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Eigenvalues and Eigenvectors
In general, the ket
is not a constant multiple of the ket
.
However, there are some special kets
known as the eigenkets of operator
. These are denoted
|
(1.45) |
and have the property
where
,
,
,
are complex numbers called
eigenvalues. Clearly, applying
to one of its
eigenkets yields the same eigenket multiplied by the associated eigenvalue.
Consider the eigenkets and eigenvalues of an Hermitian operator
. These are
denoted
|
(1.47) |
where
is the eigenket associated with the eigenvalue
.
Three important results are readily deduced:
- The eigenvalues are all real numbers, and the eigenkets corresponding
to different eigenvalues are orthogonal.
Because
is Hermitian, the dual equation to Equation (1.47) (for the eigenvalue
) reads
|
(1.48) |
If we left-multiply Equation (1.47) by
, right-multiply the previous
equation by
, and take the difference, then we obtain
|
(1.49) |
Suppose that the eigenvalues
and
are the same. It follows from the
previous equation that
|
(1.50) |
where we have used the fact that
is not the null ket. This proves
that the eigenvalues are real numbers. Suppose that the eigenvalues
and
are different. It follows that
|
(1.51) |
which demonstrates that eigenkets corresponding to different eigenvalues are
orthogonal.
- The eigenvalues associated with eigenkets are the same as the eigenvalues
associated with eigenbras. An eigenbra of
corresponding to an eigenvalue
is defined
|
(1.52) |
- The dual of any eigenket is an eigenbra belonging to the same eigenvalue,
and conversely.
Next: Observables
Up: Fundamental Concepts
Previous: Outer Product
Richard Fitzpatrick
2016-01-22