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Volumn 53, Issue 8, 1996, Pages 4298-4310

Uncertainties of predictions in models of eternal inflation

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[No Author keywords available]

Indexed keywords


EID: 0000137879     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.53.4298     Document Type: Article
Times cited : (49)

References (41)
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    • Tufts University Report No. gr-qc/9507018 (unpublished
    • “Predictions From Quantum Cosmology,” Tufts University Report No. gr-qc/9507018 (unpublished).
    • Predictions From Quantum Cosmology
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    • The principle of mediocrity is a version of the anthropic principle. For a review of the latter
    • The principle of mediocrity is a version of the anthropic principle. For a review of the latter, see, e.g., B. Carter, Philos. Trans. R. Soc. London A310, 347 (1983);
    • (1983) Philos. Trans. R. Soc. London , vol.A310 , pp. 347
    • Carter, B.1
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    • Clarendon, Oxford
    • J. D. Barrow and F. J. Tipler, The Antropic Cosmological Principle (Clarendon, Oxford, 1986). Ideas related to the principle of mediocrity have also been discussed by Albrecht 5 and by Garcia-Bellido and Linde 6.
    • (1986) The Antropic Cosmological Principle
    • Barrow, J.D.1    Tipler, F.J.2
  • 11
    • 85035218129 scopus 로고    scopus 로고
    • More exactly, the probabilities are proportional to the volumes of the thermalization hypersurfaces which are the boundaries of the corresponding thermalized regions. For details, see Refs. 11,3
    • More exactly, the probabilities are proportional to the volumes of the thermalization hypersurfaces which are the boundaries of the corresponding thermalized regions. For details, see Refs. 11,3 .
  • 23
    • 4243844250 scopus 로고
    • For a recent review of quantum cosmology, see, e.g., the second paper in Ref. 3 . The distribution (5) for the tunneling wave function was obtained by
    • For a recent review of quantum cosmology, see, e.g., the second paper in Ref. 3 . The distribution (5) for the tunneling wave function was obtained by A. Vilenkin, Phys. Rev. D 30, 509 (1984).
    • (1984) Phys. Rev. D , vol.30 , pp. 509
    • Vilenkin, A.1
  • 24
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    • The same distribution was found using a different approach
    • The same distribution was found using a different approach byA. D. Linde, Lett. Nuovo Cimento 39, 401 (1984).
    • (1984) Lett. Nuovo Cimento , vol.39 , pp. 401
    • Linde, A.D.1
  • 25
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    • The Euclidean approach of
    • The Euclidean approach of J. B. Hartle and S. W. Hawking [Phys. Rev. D 28, 2960 (1983)] gives a drastically different probability distribution.
    • (1983) Phys. Rev. D , vol.28 , pp. 2960
    • Hartle, J.B.1    Hawking, S.W.2
  • 26
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    • Omitted end note
    • Omitted end note.
  • 28
    • 85035195767 scopus 로고    scopus 로고
    • This is achieved by a generalization of the method used in 15 for the potential V(φ)=λ(formula presented) and in 14 for a particular factor ordering and time variable. The transformation into a self-adjoint form can similarly be performed for a general factor ordering (13) and time variable (10
    • This is achieved by a generalization of the method used in 15 for the potential V(φ)=λ(formula presented) and in 14 for a particular factor ordering and time variable. The transformation into a self-adjoint form can similarly be performed for a general factor ordering (13) and time variable (10).
  • 31
    • 85035196729 scopus 로고    scopus 로고
    • A related observation was made by Linde and Mezhlumian 10 who noted sensitive dependence of the results on the boundary condition they imposed at the Planck scale
    • A related observation was made by Linde and Mezhlumian 10 who noted sensitive dependence of the results on the boundary condition they imposed at the Planck scale.
  • 32
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    • Omitted end note
    • Omitted end note.
  • 34
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    • The case of thermalization to continuous distribution of vacua was considered, by a different approach
    • The case of thermalization to continuous distribution of vacua was considered, by a different approach, inJ. Garcia-Bellido, A. D. Linde and D. A. Linde, Phys. Rev. D 50, 730 (1994);
    • (1994) Phys. Rev. D , vol.50 , pp. 730
    • Garcia-Bellido, J.1    Linde, A.D.2    Linde, D.A.3
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    • Omitted end note
    • Omitted end note.
  • 38
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    • Note also that if we accept Eq. (87) as the genuine uncertainty of the model, then values of &γtilde;/γ with a relative deviation of order (formula presented) from the maximum should still be assigned nonzero probabilities
    • Note also that if we accept Eq. (87) as the genuine uncertainty of the model, then values of &γtilde;/γ with a relative deviation of order (formula presented) from the maximum should still be assigned nonzero probabilities.
  • 39
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    • Proceedings of the First International Sakharov Conference on Physics, 1991 (Nova Science Publishers, New York, also available as astro-ph/9406045 (unpublished
    • A. Mezhlumian and A. A. Starobinsky, Sakharov Memorial Lectures in Physics, in Proceedings of the First International Sakharov Conference on Physics, 1991 (Nova Science Publishers, New York, 1992), p. 1119; also available as astro-ph/9406045 (unpublished).
    • (1992) Sakharov Memorial Lectures in Physics , pp. 1119
    • Mezhlumian, A.1    Starobinsky, A.A.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.