Computing an Energy-Momentum tensor given a Lagrangian

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Homework Help Overview

The discussion revolves around computing the Energy-Momentum tensor from a given Lagrangian, specifically one resembling the Lagrangian used to derive Maxwell's equations. Participants explore the properties of the Lagrangian, its invariance under Lorentz transformations, and the implications of Noether's theorem regarding conserved currents.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the derivation of the Energy-Momentum tensor from the Lagrangian, questioning the equivalence of different forms of the Lagrangian. They explore the computation of the current associated with the Lagrangian and express uncertainty about specific steps in the derivation process.

Discussion Status

The discussion is ongoing, with participants providing hints and suggestions for compacting expressions and clarifying the computation of derivatives. There is an active exchange of ideas regarding the correct formulation of the Energy-Momentum tensor and the conditions under which it satisfies certain properties.

Contextual Notes

Participants note potential confusion regarding the treatment of indices in derivatives and the implications of using the same index multiple times in expressions. There is also a mention of specific references to lecture notes that guide the discussion.

  • #31
nrqed said:
Even worse, some of the components are zero.

Ahhh you're right.

This equation

$$\partial_{\mu} \partial^{\mu} A^{\nu} = \eta^{\nu \rho} \partial_{\mu} \partial^{\mu} A_{\rho} = 0$$

It is equivalent to

$$\partial_{\mu} \partial^{\mu} A_{\nu} = \eta_{\nu \rho} \partial_{\mu} \partial^{\mu} A^{\rho} = \partial_{\mu} \partial^{\mu} A_{\nu} = 0$$

Which is what we want.
 
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