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# Differential operator

In mathematics, a differential operator is an operator defined as a function of the differentiation operator. It is helpful, as a matter of notation first, to consider differentiation as an abstract operation, accepting a function and returning another (in the style of a higher-order function in computer science).

This article considers mainly linear operators, which are the most common type. However, non-linear differential operators, such as the Schwarzian derivative also exist.

Notations

The most common differential operator is the action of taking the derivative itself. Common notations for taking the first derivative with respect to a variable x include:

\( {d \over dx}, D,\, D_x,\, and \partial_x. \)

When taking higher, nth order derivatives, the operator may also be written:

\( {d^n \over dx^n}, D^n\,, or D^n_x.\, \)

The derivative of a function f of an argument x is sometimes given as either of the following:

\( [f(x)]'\,\! \)

\( f'(x)\,\! \)

The D notation's use and creation is credited to Oliver Heaviside, who considered differential operators of the form

\( \sum_{k=0}^n c_k D^k \)

in his study of differential equations.

One of the most frequently seen differential operators is the Laplacian operator, defined by

\( \Delta=\nabla^{2}=\sum_{k=1}^n {\partial^2\over \partial x_k^2}. \)

Another differential operator is the Θ operator, or theta operator, defined by[1]

\( \Theta = z {d \over dz}. \)

This is sometimes also called the homogeneity operator, because its eigenfunctions are the monomials in z:

\( \Theta (z^k) = k z^k,\quad k=0,1,2,\dots \)

In n variables the homogeneity operator is given by

\( \Theta = \sum_{k=1}^n x_k \frac{\partial}{\partial x_k}. \)

As in one variable, the eigenspaces of Θ are the spaces of homogeneous polynomials.

The result of applying the differential to the left and to the right , and the difference obtained when applying the differential operator to the left and to the right, are denoted by arrows as follows:

\( {\mathrm{f}}{\overleftarrow\partial}_x g = g\partial_x \mathrm{f} \)

\( {\mathrm{f}}{\overrightarrow\partial}_x g = \mathrm{f}\partial_x g \)

\( {\mathrm{f}}{\overleftrightarrow\partial}_x g = \mathrm{f}\partial_x g -g\partial_x \mathrm{f} \)

Such a bidirectional-arrow notation is frequently used for describing the probability current of quantum mechanics.

Del

Main article: Del

The differential operator del is an important vector differential operator. It appears frequently in physics in places like the differential form of Maxwell's Equations. In three dimensional Cartesian coordinates, del is defined:

\( \nabla = \mathbf{\hat{x}} {\partial \over \partial x} + \mathbf{\hat{y}} {\partial \over \partial y} + \mathbf{\hat{z}} {\partial \over \partial z} \)

Del is used to calculate the gradient, curl, divergence, and laplacian of various objects.

Adjoint of an operator

See also: Hermitian adjoint

Given a linear differential operator T

\( Tu = \sum_{k=0}^n a_k(x) D^k u \)

the adjoint of this operator is defined as the operator \( T^* \) such that

\langle Tu,v \rangle = \langle u, T^*v \rangle \)

where the notation \( \langle\cdot,\cdot\rangle is used for the scalar product or inner product. This definition therefore depends on the definition of the scalar product.

Formal adjoint in one variable

In the functional space of square integrable functions, the scalar product is defined by

\( \langle f, g \rangle = \int_a^b f(x) \, \overline{g(x)} \,dx. \)

If one moreover adds the condition that f or g vanishes for x \to a and x \to b, one can also define the adjoint of T by

T^*u = \sum_{k=0}^n (-1)^k D^k [a_k(x)u].\, \)

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 (formally) self-adjoint operator is an operator equal to its own (formal) adjoint.

Several variables

If Ω is a domain in **R**^{n}, and *P* a differential operator on Ω, then the adjoint of *P* is defined in *L*^{2}(Ω) by duality in the analogous manner:

\( \langle f, P^* g\rangle_{L^2(\Omega)} = \langle P f, g\rangle_{L^2(\Omega)} \)

for all smooth *L*^{2} functions *f*, *g*. Since smooth functions are dense in *L*^{2}, this defines the adjoint on a dense subset of *L*^{2}: P^{*} is a densely-defined operator.

Example

The Sturm–Liouville operator is a well-known example of a formal self-adjoint operator. This second-order linear differential operator L can be written in the form

\( Lu = -(pu')'+qu=-(pu''+p'u')+qu=-pu''-p'u'+qu=(-p) D^2 u +(-p') D u + (q)u.\;\! \)

This property can be proven using the formal adjoint definition above.

