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Eigenvalues and Eigenvectors
In general, the ket
$ X,円\vert A\rangle$
is not a constant multiple of $ \vert A\rangle$
.
However, there are some special kets
known as the
eigenkets of operator $ X$
. These are denoted
and have the property
where $ x'$
, $ x''$
, $ \ldots$
are numbers called
eigenvalues. Clearly, applying $ X$
to one of its
eigenkets yields the same eigenket multiplied by the associated eigenvalue.
Consider the eigenkets and eigenvalues of a Hermitian operator $ \xi$
. These are
denoted
where
$ \vert\xi'\rangle$
is the eigenket associated with the eigenvalue $ \xi'$
.
Three important results are readily deduced:
(i) The eigenvalues are all real numbers, and the eigenkets corresponding
to different eigenvalues are orthogonal.
Since $ \xi$
is Hermitian, the dual equation to Equation (44) (for the eigenvalue
$ \xi''$
) reads
If we left-multiply Equation (
44) by
$ \langle \xi''\vert$
, right-multiply the above
equation by
$ \vert\xi'\rangle$
, and take the difference, we obtain
Suppose that the eigenvalues $ \xi'$
and $ \xi''$
are the same. It follows from the
above that
where we have used the fact that
$ \vert\xi'\rangle$
is not the null ket. This proves
that the eigenvalues are real numbers. Suppose that the eigenvalues
$ \xi'$
and $ \xi''$
are different. It follows that
which demonstrates that eigenkets corresponding to different eigenvalues are
orthogonal.
(ii) The eigenvalues associated with eigenkets are the same as the eigenvalues
associated with eigenbras. An eigenbra of $ \xi$
corresponding to an eigenvalue
$ \xi'$
is defined
(iii) The dual of any eigenket is an eigenbra belonging to the same eigenvalue,
and conversely.
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Richard Fitzpatrick
2013年04月08日