dc.contributor.advisor | Buchholz, Detlev Prof. Dr. | de |
dc.contributor.author | Solveen, Christoph | de |
dc.date.accessioned | 2012-04-26T15:58:02Z | de |
dc.date.accessioned | 2013-01-18T13:44:00Z | de |
dc.date.available | 2013-01-30T23:51:15Z | de |
dc.date.issued | 2012-04-26 | de |
dc.identifier.uri | http://hdl.handle.net/11858/00-1735-0000-000D-F081-9 | de |
dc.identifier.uri | http://dx.doi.org/10.53846/goediss-2969 | |
dc.identifier.uri | http://dx.doi.org/10.53846/goediss-2969 | |
dc.identifier.uri | http://dx.doi.org/10.53846/goediss-2969 | |
dc.format.mimetype | application/pdf | de |
dc.language.iso | ger | de |
dc.rights.uri | http://creativecommons.org/licenses/by-nc-nd/3.0/ | de |
dc.title | Local Equilibrium States in Quantum Field Theory in Curved Spacetime | de |
dc.type | doctoralThesis | de |
dc.title.translated | Lokale Gleichgewichtszustände in der Quantenfeldtheorie auf gekrümmter Raumzeit | de |
dc.contributor.referee | Rehren, Karl-Henning Prof. Dr. | de |
dc.date.examination | 2012-04-11 | de |
dc.subject.dnb | 530 Physik | de |
dc.subject.gok | RDI 500 | de |
dc.subject.gok | RDI 640 | de |
dc.subject.gok | RJG 200 | de |
dc.description.abstracteng | The present work concerns itself with the
conceptual problem of assigning thermal parameters to states in
quantum field theory in curved spacetime, and is based on the
concept of local thermal equilibrium in the sense of Buchholz,
Ojima and Roos. In this approach, point-like localized quantum
fields, so called thermal observables, are used to attach thermal
parameters to macroscopic systems, with the proviso that these
systems do not deviate too far from thermal equilibrium. In
contrast to many of the existing approaches, this allows for a
conceptually clear description of non-equilibrium phenomena, for
example in cosmology. The results are illustrated using the
massless, conformally coupled, free scalar field. Initially, the
structure of the set of thermal observables is discussed and it is
found that in curved spacetime these objects do not form a vector
space and must be chosen as linearly independent. However, there
can be relations between the corresponding local thermal parameters
which are induced by linear equations of state. It is shown that
these relations lead to evolution equations for the local thermal
parameters in curved spacetime. For thermal observables where no
such linear relations hold, there exist states to which the
corresponding local thermal parameters can be assigned in bounded
regions in Minkowski spacetime. Using a natural assumption
regarding the spectrum of the thermal observables, it is shown that
states exist which are in equilibrium at any given point in a
curved spacetime. Following on, it is argued that KMS states in
stationary curved spacetimes may not be viewed in analogy to global
thermal equilibrium states in Minkowski spacetime. The KMS
parameter | de |
dc.contributor.coReferee | Buchholz, Detlev Prof. Dr. | de |
dc.subject.topic | Physics | de |
dc.subject.ger | lokales thermisches Gleichgewicht | de |
dc.subject.ger | Quantenfeldtheorie auf gekrümmten Raumzeiten | de |
dc.subject.eng | local thermal equilibrium | de |
dc.subject.eng | Quantum Field Theory in Curved Spacetime | de |
dc.subject.bk | 33.24 | de |
dc.subject.bk | 33.21 | de |
dc.subject.bk | 33.28 | de |
dc.identifier.urn | urn:nbn:de:gbv:7-webdoc-3482-6 | de |
dc.identifier.purl | webdoc-3482 | de |
dc.affiliation.institute | Fakultät für Physik | de |
dc.identifier.ppn | 726655473 | de |