Is the Scalar \( R^{ji} R_{ij} - R^2 \) Recognized in Mathematical Physics?

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Discussion Overview

The discussion revolves around the scalar \( R^{ji} R_{ij} - R^2 \), where \( R_{ij} \) is the Ricci tensor and \( R \) is the Ricci scalar. Participants explore its properties, potential interpretations, and its relevance in specific mathematical contexts, particularly in relation to integrals over compact manifolds and geometric interpretations.

Discussion Character

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

Main Points Raised

  • One participant notes encountering the scalar in calculations and inquires about its properties and recognition in mathematical physics.
  • Another participant suggests that the scalar is related to the second principal invariant of the Ricci tensor and expresses interest in its geometrical and physical interpretations.
  • A different participant claims that \( R^{ji} R_{ij} = R \), leading to the simplification \( R^{ji} R_{ij} - R^2 = R(1 - R) \), but acknowledges limitations in their understanding.
  • Further clarification is provided regarding the units of the Ricci scalar and its relationship to physical quantities in the context of Einstein's equations, specifically relating it to the pressure and density of a perfect fluid.
  • One participant mentions a specific context involving Kahler supermanifolds and discusses a potential connection to Yau's theorem, indicating that the integral of the scalar over a compact manifold could have implications for a conjecture they are investigating.

Areas of Agreement / Disagreement

Participants express various interpretations and applications of the scalar, with no consensus reached on its properties or implications. Multiple competing views remain regarding its mathematical significance and physical interpretations.

Contextual Notes

Some participants note the dependence on specific contexts, such as the relationship between curvature in supermanifolds and complex manifolds, as well as the implications of the scalar in physical theories. There are unresolved questions about the existence of manifolds that could disprove certain conjectures.

joschu
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In my calculations, I come across the scalar
R^{ji} R_{ij} - R^2
(R_{ij} is the Ricci tensor, R is the Ricci scalar)
More specifically, I come across the integral of this scalar over a compact manifold.
Has anyone seen it before, and does it have any nice properties?

John Schulman
 
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It seems to me...
Up to a constant factor, that scalar is the second principal-invariant of the Ricci tensor. It is proportional to the second elementary symmetric function of its eigenvalues. How does it arise? (I've been interested in this invariant [not necessarily for Ricci] and have been searching for a geometrical interpretation [and physical interpretation] for it.)
 
Last edited:
joschu said:
In my calculations, I come across the scalar
R^{ji} R_{ij} - R^2
(R_{ij} is the Ricci tensor, R is the Ricci scalar)
More specifically, I come across the integral of this scalar over a compact manifold.
Has anyone seen it before, and does it have any nice properties?

John Schulman
Since

R^{ji} R_{ij} = R

it follows that

R^{ji} R_{ij} - R^2 = R - R^2 = R(1 - R)

That's about all I can see about it.

Pete
 
pmb_phy said:
Since

R^{ji} R_{ij} = R

it follows that

R^{ji} R_{ij} - R^2 = R - R^2 = R(1 - R)

That's about all I can see about it.

Pete

No. R=R_{ij} g^{ij}. The Ricci scalar has units, by the way...

I have no idea if the original poster is looking for a purely mathematical answer or not, but if Einstein's equations hold, and you have a perfect fluid with density \rho and pressure p, that scalar is proportional to p(\rho-p). Normally, \rho \gg p, so the square root of your scalar is basically a geometric average of the density and pressure.
 
In my earlier post, I was too lazy to write
R^{ji} R_{ij} - R^2=2R^i{}_{[j}R^j{}_{i]},
where I've used the metric to raise and lower indices.
 
Thanks for the responses, especially robphy. I'll do a little research about the eigenvalues of R^{i}_j.

Here's how I came across this quantity:
I'm working in a rather specific area: I'm studying the relationship between the curvature of a Kahler supermanifold with the curvature of the underlying complex manifold.
I found that if a supermanifold with two "fermionic" dimensions satisfies R=0 then there's a scalar differential equation with some curvature tensors that the underlying complex "bosonic" manifold must satisfy. This equation has a bunch of terms in it, but if we take the integral of the expression over a compact manifold, we get
\int (R^{ji} R_{ij} - R^2) dV=0

Here's the consequence of this calculation that interests me:
If I can find a complex manifold where the above integral CAN'T equal zero regardless of metric, it is likely that I will be able to disprove a certain conjecture concerning Yau's theorem generalized to supermanifolds. Unfortunately, I don't know if such a manifold exists.
 

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