Spacetime symmetries vs. diffeomorphism invariance

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Discussion Overview

The discussion revolves around the relationship between spacetime symmetries, specifically Lorentz invariance, and diffeomorphism invariance. Participants explore the implications of these concepts in the context of physical laws, coordinate transformations, and the nature of metrics in different geometrical frameworks.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that any physical system should be invariant under changes of coordinates, suggesting that Lorentz invariance is a special case of this general invariance.
  • Others clarify that the distinction between covariance and invariance is crucial, indicating that they are not equivalent concepts.
  • A participant argues that diffeomorphism invariance pertains to the form of the laws of physics rather than the properties of physical systems, using examples from Euclidean geometry to illustrate their point.
  • Another participant states that Lorentz transformations are a specific class of coordinate transformations that preserve the form of physical laws in local inertial frames.
  • Some participants discuss the implications of imposing Lorentz symmetry on physical laws, suggesting it may restrict the forms of these laws if not preceded by diffeomorphism invariance.
  • Questions are raised about the nature of the metric under diffeomorphisms and whether Lorentz invariance is independent of Lorentz transformations.
  • There is a proposal to consider how conditions for conformal invariance might differ from those for Lorentz invariance, particularly regarding the rescaling of the metric.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between Lorentz invariance and diffeomorphism invariance, with no consensus reached on whether Lorentz invariance is merely a special case of diffeomorphism invariance or if it imposes additional constraints on physical laws.

Contextual Notes

Some statements rely on specific definitions of invariance and covariance, and there are unresolved questions regarding the implications of these concepts for the nature of physical laws and metrics in various geometrical contexts.

  • #31
stevendaryl said:
Here is a way of thinking about theories that perhaps helps to clarify the sense in which GR is simpler than Newtonian gravity, in terms of covariance.

As people have pointed out, any theory of physics can be written in a covariant form. However, when one writes Newtonian physics in a covariant form, one finds that there is a "nondynamic" scalar field--Newton's universal time. It's nondynamic, in the sense that matter and energy and so forth don't affect it.

If you write Special Relativity in a covariant form, you will find that it has no nondynamic scalar fields. But it has a nondynamic tensor field, namely the metric tensor.

In General Relativity, there are no nondynamic scalar, vector or tensor fields. All the geometric fields are dynamic, they are affected by matter and energy.

I agree with this, and it is what the reference WNB gave in post#2 is formalizing (based on the approach given by Anderson in 1967 - where I first encountered it).

I realized there is a further terminological confusion going on, which I have contributed to (:redface:). Within covariantly formulated theories, one may produce scalar invariants. However this sense of an invariant is different from formulating a principle of general invariance that is distinct from covariance.

I have always preferred direct terminology like "no absolute objects" as the way way to formulate a theory filtering principle as opposed to a language for formulating any theory (general covariance) - rather than using the historically confused 'general invariance' for this. Some have used that the symmetry group of a theory ( as defined by Anderson - equivalently Straumann ) is the diffeomorphism group as the substantive (theory filtering) principle. To me, though, it all gets back to absolute objects, because absolute objects underpin this definition of the symmetry group of a theory.
 
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  • #32
samalkhaiat said:
Why "NOT"? From particle interaction to galaxy formation, we see "nature uses as little as possible".
I would say that nature uses Occam's in the same way it uses the principle of least action. Is the action principle a law of nature?

Why are there three particle generations not one? Why are there 4 forces, not fewer? Occam's razor is, at best, a guide, just another way of saying simpler, more elegant theories are usually right.

Least action is a very different case. From classical, pre-relativity physics, to GR, to QFT, all experience, without exception, is consistent with "theories of nature are described by action principles".
 
  • #33
PAllen said:
Well, this is exactly what I was referring to as needing to add to the requirement of coordinate independence. The law is definitely coordinate invariant if you express it appropriately (and quite naturally). What you want to add is an additional requirement: that there is no simpler expression of the law that is true in some coordinate systems. To me, that is not coordinate invariance or general covariance, but something else. Anderson and others have worked on formulating this something else, but they admit that it is something beyond coordinate invariance.

It seems like we're not actually disagreeing with each other, just that we're using different definitions for "coordinate invariant".
 
  • #34
PAllen said:
Why are there three particle generations not one? Why are there 4 forces, not fewer?

Maybe you should ask Occam. Still 3 generations is more natural than 3 millions resonances. Laws of nature show decoupling at different length scales, and this exactly why we are still working towards unification.


Least action is a very different case. From classical, pre-relativity physics, to GR, to QFT, all experience, without exception, is consistent with "theories of nature are described by action principles".

Isn’t this what I was trying to tell you? So, Is the action principle a law of nature?

Sam
 
  • #35
samalkhaiat said:
Maybe you should ask Occam. Still 3 generations is more natural than 3 millions resonances. Laws of nature show decoupling at different length scales, and this exactly why we are still working towards unification.




Isn’t this what I was trying to tell you? So, Is the action principle a law of nature?

Sam

Yes, I'm agreeing with that (action principle), emphatically. While I think Occam's razor is not a law of nature but only a guide, effectively the same as 'seek the simplest possible laws', with a lot of judgment about what that means.
 

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