MHB Lagrange thm: orbits as equivalence classes and cosets

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The discussion revolves around understanding Lagrange's Theorem and the Orbit-Stabilizer Theorem, specifically how equivalence classes relate to left cosets in a group. The relation defined on group G by \( x \equiv_H y \) if \( x^{-1}y \in H \) is confirmed as an equivalence relation. The proof demonstrates that if \( x \equiv_H y \), then both elements belong to the same left coset \( yH \), leading to the conclusion that the equivalence classes correspond to the left cosets \( gH \) of subgroup H in G. Additionally, the conversation highlights the need to show that equivalence classes partition the group and that if \( xH = yH \), then \( x \equiv_H y \). This establishes a deeper understanding of the relationship between cosets and equivalence classes in group theory.
buckeye1973
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Hi all, first post, please bear with me!

I am trying to understand Lagrange's Theorem by working through some exercises relating to the Orbit-Stabilizer Theorem (which I also do not fully understand.) I think essentially I'm needing to learn how to show cosets are equivalent to other things or each other.

Here's the setup:
Let $G$ be a group and $H$ be a subgroup of $G$. Define a relation on $G$ by:

$x \equiv_H y$ if and only if $x^{-1}y \in H$

I have already shown that $\equiv_H$ is an equivalence relation. Now I need to show that the $\equiv_H$ equivalence classes are the left cosets $gH$ of $H$ in $G$.

Here is my try:

Let $x,y \in G$ such that $x \equiv_H y$.
Then $x^{-1}y \in H$, which implies $(x^{-1}y)^{-1} = y^{-1}x \in H$.
So $y^{-1}x = h_y$ for some $h_y \in H$.
Then $y(y^{-1}x) = yh_y \in yH$.
thus $x = yh_y \in yH$.
Now $e \in H$, so there exists $h_x \in H$ such that $xh_x = yh_y$.

Um, Q.E.D.?

The logic flow doesn't feel right to me here. My other plan was to assume $xH \neq yH$ and show that that implies $x \not\equiv_H y$, but I couldn't even get that off the ground.

I'd really appreciate any ideas I can get here. Thanks!

Brian
 
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buckeye1973 said:
Hi all, first post, please bear with me!

I am trying to understand Lagrange's Theorem by working through some exercises relating to the Orbit-Stabilizer Theorem (which I also do not fully understand.) I think essentially I'm needing to learn how to show cosets are equivalent to other things or each other.

Here's the setup:
Let $G$ be a group and $H$ be a subgroup of $G$. Define a relation on $G$ by:

$x \equiv_H y$ if and only if $x^{-1}y \in H$

I have already shown that $\equiv_H$ is an equivalence relation. Now I need to show that the $\equiv_H$ equivalence classes are the left cosets $gH$ of $H$ in $G$.

Here is my try:

Let $x,y \in G$ such that $x \equiv_H y$.
Then $x^{-1}y \in H$, which implies $(x^{-1}y)^{-1} = y^{-1}x \in H$.
So $y^{-1}x = h_y$ for some $h_y \in H$.
Then $y(y^{-1}x) = yh_y \in yH$.
thus $x = yh_y \in yH$.

Since \(x\equiv_{\small{H}}y\Rightarrow x\in yH\) we can conclude that this equivalence relation divides the group into left cosets. In other words if x and y are equivalent to each other then both belong to the same coset, yH. You can finish the proof here.

Now $e \in H$, so there exists $h_x \in H$ such that $xh_x = yh_y$.

The statement written above(highlighted in red) is correct. But it does not directly imply that both x and y belong to the same coset of G.

Um, Q.E.D.?

The logic flow doesn't feel right to me here. My other plan was to assume $xH \neq yH$ and show that that implies $x \not\equiv_H y$, but I couldn't even get that off the ground.

I'd really appreciate any ideas I can get here. Thanks!

Brian

...
 
Aha, I see, then. The obvious fact that $y \in yH$ (by the identity in the subgroup $H$) had not come to mind. So my proof concludes:

Let $x,y \in G$ such that $x \equiv_H y$.
Then $x^{-1}y \in H$, which implies $(x^{-1}y)^{-1} = y^{-1}x \in H$.
So $y^{-1}x = h_y$ for some $h_y \in H$.
Then $y(y^{-1}x) = yh_y \in yH$.
thus $x = yh_y \in yH$.
Now, $y \in yH$ (because $e \in H$,) so $x$ and $y$ belong to the same left coset $yH$.
Further, by symmetry of the equivalence relation, $x$ and $y$ belong to the same left coset $xH$.
Therefore, $x \equiv_H y \Rightarrow xH = yH$.
In other words, the $\equiv_H$ equivalence classes are the left cosets $gH$ of $H$ in $G$.
$\square$I think this is correct, yes?

Thanks again for your help!

Brian
 
buckeye1973 said:
Aha, I see, then. The obvious fact that $y \in yH$ (by the identity in the subgroup $H$) had not come to mind. So my proof concludes:

Let $x,y \in G$ such that $x \equiv_H y$.
Then $x^{-1}y \in H$, which implies $(x^{-1}y)^{-1} = y^{-1}x \in H$.
So $y^{-1}x = h_y$ for some $h_y \in H$.
Then $y(y^{-1}x) = yh_y \in yH$.
thus $x = yh_y \in yH$.
Now, $y \in yH$ (because $e \in H$,) so $x$ and $y$ belong to the same left coset $yH$.
Further, by symmetry of the equivalence relation, $x$ and $y$ belong to the same left coset $xH$.
Therefore, $x \equiv_H y \Rightarrow xH = yH$.
In other words, the $\equiv_H$ equivalence classes are the left cosets $gH$ of $H$ in $G$.
$\square$I think this is correct, yes?

Thanks again for your help!

Brian

Hi Brian,

Yes. I don't see any mistake in it.
 
there's nothing wrong with what you did, but your proof implicitly relies on the fact that equivalence classes of an equivalence relation are disjoint (they partition the set they are defined on, the group G in this case).

i would be inclined to prove it like so: suppose x~y (where ~ is the given equivalence via H).

suppose xh is any element of xH. since x~y, $x^{-1}y \in H$, call it h'.

now H is a subgroup, so $h = eh = h'h'^{-1}h$, and $h'^{-1}h$ is another element of H, call it h".

then $xh = xh'h'' = x(x^{-1}y)h'' = yh''$, which is in yH, so xH is contained in yH.

using the fact that y~x (by symmetry of ~), we can prove yH is contained in xH in a similar fashion, thus xH = yH.

another minor point: it could perhaps be, that there are fewer left cosets than equivalence classes, that the partitioning of G into equivalence classes is a refinement of the partition into left cosets. so you need to show this, too:

if xH = yH, then x~y. this isn't too hard, we have that for every xh in xH, xh = yh', for some h' in H. multiplying both sides by $x^{-1}$ on the left:

$h = x^{-1}yh'$ and multiplying both sides by $h'^{-1}$ on the right, we have:

$hh'^{-1} = x^{-1}y$, and by closure (since H is a subgroup), the LHS is in H, so x~y.
 
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