As for several nuclear reactions, the electroweak interaction is simply explained by a law of conservation of particle number. We find that the positron and electron consist of the three fundamental particles, and , respectively. Furthermore, the members of the second and third generations quark composites consist of the first generation quark and the neutrino of fundamental particles. The particle and its anti- particle pair(or neutrino and its antineutrino pair) have to be an energy quantum (or a photon). The minimum Higgs boson (called “God particle”) might be a neutral pion. The fundamental particles are simply up and down quark, neutrino, muon-neutrino, and those anti-particles.
References
[1]
Ryden, B. (2003) Introduction to Cosmology, 1st edition, Japanese language edition, (Pearson Education, Inc.), Chapter 10.
[2]
M. Gell-Mann, “A Schematic Model of Baryons and Mesons,” Physics Letters Vol 8, 1964, PP. 214-215.
[3]
Zweig, G. (1964) “AN MODEL FOR STRONG INTERACTION SYMMETRY AND ITS BREAKING I,” CERN Reports 8182/TH.401 and “AN MODEL FOR STRONG INTERACTION SYMMETRY AND ITS BREAKING II 8419/TH.412”
[4]
Hamatsu, R. (1990) High Energy Physics of physics lecture course, Tokyo Metropolitan University.
[5]
A. Kernan, W. M. Powell, C. L. Sandler, W.L. Knight, and F. Russell Stannard, “Muonic-Decay Branching Ratio of the Lambda Hyperon,” Phys. Rev. Vol 133, 1964, B1271-B1273.
[6]
Yuksel, H, (2006) “Positron Annihilations at the Galactic Center: Generating More Questions Than Answers,” arXiv:astro-ph/0609139v1.
[7]
W. M. Yao et al. (Particle Data Group), “Review of Particle Physics,” J. Phys. G Vol 33, 2006, PP. 1-1232. and 2007 partial update for edition 2008,
http://pdg.lbl.gov/
[8]
A. F. Falk, A Lewandowski, A.A. Petrov, “Effects from the charm scale in ,” Phys. Lett. B Vol 505, 2001, PP. 107-112.
[9]
J.-E. Augustin et al., “Discovery of a Narrow Resonance in Annihilation,” Phys. Rev. Lett. Vol 33, 1974, PP. 1406-1408.
[10]
F. Abe et al., “Identification of top quarks using kinematic variables,” Phys. Rev. D Vol 52, 1995, PP. R2605-R2609.
[11]
P. Igo-Kemenes, “Searches for Higgs bosons at LEP2,” J. Phys. G: Nucl. Part. Phys. Vol 24, 1998, PP. 325-335 and Updated October 2005 by P. Igo-Kemenes.
[12]
P.W. Higgs, “Broken Symmetries and the Masses of Gauge Bosons,” Phys. Rev. Lett. Vol 13, 1964, PP. 508-509.
[13]
T. Nakano et al., “Evidence for a Narrow S = + 1 Baryon Resonance in Photoproduction from the Neutron,” Phys. Rev. Lett. Vol 91, 2003, PP. 012002.
D. Atwood, I. Dunietz, and A. Soni, “Enhanced CP Violation with Modes and Extraction of the Cabibbo-Kobayashi-Maskawa Angle ,” Phys. Rev. Lett. Vol 78, 1997, PP. 3257-3260.
[16]
S. Eidelman, et al., “Charm Dalitz Plot Analysis Formalism and Results,” Phys. Lett. B Vol 592, 2004, PP. 1-1109.
[17]
Horii, Y, et al., (2010) First Evidence of the Decay Followed by ,
http://belle.kek.jp/results/summer10/dk_ads/.