Matrix Representation of an Operator (from Sakurai)

[jaurandt]

Look, I am sorry for not being able to post any LaTeX. But I am stuck at a place where I feel I should not be stuck.

I can not figure out how to correctly do this. I can't seem to recreate the Pauli matrices with that form using the 3 2-dimensional bases representing x, y, and z spin up/down.

Does anyone have any advice on this?

 

[HomogenousCow]

Just to be clear, you're trying to project the spin matrices in an eigenspin bases right? (say in the z-direction) You only need the spin up and spin down vectors in anyone direction to form a complete basis.
For $\sigma_z$ this is trivial in its eigenbasis:
$$\sigma_z = \sum_s \sum_r |s\rangle\langle s|\sigma_z|r\rangle\langle r|$$
$$\sigma_z = |\uparrow \rangle \langle \uparrow | - | \downarrow \rangle \langle \downarrow |$$

For $\sigma_x$ and $\sigma_y$ you could use the raising and lowering operators to make the same decomposition.

 

[jaurandt]

Just to be clear, you're trying to project the spin matrices in an eigenspin bases right? (say in the z-direction) You only need the spin up and spin down vectors in anyone direction to form a complete basis.
For $\sigma_z$ this is trivial in its eigenbasis:
$$\sigma_z = \sum_s \sum_r |s\rangle\langle s|\sigma_z|r\rangle\langle r|$$
$$\sigma_z = |\uparrow \rangle \langle \uparrow | - | \downarrow \rangle \langle \downarrow |$$

For $\sigma_x$ and $\sigma_y$ you could use the raising and lowering operators to make the same decomposition.

Can you please give the same example, but with the $\sigma_y$ operator? What I'm trying to say is that I don't understand how

$$\sigma_z = \sum_s \sum_r |s\rangle\langle s|\sigma_z|r\rangle\langle r|$$

Reveals the entries of the matrix...

 

[andresB]

The numbers $$\left\langle a'\right|X\left|a''\right\rangle $$
are the entries of the matrix. For the z Pauli matrix we have $$
\left\langle \uparrow\right|\sigma_{z}\left|\uparrow\right\rangle =1;
\left\langle \downarrow\right|\sigma_{z}\left|\uparrow\right\rangle =0;
\left\langle \uparrow\right|\sigma_{z}\left|\downarrow\right\rangle =0;
\left\langle \downarrow\right|\sigma_{z}\left|\downarrow\right\rangle =-1$$

 

[HomogenousCow]

You don't even have to deal with matrices if you don't want to, all that's happening is we're rewriting the operator by inserting some identity operators. Since $$I = \sum_s |s\rangle\langle s|,$$ we can just stick one in front of and behind an operator to rewrite it in terms of the operator basis $|s \rangle \langle r|$,
$$A = I A I = \sum_s \sum_r |s\rangle\langle s| A |r\rangle\langle r| = \sum_s \sum_r A_{sr} |s\rangle \langle r|,$$ where $A_{sr}$ are the matrix elements.

 

[jaurandt]

The numbers $$\left\langle a'\right|X\left|a''\right\rangle $$
are the entries of the matrix. For the z Pauli matrix we have $$
\left\langle \uparrow\right|\sigma_{z}\left|\uparrow\right\rangle =1;
\left\langle \downarrow\right|\sigma_{z}\left|\uparrow\right\rangle =0;
\left\langle \uparrow\right|\sigma_{z}\left|\downarrow\right\rangle =0;
\left\langle \downarrow\right|\sigma_{z}\left|\downarrow\right\rangle =-1$$

So then what happens to the rest of the construct if you just pull out

$$\left\langle a'\right|X\left|a''\right\rangle $$

What happened to the summation and what becomes of $$\left|a'\right\rangle\left\langle a''\right| $$

 

[andresB]

So then what happens to the rest of the construct if you just pull out

$$\left\langle a'\right|X\left|a''\right\rangle $$

What happened to the summation and what becomes of $$\left|a'\right\rangle\left\langle a''\right| $$

Put everything in the formula and you have the representation of the operator in that basis of vectors. HomogenousCow already showed how the z Pauli operator looks like written in terms of its own set of eigenvectors.

 

[kith]

The object $|a' \rangle \langle a''|$ is an operator. Every entry in a representation matrix is tied to such an operator.

Consider this rewrite of the third Pauli matrix:
<br /> \begin{pmatrix}<br /> 1 &amp; 0\\<br /> 0 &amp; -1<br /> \end{pmatrix}<br /> <br /> =<br /> <br /> 1 \cdot<br /> \begin{pmatrix}<br /> 1 &amp; 0\\<br /> 0 &amp; 0<br /> \end{pmatrix}<br /> <br /> +<br /> <br /> 0 \cdot<br /> \begin{pmatrix}<br /> 0 &amp; 1\\<br /> 0 &amp; 0<br /> \end{pmatrix}<br /> <br /> +<br /> <br /> 0 \cdot<br /> \begin{pmatrix}<br /> 0 &amp; 0\\<br /> 1 &amp; 0<br /> \end{pmatrix}<br /> <br /> +<br /> <br /> (-1) \cdot<br /> \begin{pmatrix}<br /> 0 &amp; 0\\<br /> 0 &amp; 1<br /> \end{pmatrix}<br />
This is what corresponds to the operator equation
$\sigma_z = 1 \cdot |\!\uparrow_z \rangle \langle \uparrow_z \!| + 0 \cdot |\!\uparrow_z \rangle \langle \downarrow_z\!| + 0 \cdot |\!\downarrow_z \rangle \langle \uparrow_z\!| + (-1) \cdot |\!\downarrow_z \rangle \langle \downarrow_z\!|.$

(Note that the symbol $\sigma_z$ is ofen used to symbolize both the operator and its matrix representation in the z-basis. This is a sloppy but very common notation.)