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Volumn 56, Issue 8, 1997, Pages 4948-4961

Perturbations in the Kerr-Newman dilatonic black hole background: Maxwell waves

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EID: 0040724978     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.56.4948     Document Type: Article
Times cited : (11)

References (18)
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    • Proceedings of the Texas/PASCOS Conference, 92: Relativistic Astrophysics and Particle Cosmology, edited by C. W. Ackerlof and M. A. Srednicki [Ann. (N.Y.) Acad. Sci. 688, 454 (1993)].ANYAA
    • B. Harms and Y. Leblanc, in Proceedings of the Texas/PASCOS Conference, 92: Relativistic Astrophysics and Particle Cosmology, edited by C. W. Ackerlof and M. A. Srednicki [Ann. (N.Y.) Acad. Sci. 688, 454 (1993)].ANYAA9
    • Harms, B.1    Leblanc, Y.2
  • 9
    • 85038282556 scopus 로고    scopus 로고
    • B. Harms and Y. Leblanc, in Supersymmetry and Unification of Fundamental Interactions, edited by Pran Nath (World Scientific, Singapore, 1994) p. 337
    • B. Harms and Y. Leblanc, in Supersymmetry and Unification of Fundamental Interactions, edited by Pran Nath (World Scientific, Singapore, 1994) p. 337.
  • 10
    • 85038307214 scopus 로고    scopus 로고
    • edited by F. C. Khanna, R. Kobes, G. Kunstatter, and H. Umezawa (World Scientific, Singapore, 1994), p. 387
    • B. Harms and Y. Leblanc, in Banff/CAP Workshop on Thermal Field Theory, edited by F. C. Khanna, R. Kobes, G. Kunstatter, and H. Umezawa (World Scientific, Singapore, 1994), p. 387.
    • Banff/CAP Workshop on Thermal Field Theory
    • Harms, B.1    Leblanc, Y.2
  • 12
    • 85038332232 scopus 로고    scopus 로고
    • The ratio (Formula presented) for physical particles can be estimated using mks units once one reintroduces the conventional values of (Formula presented) and (Formula presented) One then has (Formula presented) which is approximately equal to (Formula presented) for an electron (Formula presented) and (Formula presented)) and to (Formula presented) for a particle of the same charge but of Planck mass. This implies that our approximation ((Formula presented) small) does not apply to most known elementary particles, but can be valid for black holes produced during the gravitational collapse of massive stars and also for cosmological black holes of Planck mass size. On the other hand, the opposite approximation ((Formula presented) large) corresponds to a naked singularity
    • The ratio (Formula presented) for physical particles can be estimated using mks units once one reintroduces the conventional values of (Formula presented) and (Formula presented) One then has (Formula presented) which is approximately equal to (Formula presented) for an electron (Formula presented) and (Formula presented)) and to (Formula presented) for a particle of the same charge but of Planck mass. This implies that our approximation ((Formula presented) small) does not apply to most known elementary particles, but can be valid for black holes produced during the gravitational collapse of massive stars and also for cosmological black holes of Planck mass size. On the other hand, the opposite approximation ((Formula presented) large) corresponds to a naked singularity.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.