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Buras, A.J.1
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edited by F. David and R. Gupta (Elsevier, New York, in press)
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A.J. Buras, Eur. Phys. J. C, 11, 93 (1999); in Probing the Standard Model of Particle Interactions, Les Houches Lectures, edited by F. David and R. Gupta (Elsevier, New York, in press), and references therein.
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Cirigliano, V.1
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17044410404
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The specific results we include come from the latter reference
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V. Cirigliano, J.F. Donoghue, and E. Golowich, Phys. Rev. D 61, 093001 (2000); 61, 093002 (2000). The specific results we include come from the latter reference.
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21
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33744659655
-
-
note
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- is a factor of 2 larger than suggested by Eq. (2.2).
-
-
-
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22
-
-
85104159677
-
-
note
-
2=l, so that the J=0 state is of odd parity.
-
-
-
-
23
-
-
85104160541
-
-
note
-
K is the transition of 2π→4π with a threshold of √s≃0.56 GeV; this reaction is also strongly phase-space suppressed near threshold, so that no significant inelasticity exists for √s<0.8 GeV [3].
-
-
-
-
24
-
-
0003881681
-
-
Addison-Wesley, Reading, MA
-
In writing Eq. (2.8), we follow the form of the coupled-channel S matrix for J=1, S=1 nucleon-nucleon scattering in the presence of a tensor force; note M.A. Preston and R.K. Bhaduri, Structure of the Nucleus (Addison-Wesley, Reading, MA, 1975), p. 141ff.
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(1975)
Structure of the Nucleus
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Preston, M.A.1
Bhaduri, R.K.2
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28
-
-
85104160610
-
-
note
-
I,I3, where I =0,2, is identically zero.
-
-
-
-
29
-
-
85104160191
-
-
note
-
2 assumes that these neglected terms are negligible relative to the electromagnetic effects we consider.
-
-
-
-
30
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16644379868
-
-
hep-ph/9906269
-
5/2 contributions - so that, in this basis, the extra amplitude is labeled "I=1".
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(1999)
Phys. Rev. D
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Gardner, S.1
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Caso, C.1
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32
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33744671038
-
-
Choosing the - sign in Eq. (3.5) yields |y|>|x|, which is unacceptable
-
Choosing the - sign in Eq. (3.5) yields |y|>|x|, which is unacceptable.
-
-
-
-
33
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0032543008
-
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M. Knecht and R. Urech, Nucl. Phys. B519, 329 (1998); U.-G. Meissner, G. Müller, and S. Steininger, Phys. Lett. B 406, 154 (1997); 407, 454(E) (1997).
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M. Knecht and R. Urech, Nucl. Phys. B519, 329 (1998); U.-G. Meissner, G. Müller, and S. Steininger, Phys. Lett. B 406, 154 (1997); 407, 454(E) (1997).
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M. Knecht and R. Urech, Nucl. Phys. B519, 329 (1998); U.-G. Meissner, G. Müller, and S. Steininger, Phys. Lett. B 406, 154 (1997); 407, 454(E) (1997).
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36
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33744580295
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We thank M. Sevior and G. Smith for discussions concerning this point
-
We thank M. Sevior and G. Smith for discussions concerning this point.
-
-
-
-
41
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33744639723
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-
The authors of Ref. [15] also conclude this
-
The authors of Ref. [15] also conclude this.
-
-
-
-
42
-
-
85104160229
-
-
note
-
- branching ratio were varied by +3σ or +0.84%, the value of y decreases by 50%.
-
-
-
-
46
-
-
85104160306
-
-
note
-
I or of the amplitudes themselves, but the form of the parametrization in Eq. (2.25) persists.
-
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-
47
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private communication
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85104160445
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note
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η+η′=0.16 of Ref. [12].
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