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2
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85035239746
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World Scientific, Singapore, 1994), and references therein
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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.
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Gould, C.R.1
Bowman, D.2
Popov, Y.P.3
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19
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25544460978
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Particle Data Group, L. Montanet, et al., Phys. Rev. D 50, 1173 (1994).
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(1994)
Phys. Rev. D
, vol.50
, pp. 1173
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Montanet, L.1
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20
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85035234760
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are currently analyzing a model with a light boson [P. Herczeg (private communication)]
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P. Herczeg, J. Kambor, M. Simonius, and D. Wyler are currently analyzing a model with a light boson [P. Herczeg (private communication)].
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Herczeg, P.1
Kambor, J.2
Simonius, M.3
Wyler, D.4
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21
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4244121081
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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
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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);
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(1987)
Nucl. Phys.
, vol.B268
, pp. 621
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Buchmüller, W.1
Wyler, D.2
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23
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85035197971
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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
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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
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24
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85035227768
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(formula presented) (formula presented), a field strength tensor, and a Higgs scalar
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(formula presented) (formula presented), a field strength tensor, and a Higgs scalar.
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27
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85035232982
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This operator was pointed out to us by D. Kaplan
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This operator was pointed out to us by D. Kaplan.
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|