Active Diffeomorphisms of Schwarzschild Metric

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Discussion Overview

The discussion revolves around the concept of active diffeomorphisms in the context of the Schwarzschild metric. Participants explore the implications of these transformations on the metric and the nature of the manifold, questioning the relationship between active and passive transformations in general relativity.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents an example of the Schwarzschild metric and attempts to define active diffeomorphism, suggesting that dragging points in the metric introduces distortions.
  • Another participant points out a potential error in the formulation of the Schwarzschild metric, indicating a need for correction in the expression used.
  • Questions are raised about the meaning of "identify" in the context of the transformation and the explicit transformation equations for the diffeomorphism.
  • There is a discussion about the nature of active diffeomorphisms and their relationship to isometries, with some participants expressing uncertainty about how dragging points works in a general spacetime manifold.
  • It is noted that if an active diffeomorphism is not an isometry, the manifold itself changes, which complicates the notion of dragging points in a fixed background.

Areas of Agreement / Disagreement

Participants express differing views on the nature and implications of active diffeomorphisms, particularly regarding their relationship to isometries and the effects on the manifold. There is no consensus on the correctness of the initial claims or the interpretations of the transformations.

Contextual Notes

Some participants highlight potential errors in the mathematical formulation of the Schwarzschild metric, which may affect the discussion. The implications of active versus passive transformations remain unresolved, with various assumptions and interpretations at play.

Prathyush
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TL;DR
Active diffeomorphism of a Schwarzschild metric under r ->c r
I am trying to understand active diffeomorphism by looking at Schwarzschild metric as an example.

Consider the Schwarzschild metric given by the metric

$$g(r,t) = (1-\frac{r_s}{r}) dt^2 - \frac{1}{(1-\frac{r_s}{r})} dr^2 - r^2 d\Omega^2 $$

We identify the metric new metric at r with the old metric at ##c r##

this gives
$$g(r,t) = (1-\frac{r_s}{ c r}) dt^2 - \frac{1}{(1-\frac{r_s}{c r})} dr^2 - c^2 r^2 d\Omega^2 $$

We can do a passive transformation to re-define the metric so that we have a Minkowski metric as ##r->\infty## We can define ##\tilde{r} = c r##

and we get the metric
$$g(r,t) = (1-\frac{\tilde{r_s}}{r}) dt^2 - \frac{1}{c^2 (1-\frac{\tilde{r_s}}{r})} d\tilde{r}^2 - \tilde{r}^2 d\Omega^2 $$

This does not look like the Schwarzschild metric and should not be a solution of GR.

This is not surprising because we simply dragged the metric numerically and hence introduced distortions to the original manifold.

Now I can define active diffeomorphism such that distance between ##(r, r+dr)## is actually the same as the distance between ##(c r, c r + cdr)## at fixed time then I won't introduce distortions(the ##c^2## in the denominator just cancels) but that is just an ordinary passive transformation. Maybe this is what duality between active and passive transformations means?

Please correct me if I am making a mistake or I have misunderstood something. I heard a claim that an active diffeomorphism is a symmetry in GR and generates new solutions of GR, I don't think it is correct.
 
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Prathyush said:
Consider the Schwarzschild metric given by the metric

You have written this metric down incorrectly. Where you have the factor ##1 - \frac{r}{r_s}##, it should be ##1 - \frac{r_s}{r}##.

You need to correct this error and then rethink your post.
 
Prathyush said:
We identify the metric new metric at r with the old metric at cr

What does "identify" mean? Can you write down the explicit transformation equations for the diffeomorphism you are describing?
 
PeterDonis said:
What does "identify" mean? Can you write down the explicit transformation equations for the diffeomorphism you are describing?
As I understand that the concept of active diffeomorphism means to drag the P to another P'. I can understand what it means to drag things on a Minkowski space, but its unclear to me what It means to drag in a general spacetime manifold.

So the active diffeomorphism that I am interested in drags the point ##(r,t)## to ##(c r,t)## keeping the angular co-ordinates fixed
 
Prathyush said:
its unclear to me what It means to drag in a general spacetime manifold

If your active diffeomorphism is not an isometry, the manifold itself changes. So the notion of "dragging" something in a fixed background manifold doesn't really work for a general active diffeomorphism.
 
PeterDonis said:
If your active diffeomorphism is not an isometry, the manifold itself changes. So the notion of "dragging" something in a fixed background manifold doesn't really work for a general active diffeomorphism.

So active diffeomorphisms are only well defined when there are isometries ?
 
Prathyush said:
So active diffeomorphism only well defined when there are isometries ?

I'm not saying that. I'm just saying that the view of an active diffeomorphism as "dragging points" does not work if the active diffeomorphism is not an isometry.
 
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