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Volumn 71, Issue 10, 1993, Pages 1486-1489

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EID: 0000631121     PISSN: 00319007     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevLett.71.1486     Document Type: Article
Times cited : (504)

References (20)
  • 2
    • 84927844761 scopus 로고    scopus 로고
    • (to be published).
  • 4
    • 84927844760 scopus 로고    scopus 로고
    • The averaged null energy conditions is enough to guarantee the null convergence condition and prove the relevant theorem (Corollary 1.2).
  • 8
    • 84927844759 scopus 로고    scopus 로고
    • The conjecture, due to two of the authors (J.F. and D.W.) appears in J. L. Friedman, in Conceptual Problems of Quantum Gravity, edited by A. Ashtekar and J. Stachel (Bikhäuser, Boston, 1991).
  • 11
    • 84927844758 scopus 로고    scopus 로고
    • The weak energy condition is Tabwawb>= 0 for all timelike vectors wa. The dominant energy condition is the weak condition with the additional requirement that Tabwb be causal. The strong energy condition is ( Tab- 1/2 T gab) times wawb>= 0 for timelike vectors wa.
  • 16
    • 84927844757 scopus 로고    scopus 로고
    • The universal covering manifold scrM of a smooth path-connected manifold M can be constructed as follows. Pick a point x0member M and consider the set of smooth paths P = lcurl c : [0,1] -> M | c ( 0 ) = x0rcurl. A projection map pi: P -> M is defined by π ( c ( t ) ) = c ( 1 ). Let scrM be P modulo the equivalence relation, c1app c2 if and only if c1( 1 ) = c2( 1 ) and c1 is homotopic to c2 with end points fixed. The projection map pi is then well defined and smooth as a map pi: scrM -> M.
  • 17
    • 84927844756 scopus 로고    scopus 로고
    • ``A Positive Mass Theorem Based on the Focusing and Retardation of Null Geodesics, '' Syracuse report, 1993 (to be published).
    • Penrose, R.1    Sorkin, R.D.2    Woolgar, E.3


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.