Group Theory Notation: SO(n,1) & Poincare Groups Explained

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SUMMARY

The discussion clarifies the meanings of the groups SO(n,1) and Poincaré(n,1) in the context of group theory and physics. SO(n,1) represents the indefinite orthogonal group, which generalizes the Lorentz group SO(3,1) that preserves the Lorentz invariant form. The Poincaré group, which includes translations in addition to the SO(3,1) transformations, is suggested to be represented as Poincaré(n,1) for n+1 dimensions. The importance of double covers in physics is highlighted, particularly in relation to irreducible representations of Lie groups and their topological properties.

PREREQUISITES
  • Understanding of Lie groups and their representations
  • Familiarity with the Lorentz group SO(3,1)
  • Knowledge of quantum mechanics and particle physics
  • Basic concepts of topology and covering groups
NEXT STEPS
  • Research the properties of the Poincaré group and its applications in special relativity
  • Study the concept of double covers in the context of Lie groups
  • Explore the role of irreducible representations in quantum mechanics
  • Investigate the significance of topological properties in group theory
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Physicists, mathematicians, and students studying group theory, particularly those interested in the applications of SO(n,1) and Poincaré groups in theoretical physics and quantum mechanics.

arroy_0205
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1. I understand the meaning of group SO(3) etc, but what is meant by say SO(n,1) or Poincare(n,1)group?

2. what is the importance of double cover of a group in physics?
 
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I'll give my two cents, since this has not received any answer yet.
arroy_0205 said:
1. I understand the meaning of group SO(3) etc, but what is meant by say SO(n,1) or Poincare(n,1)group?
I never saw the notation Poincare(n,1), and I don't know if it is standard.
SO(n,1) correspond to the so-called indefinite orthogonal group in which some of the signs in the signature have been flipped.

2. what is the importance of double cover of a group in physics?
This is a very general question. Covering groups apprear everywhere really, from elementary spin in quantum mechanics to orbifold and Thurston's geometrization conjecture. A group and its cover have identical local properties but can have global (topological) different features. The basics in quantum mechanics for particle physics is that you are interested in irreducible representations of Lie groups. There is a unique simply connected group given the corresponding Lie algebra. As far as I understand, further topological properties will give you additional discrete (quantum numbers) symmetries, the breaking of which are usually studied separately from the representation theory.

This is not very clear to me, I hope I do not confuse you more than I help :smile:
 
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SO(3) is the group of transformations on R^3 which preserves the bilinear form x_1^2 + x_2^2 + x_3^2 and does not perform an inversion on the space.

SO(3,1) is the group which preserves x_0^2 - x_1^2 - x_2^2 - x_3^2, i.e. the Lorentz invariant form.

SO(n,1) is the obvious generalization of that.

I've never seen the notation Poincaré(n,1) either. However, I know that the Poincaré group is SO(3,1) and the translation group in 4 dimensions (i.e. all the symmetries of special relativity), so I assume Poincaré(n,1) is SO(n,1) along with the translation group in n+1 dimensions.
 
From wikipedia, it appears that masudr is right : Poincare(n,1) is the isometric or affine of spacetime with signature (n,1). This notation of the author ot the anyon article directs to "Poincare group" where this notation is not used. The reason is was not positive that it is simply the Poincare group is that this notation is kind of odd. The raison d'etre of this notation is to allow for Poincare(p,q) with q time dimensions. I don't know that anybody really uses that, so does it really deserve a notation on wiipedia ?

Not even to mention the fact that everybody would use the (semi-direct) product of SO(p,q) with \mathbb{R}^{p,q}, so there is already such a notation in principle.
 

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