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Structure of K3π Decay

Henry D. I. Abarbanel

Open publisher page 36 citations

Abstract

Using the partially conserved axial-vector current and the commutation relations of the vector and axial-vector currents with themselves and with the Hamiltonian responsible for weak nonleptionic decays, we demonstrate how to expand weak-decay amplitudes in the momenta of pions involved in the decays. The resulting expansion gives the on-mass-shell decay amplitude up to first order in pion momenta. We apply these techniques to the three-pion decays of kaons and show that they quantitatively reproduce the experimental situation of an amplitude linearly dependent on the "odd"-pion kinetic energy. All three pions are treated on an equal footing, and on-the-mass-shell quantities are dealt with everywhere.

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What this paper is about

Using the partially conserved axial-vector current and the commutation relations of the vector and axial-vector currents with themselves and with the Hamiltonian responsible for weak nonleptionic decays, we demonstrate how to expand weak-decay amplitudes in the momenta of pions involved in the decays. The resulting expansion gives the on-mass-shell decay amplitude up to first order in pion momenta. We apply these techniques to the three-pion decays of kaons and show that they quantitatively reproduce the experimental situation of an amplitude linearly dependent on the "odd"-pion kinetic energy. All three pions are treated on an equal footing, and on-the-mass-shell quantities are dealt with everywhere.

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Available abstract

Using the partially conserved axial-vector current and the commutation relations of the vector and axial-vector currents with themselves and with the Hamiltonian responsible for weak nonleptionic decays, we demonstrate how to expand weak-decay amplitudes in the momenta of pions involved in the decays. The resulting expansion gives the on-mass-shell decay amplitude up to first order in pion momenta. We apply these techniques to the three-pion decays of kaons and show that they quantitatively reproduce the experimental situation of an amplitude linearly dependent on the "odd"-pion kinetic energy. All three pions are treated on an equal footing, and on-the-mass-shell quantities are dealt with everywhere.

Key concepts: Pion, Physics, Amplitude, Hamiltonian (control theory), Particle physics, Kinetic energy, Nuclear physics, Mathematical physics

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