메뉴 건너뛰기




Volumn 55, Issue 2, 1997, Pages 739-753

Dilatonic black holes with a Gauss-Bonnet term

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0000852959     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.55.739     Document Type: Article
Times cited : (335)

References (70)
  • 8
    • 0001586120 scopus 로고
    • B. Whitt, 38, 3000 (1988);
    • (1988) , vol.38 , pp. 3000
    • Whitt, B.1
  • 19
    • 0000542279 scopus 로고
    • JTPLA2
    • M. S. Volkov and D. V. Galt’sov, Pis’ma Zh. Eksp. Teor. Fiz. 50, 312 (1989) [JETP Lett.50, 346 (1989)]; JTPLA2
    • (1989) JETP Lett. , vol.50 , pp. 346
    • Volkov, M.S.1    Galt’sov, D.V.2
  • 28
    • 85038297620 scopus 로고
    • P. Bizon and R. M. Wald, 259, 173 (1991).
    • (1991) , vol.259 , pp. 173
    • Bizon, P.1    Wald, R.M.2
  • 36
  • 38
    • 84927285721 scopus 로고    scopus 로고
    • edited by H. J. de Vega and N. Sanchez (World Scientific, Singapore, 1987), p. 455
    • H. C. Luckock, in String Theory and Quantum Gravity, edited by H. J. de Vega and N. Sanchez (World Scientific, Singapore, 1987), p. 455.
    • String Theory and Quantum Gravity
    • Luckock, H.C.1
  • 42
    • 0001102953 scopus 로고
    • JTPLA2
    • A. M. Polyakov, Pis’ma Zh. Eksp. Teor. Fiz. 20, 430 (1974) [JETP Lett.20, 194 (1994)].JTPLA2
    • (1994) JETP Lett. , vol.20 , pp. 194
    • Polyakov, A.M.1
  • 48
    • 0001571293 scopus 로고
    • N. S. Manton, 28, 2019 (1983);
    • (1983) , vol.28 , pp. 2019
    • Manton, N.S.1
  • 51
    • 0001055235 scopus 로고
    • Nucl. Phys.B410, 407 (1993);
    • (1993) Nucl. Phys. , vol.B410 , pp. 407
  • 57
    • 85038342118 scopus 로고
    • 5, 2403 (1972);
    • (1972) , vol.5 , pp. 2403
  • 58
    • 85038323461 scopus 로고
    • 51, R6608 (1995).
    • (1995) , vol.51
  • 60
    • 85038286058 scopus 로고    scopus 로고
    • our analysis, we set (Formula presented) (Formula presented)instead of the condition (27) in order to simplify the numerical calculations. This difference in (Formula presented) is recovered by rescaling the time coordinate as (Formula presented)
    • In our analysis, we set (Formula presented) (Formula presented)instead of the condition (27) in order to simplify the numerical calculations. This difference in (Formula presented) is recovered by rescaling the time coordinate as (Formula presented).
  • 61
    • 85038269271 scopus 로고    scopus 로고
    • Since the value of the dilaton field (Formula presented) is not fixed up to a constant because the constant difference can be absorbed in the radial coordinate by rescaling, we can relax the condition (31). For example, we can assume that the dilaton field approaches to some unknown constant value (Formula presented) as (Formula presented). Introducing (Formula presented) defined by (Formula presented) and rescaling the variables as (Formula presented), (Formula presented), and (Formula presented), we find our boundary condition. However, in our numerical analysis, because we have fixed a charge of black hole in each branch, we have to search for the value of (Formula presented) by use of an iteration method such that (Formula presented) vanishes. Otherwise, (Formula presented) must be rescaled if (Formula presented), giving a different value of charge. Hence, (Formula presented) is not a free parameter but a shooting parameter in the electrically charged black hole case
    • Since the value of the dilaton field (Formula presented) is not fixed up to a constant because the constant difference can be absorbed in the radial coordinate by rescaling, we can relax the condition (31). For example, we can assume that the dilaton field approaches to some unknown constant value (Formula presented) as (Formula presented). Introducing (Formula presented) defined by (Formula presented) and rescaling the variables as (Formula presented), (Formula presented), and (Formula presented), we find our boundary condition. However, in our numerical analysis, because we have fixed a charge of black hole in each branch, we have to search for the value of (Formula presented) by use of an iteration method such that (Formula presented) vanishes. Otherwise, (Formula presented) must be rescaled if (Formula presented), giving a different value of charge. Hence, (Formula presented) is not a free parameter but a shooting parameter in the electrically charged black hole case.
  • 66
  • 70
    • 85038344233 scopus 로고    scopus 로고
    • See Ref. 14
    • See Ref. 14. They also calculated the scalar charge up to (Formula presented).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.