Abstract
dc:description.abstractConsider the operator${\bf P} = {\partial\over\partial t} + α{\partial m\over \partial z m},\qquad α \in {\bf C} - \{0\}$where $$\partial\over{\partial z}$$ is the usual complex operator:${\partial\over\partial z} = {1\over 2} \left({\partial\over\partial x} - i{\partial\over\partial y}\right).$When m = 2 and $\alpha$ = $-$1, P bears a remarkable resemblance to the heat operator in one space variable. The "only" difference is that the space variable is now complex. In spite of this superficial similarity, P is quite different from the heat operator. It is neither hypoelliptic nor parabolic. The key result is a formula for a fundamental solution, E. It is obtained formally using Fourier transforms. The formula is a linear combination of Fresnel-like integrals, divided by z and a power of t. It is a $$C\infty$$ function except across t = 0. It has a homogeneity property which is similar to the one the standard fundamental solution for the heat operator possesses. It has a skew-reflection property in the time variable. The proof that E is a fundamental solution is done by applying PE to a test function. It is similar to the standard analogous proof for the heat equation. The main difference is that E is not integrable for fixed non-zero t. Thus we do our calculations with Fourier transforms. This requires making some of the formal arguments in the derivation of E into rigorous ones. The basic tools for this are approximating functions, Cauchy's integral theorem, and Lebesgue's dominated convergence theorem.
Degree
thesis:*- Name thesis:degree_name
- Doctor of Philosophy
- Level thesis:degree_level
- Doctoral
- Discipline thesis:degree_discipline
- Natural Sciences
- Grantor
- Rice University
- Year dc:date.issued
- 1991
Author and committee
dc:creator, dc:contributor.*- Author dc:creator
-
- Tomlinson, Kathy Adiene
- Advisor dc:contributor.advisor
-
- Jones, Frank
Subjects
dc:subject × 1Rights
dc:rights- Statement dc:rights
-
- Copyright is held by the author, unless otherwise indicated. Permission to reuse, publish, or reproduce the work beyond the bounds of fair use or other exemptions to copyright law must be obtained from the copyright holder.
- Language dc:language.iso
- eng
Identifiers
dc:identifier.*- Handle dc:identifier.uri
- https://hdl.handle.net/1911/16489
- OAI identifier oai:identifier
- oai:repository.rice.edu:1911/16489