Metric Compatibility: Is It Forbidden?

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SUMMARY

The discussion centers on the compatibility of connections with metrics in the context of theoretical physics, particularly in relation to gravity theories. It is established that connections do not always require metric compatibility, and models with non-metric compatible connections can be mathematically consistent, although they may not align well with physical observations. The Geneva Convention is humorously referenced to emphasize the strictness of the term "forbidden," but the consensus is that the definition of "forbidden" varies based on context. Notably, Weyl gravity is mentioned as an example of a theory that operates without metric compatibility.

PREREQUISITES
  • Understanding of differential geometry and manifolds
  • Familiarity with covariant derivatives and connections
  • Knowledge of pseudo-Riemannian manifolds
  • Basic concepts of theoretical physics, particularly in gravity theories
NEXT STEPS
  • Study the implications of Weyl gravity and its non-metric compatible connections
  • Explore the mathematical foundations of covariant derivatives in Sean Carroll's lecture notes
  • Investigate the relationship between metric compatibility and physical observations in gravity theories
  • Review discussions on metric and connection independence in theoretical physics forums
USEFUL FOR

The discussion is beneficial for theoretical physicists, mathematicians specializing in geometry, and graduate students exploring advanced concepts in gravity and differential geometry.

kent davidge
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My question is, is it forbidden to have a connection not compatible with the metric?
 
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What do you mean by ”forbidden”?
 
Orodruin said:
What do you mean by ”forbidden”?
Senseless, not allowed
 
kent davidge said:
Senseless, not allowed
You are not helping yourself by not being more specific. You need to define the context of your question.
 
All texts I read on the topic assume a metric compatible metric. Then I was thinking if this is because a non compatible connection is ill defined or something like that
 
kent davidge said:
My question is, is it forbidden to have a connection not compatible with the metric?
Yes it is strictly forbidden. It is in the Geneva convention.
 
martinbn said:
Yes it is strictly forbidden. It is in the Geneva convention.
Name, rank (both co- and contra-variant parts), and serial number only, right?
 
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kent davidge said:
Senseless, not allowed

As @Orodruin has said, that doesn't help.

If you are asking if a model with a connection that is not metric compatible is mathematically consistent, it is.

If you are asking if a model with a connection that is not metric compatible is physically reasonable, such models don't seem to have worked well so far in matching observations, but AFAIK the question is not completely closed.

If you are asking something other than the above, it should be evident that nobody understands what. So if that's the case, either you need to clarify your question further, or this thread will be closed.
 
It is possible to have theories of gravity that arent metric compatible; see Weyl gravity.

The answer to your question is no, connections don't always have metric compatibility.
 
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  • #10
romsofia said:
The answer to your question is no, connections don't always have metric compatibility.
To expand on that, it is perfectly possible to have a connection without your manifold having a metric at all so quite clearly metric compatibility cannot be a constraint on a general connection. There are many possible meanings of ”forbidden” or ”senseless” depending on the context of the use of those words. Hence my request for specification.
 
  • #11
A clarifying (I hope) question. If I use a different connection on a pseudo-Riemannian manifold, I have a new theory of gravity (that may or may not be physically plausible and/or consistent with experiment) right? That seems to be what @romsofia and @PeterDonis are saying in #9 and #8 respectively.

However, Sean Carroll's lecture notes seem to me to define the covariant derivative by blunt assertion: we keep defining the characteristics we'd like it to have until we've picked out a unique covariant derivative operator (and hence connection - unless I'm missing something). His notes don't really justify these characteristics in physical terms, so I kind of came away with the impression that we were picking it for mathematical convenience. I'm trying to work out if I need to re-evaluate that. Reference: https://preposterousuniverse.com/wp-content/uploads/grnotes-three.pdf, first four pages, in particular on the last one: We do not want to make [zero torsion and metric compatibility] part of the definition of a covariant derivative; they simply single out one of the many possible ones.
 
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  • #13
That turns into quite a reading list if you follow the links you linked, and the links they link. Thanks.
 
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