HAWKING RADIATION AND PARTICLE EMISSIONS ON KERR - NEWMAN - VAIDYA BLACK HOLES

In this research, the analysis of Hawking radiation on a nonstationary Kerr – Newman – Vaidya black hole was analyzed using semiclassical approaches. The nonstationary term ???? in the black hole is equivalent to a mass change with respects to time and radial coordinates. The Hawking temperatures we...

Full description

Saved in:
Bibliographic Details
Main Author: Hasbi Salimi, Ahmad
Format: Final Project
Language:Indonesia
Online Access:https://digilib.itb.ac.id/gdl/view/60494
Tags: Add Tag
No Tags, Be the first to tag this record!
Institution: Institut Teknologi Bandung
Language: Indonesia
id id-itb.:60494
spelling id-itb.:604942021-09-18T07:35:07ZHAWKING RADIATION AND PARTICLE EMISSIONS ON KERR - NEWMAN - VAIDYA BLACK HOLES Hasbi Salimi, Ahmad Indonesia Final Project Complex path method, Bekenstein – Hawking formulations, Dirac equation, Hawking radiation, Kerr – Newman – Vaidya black holes, Klein – Gordon equation, non-stationary term, particle emissions, radial null geodesic. INSTITUT TEKNOLOGI BANDUNG https://digilib.itb.ac.id/gdl/view/60494 In this research, the analysis of Hawking radiation on a nonstationary Kerr – Newman – Vaidya black hole was analyzed using semiclassical approaches. The nonstationary term ???? in the black hole is equivalent to a mass change with respects to time and radial coordinates. The Hawking temperatures were derived using three methods: Two semiclassical methods, including the radial null geodesic method and the complex path analysis, and the Bekenstein – Hawking temperature formulation. These three methods gave the same temperature. In general, the Hawking temperature obtained was inversely proportional to the mass and nonstationary term. In order for the temperatures not to be imaginary values, the black holes must satisfy (????+????)2?????2+????2 condition, with ???? is the mass, ???? is the angular momentum and ???? is the electric charge of the black holes. The entropy of black holes was derived using the Bekenstein – Hawking formulation in ???????????? form and the black hole dynamics equation in the form of ????????????????/????????. The two types of particle emission as Hawking radiation were analyzed: particle emission using the Klein-Gordon equation and Dirac particle emission using the Dirac equation. The wave functions of these two particle emissions are then analyzed using the WKB approximation to calculate the effect of particle emission on the Hawking temperature of the black hole. The main difference between the emission results of scalar particles and Dirac particles is that there is a characterization term consisting of E the energy of the Dirac particle, j the angular momentum of the Dirac particle and e the electric charge of the Dirac particle. In order for the temperature to remain positive, the particle and the black hole must satisfy ????(????+????)?????????+????????. text
institution Institut Teknologi Bandung
building Institut Teknologi Bandung Library
continent Asia
country Indonesia
Indonesia
content_provider Institut Teknologi Bandung
collection Digital ITB
language Indonesia
description In this research, the analysis of Hawking radiation on a nonstationary Kerr – Newman – Vaidya black hole was analyzed using semiclassical approaches. The nonstationary term ???? in the black hole is equivalent to a mass change with respects to time and radial coordinates. The Hawking temperatures were derived using three methods: Two semiclassical methods, including the radial null geodesic method and the complex path analysis, and the Bekenstein – Hawking temperature formulation. These three methods gave the same temperature. In general, the Hawking temperature obtained was inversely proportional to the mass and nonstationary term. In order for the temperatures not to be imaginary values, the black holes must satisfy (????+????)2?????2+????2 condition, with ???? is the mass, ???? is the angular momentum and ???? is the electric charge of the black holes. The entropy of black holes was derived using the Bekenstein – Hawking formulation in ???????????? form and the black hole dynamics equation in the form of ????????????????/????????. The two types of particle emission as Hawking radiation were analyzed: particle emission using the Klein-Gordon equation and Dirac particle emission using the Dirac equation. The wave functions of these two particle emissions are then analyzed using the WKB approximation to calculate the effect of particle emission on the Hawking temperature of the black hole. The main difference between the emission results of scalar particles and Dirac particles is that there is a characterization term consisting of E the energy of the Dirac particle, j the angular momentum of the Dirac particle and e the electric charge of the Dirac particle. In order for the temperature to remain positive, the particle and the black hole must satisfy ????(????+????)?????????+????????.
format Final Project
author Hasbi Salimi, Ahmad
spellingShingle Hasbi Salimi, Ahmad
HAWKING RADIATION AND PARTICLE EMISSIONS ON KERR - NEWMAN - VAIDYA BLACK HOLES
author_facet Hasbi Salimi, Ahmad
author_sort Hasbi Salimi, Ahmad
title HAWKING RADIATION AND PARTICLE EMISSIONS ON KERR - NEWMAN - VAIDYA BLACK HOLES
title_short HAWKING RADIATION AND PARTICLE EMISSIONS ON KERR - NEWMAN - VAIDYA BLACK HOLES
title_full HAWKING RADIATION AND PARTICLE EMISSIONS ON KERR - NEWMAN - VAIDYA BLACK HOLES
title_fullStr HAWKING RADIATION AND PARTICLE EMISSIONS ON KERR - NEWMAN - VAIDYA BLACK HOLES
title_full_unstemmed HAWKING RADIATION AND PARTICLE EMISSIONS ON KERR - NEWMAN - VAIDYA BLACK HOLES
title_sort hawking radiation and particle emissions on kerr - newman - vaidya black holes
url https://digilib.itb.ac.id/gdl/view/60494
_version_ 1822275915830263808