# Conserved quantity corresponding to reflection symmetry

I know about Noether's theorem, but I don't actually know how to use it myself. Suppose our universe were symmetric with respect to reflections about planes. What conserved quantity would then exist by Noether's theorem?

But, in quantum mechanics, you have the parity operator $P$, that reflects the coordinates $$P\psi(\vec{r}) = \psi(-\vec{r})$$ Since $P^2 = I$, the operator $P$ has eigenvalues $\pm 1$. If the hamiltonian is invariant under reflection, i.e. $[H,P]=0$, every eigenfunction of the hamiltonian is also a eigenfunction of the parity operator with eigenvalue $p$ (called intrinsic parity). Then, the intrinsic parity is conserved.
• If we had reflectional symmetry, then we would have $O(3)$ symmetry, which is a Lie group. Jun 20, 2015 at 22:03
• No, reflections are a discrete subgroup of $O(3)$, namely $O(3) = SO(3) \times \{I, -I\}$ is the direct product of the group of rotations (which is the Lie group) and the reflection group. In fact, is quite easy to find examples with reflection symmetry but not the whole $O(3)$ symmetry: a cube or an octahedron with the origin at their centers, for example. Jun 20, 2015 at 22:47
• I meant that our universe is already symmetric under $SO(3)$, so adding in rotational symmetry yields $O(3)$ symmetry. Jun 20, 2015 at 22:56
• Right, but the conserved quantities via Noether's theorem for $SO(3)$ and $O(3)$ are the same (angular moment). Adding the reflections doesn't add any new conserved quantity because they aren't a Lie group but a discrete group. Jun 20, 2015 at 23:06