Quantum Mechanics: Matrix Representation

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The discussion focuses on finding the matrix representation of the operator \(\mathbb{\hat J}_z\) using the states \(|+y\rangle\) and \(|-y\rangle\) as a basis. The solution involves expressing \(|\pm y\rangle\) in terms of the \(|\pm z\rangle\) states and utilizing the completeness relation to transform the known matrix elements of \(\mathbb{\hat J}_z\) in the z-basis to the y-basis. The matrix representation is derived as \(\frac{\hbar}{2}\left[\begin{array}{cc} 0 & 1 \\ 1 & 0 \end{array}\right]\). The conversation clarifies the process of inserting the identity matrix and the importance of understanding the notation for matrix elements versus the matrices themselves. Overall, the explanation helps solidify the concept of changing bases in quantum mechanics.
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Homework Statement


What is the matrix representation of ##\mathbb{\hat J}_z## using the states ##|+y\rangle## and ##|-y\rangle## as a basis?

Homework Equations



##|\pm y\rangle =\frac{1}{\sqrt{2}}|+z\rangle \pm \frac{i}{\sqrt{2}}|-z\rangle##

The Attempt at a Solution



A solution was given:

##\mathbb{\hat J}_z =\left[{\begin{array}{cc} \langle +y|+z\rangle & \langle +y|-z\rangle \\ \langle -y|+z\rangle & \langle -y|-z\rangle \\\end{array}}\right]\frac{\hbar}{2}\left[{\begin{array}{cc} 1 & 0 \\ 0 & -1 \\\end{array}}\right]
\left[{\begin{array}{cc} \langle +z|+y\rangle & \langle +z|-y\rangle \\ \langle -z|+y\rangle & \langle -z|-y\rangle \\\end{array}}\right] = \frac{\hbar}{2}\left[{\begin{array}{cc} 0 & 1 \\ 1 & 0 \\\end{array}}\right],##

but I am confused on what is going on? Can anyone explain exactly what is going on, please?
 
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You have the operator \mathbb{\hat J}_z. Normally you represent that in the z-basis, so in matrix notation the 4 matrix elements that you already know are \langle \pm z \mid \mathbb{\hat J}_z \mid \pm z \rangle. If you want to represent \mathbb{\hat J}_z in another basis like y you have to know the matrix elements \langle \pm y \mid \mathbb{\hat J}_z \mid \pm y \rangle . One way to do this is to insert a unit operator/identity matrix on both sides as this has no effect:
\langle \pm z \mid \mathbb{I} \mathbb{\hat J}_z \mathbb{I} \mid \pm z \rangle

Now if you know that you can write the identity matrix as \sum \mid z \rangle \langle z \mid using the completeness relation you are practically done:

\langle \pm y \mid \mathbb{I} \mathbb{\hat J}_z \mathbb{I} \mid \pm y \rangle = \langle \pm y \mid z \rangle \langle z \mid \mathbb{\hat J}_z \mid z \rangle \langle z \mid \pm y \rangle

So the middle part \langle z \mid \mathbb{\hat J}_z \mid z \rangle is the matrix in the already known basis
\frac{\hbar}{2}\left[{\begin{array}{cc} 1 & 0 \\ 0 & -1 \\\end{array}}\right] And the outer parts are the matrices to transform it into an y basis.

(Note: I mix up the notation for matrix elements and the matrix itself. I probably miss a summation here and there, but I hope you understand the difference)
 
I think I understand now. Thank you very much!
 

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