Abstract
It is proposed that the Generation Model (GM) of particle physics, which describes the elementary particles, the six leptons, the six quarks and the three weak bosons, of the Standard Model (SM) as composite particles in terms of three kinds of rishons and their antiparticles may be mimicking a simpler model, employing only two kinds of rishons and their antiparticles.
Highlights
The Two-Rishon Generation ModelIn the GM [2] [8] it is assumed that each of the three kinds of rishons, T, V and U, carries a color charge, red, green or blue, while each of their antiparticles, T , V and U , carries an anticolor charge, antired, antigreen or antiblue
It is proposed that the Generation Model (GM) of particle physics, which describes the elementary particles, the six leptons, the six quarks and the three weak bosons, of the Standard Model (SM) as composite particles in terms of three kinds of rishons and their antiparticles may be mimicking a simpler model, employing only two kinds of rishons and their antiparticles
It has been demonstrated that the GM of particle physics, which describes the elementary particles of the SM of particle physics as composite particles in terms of three kinds of rishons and their antiparticles, may be replaced by a simpler equivalent model employing only two kinds of rishons and their antiparticles
Summary
In the GM [2] [8] it is assumed that each of the three kinds of rishons, T, V and U, carries a color charge, red, green or blue, while each of their antiparticles, T , V and U , carries an anticolor charge, antired, antigreen or antiblue. It should be noted that for any given transition the generation quantum number is required to be conserved, each particle of the second generation has two possible values of g. The additional colorless rishon-antirishon pair, ( V *V ) or (VV * ), essentially acts as a spectator during the weak interaction process thereby conserving the generation quantum number g,. In the GM the rishon structures of the third generation of leptons and quarks are the same as the corresponding leptons and quarks of the first generation plus the addition of two rishon-antirishon pairs, Π , that are given by Equation (1). It should be noted that for any given transition the generation quantum number is required to be conserved, each particle of the third generation has three possible values of g. Which proceeds via the four transitions: TTT (V *V )(V *V ) → VVV (V *V )(V *V ) + TTTVVV ,
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