistic systems, and, if so, is this manifested through the prevalence of gamma in the transforms?

Any guidance would be appreciated. Thanks!
 
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No. The Jacobian of a Lorentz transformation is 1. That's why in special relativistic field theories you don't need to consider the subtlety that the measure is actually a scalar density., and you can define

<br /> S[\phi] = \int d^4 x L<br />

For general coordinate transformations the measure is NOT invariant, and you would obtain the action

<br /> S[\phi] = \int \sqrt{|g|}d^4 x L<br />

The squareroot becomes 1 for the Minkowski metric.

The gamma is part of the Lorentz transformation itself, NOT of the corresponding Jacobian.
 
For a relatively lowbrow discussion, see p. 629 of this book: http://www.lightandmatter.com/lm.pdf
 

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