메뉴 건너뛰기




Volumn 67, Issue 4, 2003, Pages

Null energy conditions in quantum field theory

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE; ENERGY; MATHEMATICAL ANALYSIS; QUANTUM MECHANICS; QUANTUM THEORY; STRESS;

EID: 0037441213     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.67.044003     Document Type: Article
Times cited : (92)

References (47)
  • 5
    • 85038281734 scopus 로고    scopus 로고
    • A matter model violating the NEC is the nonminimally coupled scalar field
    • A matter model violating the NEC is the nonminimally coupled scalar field 6.
  • 8
    • 0000843028 scopus 로고    scopus 로고
    • É. É. Flanagan, Phys. Rev. D 56, 4922 (1997).
    • (1997) , vol.56 , pp. 4922
  • 9
  • 10
    • 85038335754 scopus 로고    scopus 로고
    • Minkowski space, a state is Hadamard if and only if its normal ordered two-point function (Formula presented) is smooth in x and (Formula presented)
    • In Minkowski space, a state is Hadamard if and only if its normal ordered two-point function (Formula presented) is smooth in x and (Formula presented)
  • 11
    • 85038307021 scopus 로고    scopus 로고
    • It would be interesting to understand whether, conversely, the weak energy condition can be regarded as a classical limit of the QWEIs.
    • It would be interesting to understand whether, conversely, the weak energy condition can be regarded as a classical limit of the QWEIs.
  • 13
    • 0000402488 scopus 로고    scopus 로고
    • L. H. Ford and T. A. Roman, Phys. Rev. D 55, 2082 (1997).
    • (1997) , vol.55 , pp. 2082
    • Ford, L.H.1    Roman, T.A.2
  • 18
    • 0037113811 scopus 로고    scopus 로고
    • É. É. Flanagan, Phys. Rev. D 66, 104007 (2002).
    • (2002) , vol.66 , pp. 104007
  • 21
    • 85038331478 scopus 로고    scopus 로고
    • C. J. Fewster and M. J. Pfenning (in preparation).
    • C. J. Fewster and M. J. Pfenning (in preparation).
  • 22
    • 85038310279 scopus 로고    scopus 로고
    • For general Hadamard states one has the weaker result (Formula presented)
    • For general Hadamard states one has the weaker result (Formula presented)
  • 23
    • 85038292382 scopus 로고    scopus 로고
    • Although this class was not precisely delineated in Ref.
    • Although this class was not precisely delineated in Ref. 11, one expects the bound to hold for all Hadamard states for which the left-hand side exists.
  • 24
    • 85038271382 scopus 로고    scopus 로고
    • At least for those states in which the integral in Eq. (1.4) converges absolutely.
    • At least for those states in which the integral in Eq. (1.4) converges absolutely.
  • 27
    • 85038314935 scopus 로고    scopus 로고
    • Although B is real-valued, we shall write complex conjugations where they would be appropriate for complex B
    • Although B is real-valued, we shall write complex conjugations where they would be appropriate for complex B.
  • 31
    • 85038281836 scopus 로고    scopus 로고
    • Had QNEIs existed, one could have derived the ANEC as a consequence, just as the AWEC may be derived from the QWEIs (see Ref.
    • Had QNEIs existed, one could have derived the ANEC as a consequence, just as the AWEC may be derived from the QWEIs (see Ref. 11). However, the reverse implication is not valid, so there is not contradiction between nonexistence of QNEIs and the validity of the ANEC.
  • 32
    • 85038314076 scopus 로고    scopus 로고
    • Note that Ref.
    • Note that Ref. 18 used a different convention for the Fourier transform in which Eq. (3.1) would involve (Formula presented) rather than (Formula presented)
  • 33
    • 85038303500 scopus 로고    scopus 로고
    • As an example, consider the distribution (Formula presented) which has a sensible restriction (Formula presented) to lines of the form (Formula presented) but no well-defined restriction to the line (Formula presented)
    • As an example, consider the distribution (Formula presented) which has a sensible restriction (Formula presented) to lines of the form (Formula presented) but no well-defined restriction to the line (Formula presented)
  • 34
    • 85038325867 scopus 로고    scopus 로고
    • This qualification is required in order to extend the result of Theorem III.1 to noncompactly supported g. To obtain a statement valid for all Hadamard states, one could alternatively replace the left-hand side by (Formula presented) where (Formula presented) is smooth, equal to 1 for (Formula presented) vanishing for (Formula presented) and monotone decreasing as |s| increases.
