What is the commutator between S_{z}^{n} and S_{y}?

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SUMMARY

The discussion focuses on calculating the commutator \(\left[ S_{z}^{n}, S_{y} \right]\) where \(S_{z}\) and \(S_{y}\) are quantum mechanical spin matrices. The established result is that the commutator is non-zero and equals \(-i\hbar S_{x} S_{z}^{n-1}\) when \(n\) is odd, while it commutes to zero for even \(n\). This conclusion is derived from the properties of Pauli matrices and their commutation relations, specifically \(\left[ S_{z}, S_{y} \right] = -i\hbar S_{x}\) and \(\{ S_{x}, S_{z} \} = 0\).

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Homework Statement


The entire problem is quite in depth. But what I am having trouble with is just a small part of it, and it boils down to finding the following commutator:
\left[ S_{z}^{n},S_{y}\right]
where S_{z} and S_{y} are the quantum mechanical spin matrices.

The reason is that I have to commute S_{y} with an exponential that has S_{z} in it. So I expand the exponential as a series which contains S_{z}^{n}, so I need to find the above commutator.

Homework Equations


\left[ S_{z},S_{y}\right] =-i\hbar S_{x}
\{ S_{x},S_{z}\}=0

The Attempt at a Solution


S_{z}^{n}S_{y}=S_{z}^{n-1}(S_{z}S_{y})=S_{z}^{n-1}(S_{y}S_{z}-i\hbar S_{x})
=S_{z}^{n-2}(S_{z}S_{y}S_{z}-i\hbar S_{z}S_{x})
=S_{z}^{n-2}((S_{y}S_{z}-i\hbar S_{x})S_{z}-i\hbar S_{z}S_{x})
=S_{z}^{n-2}(S_{y}S_{z}S_{z}-i\hbar (S_{x}S_{z}+S_{z}S_{x}))
By the anticommutator relation for X and Z given above, the inner parenthesis is zero:
=S_{z}^{n-2}S_{y}S_{z}S_{z}

This seems very strange though, otherwise it appears that if I keep doing this then as long as "n" is an even number, then \left[ S_{z}^{n},S_{y}\right] will commute.
and that the commutator will only be different from zero, with a value of -i\hbar S_{x}S_{z}^{n-1} only if "n" is odd.

Is this right?
 
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Try taking a few powers of the pauli matrices and notice what happens to even and odd powers of them, you should see why an even power of any pauli matrix commutes with any power of any pauli matrix
With this knowledge in hand, notcie what -i \hbar S_x S_z^{n-1} reduces to for odd n!

You are right but you went on quite a convoluted path to get there :p
 

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