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Volumn 14, Issue 2, 1997, Pages 407-420

3 + 1 Approach to the long-wavelength iteration scheme

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EID: 0031540303     PISSN: 02649381     EISSN: None     Source Type: Journal    
DOI: 10.1088/0264-9381/14/2/014     Document Type: Article
Times cited : (8)

References (29)
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  • 6
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    • Salopek D S 1991 Phys. Rev D 43 3214 Salopek D S and Stewart J M 1993 Phys. Rev. D 47 3235 Parry J, Salopek D S and Stewart J M 1994 Phys. Rev. D 49 2872 Croudace K M, Parry J, Salopek D S and Stewart J M 1994 App. J. 423 22
    • (1993) Phys. Rev. D , vol.47 , pp. 3235
    • Salopek, D.S.1    Stewart, J.M.2
  • 7
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    • Salopek D S 1991 Phys. Rev D 43 3214 Salopek D S and Stewart J M 1993 Phys. Rev. D 47 3235 Parry J, Salopek D S and Stewart J M 1994 Phys. Rev. D 49 2872 Croudace K M, Parry J, Salopek D S and Stewart J M 1994 App. J. 423 22
    • (1994) Phys. Rev. D , vol.49 , pp. 2872
    • Parry, J.1    Salopek, D.S.2    Stewart, J.M.3
  • 8
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    • Salopek D S 1991 Phys. Rev D 43 3214 Salopek D S and Stewart J M 1993 Phys. Rev. D 47 3235 Parry J, Salopek D S and Stewart J M 1994 Phys. Rev. D 49 2872 Croudace K M, Parry J, Salopek D S and Stewart J M 1994 App. J. 423 22
    • (1994) App. J. , vol.423 , pp. 22
    • Croudace, K.M.1    Parry, J.2    Salopek, D.S.3    Stewart, J.M.4
  • 11
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    • Kinematics and dynamics of general relativity
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    • Methods of numerical relativity
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    • Piran, T.1
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    • 0039016829 scopus 로고    scopus 로고
    • The K = k(t) slicing condition also causes the Hamiltonian and momentum constraints (cf equations (4) and (5)) to be completely decoupled (see [10])
    • The K = k(t) slicing condition also causes the Hamiltonian and momentum constraints (cf equations (4) and (5)) to be completely decoupled (see [10]).
  • 23
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    • Tomita K 1972 Prog. Theor. Phys. 48 1503 Tomita K 1975 Prog. Theor. Phys. 54 185
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    • Our definition for the extrinsic curvature agrees with that of [8] but differs by a minus sign and a factor of two from that of [1]
    • Our definition for the extrinsic curvature agrees with that of [8] but differs by a minus sign and a factor of two from that of [1].
  • 27
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    • 2/2! + ... . When x ≪ 1 then the extra terms make only refinements, but when x ≥ 1 they are a necessity
    • 2/2! + ... . When x ≪ 1 then the extra terms make only refinements, but when x ≥ 1 they are a necessity.
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    • unpublished notes
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    • in preparation
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.