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In particular, if are classical pseudo-differential operators of orders and , then is a classical pseudo-differential operator of order with principal symbol , where and are the principal symbols of and. If , , then there exists a, moreover unique, adjoint pseudo-differential operator for which , , where is the inner product of and in.

Pseudo-Differential Operators and Generalized Functions

If, moreover, , is the symbol of and is the symbol of , then. Thus, the properly supported pseudo-differential operators for form an algebra with involution given by transition to the adjoint operator. The arbitrary pseudo-differential operators form a module over this algebra.

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In particular, under the conditions 5 pseudo-differential operators of the form 1 with symbols satisfying conditions 2 uniformly in i. This implies, e. For or for , operators of such a form need not be bounded [19a]. Analogously, in general, if one of the two latter conditions of 5 are not fulfilled, then one already obtains a class of pseudo-differential operators that contains unbounded ones.

If an operator is given on , where , and where 2 holds uniformly in , then this operator can be extended to a bounded operator , , where denotes the usual Sobolev space over which is sometimes denoted also by. The class of pseudo-differential operators in for is naturally invariant under diffeomorphisms. Its subclass of classical pseudo-differential operators has the same property.

This makes it possible to define the class and classical pseudo-differential operators on an arbitrary smooth manifold. The formula for change of variables in the symbol under a diffeomorphism , where are domains in , has the form. Here is the symbol of ; is the symbol of the operator given by , i. In particular, this implies that the principal symbol of a classical pseudo-differential operator on a manifold is a well-defined function on the cotangent bundle. If is a compact manifold without boundary , then the pseudo-differential operators on form an algebra with involution, if the involution is introduced by means of an inner product, given by a smooth positive density.

An operator is bounded in , and if for , then it is compact in. For classical pseudo-differential operators of order on ,.

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An operator can by continuity be extended to a bounded linear operator from into for any. A parametrix of a pseudo-differential operator is a pseudo-differential operator such that and are pseudo-differential operators of order , i. Suppose that , , and that is the symbol of.

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A sufficient condition for to have a parametrix is that the conditions. In this case a parametrix exists. The simplest implication from the existence of a parametrix is that is a hypo-elliptic operator: If , where , then. In other words, cf. Support of a generalized function. The following exact result the regularity theorem is also valid: If , then.

A micro-local regularity theorem is also valid: , where denotes the wave front of the generalized function. Condition 6 is invariant under diffeomorphisms for. Therefore the corresponding class of pseudo-differential operators on a manifold has a meaning.

If is compact, then such an operator is Fredholm in cf. Fredholm operator , i. A classical pseudo-differential operator of order with smooth symbol is called elliptic if for. For such an operator condition 6 holds with , and has a parametrix that is also a classical pseudo-differential operator of order. On a compact manifold such an operator gives rise to a Fredholm operator. All these definitions and statements can be transferred to pseudo-differential operators acting on vector functions, or, more generally, on sections of vector bundles. For an elliptic operator on a compact manifold the index of the mapping determined by it on the Sobolev classes of sections does not depend on and can be explicitly computed cf.

Index formulas. The role of pseudo-differential operators lies in the fact that there is a number of operations leading outside the class of differential operators but preserving the class of pseudo-differential operators. There are several versions of the theory of pseudo-differential operators, adapted to the solution of various problems in analysis and mathematical physics. Often, pseudo-differential operators with a parameter arise; they are necessary, e.

An important role is played by different versions of the theory of pseudo-differential operators in , taking into account effects related to the description of the behaviour of functions at infinity, and often inspired by mathematical problems in quantum mechanics arising in the study of quantization of classical systems cf. In the theory of local solvability of partial differential equations and in spectral theory it is expedient to use pseudo-differential operators whose behaviour can be described by weight functions replacing in estimates of the type 2 cf.

Featuring both essays and research articles, the book will be of great interest to graduate students and researchers working in analysis, PDE and mathematical physics, while also offering a valuable complement to the volumes on this topic previously published in the OT series. Skip to main content Skip to table of contents. Advertisement Hide.

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Pseudo-Differential Operators and Generalized Functions. Conference proceedings.

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Papers Table of contents 19 papers About About these proceedings Table of contents Search within book. Front Matter Pages i-viii. See all formats and pricing Online. Prices are subject to change without notice. Prices do not include postage and handling if applicable. Volume 21 Issue 6 Dec , pp.

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Volume 15 Issue 4 Dec , pp. Volume 14 Issue 4 Dec , pp. Previous Article. Next Article. Dissipation and free energies Recent developments on stochastic heat equation with additive fractional-colored noise Justification of the empirical laws of the anomalous dielectric relaxation in the framework of the memory function formalism LP-solutions for fractional integral equations Remark to the paper of S.

Boundedness of pseudo-differential operator associated with fractional Hankel transform.