Question on conjugation closure of subgroups

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Discussion Overview

The discussion centers on the structure of the conjugate closure of the group of rotations \( R = SO(2) \) with respect to the group \( \Omega = RT \), where \( T \) represents translations in the 2D Cartesian plane. Participants explore whether this conjugate closure remains a Lie group and what manifold it might be associated with, delving into the implications of \( \Omega \) being abelian and the normality of subgroups.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that since \( \Omega \) is abelian, the conjugate closure \( \langle R \rangle^\Omega \) equals \( R \).
  • Others argue that \( \Omega \) cannot be assumed to be abelian because \( R \) is not a normal subgroup of \( \Omega \), leading to the conclusion that \( rt \neq tr \) in general.
  • A later reply suggests that analyzing the general case might lead to \( \langle R \rangle^\Omega = \Omega \).
  • One participant expresses uncertainty about proving that \( T \subseteq \langle R^\Omega \rangle \) from the definition of conjugate closure, but later proposes a potential reasoning involving elements of the form \( (t^{-1}rt)(\tau^{-1}r^{-1}\tau) \) and the normality of \( T \).

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether \( \Omega \) is abelian or the implications of that for the conjugate closure. There are competing views regarding the structure of \( \langle R \rangle^\Omega \) and the relationship between \( R \), \( T \), and \( \Omega \).

Contextual Notes

Participants note that the analysis of the conjugate closure involves assumptions about the normality of subgroups and the properties of the groups involved, which remain unresolved.

mnb96
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Hello,

I consider the groups of rotations R=SO(2) and the group T of translations on the 2D Cartesian plane.
Let's define Ω as the group Ω=RT.
Thus Ω is essentially SE(2), the special Euclidean group.

It is known that R and T are respectively 1-dimensional and 2-dimensional Lie groups diffeomorphic to the unit circle and the 2D plane.

My question is:
If I consider now \left\langle R \right\rangle ^\Omega, the conjugate closure of R with respect to Ω, what is the "structure" of such a group? Is it still a Lie group? if so, what is the manifold associated with it?
 
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mnb96 said:
Hello,

I consider the groups of rotations R=SO(2) and the group T of translations on the 2D Cartesian plane.
Let's define Ω as the group Ω=RT.
Thus Ω is essentially SE(2), the special Euclidean group.

It is known that R and T are respectively 1-dimensional and 2-dimensional Lie groups diffeomorphic to the unit circle and the 2D plane.

My question is:
If I consider now \left\langle R \right\rangle ^\Omega, the conjugate closure of R with respect to Ω, what is the "structure" of such a group? Is it still a Lie group? if so, what is the manifold associated with it?


Since ##\Omega## is abelian, it seems straightforward that \left\langle R \right\rangle ^\Omega =R. If we were to consider a higher-dimensional Euclidean group, it seems that this continues to hold, since the result follows from ##T## being a normal subgroup of ##\Omega##.

A slightly more interesting example would be to consider a rank ##m## subgroup ##R_m## of a sufficiently large ##R_n## and study ## \left\langle R_m \right\rangle ^{\Omega_n} ##. It seems easy to convince yourself that this is just ##R_n## itself, though a formal proof would probably be illuminating.
 
fzero said:
Since ##\Omega## is abelian...

Why is Ω supposed to be abelian?
For sure T and R are abelian groups, but I don't think Ω=RT is abelian, because R is not a normal subgroup of Ω. In general rt≠tr. Or am I missing something?
 
mnb96 said:
Why is Ω supposed to be abelian?
For sure T and R are abelian groups, but I don't think Ω=RT is abelian, because R is not a normal subgroup of Ω. In general rt≠tr. Or am I missing something?

No, you're correct. So let's work through it explicitly, like I should have done in the first place. A general element of ##\Omega## is

$$ g(a,b,\theta) = t_1 (a) t_2(b) r(\theta). $$

We are to consider ##g^{-1} r g##. A particular combination would be ## t_1(a)^{-1}r(\phi )t_1(a) = t_1 (a(\cos\phi-1)) t_2(a\sin\phi)##. I expect that considering the general case would lead to ##\langle R\rangle^\Omega = \Omega##.

Perhaps my more complicated example would lead to ##\langle R_m\rangle^{\Omega_n} = \Omega_m## when properly analyzed.
 
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Hi fzero,

thanks for your help. I think you are right when you suggest that \Omega = \left\langle R^\Omega \right\rangle, because \left\langle R^\Omega \right\rangle is supposed to be a group anyway, and if it's neither T nor R, then I don't know what else it can be, besides Ω itself.

The thing that bothers me is that, I can't prove that T \subseteq \left\langle R^\Omega \right\rangle from the definition of conjugate closure.

---EDIT:---
Maybe I got it: the conjugate closure contains also elements of the kind: (t^{-1}rt)\,(\tau^{-1}r^{-1}\tau) and since T is normal we have that r(t\tau^{-1})r^{-1}=t' \in T, thus the above quantity reduces to tt'\tau which is an element of T.
 
Last edited:

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