Matrix Representation: What Happens to |a''><a'|?

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SUMMARY

The discussion focuses on the matrix representation of operators in quantum mechanics, specifically examining the transformation of the expression X = ∑_{a''} ∑_{a'} |a''> and |a'> are not disregarded but are represented as matrix elements, where |a'> corresponds to column indices and |a''> to row indices. The transformation to matrix notation involves summing over orthonormal sets, leading to a clear representation of operators as matrices defined by their elements .

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indigojoker
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let X be an operator, we can write X as a matrix where:

[tex]X = \sum_{a''} \sum_{a'} |a''><a''|X|a'><a'|[/tex]

where [tex]<a''|X|a'>[/tex] a'' are the rows and a' are the columns. I was wondering what happened to the |a''> <a'|?

It seems like they are disregarded when transforming to matrix notation. I was wondering why that is?
 
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this is "only" a representation.

<a'| is a ket and "runs" like a column matrix; so the a' in the matrix element <a'' | X | a'> becomes the column indicies. |a''> is a bra and "runs" like a row matrix; so the a'' becomes row indices.
 
indigojoker said:
let X be an operator, we can write X as a matrix where:

[tex]X = \sum_{a''} \sum_{a'} |a''><a''|X|a'><a'|[/tex]

where [tex]<a''|X|a'>[/tex] a'' are the rows and a' are the columns. I was wondering what happened to the |a''> <a'|?

It seems like they are disregarded when transforming to matrix notation. I was wondering why that is?

let's look at a simple example where
[tex]|a''\rangle, |a'\rangle \in \left\{ \begin{bmatrix}1\\0 \end{bmatrix}, <br /> \begin{bmatrix}0\\1\end{bmatrix} \right\}[/tex]
are orthonormal sets
so eg.
[tex]\sum_{a'} |a'\rangle\langle a'| = <br /> \begin{bmatrix}1 \\ 0 \end{bmatrix}<br /> \begin{bmatrix}1&0 \end{bmatrix}+<br /> \begin{bmatrix}0 \\ 1 \end{bmatrix}<br /> \begin{bmatrix}0&1 \end{bmatrix} = \begin{bmatrix}1 & 0\\ 0& 1 \end{bmatrix}[/tex]
and now

[tex]\sum_{a', a''} |a''\rangle\langle a''| X |a'\rangle\langle a'| =<br /> \sum_{a', a''} \langle a''| X |a'\rangle |a''\rangle\langle a'|[/tex]
because [tex]\langle a''| X |a'\rangle[/tex] is just a complex number at the appropriate position defined by the "index" of a' and a''
and because
[tex]\sum_{a', a''} |a''\rangle\langle a'| = <br /> \begin{bmatrix}1 \\ 0 \end{bmatrix}<br /> \begin{bmatrix}1&0 \end{bmatrix}+<br /> \begin{bmatrix}1 \\ 0 \end{bmatrix}<br /> \begin{bmatrix}0&1 \end{bmatrix}+<br /> \begin{bmatrix}0 \\ 1 \end{bmatrix}<br /> \begin{bmatrix}0&1 \end{bmatrix} +<br /> \begin{bmatrix}0 \\ 1 \end{bmatrix}<br /> \begin{bmatrix}1&0 \end{bmatrix} <br /> = \begin{bmatrix}1 & 0\\ 0& 0 \end{bmatrix} +<br /> \begin{bmatrix}0 & 1\\ 0& 0 \end{bmatrix}+<br /> \begin{bmatrix}0 & 0\\ 0& 1 \end{bmatrix}+<br /> \begin{bmatrix}0 & 0\\ 1& 0 \end{bmatrix}[/tex]

the above four 2x2 matrices form a set of basis states for any generic 2x2 operator X with complex entries. As you can see from the original sum of X, for each a' and a'', the basis matrix is multiplied by the corresponding complex number defined by [tex]\langle a''| X |a'\rangle[/tex]. does this answer your question:
what happened to the |a''> <a'|?
all you have done in going to the index notation is implicitly assumed a set of basis matrices so that [tex]\langle i| X |j\rangle[/tex] means ij element of the matrix.
 

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