FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2117715618> ?p ?o ?g. }

• W2117715618 abstract "We discuss and compare at length the results of two methods used recently to describe the thermodynamics of Taub-NUT solutions in a deSitter background. In the first approach ($mathbb{% C}$-approach), one deals with an analytically continued version of the metric while in the second approach ($mathbb{R}$-approach), the discussion is carried out using the unmodified metric with Lorentzian signature. No analytic continuation is performed on the coordinates and/or the parameters that appear in the metric. We find that the results of both these approaches are completely equivalent modulo analytic continuation and we provide the exact prescription that relates the results in both methods. The extension of these results to the AdS/flat cases aims to give a physical interpretation of the thermodynamics of nut-charged spacetimes in the Lorentzian sector. We also briefly discuss the higher dimensional spaces and note that, analogous with the absence of hyperbolic nuts in AdS backgrounds, there are no spherical Taub-Nut-dS solutions." @default.
• W2117715618 created "2016-06-24" @default.
• W2117715618 creator A5048807416 @default.
• W2117715618 creator A5077727766 @default.
• W2117715618 date "2005-10-27" @default.
• W2117715618 modified "2023-10-06" @default.
• W2117715618 title "Thermodynamics of Newman-Unti-Tamburino charged spaces" @default.
• W2117715618 cites W1518546648 @default.
• W2117715618 cites W1901994727 @default.
• W2117715618 cites W1981283695 @default.
• W2117715618 cites W1982722342 @default.
• W2117715618 cites W1990393733 @default.
• W2117715618 cites W1992039737 @default.
• W2117715618 cites W1993199738 @default.
• W2117715618 cites W1996647414 @default.
• W2117715618 cites W1999913414 @default.
• W2117715618 cites W2002580560 @default.
• W2117715618 cites W2017895398 @default.
• W2117715618 cites W2028420788 @default.
• W2117715618 cites W2039116423 @default.
• W2117715618 cites W2039337311 @default.
• W2117715618 cites W2049008031 @default.
• W2117715618 cites W2051135301 @default.
• W2117715618 cites W2058177016 @default.
• W2117715618 cites W2068974261 @default.
• W2117715618 cites W2074413703 @default.
• W2117715618 cites W2092852831 @default.
• W2117715618 cites W2099204364 @default.
• W2117715618 cites W2106704391 @default.
• W2117715618 cites W2118556056 @default.
• W2117715618 cites W2125499150 @default.
• W2117715618 cites W2127955194 @default.
• W2117715618 cites W2135779038 @default.
• W2117715618 cites W2137060839 @default.
• W2117715618 cites W2139496359 @default.
• W2117715618 cites W2141998623 @default.
• W2117715618 cites W2144012213 @default.
• W2117715618 cites W2146203925 @default.
• W2117715618 cites W2162081237 @default.
• W2117715618 cites W2163851871 @default.
• W2117715618 cites W2594235370 @default.
• W2117715618 cites W3021444466 @default.
• W2117715618 cites W3098806824 @default.
• W2117715618 cites W3100440069 @default.
• W2117715618 cites W3102131621 @default.
• W2117715618 cites W3105717872 @default.
• W2117715618 doi "https://doi.org/10.1103/physrevd.72.084032" @default.
• W2117715618 hasPublicationYear "2005" @default.
• W2117715618 type Work @default.
• W2117715618 sameAs 2117715618 @default.
• W2117715618 citedByCount "39" @default.
• W2117715618 countsByYear W21177156182012 @default.
• W2117715618 countsByYear W21177156182015 @default.
• W2117715618 countsByYear W21177156182017 @default.
• W2117715618 countsByYear W21177156182019 @default.
• W2117715618 countsByYear W21177156182020 @default.
• W2117715618 countsByYear W21177156182021 @default.
• W2117715618 countsByYear W21177156182022 @default.
• W2117715618 countsByYear W21177156182023 @default.
• W2117715618 crossrefType "journal-article" @default.
• W2117715618 hasAuthorship W2117715618A5048807416 @default.
• W2117715618 hasAuthorship W2117715618A5077727766 @default.
• W2117715618 hasBestOaLocation W21177156182 @default.
• W2117715618 hasConcept C114614502 @default.
• W2117715618 hasConcept C121332964 @default.
• W2117715618 hasConcept C134306372 @default.
• W2117715618 hasConcept C151602998 @default.
• W2117715618 hasConcept C162324750 @default.
• W2117715618 hasConcept C176217482 @default.
• W2117715618 hasConcept C199360897 @default.
• W2117715618 hasConcept C206391251 @default.
• W2117715618 hasConcept C21547014 @default.
• W2117715618 hasConcept C24890656 @default.
• W2117715618 hasConcept C2778029271 @default.
• W2117715618 hasConcept C33332235 @default.
• W2117715618 hasConcept C33923547 @default.
• W2117715618 hasConcept C37914503 @default.
• W2117715618 hasConcept C41008148 @default.
• W2117715618 hasConcept C527412718 @default.
• W2117715618 hasConcept C54732982 @default.
• W2117715618 hasConcept C88626702 @default.
• W2117715618 hasConcept C97355855 @default.
• W2117715618 hasConceptScore W2117715618C114614502 @default.
• W2117715618 hasConceptScore W2117715618C121332964 @default.
• W2117715618 hasConceptScore W2117715618C134306372 @default.
• W2117715618 hasConceptScore W2117715618C151602998 @default.
• W2117715618 hasConceptScore W2117715618C162324750 @default.
• W2117715618 hasConceptScore W2117715618C176217482 @default.
• W2117715618 hasConceptScore W2117715618C199360897 @default.
• W2117715618 hasConceptScore W2117715618C206391251 @default.
• W2117715618 hasConceptScore W2117715618C21547014 @default.
• W2117715618 hasConceptScore W2117715618C24890656 @default.
• W2117715618 hasConceptScore W2117715618C2778029271 @default.
• W2117715618 hasConceptScore W2117715618C33332235 @default.
• W2117715618 hasConceptScore W2117715618C33923547 @default.
• W2117715618 hasConceptScore W2117715618C37914503 @default.
• W2117715618 hasConceptScore W2117715618C41008148 @default.
• W2117715618 hasConceptScore W2117715618C527412718 @default.
• W2117715618 hasConceptScore W2117715618C54732982 @default.
• W2117715618 hasConceptScore W2117715618C88626702 @default.

• next