Can We Consider Elementary Particles and Gravity Without a Minkowski Metric?

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Discussion Overview

The discussion revolves around the implications of using a Minkowski metric in the context of elementary particle physics and gravity. Participants explore whether it is appropriate to apply flat spacetime metrics when considering phenomena influenced by gravity, particularly in relation to solar neutrinos and other particle interactions in curved spacetime.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants express unease about deriving results from a Minkowski metric, questioning its validity in regions where gravity is present.
  • One participant suggests that the Schwarzschild metric may provide a better description of spacetime around the sun compared to Minkowski.
  • Another participant raises concerns about whether weak interactions behave differently in curved spacetime, potentially affecting predictions of neutrino rates from the sun.
  • It is noted that spacetime curvature in the solar system is minimal, allowing for a good approximation to flat Minkowski space for local interactions.
  • Some participants acknowledge that while there is a small effect on neutrinos due to spacetime curvature, it is generally negligible for the solar neutrino problem.
  • There is a discussion about the necessity of defining fields with spacelike separations, which requires a metric, and whether using a non-flat metric would significantly alter outcomes.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the appropriateness of using a Minkowski metric in the presence of gravity. Multiple competing views remain regarding the impact of spacetime curvature on particle interactions and the relevance of corrections in specific contexts.

Contextual Notes

Limitations include the dependence on the assumptions about spacetime curvature and the specific conditions under which particle interactions are analyzed. The discussion does not resolve whether corrections due to curvature are significant in various scenarios.

ChrisVer
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I am not sure whether this belongs here or not, but I'll try this topic insteed of SR+GR
I was wondering, since everytime I came across elementary particle equations, such as Dirac or Klein-Gordon, they all consider a metric in the process of a Minkowski space.
I am not sure but I feel uneasiness when I extract results out of a Minkowski metric. Of course these results might be true,for let's say regions where gravity is absent. But what about regions where it's not?
For an example, I can think of the solar neutrinos. Why do we want to think that neutrinos are generated and propagating from the sun according to a flat space's metric, whereas we accept that photons can indeed be bend by the sun's gravitation?

Also, what's the problem of using in particle physics a general metric g^{\mu\nu}(x^{ρ}) instead of the constant g^{\mu\nu}=diag(+---)?
 
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The rule is (As Einstein once said) to make a problem as simple as possible but not simpler. If you don't need general coordinates to solve a problem than use the simpler Minkowsky coordinates.
 
For example, wouldn't the Schwarchild's metric (instead of Minkowski) be a better description of how the geometry around and near the sun is?
 
ChrisVer said:
For example, wouldn't the Schwarchild's metric (instead of Minkowski) be a better description of how the geometry around and near the sun is?

Yes, it is a better description. The question is what problem are you solving and do you need to use Schwartzchild's metric in order to solve it accurately?
 
For example?
The solar neutrinos I mentioned above... By -for example- weak interactions we can predict the number of neutrinos reaching the Earth from the sun. Of course the number we measure here is by far less than the one predicted (and that's a reason we speak about neutrino oscillations). On the other hand, I'm asking...don't weak interactions behave differently to a curved spacetime than they do in the flat minkowski space? so that there will be also a contribution in the rates we predict by that?

Someone would also say that gravitation of the sun (or better put the curvature of spacetime around the sun) does not affect neutrinos or elementary particles in general...However we can observe the gravitational lensing happening by the sun onto the photons...

The same example I could also use for a more extreme limit- for example when we study the behavior of particles in the early universe times... (eg leptogenesis, baryongenesis, etc- of course some of them are consequences of symmetries so it's not exactly that I'm asking about). More specifically that even if on Earth we can study energies ~14TeV of the early universe, these studies are "closed" into the region of a by far "uncurved" spacetime in contrast to what should be the case when universe was still some seconds old.
 
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Quantum field theory in curved spacetimes is ... tricky.
You don't need it for solar neutrinos. Spacetime curvature everywhere in the solar system is tiny, and locally you always have a good approximation to a flat minkowski space (and weak interactions are very locally!).

Of course the number we measure here is by far less than the one predicted (and that's a reason we speak about neutrino oscillations).
There are many independent oscillation measurements now, and they are well in agreement with each other. The solar neutrino problem is solved.
Someone would also say that gravitation of the sun (or better put the curvature of spacetime around the sun) does not affect neutrinos or elementary particles in general...
Who said this? There is some influence - the neutrinos lose a tiny bit of energy. So tiny that it is way below the sensitivity of our detectors. Photon detection methods are much more sensitive, so there the effect has been observed.
 
There is an effect on observed rate due to time dilation but it is too small to be relevant to the solar neutrino problem.
 
Yeah I am not trying to solve the solar neutrino problem (I accept neutrino oscillations :smile:). But I guess physicists before introducing that phenomenon, would also try to do some corrections?
But I guess that the corrections should be totally negligible... One more motivation for asking that, is that in general when we define fields, we ask for them to have a spacelike separation...in order for us to define spacelike separations we need a metric before... am I wrong?
But before dealing with the metric as a dynamical variable-solution of Einstein's equation (since I don't want to get into Quantum Gravity)- I would ask for a given -not flat metric- would things change dramatically or not?
 

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