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Differential operator - Adjoint of an operator |  | Differential operator - Adjoint of an operator: Encyclopedia II - Differential operator - Adjoint of an operator |  | Given a linear differential operator
the adjoint of this operator is defined as the operator T * such that
where the notation is used for the scalar product or inner product. This definition therefore depends on the definition of the scalar product. In the functional space of square integrable functions, the scalar product is defined by
.
If one moreover adds the condition that f and g vanish for and , one ...
See also:Differential operator, Differential operator - Notations, Differential operator - Adjoint of an operator, Differential operator - Properties of differential operators, Differential operator - Several variables, Differential operator - Coordinate-independent description, Differential operator - Examples |  | | Differential operator, Differential operator - Adjoint of an operator, Differential operator - Coordinate-independent description, Differential operator - Examples, Differential operator - Notations, Differential operator - Properties of differential operators, Differential operator - Several variables, Difference operator, Delta operator, Elliptic operator, Fractional calculus |  | |
|  |  | Differential operator: Encyclopedia II - Differential operator - Adjoint of an operator
Differential operator - Adjoint of an operator
Given a linear differential operator
the adjoint of this operator is defined as the operator T * such that
where the notation is used for the scalar product or inner product. This definition therefore depends on the definition of the scalar product. In the functional space of square integrable functions, the scalar product is defined by
.
If one moreover adds the condition that f and g vanish for and , one can also define the adjoint of T by
.
This formula does not explicitly depend on the definition of the scalar product. It is therefore sometimes chosen as a definition of the adjoint operator. When T * is defined according to this formula, it is called the formal adjoint of T.
A self-adjoint operator is an operator adjoint of itself.
The Sturm-Liouville operator is a well-known example of formal self-adjoint operator. This second order linear differential operators L can be written in the form
This property can be proven using the formal adjoint definition above.
This operator is central to Sturm-Liouville theory where the eigenfunctions (analogues to eigenvectors) of this operator are considered.
Other related archivesDelta operator, Difference operator, Differential operators, Elliptic operator, Fractional calculus, Laplace operator, Laplacian operator, Lie derivative, Multivariate calculus, Oliver Heaviside, Peetre theorem, Sturm-Liouville, Sturm-Liouville theory, abstract algebra, algebraic geometry, commutative, commutative algebra, computer science, coordinate, derivation, differentiable, differential equations, differential geometry, differential topology, differentiation, eigenfunctions, eigenvectors, exterior derivative, fibre, germs, higher-order function, inner product, jet bundle, linear, linear operator, manifold, mathematics, operator, partial derivatives, partial differential equations, quantum mechanics, ring, scalar product, sections, sheaf, square integrable, stalk, symmetry of second derivatives, vector bundles
 Adapted from the Wikipedia article "Adjoint of an operator", under the G.N U Free Docmentation License. Please also see http://en.wikipedia.org/wiki |
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