Curved twistor spaces

This thesis is concerned with the problem of "coding" the information of various zero-rest-mass fields into the complex structure of "curved twistor spaces". Chapter 2 is devoted to various preliminaries: a brief outline of twistor theory; an introduction to vector bundles and sh...

Full description

Bibliographic Details
Main Author: Ward, R. S.
Published: University of Oxford 1977
Subjects:
519
Online Access:http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.476496
id ndltd-bl.uk-oai-ethos.bl.uk-476496
record_format oai_dc
spelling ndltd-bl.uk-oai-ethos.bl.uk-4764962016-09-03T03:16:21ZCurved twistor spacesWard, R. S.1977This thesis is concerned with the problem of "coding" the information of various zero-rest-mass fields into the complex structure of "curved twistor spaces". Chapter 2 is devoted to various preliminaries: a brief outline of twistor theory; an introduction to vector bundles and sheaf cohomology and some of their applications in twistor theory; and a discussion of potentials for electromagnetic fields. Chapter 3 deals with left-handed (i.e. anti-self-dual) electromagnetic fields and describes in some detail the associated curved twistor spaces. It is shown how holomorphic functions on the curved spaces give rise to "charged" zero-rest-mass fields on space-time. The first section of Chapter 4 gives the corresponding results for left-handed gravitational fields, using Penrose's "nonlinear graviton" construction. The rest of Chapter 4 is devoted to the concept of twistors relative to a hypersurface in a general curved space-time. In §4.2 the hypersurface is taken to be spacelike; the hypersurface twistors are described and the problem of using holomorphic hypersurface twistor functions to generate fields on the hypersurface and in space-time is discussed. Next the hypersurface is taken to be null. The structure of the associated hypersurface twistor space and and H-space are described in some detail. The twistor space has a natural inner product and, if the hypersurface is shear-free, then it has a "fibred" structure as well. In §4.4 the hypersurface twistor language is used to show that the propagation of twistors through an analytic pp-wave is given by the unfolding of a canonical transformation. Chapter 5 extends the "electromagnetic" construction of Chapter 3 to non-Abelian gauge theories; left-handed gauge fields are described in terms of complex vector bundles over protective twistor space.519University of Oxfordhttp://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.476496http://ora.ox.ac.uk/objects/uuid:8ea3ffe7-c739-4e83-8437-7a136747b267Electronic Thesis or Dissertation
collection NDLTD
sources NDLTD
topic 519
spellingShingle 519
Ward, R. S.
Curved twistor spaces
description This thesis is concerned with the problem of "coding" the information of various zero-rest-mass fields into the complex structure of "curved twistor spaces". Chapter 2 is devoted to various preliminaries: a brief outline of twistor theory; an introduction to vector bundles and sheaf cohomology and some of their applications in twistor theory; and a discussion of potentials for electromagnetic fields. Chapter 3 deals with left-handed (i.e. anti-self-dual) electromagnetic fields and describes in some detail the associated curved twistor spaces. It is shown how holomorphic functions on the curved spaces give rise to "charged" zero-rest-mass fields on space-time. The first section of Chapter 4 gives the corresponding results for left-handed gravitational fields, using Penrose's "nonlinear graviton" construction. The rest of Chapter 4 is devoted to the concept of twistors relative to a hypersurface in a general curved space-time. In §4.2 the hypersurface is taken to be spacelike; the hypersurface twistors are described and the problem of using holomorphic hypersurface twistor functions to generate fields on the hypersurface and in space-time is discussed. Next the hypersurface is taken to be null. The structure of the associated hypersurface twistor space and and H-space are described in some detail. The twistor space has a natural inner product and, if the hypersurface is shear-free, then it has a "fibred" structure as well. In §4.4 the hypersurface twistor language is used to show that the propagation of twistors through an analytic pp-wave is given by the unfolding of a canonical transformation. Chapter 5 extends the "electromagnetic" construction of Chapter 3 to non-Abelian gauge theories; left-handed gauge fields are described in terms of complex vector bundles over protective twistor space.
author Ward, R. S.
author_facet Ward, R. S.
author_sort Ward, R. S.
title Curved twistor spaces
title_short Curved twistor spaces
title_full Curved twistor spaces
title_fullStr Curved twistor spaces
title_full_unstemmed Curved twistor spaces
title_sort curved twistor spaces
publisher University of Oxford
publishDate 1977
url http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.476496
work_keys_str_mv AT wardrs curvedtwistorspaces
_version_ 1718381435678621696