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Traversable Wormholes and the Simpson-Visser Model

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dc.contributor.author Δορλής, Παναγιώτης el
dc.contributor.author Dorlis, Panagiotis en
dc.date.accessioned 2022-02-09T12:22:37Z
dc.date.available 2022-02-09T12:22:37Z
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/54615
dc.identifier.uri http://dx.doi.org/10.26240/heal.ntua.22313
dc.rights Default License
dc.subject Σκουληκότρυπες el
dc.subject Γενική Θεωρία της Σχετικότητας el
dc.subject Wormholes en
dc.subject Traversable en
dc.title Traversable Wormholes and the Simpson-Visser Model en
dc.contributor.department Εθνικό Μετσόβιο Πολυτεχνείο--Μεταπτυχιακή Εργασία. Διεπιστημονικό-Διατμηματικό Πρόγραμμα Μεταπτυχιακών Σπουδών (Δ.Π.Μ.Σ.) “Φυσική και Τεχνολογικές Εφαρμογές” el
heal.type masterThesis
heal.classification Φυσική el
heal.language en
heal.access free
heal.recordProvider ntua el
heal.publicationDate 2021-06-24
heal.abstract The goal of this thesis is to extend the Simpson-Visser technique for regularising the Schwarzschild metric by the introduction of a cosmological constant and charge. Before that, this thesis starts with an introduction that clarifies that the Schwarzschild black hole, even if it possesses a wormhole-like geometry, is not a traversable wormhole; something that is forbidden by the principle of General Relativity. After that, we pose the basic criteria for a metric to describe a traversable wormhole in principle. This is a review for traversable wormholes in the sense of Morris and Thorne, in which the Bronnikov formalism is enforced. Wormholes are characterized as static and spherical symmetric spacetimes without centre and horizons; that is, a geometry possessing a minimum coordinate sphere radius different than zero, which is the definition of the throat of the wormhole and no null Killing horizons, which is the definition of a horizon in this class of spacetimes. In order to succeed that, a NEC violating Energy-Momentum tensor is unavoidable, so "exotic matter" is appropriate for the structure of the throat. After, recovering the original Morris and Thorne formalism and present the simplest example of a wormhole, we extract the Penrose diagram of such a spacetime in order to illustrate its causal structure. A causal structure which is like that of Minkowski, but with a different interpretation. What we are going to see in chapter 3 is the technique of Simpson and Visser in order to regularize the Schwarzschild metric by the introduction of some parameter η. Specifically, on the values of this parameter depends the kind of the geometry that the metric describes, starting from the original Schwarzschild black hole to a traversable wormhole. For the wormhole, it turns out that this parameter corresponds to the throat radius. The intermediate "states" are those of a regular black hole and a one-way traversable wormhole. We present this technique in its general state, which allows us to extend the technique of Simpson and Visser to more spacetimes rather than the Schwarzschild one. Namely, we extend this procedure by introducing a cosmological constant and charge (Reissner–Nordström). In chapter 4, we present an observational distinction between the initial black hole and the corresponding wormhole. With the circular orbits being our tool, we see that as we grow the parameter η , the ISCO and the photon sphere become smaller and smaller until their final disappearance. In the final chapter, some comments for future work on this spacetimes are presented. en
heal.advisorName Παπαντωνόπουλος, Ελευθέριος el
heal.committeeMemberName Παπαντωνόπουλος, Λευτέρης el
heal.committeeMemberName Σαρηδάκης, Μανόλης el
heal.committeeMemberName Κουτσούμπας, Γιώργος el
heal.academicPublisher Εθνικό Μετσόβιο Πολυτεχνείο. Σχολή Εφαρμοσμένων Μαθηματικών και Φυσικών Επιστημών el
heal.academicPublisherID ntua
heal.numberOfPages 80 σ. el
heal.fullTextAvailability false


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