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Prog. Theor. Phys. Vol. 47 No. 4 (1972) pp. 1418-1420
Letters
An Explanation of Helicity Conservation from the Quark Model and Tensor Coupling
Minoru Biyajima,
Masakatsu Kenmoku and
Toshiyuki Minamikawa*
Department of Physics, Tokyo University of Education, Tokyo
*Tokyo University of Mercantile Marine, Tokyo
(Received October 12, 1971)
URL :
http://ptp.ipap.jp/link?PTP/47/1418/
DOI : 10.1143/PTP.47.1418
References:
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H. H. Bingham et al., Phys. Rev. Lett. 24 (1970), 955[APS].
J Ballam et al., Phys. Rev. Lett. 24 (1970), 960[APS].
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Aachen-Berlin-Bonn-CERN-Cracow-Heidelberg-London-Vienna Collaboration. Phys. Lett. B 34 (1971), 160[CrossRef].
G. Ascoli et al., Phys. Rev. Lett. 26 (1971), 929[APS].
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F. G. Gilman, J. Pumplin, A. Schwimmer and L. Stodolsky, Phys. Lett. B 31 (1970), 387[CrossRef]; Many published literatures and preprints.
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H. F. Jones and A. Salam, Phys. Lett. B 34 (1971), 149[CrossRef].
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B. Sakita and K. Wali, Phys. Rev. 131 (1965), B1335[APS].
A. Salam et al., Proc. Roy. Soc. A 284 (1965), 146.
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R. Gatto, L. Maiami and G. Preparata, Phys. Rev. 140 (1965), B1579[APS].
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R. P. Feynman, M. Kislinger and F. Ravndal, Phys. Rev. D 3 (1971), 2706[APS].
- The connection between Σµ Σν and θµν: By the identity i φ γµ φ= φφΣµ/2mN + φ σµν Δν φ/2mN, we find that Σµ φ γµ φ and Σµ Σν φ φ are helicity conserving in the s →∞ limit, though the s-channel H. C. matrix element of φ φ tends to zero.
Citing Article(s) :
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Progress of Theoretical Physics Vol. 47 No. 5 (1972) pp. 1601-1609
:
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Helicity Conservation in πN →A1N Scattering
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Minoru Biyajima