\( \begin{align} L^*u & {} = (-1)^2 D^2 [(-p)u] + (-1)^1 D [(-p')u] + (-1)^0 (qu) \\ & {} = -D^2(pu) + D(p'u)+qu \\ & {} = -(pu)''+(p'u)'+qu \\ & {} = -p''u-2p'u'-pu''+p''u+p'u'+qu \\ & {} = -p'u'-pu''+qu \\ & {} = -(pu')'+qu \\ & {} = Lu \end{align} \)

This operator is central to Sturm–Liouville theory where the eigenfunctions (analogues to eigenvectors) of this operator are considered.

Properties of differential operators

Differentiation is linear, i.e.,

\( D(f+g) = (Df)+(Dg)\, \)

\( D(af) = a(Df)\, \)

where f and g are functions, and a is a constant.

Any polynomial in D with function coefficients is also a differential operator. We may also compose differential operators by the rule

\( (D_1 \circ D_2)(f) = D_1(D_2(f)).\, \)

Some care is then required: firstly any function coefficients in the operator *D*_{2} must be differentiable as many times as the application of *D*_{1} requires. To get a ring of such operators we must assume derivatives of all orders of the coefficients used. Secondly, this ring will not be commutative: an operator *gD* isn't the same in general as *Dg*. In fact we have for example the relation basic in quantum mechanics:

\( Dx - xD = 1.\, \)

The subring of operators that are polynomials in D with constant coefficients is, by contrast, commutative. It can be characterised another way: it consists of the translation-invariant operators.

The differential operators also obey the shift theorem.

Several variables

The same constructions can be carried out with partial derivatives, differentiation with respect to different variables giving rise to operators that commute (see symmetry of second derivatives).

Coordinate-independent description

In differential geometry and algebraic geometry it is often convenient to have a coordinate-independent description of differential operators between two vector bundles. Let *E* and *F* be two vector bundles over a differentiable manifold *M*. An **R**-linear mapping of sections *P* : Γ(*E*) → Γ(*F*) is said to be a ** kth-order linear differential operator** if it factors through the jet bundle

*J*

^{k}(

*E*). In other words, there exists a linear mapping of vector bundles

\( i_P: J^k(E) \rightarrow F\, \)

such that

P = i_P\circ j^k \)

where jk: Γ(E) → Γ(Jk(E)) is the prolongation that associates to any section of E its k-jet.

This just means that for a given sections s of E, the value of P(s) at a point x ∈ M is fully determined by the kth-order infinitesimal behavior of s in x. In particular this implies that P(s)(x) is determined by the germ of s in x, which is expressed by saying that differential operators are local. A foundational result is the Peetre theorem showing that the converse is also true: any (linear) local operator is differential.

Relation to commutative algebra

An equivalent, but purely algebraic description of linear differential operators is as follows: an R-linear map P is a kth-order linear differential operator, if for any k + 1 smooth functions \( f_0,\ldots,f_k \in C^\infty(M) \) we have

\( [f_k,[f_{k-1},[\cdots[f_0,P]\cdots]]=0. \)

Here the bracket [f,P]:\Gamma(E)\rightarrow \Gamma(F) is defined as the commutator

\( [f,P](s)=P(f\cdot s)-f\cdot P(s).\, \)

This characterization of linear differential operators shows that they are particular mappings between modules over a commutative algebra, allowing the concept to be seen as a part of commutative algebra.

Examples

In applications to the physical sciences, operators such as the Laplace operator play a major role in setting up and solving partial differential equations.

In differential topology the exterior derivative and Lie derivative operators have intrinsic meaning.

In abstract algebra, the concept of a derivation allows for generalizations of differential operators which do not require the use of calculus. Frequently such generalizations are employed in algebraic geometry and commutative algebra. See also jet (mathematics).

History

The conceptual step of writing a differential operator as something free-standing is attributed to Louis François Antoine Arbogast in 1800.[2]

See also

Difference operator

Delta operator

Elliptic operator

Fractional calculus

Invariant differential operator

Differential calculus over commutative algebras

Lagrangian system

Spectral theory

References

^ E. W. Weisstein. "Theta Operator". Retrieved 2009-06-12.

^ James Gasser (editor), A Boole Anthology: Recent and classical studies in the logic of George Boole (2000), p. 169; Google Books.

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