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)
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with differential operator
|
(2)
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where and
, the adjoint operator
is defined by
|
(3)
| |||
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(4)
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Writing the two linearly independent solutions as and
, the adjoint operator can then also be written
|
(5)
| |||
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(6)
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In general, given two adjoint operators and
,
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(7)
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which can be generalized to
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(8)
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