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\newtheorem{prop}{Proposition} \newtheorem{cor}{Corollary} \newtheorem*{utheorem}{Theorem} \newtheorem*{ulemma}{Lemma} \newtheorem*{uprop}{Proposition} \newtheorem*{ucor}{Corollary} \theoremstyle{definition} \newtheorem{defn}{Definition} \newtheorem{example}{Example} \newtheorem*{udefn}{Definition} \newtheorem*{uexample}{Example} \theoremstyle{remark} \newtheorem{remark}{Remark} \newtheorem{note}{Note} \newtheorem*{uremark}{Remark} \newtheorem*{unote}{Note} %------------------------------------------------------------------- \begin{document} %------------------------------------------------------------------- \section*{SO(3)} \hypertarget{context}{}\subsubsection*{{Context}}\label{context} \hypertarget{group_theory}{}\paragraph*{{Group Theory}}\label{group_theory} [[!include group theory - contents]] \hypertarget{contents}{}\section*{{Contents}}\label{contents} \noindent\hyperlink{idea}{Idea}\dotfill \pageref*{idea} \linebreak \noindent\hyperlink{properties}{Properties}\dotfill \pageref*{properties} \linebreak \noindent\hyperlink{cohomology}{Cohomology}\dotfill \pageref*{cohomology} \linebreak \noindent\hyperlink{finite_subgroups}{Finite subgroups}\dotfill \pageref*{finite_subgroups} \linebreak \noindent\hyperlink{related_concepts}{Related concepts}\dotfill \pageref*{related_concepts} \linebreak \noindent\hyperlink{references}{References}\dotfill \pageref*{references} \linebreak \hypertarget{idea}{}\subsection*{{Idea}}\label{idea} The [[special orthogonal group]] in [[dimension]] 3. \hypertarget{properties}{}\subsection*{{Properties}}\label{properties} \hypertarget{cohomology}{}\subsubsection*{{Cohomology}}\label{cohomology} \begin{prop} \label{}\hypertarget{}{} The [[integral cohomology|integral]] [[cohomology ring]] of the [[classifying space]] $B SO(3)$ is \begin{displaymath} H^\bullet\big( B SO(3), \mathbb{Z} \big) \;\simeq\; \mathbb{Z}\big[ p_1, W_3\big] / (2 W_3) \,, \end{displaymath} where \begin{itemize}% \item $p_1 \in H^4\big(B SO(3), \mathbb{Z}\big)$ is the [[universal characteristic class|universal]] [[first Pontryagin class]]; \item $W_3 = \beta(w_2) \in H^3\big( B SO(3), \mathbb{Z}\big)$ is the [[universal characteristic class|universal]] degree-3 [[integral Stiefel-Whitney class]]. \end{itemize} \end{prop} This is a special case of \hyperlink{Brown82}{Brown 82, theorem 1.5}, which is also reviewed as \hyperlink{RudolphSchmidt17}{Rudolph-Schmidt 17, Thm. 4.2.23 with Remark 4.2.25}. $\backslash$linebreak \hypertarget{finite_subgroups}{}\subsubsection*{{Finite subgroups}}\label{finite_subgroups} \begin{theorem} \label{ClassificationOfFiniteSubgroupsOfSO3}\hypertarget{ClassificationOfFiniteSubgroupsOfSO3}{} \textbf{([[ADE classification]] of [[finite group|finite]] [[subgroups]] of [[SO(3)]] and [[spin group|Spin(3)]]$\simeq$ [[SU(2)]])} The [[finite group|finite]] [[subgroups]] of the [[special orthogonal group]] $SO(3)$ as well as the [[finite group|finite]] [[subgroups]] of the [[special unitary group]] [[SU(2)]] are, up to [[conjugation]], given by the following classification: [[!include ADE -- table]] Here under the [[double cover]] projection (using the \href{spin+group#ExceptionalIsomorphisms}{exceptional isomorphism} $SU(2) \simeq Spin(3)$) \begin{displaymath} SU(2) \simeq Spin(3) \overset{\pi}{\longrightarrow} SO(3) \end{displaymath} all the finite subgroups of $SU(2)$ except the [[odd number|odd]]-[[order of a group|order]] [[cyclic groups]] are the [[preimages]] of the corresponding finite subgroups of $SO(3)$, in that we have [[pullback]] [[diagrams]] \begin{displaymath} \itexarray{ \left\langle \exp \left( \pi \mathrm{i} \tfrac{1}{n} \right) \right\rangle & = & \mathbb{Z}/(2n) &\overset{\phantom{AA}}{\hookrightarrow}& Spin(2) &\overset{\phantom{AA}}{\hookrightarrow}& Spin(3) \\ && \big\downarrow &{}^{(pb)}& \big\downarrow &{}^{(pb)}& \big\downarrow^{ \mathrlap{\pi} } \\ \left\langle Ad_{ \exp \left( \pi \mathrm{i} \tfrac{1}{n} \right) } \right\rangle & = & \mathbb{Z}/n &\overset{\phantom{AA}}{\hookrightarrow}& SO(2) &\overset{\phantom{AA}}{\hookrightarrow}& SO(3) } \end{displaymath} exhibiting the [[even number|even]] [[order of a group|order]] [[cyclic groups]] as subgroups of [[Spin(2)]], including the the minimal case of the [[group of order 2]] \begin{displaymath} \itexarray{ \left\langle \exp \left( \pi \mathrm{i} \right) = -1 \right\rangle & = & \mathbb{Z}/2 &\overset{\phantom{AA}}{\hookrightarrow}& Spin(2) &\overset{\phantom{AA}}{\hookrightarrow}& Spin(3) \\ && \big\downarrow &{}^{(pb)}& \big\downarrow &{}^{(pb)}& \big\downarrow^{ \mathrlap{\pi} } \\ \left\langle Ad_{ \exp \left( \pi \mathrm{i} \right) } = e \right\rangle & = & 1 &\overset{\phantom{AA}}{\hookrightarrow}& SO(2) &\overset{\phantom{AA}}{\hookrightarrow}& SO(3) } \end{displaymath} as well as \begin{displaymath} \itexarray{ \left\langle \exp\left( \pi \mathrm{i} \tfrac{1}{n} \right), \, \mathrm{j} \right\rangle &=& 2 D_{2n} &\overset{\phantom{AA}}{\hookrightarrow}& Pin_-(2) &\overset{\phantom{AA}}{\hookrightarrow}& Spin(3) \\ && \big\downarrow &{}^{(pb)}& \big\downarrow &{}^{(pb)}& \big\downarrow^{ \mathrlap{\pi} } \\ \left\langle Ad_{\exp\left( \pi \mathrm{i} \tfrac{1}{n} \right) }, \, Ad_{\mathrm{j}} \right\rangle && D_{2n} &\overset{\phantom{AA}}{\hookrightarrow}& O(2) &\overset{\phantom{AA}}{\hookrightarrow}& SO(3) } \end{displaymath} exhibiting the [[binary dihedral groups]] as sitting inside the [[Pin(2)]]-[[subgroup]] of [[Spin(3)]], but only [[commuting diagrams]] \begin{displaymath} \itexarray{ \left\langle \exp \left( 2 \pi \mathrm{i} \tfrac{1}{{2n+1}} \right) \right\rangle & = & \mathbb{Z}/(2n+1) &&\overset{\phantom{AA}}{\hookrightarrow}&& Spin(3) \\ && \big\downarrow && && \big\downarrow^{ \mathrlap{\pi} } \\ \left\langle Ad_{ \exp \left( 2 \pi \mathrm{i} \tfrac{1}{2n+1} \right) } \right\rangle & = & \mathbb{Z}/(2n+1) &\overset{\phantom{AA}}{\hookrightarrow}& SO(2) &\overset{\phantom{AA}}{\hookrightarrow}& SO(3) } \end{displaymath} for the [[odd number|odd]] [[order of a group|order]] [[cyclic group|cyclic]] [[subgroups]]. \end{theorem} This goes back to (\href{finite+rotation+group#Klein1884}{Klein 1884, chapter I}). Full proof for $SO(3)$ is spelled out for instance in (\href{finite+rotation+group#Rees05}{Rees 05, theorem 11}, \href{finite+rotation+group#DeVisscher11}{De Visscher 11}). The proof for the case of $SL(2,\mathbb{C})$ is spelled out in (\href{finite+rotation+group#MillerBlichfeldtDickson16}{Miller-Blichfeldt-Dickson 16}) reviewed in (\href{finite+rotation+group#Serrano14}{Serrano 14, section 2}). The proof of the case for $SU(2)$ given the result for $SO(3)$ is spelled out in \href{finite+rotation+group#Keenan03}{Keenan 03, theorem 4}. $\backslash$linebreak \hypertarget{related_concepts}{}\subsection*{{Related concepts}}\label{related_concepts} [[!include low dimensional rotation groups -- table]] \begin{itemize}% \item [[Euclidean group]] \item [[rigid body dynamics]] \end{itemize} $\backslash$linebreak \hypertarget{references}{}\subsection*{{References}}\label{references} \begin{itemize}% \item Jason Hanson, \emph{Rotations in three, four, and five dimensions} (\href{https://arxiv.org/abs/1103.5263}{arXiv:1103.5263}) \end{itemize} See also \begin{itemize}% \item Wikipedia, \emph{\href{https://en.wikipedia.org/wiki/3D_rotation_group}{3D rotation group}} \end{itemize} On the [[integral cohomology]] of the [[classifying space]]: \begin{itemize}% \item [[Edgar H. Brown]], \emph{The Cohomology of $B SO_n$ and $BO_n$ with Integer Coefficients}, Proceedings of the American Mathematical Society, Vol. 85, No. 2 (Jun., 1982), pp. 283-288 (\href{https://www.jstor.org/stable/2044298}{jstor:2044298}) \end{itemize} reviewed in \begin{itemize}% \item Gerd Rudolph, Matthias Schmidt, around Theorem 4.2.23 of \emph{Differential Geometry and Mathematical Physics: Part II. Fibre Bundles, Topology and Gauge Fields}, Theoretical and Mathematical Physics series, Springer 2017 (\href{https://link.springer.com/book/10.1007/978-94-024-0959-8}{doi:10.1007/978-94-024-0959-8}) \end{itemize} \end{document}