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While answering this question my interest in the rotation/reflection group was piqued.

I personally know very basic group theory, not much more than what a group really is. I understand that the techniques I used in the answer to that question are similar to group theoretical techniques.

Could someone explain how chirality appears in $n$ dimensional objects living in $m>n$ dimensional space if and only if $n=m$ using group theory? Preferably (but not necessarily) giving some background on the techniques being used to better suit my current understanding of group theory.

Note thatwhen I say an $n$ dimensional object, I mean an object that can occupy a minimum of $n$ dimensions. A helix is thus a "three dimensional object", even if its topological dimension is 1.

Apologies if the question is too broad.

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    $\begingroup$ I am confused by "$m\gt n$ dimensional space if and only if $n=m$". $\endgroup$ – robjohn Oct 20 '13 at 13:50
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When a dimension is added, one can rotate the axis of reflection and the added dimension by $180^\circ$ so that the reflection in the lower dimension is realizable as a rotation in the higher dimension. In the higher dimension, there is a rotation (determinant $1$) and a reflection (determinant $-1$) that affect the lower dimension in the same way.

To be precise (in the spirit of this answer), consider a reflection in $\mathbb{R}^n$ that negates $x_n$ $$ A=\begin{bmatrix} 1&0&0&\dots&0\\ 0&1&0&\dots&0\\ 0&0&1&\dots&0\\ \vdots&\vdots&\vdots&\ddots&\vdots\\ 0&0&0&\dots&-1 \end{bmatrix} $$ This can be lifted to an isometry in $\mathbb{R}^{n+1}$ in two ways, as a reflection (determinant $=-1$) $$ B=\begin{bmatrix} 1&0&0&\dots&0&0\\ 0&1&0&\dots&0&0\\ 0&0&1&\dots&0&0\\ \vdots&\vdots&\vdots&\ddots&\vdots&\vdots\\ 0&0&0&\dots&-1&0\\ 0&0&0&\dots&0&1 \end{bmatrix} $$ or as a rotation of $\theta=\pi$ (determinant $=1$) $$ C=\begin{bmatrix} 1&0&0&\dots&0&0\\ 0&1&0&\dots&0&0\\ 0&0&1&\dots&0&0\\ \vdots&\vdots&\vdots&\ddots&\vdots&\vdots\\ 0&0&0&\dots&\cos(\theta)&-\sin(\theta)\\ 0&0&0&\dots&\sin(\theta)&\cos(\theta) \end{bmatrix} $$ Since this determinant is a continuous function and the determinant of an isometry is $\pm1$, we cannot get from the identity to $A$ or $B$ via rotations. However, we can get to $C$ via rotation in $\mathbb{R}^{n+1}$, and the action of $C$ is indistinguishable from the action of $A$ as viewed within $\mathbb{R}^n$. Thus, chirality is lost when we add even one dimension.

Of course, you posted this answer, so perhaps I am misunderstanding your question.

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  • $\begingroup$ @Manishearth: I am sorry I can't help with algebraic understanding beyond linear algebra. I hope this helps, but let me know if I am totally missing the point. $\endgroup$ – robjohn Oct 20 '13 at 16:35
  • $\begingroup$ @Landscape: not uncomfortable at all. Your comments were constructive and my answer is better now. Thanks. $\endgroup$ – robjohn Oct 20 '13 at 21:38
  • $\begingroup$ You are welcome and thank you for your understanding. $\endgroup$ – 23rd Oct 20 '13 at 21:42
  • $\begingroup$ @robjohn I'd asked this question to get a better understanding of group theory. I already know the matrix approach :P $\endgroup$ – Manishearth Oct 21 '13 at 5:50
  • $\begingroup$ @Manishearth: I figured as much, considering you had written the answer I cited. I meant no offense, but this is what I could offer, and there weren't any other answers. $\endgroup$ – robjohn Oct 21 '13 at 7:38

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