Commutator SO(3) - what am I doing wrong?

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    Commutator So(3)
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The discussion centers on the commutation of rotation matrices in the context of the special orthogonal group SO(3). The user attempted to compute the commutator of two rotation matrices using Maxima, resulting in a matrix with a determinant of zero, indicating it is not part of SO(3). The resolution highlights the distinction between the Lie group SO(3) and its Lie algebra, emphasizing that the commutation relation applies to the generators of the Lie algebra rather than the group itself.

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BWV
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reading that the commutator of rotations on two orthogonal axes is i * the rotation matrix for the third axis

but if I commute this

\begin{pmatrix}\mathrm{cos}\left( \theta\right) & -\mathrm{sin}\left( \theta\right) & 0\cr \mathrm{sin}\left( \theta\right) & \mathrm{cos}\left( \theta\right) & 0\cr 0 & 0 & 1\end{pmatrix}

with this

\begin{pmatrix}1 & 0 & 0\cr 0 & \mathrm{cos}\left( \theta\right) & -\mathrm{sin}\left( \theta\right) \cr 0 & \mathrm{sin}\left( \theta\right) & \mathrm{cos}\left( \theta\right) \end{pmatrix}

I get (using innerproduct function in Maxima)
\begin{pmatrix}0 & \mathrm{cos}\left( \theta\right) \,\mathrm{sin}\left( \theta\right) -\mathrm{sin}\left( \theta\right) & -{\mathrm{sin}\left( \theta\right) }^{2}\cr \mathrm{cos}\left( \theta\right) \,\mathrm{sin}\left( \theta\right) -\mathrm{sin}\left( \theta\right) & 0 & \mathrm{cos}\left( \theta\right) \,\mathrm{sin}\left( \theta\right) -\mathrm{sin}\left( \theta\right) \cr {\mathrm{sin}\left( \theta\right) }^{2} & \mathrm{cos}\left( \theta\right) \,\mathrm{sin}\left( \theta\right) -\mathrm{sin}\left( \theta\right) & 0\end{pmatrix}

which has a determinant of zero and therefore not part of SO(3)

obviously I am not getting something, but don't see it. Any help is much appreciated
 
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you are confusing the Lie group and the Lie algebra. The commutation
relation applies to the Lie algebra (ie the generators of the Lie group).
 
ah, thanks.
 

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