The word adjoint has a number of related meanings. In linear algebra, it refers to the conjugate transpose and is most commonly
denoted . The analogous concept applied to
an operator instead of a matrix, sometimes also known
as the Hermitian conjugate (Griffiths 1987, p. 22), is most commonly denoted
using dagger notation
(Arfken 1985). The adjoint operator is very common in both
Sturm-Liouville theory and quantum mechanics.
For example, Dirac (1982, p. 26) denotes the adjoint of the bra
vector
as
, or
.
Given a second-order ordinary differential equation
(1)
|
with differential operator
(2)
|
where and
, the adjoint operator
is defined by
(3)
| |||
(4)
|
Writing the two linearly independent solutions as and
, the adjoint operator can then also be written
(5)
| |||
(6)
|
In general, given two adjoint operators and
,
(7)
|
which can be generalized to
(8)
|