메뉴 건너뛰기




Volumn 53, Issue 9, 1996, Pages 5112-5114

Effective Lagrangians and parity-conserving time-reversal violation at low energies

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0001229617     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.53.5112     Document Type: Article
Times cited : (24)

References (29)
  • 2
    • 85035239746 scopus 로고    scopus 로고
    • World Scientific, Singapore, 1994), and references therein
    • See Time Reversal Invariance and Parity Violation in Neutron Reactions, edited by C.R. Gould, D. Bowman, and Y.P. Popov (World Scientific, Singapore, 1994), and references therein.
    • Gould, C.R.1    Bowman, D.2    Popov, Y.P.3
  • 19
    • 25544460978 scopus 로고
    • Particle Data Group, L. Montanet, et al., Phys. Rev. D 50, 1173 (1994).
    • (1994) Phys. Rev. D , vol.50 , pp. 1173
    • Montanet, L.1
  • 20
    • 85035234760 scopus 로고    scopus 로고
    • are currently analyzing a model with a light boson [P. Herczeg (private communication)]
    • P. Herczeg, J. Kambor, M. Simonius, and D. Wyler are currently analyzing a model with a light boson [P. Herczeg (private communication)].
    • Herczeg, P.1    Kambor, J.2    Simonius, M.3    Wyler, D.4
  • 21
    • 4244121081 scopus 로고
    • One that might appear to be relevant is, ψ-|Amψ (formula presented) (formula presented) (formula presented)(formula presented) ψ+H.c., where (formula presented) is the gluon field-strength tensor and the (formula presented) ‘s are SU(3) color matric es. However, the equations of motion (formula presented) (formula presented)ψ=mψ can be used to show that the operator vanishes up to a surface te rm. This statement, which remains true with the addition of a (formula presented), implies that not all of the 81 dimension-six standard-model operators
    • One that might appear to be relevant is ψ-|Amψ (formula presented) (formula presented) (formula presented)(formula presented) ψ+H.c., where (formula presented) is the gluon field-strength tensor and the (formula presented) ‘s are SU(3) color matric es. However, the equations of motion (formula presented) (formula presented)ψ=mψ can be used to show that the operator vanishes up to a surface te rm. This statement, which remains true with the addition of a (formula presented), implies that not all of the 81 dimension-six standard-model operators inW. Buchmüller and D. Wyler, Nucl. Phys. B268, 621 (1987);
    • (1987) Nucl. Phys. , vol.B268 , pp. 621
    • Buchmüller, W.1    Wyler, D.2
  • 23
    • 85035197971 scopus 로고    scopus 로고
    • the 10 involving fermions and vectors can be reduced up to a surface term through equations of motion (with Higgs scalars instead of explicit masses) to one of the operators involving &ψ
    • the 10 involving fermions and vectors can be reduced up to a surface term through equations of motion (with Higgs scalars instead of explicit masses) to one of the operators involving &ψ
  • 24
    • 85035227768 scopus 로고    scopus 로고
    • (formula presented) (formula presented), a field strength tensor, and a Higgs scalar
    • (formula presented) (formula presented), a field strength tensor, and a Higgs scalar.
  • 27
    • 85035232982 scopus 로고    scopus 로고
    • This operator was pointed out to us by D. Kaplan
    • This operator was pointed out to us by D. Kaplan.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.