Geometry Behind g_μν Λμ ρ Λν φ = g_ρ φ ?

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The equation g_{\mu \nu} \Lambda^{\mu}\; _\rho \Lambda^{\nu}\; _\phi = g_{\rho \phi} illustrates the invariance of the metric tensor under Lorentz transformations. This indicates that two reference frames share the same metric, allowing observers to compute dot products consistently and observe identical physical phenomena. The discussion emphasizes the importance of defining the symbols involved to derive a meaningful physical interpretation of the equation.

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Hymne
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What is the physical interpretation of the equation:

[tex]g_{\mu \nu} \Lambda^{\mu}\; _\rho \Lambda^{\nu}\; _\phi = g_{\rho \phi}[/tex]?

I see that all the sub- and superindicies add up but what's the geometry behind it?
 
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This may sound naive. But unless you define the physical meaning of the various symbols, there is no way to give a physical interpretation to the equation.
 
Hymne said:
What is the physical interpretation of the equation:

[tex]g_{\mu \nu} \Lambda^{\mu}\; _\rho \Lambda^{\nu}\; _\phi = g_{\rho \phi}[/tex]?

I see that all the sub- and superindicies add up but what's the geometry behind it?

I prefer the [tex]\Lambda 's[/tex] to have an inverse sign on them, but that's all right.

Basically that equation says two reference frames have the same metric, or that the metric tensor is invariant under Lorentz transformation.

This implies that two observers take dot products in the same way, and that both observers observe the same physics.
 

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