Quantum Mechanics: Matrix Representation

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SUMMARY

The matrix representation of the angular momentum operator ##\mathbb{\hat J}_z## in the ##|+y\rangle## and ##|-y\rangle## basis is derived using the completeness relation and the known matrix elements in the ##|+z\rangle## and ##|-z\rangle## basis. The solution shows that ##\mathbb{\hat J}_z## can be expressed as ##\frac{\hbar}{2}\left[{\begin{array}{cc} 0 & 1 \\ 1 & 0 \\\end{array}}\right]## after transforming the basis. The process involves inserting the identity operator and calculating the necessary inner products to transition between bases.

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Robben
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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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