    • This qualification is required in order to extend the result of Theorem III.1 to noncompactly supported g. To obtain a statement valid for all Hadamard states, one could alternatively replace the left-hand side by (Formula presented) where (Formula presented) is smooth, equal to 1 for (Formula presented) vanishing for (Formula presented) and monotone decreasing as |s| increases.
  • 35
    • 85038324218 scopus 로고    scopus 로고
    • more detail, we consider theories described by von Neumann algebras (Formula presented) indexed by open sets O of Minkowski space and consisting of bounded operators on a Hilbert space H. The assignment (Formula presented) is assumed to be isotonous [i.e., (Formula presented) implies that (Formula presented) is a subalgebra of (Formula presented) and local [i.e., if (Formula presented) and (Formula presented) are spacelike separated then any element of (Formula presented) commutes with every element of (Formula presented). In addition, the group of translations is implemented on H by unitary operators (Formula presented) such that (Formula presented) and which obey the spectral condition: (Formula presented) where the spectral measure (Formula presented) is supported in the forward light cone (Formula presented) It is also assumed that there is a unique translationally invariant vacuum state (Formula presented) and that Ω is cyclic [i.e., (Formula presented) is dense in H for each O
    • In more detail, we consider theories described by von Neumann algebras (Formula presented) indexed by open sets O of Minkowski space and consisting of bounded operators on a Hilbert space H. The assignment (Formula presented) is assumed to be isotonous [i.e., (Formula presented) implies that (Formula presented) is a subalgebra of (Formula presented) and local [i.e., if (Formula presented) and (Formula presented) are spacelike separated then any element of (Formula presented) commutes with every element of (Formula presented). In addition, the group of translations is implemented on H by unitary operators (Formula presented) such that (Formula presented) and which obey the spectral condition: (Formula presented) where the spectral measure (Formula presented) is supported in the forward light cone (Formula presented) It is also assumed that there is a unique translationally invariant vacuum state (Formula presented) and that Ω is cyclic [i.e., (Formula presented) is dense in H for each O].
  • 36
    • 85038304862 scopus 로고    scopus 로고
    • Under the assumptions in the previous reference, let K be a compact subset of Minkowski space such that (Formula presented) for all (Formula presented) (Formula presented) Suppose that there exist vectors (Formula presented) and (Formula presented) such that (Formula presented) (Formula presented) and with the property that, for all (Formula presented) (Formula presented) (Formula presented) (Formula presented) Then a theorem of Woronowicz
    • Under the assumptions in the previous reference, let K be a compact subset of Minkowski space such that (Formula presented) for all (Formula presented) (Formula presented) Suppose that there exist vectors (Formula presented) and (Formula presented) such that (Formula presented) (Formula presented) and with the property that, for all (Formula presented) (Formula presented) (Formula presented) (Formula presented) Then a theorem of Woronowicz 46 entails that the algebra (Formula presented) of observables localized on K consists only of scalar multiples of the identity. In the case of a bounded null line segment (Formula presented) where (Formula presented) is null, it is readily verified that (Formula presented) (Formula presented) satisfy these conditions for any spacelike vector (Formula presented) with (Formula presented) and (Formula presented) Such vectors (Formula presented) exist in dimensions (Formula presented) thus justifying the claim made in the text.
  • 45
    • 0542418896 scopus 로고    scopus 로고
    • H. Yu, Phys. Rev. D 58, 064017 (1998).
    • (1998) Phys. Rev. D , vol.58 , pp. 64017
    • Yu, H.1
  • 46
    • 0001300845 scopus 로고    scopus 로고
    • É. É. Flanagan and R. M. Wald, Phys. Rev. D 54, 6233 (1996).
    • (1996) Phys. Rev. D , vol.54 , pp. 6233
    • Wald, R.M.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.