Formulating the Poincare group and its double cover

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SUMMARY

The discussion focuses on the formulation of the Poincaré group and its double cover, specifically addressing the full Poincaré group as ##\mathbb{R}^{3,1} \rtimes O(3,1)## and the restricted version as ##\mathbb{R}^{3,1} \rtimes SO(3,1)##. It clarifies that the correct representation of the full Lorentz group is ##O(3,1) = SO(3,1) \rtimes \mathbb{Z}_2##, where ##\mathbb{Z}_2## is an abelian normal subgroup. The discussion also explores the double cover of the full Poincaré group, suggesting formulations involving ##Spin(3,1)##. Key insights include the nature of the adjoint action of inversions on rotations and the implications for group structure.

PREREQUISITES
  • Understanding of group theory, particularly semi-direct products
  • Familiarity with the Lorentz group and its representations
  • Knowledge of Poincaré group structure and properties
  • Concepts of normal and abelian subgroups in group theory
NEXT STEPS
  • Study the properties of the Poincaré group and its applications in physics
  • Learn about the structure and significance of the double cover groups, specifically ##Spin(3,1)##
  • Explore the implications of adjoint actions in group theory
  • Investigate the relationship between normal subgroups and quotient groups in various contexts
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The discussion is beneficial for theoretical physicists, mathematicians specializing in group theory, and anyone interested in the mathematical foundations of spacetime symmetries.

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TL;DR
As direct/semi-direct products
Given the full Lorentz group is ##O(3,1)## and the restricted Lorentz group is ##SO(3,1)##, the full Poincare group is ##\mathbb{R}^{3,1} \rtimes O(3,1)## and the restricted Poincare group is ##\mathbb{R}^{3,1} \rtimes SO(3,1)##.

Given that ##O(3,1) = \mathbb{Z}_2 \rtimes SO(3,1)##, how might one formulate the full Poincare group as the direct/semi-direct product of ##\mathbb{Z}_2, \mathbb{R}^{3,1}, SO(3,1)##?

Would it be any of the following?:
$$ (\mathbb{Z}_2 \times \mathbb{R}^{3,1}) \rtimes SO(3,1)$$
$$ \mathbb{Z}_2 \rtimes \mathbb{R}^{3,1} \rtimes SO(3,1)$$


For the full Lorentz group ##O(3,1)## the double cover is ##Pin(3,1)##, and for the restricted Lorentz group is ##SO(3,1)##, the double cover is ##Spin(3,1)##.

And a similar question for the double cover of the full Poincare group?:
$$ (\mathbb{Z}_2 \times \mathbb{R}^{3,1}) \rtimes Spin(3,1)$$
$$ \mathbb{Z}_2 \rtimes \mathbb{R}^{3,1} \rtimes Spin(3,1)$$
 
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I don't think your characterization of O(3,1) as \mathbb{Z}_2\rtimes SO(3,1) isn't quite correct. There is no direct action of SO(3,1) on \mathbb{Z}_2.

Rather, I believe your semi-direct product should be reversed as it is SO(3,1) that is the normal subgroup. Recall that two inversions will result in a (regular or pseudo)rotation. Hence, the adjoint action of an inversion on a rotation will yield a rotation.
Rather: O(3,1) = SO(3,1)\rtimes \mathbb{Z}_2.
 
My understanding is that ##\mathbb{Z}_2## is abelian and therefore a normal subgroup.
 
There are several \mathbb{Z}_2's in O(p,n) you must be careful which one you are considering. Let me think out loud and see where this goes:

Simple example: ISO(3) = \mathbb{R}^3 \rtimes SO(3). The action of the rotation group(s) on the translation subgroup (normal subgroup) is to rotate it as a vector. The quotient structure is defined by the short exact sequence: 1 \to \mathbb{R}^3 \to ISO(3) \to SO(3) \to 1 hence SO(3)=ISO(3)/\mathbb{R}^3. The normality of \mathbb{R}^3 is why the quotient is a group. All standard group theory.

Now when you reverse the quotient structure you get a manifold:
1 \to SO(3)\to ISO(3)\to \mathbb{R}^3 however this ISO(3)/SO(3) =\mathbb{R}^3 is not a group (the cosets fail to close) but rather the manifold of SO(3) subgroups of ISO(3) identifiable with each fixed center point for a given rotation in space. This reversed quotient is in a sense dual to the translation subgroup as it is what gets translated by the adjoint action of the translators on rotators.

If we quotent out the central \mathbb{Z}_2 subgroup of O(n) we get the projective orthogonal group PO(n).
1\to \mathbb{Z}_2 \to O(n)\to PO(n)\to 1
This is not how the special orthogonal subgroup is defined. Rather the special orthogonal group is obtained by removing all inversions (reflections in one direction in the vector irrep). This is a whole manifold of {Z}_2 subgroups none of which are central or normal but are rotated by the SO(n) subgroup.

But note that inversions acting adjointly on rotations are again rotations. Hence SO(n) is a normal subgroup of O(n).
1 \to SO(n)\to O(n)\to O(n)/SO(n) \to 1
Yep, O(n)/SO(n)= \mathbb{Z}_2 is necessarily the image of the inverting and non-inverting orthogonal transformations with the non-inverting mapping to the identity (exactness of the sequence).

While we're here, we can consider the reverse sequence:
1 \to \mathbb{Z}_2 \to O(n)\to Q \to 1
Here the quotient Q is not a group since the first mapping is necessarily (as a reversial of the above) not a whole-space inversion but it maps \mathbb{Z}_2 to one of the vector inversion subgroups in O(n) it is not a normal subgroup. I'm not clear on what Q is; it must incorporate the manifold of inversion subgroups in O(n) but also, I think, the rotations leaving it invariant. I think that will end up being homeomorphic to SO(n) but I'm guessing at this point as I'm now reaching a bit beyond my understanding of the topic.
 
redtree said:
My understanding is that ##\mathbb{Z}_2## is abelian and therefore a normal subgroup.

Abelian subgroups do not need to be normal. For example, if ##\tau## is a transposition in ##S_n## with ##n>2,## then ##\{1,\tau\}## is abelian but not normal in ##S_n.##

On the other hand, index 2 subgroups, like ##SO(3,1)\subset O(3,1),## are always normal.
 

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