Minkowski Metric Sign Convention

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SUMMARY

The discussion centers on the Minkowski metric sign conventions, specifically the (-+++) and (+---) conventions. Users clarify that both conventions are internally consistent, but they yield different signs for the squared four-momentum. In the (+---) convention, the four-momentum squared is expressed as P² = m²c², while in the (-+++) convention, it is P² = -m²c². Participants emphasize the importance of consistency in calculations and the interpretation of signs in dot products, particularly when dealing with timelike intervals.

PREREQUISITES
  • Minkowski spacetime concepts
  • Four-momentum definition and properties
  • Understanding of inner products in vector spaces
  • Familiarity with metric tensor notation
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  • Learn about the physical interpretations of timelike and spacelike intervals
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PLuz
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Hello,

I believe this is a really stupid question but I can't seem to figure it out. So given a Minkowski spacetime one can choose either the convention (-+++) or (+---).

Supposedly it's the same. But given the example of the four momentum:

Choosing (+---) in a momentarily comoving frame the only non null component is p^0. Taking the inner product <p,p> one gets p^2=m^2c^2 which is the expected result.

Choosing the other convention, (-+++), doing the same calculation one gets p^2=-m^2c^2.


So one has to add a minus sign...do we have to always add this minus sign by hand in every inner product with whatever vectors or something is missing me?

Thank you in advance
 
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Yes, this is the same way that a positive magnitude of a spacetime interval will mean timelike in one convention and spacelike in the other. There is no physical difference between the two, because the systems are internally consistent.
 
As Muphrid mentioned, either convention is internally consistent and both correctly represent the physics. You just have to be consistent with the convention you are using in the signs of all of your dot products. Timelike intervals squared are positive under one convention and negative under the other.

Personally, I use the following approach to keep the convention straight.

If I am using the (-+++) convention then I will write the metric as:
ds^2= -c^2 dt^2 + dx^2 + dy^2 + dz^2

If I am using the (+---) convention then I will write the metric as:
c^2 d\tau^2= c^2 dt^2 - dx^2 - dy^2 - dz^2
 
I understood what both told me, thank you once again for the fast answer, but something is still not clear to me.

Given two vector fields, say V and U. If I'm working in the convention (+---) the dot product is given by: <V,U>=\eta_{\mu \nu} V^{\mu}U^{\nu}=V^0 U^0 -V^i U^j
, where the roman letters mean only the spatial components and \eta_{\mu \nu} is the Minkowski metric.

Choosing the other convention (-+++) the dot product is given by <V,U>=\eta_{\mu \nu} V^{\mu}U^{\nu}=-V^0 U^0 +V^i U^j

So you said that both are correct and I just have to stick with one in the calculations, yes I understand that, but if V=U=P where P is the 4 momentum. They state diferent things. In one convention we find P^2=m^2c^2 and in the other P^2=-m^2c^2, in a momentarily comoving frame.

So if I want them to state the same, expected, result, in the (-+++) convention I have to change the dot product to <V,U>=-\eta_{\mu \nu} V^{\mu}U^{\nu}=V^0 U^0 -V^i U^j. Can I do this?Is this incorrect?
 
Last edited:
PLuz said:
So if I what them to state the same, expected, result, in the (-+++) convention I have to change the dot product to <V,U>=-\eta_{\mu \nu} V^{\mu}U^{\nu}=V^0 U^0 -V^i U^j. Can I do this?Is this incorrect?

In the (+,-,-,-) convention <V,U>=\eta_{\mu \nu} V^{\mu}U^{\nu}=V^0 U^0 -V^i U^j, note that there is no minus sign in front of the metric. Since you *already* use (+,-,-,-) convention your metric \eta_{\mu \nu} already is the diagonal matrix [1,-1,-1,-1].
 
PLuz said:
So you said that both are correct and I just have to stick with one in the calculations, yes I understand that, but if V=U=P where P is the 4 momentum. They state diferent things. In one convention we find P^2=m^2c^2 and in the other P^2=-m^2c^2, in a momentarily comoving frame.
That is correct. In one convention timelike intervals squared are positive, and under the other convention timelike intervals squared are negative. So in both cases P² is a timelike interval squared.

PLuz said:
So if I want them to state the same, expected, result, in the (-+++) convention I have to change the dot product to <V,U>=-\eta_{\mu \nu} V^{\mu}U^{\nu}=V^0 U^0 -V^i U^j. Can I do this?Is this incorrect?
This is incorrect to the best of my knowledge. The dot product is not changed, just the intrepretation of positive or negative as timelike.
 
OK, now I understand perfectly well what all of you told me. Thank you very much.

Can anyone then explain me what is written in wikipedia:

"en.wikipedia.org/wiki/Four-momentum"

in the second section "Minkowski Norm" because they put the minus sign...
 
No, they didn't. Look carefully, the dot product is defined as normal. They used the convention that negative intervals squared are timelike. Therefore m²c² is not equal to the interval squared but the negative of the interval squared. If they had redefined the dot product then they would not have needed the minus sign.
 

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