GR as Gauge Theory

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SUMMARY

The discussion centers on the modeling of General Relativity (GR) as a gauge theory, specifically referencing a 1990 dissertation titled "Die Allgemeine Relativitätstheorie als SO(3)-Eichtheorie". The author highlights that while GR can be approached as a gauge theory, the conventional method treats it as the gauge theory of the Poincaré algebra, imposing constraints to eliminate unwanted transformations. Further exploration into other algebras, such as N = 1 super Poincaré and the Bargmann algebra, reveals connections to Newton-Cartan theory, which also contains an SO(3) subalgebra. The discussion raises questions about the relevance and evolution of the SO(3) gauge theory approach over the past 35 years.

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  • Understanding of General Relativity principles
  • Familiarity with gauge theory concepts
  • Knowledge of Poincaré algebra and its applications
  • Basic grasp of supergravity and Newton-Cartan theory
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  • Research the implications of treating GR as a gauge theory of the Poincaré algebra
  • Explore the connections between N = 1 super Poincaré and supergravity
  • Investigate the role of the Bargmann algebra in Newton-Cartan theory
  • Read the dissertation "Die Allgemeine Relativitätstheorie als SO(3)-Eichtheorie" for historical context
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fresh_42
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TL;DR
I found a dissertation from 1990 that attempted to model the general relativity theory as an ##SO(3)## gauge theory. What has happened to that idea?
While searching the internet for milestones in physics, mainly for those that led to the standard model, I came to ask myself why general relativity cannot be modeled by a gauge theory. Searching for "Relativitätstheorie als Eichtheorie" brought up a dissertation from 1990 titled: "Die Allgemeine Relativitätstheorie als ##SO(3)##-Eichtheorie", "The General Relativity Theory as ##SO(3)## Gauge Theory".
https://arxiv.org/pdf/gr-qc/0310111

The author wrote:
This work is intended to provide an answer to both the successes and the problems of the general theory of relativity. Since the successes mentioned are based entirely on the (at least approximate) validity of Einstein's equations, these equations of motion must also retain their validity in the modified theory. On the other hand, the weak points of Einstein's theory explained above must also be taken into account, which means that the Einstein equations must be given a new interpretation within the framework of the modified theory. The three basic pillars of the modified theory of gravitation are briefly presented:
  1. General Structure of the Theory
  2. Energie-Impuls der Gravitation
  3. The Vacuum

The dissertation is in German so I don't expect you to read it. On the other hand, it is now 35 years old, so my question is simple: What has happened to that idea and have there been further approaches, eventually with other gauge groups?
 
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fresh_42 said:
I came to ask myself why general relativity cannot be modeled by a gauge theory.
It can be, in a sense, but the "gauge group" is not any compact group. See this Insights article by haushofer, which I believe gives a good discussion of the "mainstream" view among relativity physicists on this topic:

https://www.physicsforums.com/insights/general-relativity-gauge-theory/
 
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fresh_42 said:
TL;DR Summary: I found a dissertation from 1990 that attempted to model the general relativity theory as an ##SO(3)## gauge theory. What has happened to that idea?

While searching the internet for milestones in physics, mainly for those that led to the standard model, I came to ask myself why general relativity cannot be modeled by a gauge theory. Searching for "Relativitätstheorie als Eichtheorie" brought up a dissertation from 1990 titled: "Die Allgemeine Relativitätstheorie als ##SO(3)##-Eichtheorie", "The General Relativity Theory as ##SO(3)## Gauge Theory".
https://arxiv.org/pdf/gr-qc/0310111

The author wrote:


The dissertation is in German so I don't expect you to read it. On the other hand, it is now 35 years old, so my question is simple: What has happened to that idea and have there been further approaches, eventually with other gauge groups?
As Peter points out, the "standard approach" (afaik) is to treat GR as the gauge theory of the Poincaré algebra (i.e. the algebra describing the full isometry group of the vacuum) and impose constraints. These constraints eliminate unwanting transformations (the local translations) directly, and indirectly by making certain gauge fields dependent on other gauge fields (the spin connection becomes a dependent field). This procedure can be extended to other algebras, like N = 1 super Poincaré, giving N = 1 supergravity, the Bargmann algebra, which gives you Newton-Cartan theory, and even a stringy version of this Bargmann algebra which leaves you with a Newton-Cartan theory for strings. Note that all these algebras have an SO(3) subalgebra. I don't know why one would only use SO(3) to obtain GR, but for that I have to read the thesis, I guess :P

If you want more details, maybe you can find them in my PhD-thesis:

https://research.rug.nl/en/publications/newton-cartan-gravity-revisited
 
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