Abstract:We study internal structure of the Duffin-Kemmer-Petiau equations for spin 0 and spin 1 mesons. We show that in the noninteracting case full covariant solutions of thes=0ands=1DKP equations are generalized solutions of the Dirac equation.
“…In the next Section we transform the Hagen-Hurley equations, in the interacting case, into two Dirac equations with non-standard solutions involving higher-order spinors, extending our earlier results described in [1]. These generalized solutions bear some analogy to generalized solutions of the Dirac equation argued to describe a lepton and three quarks [21].…”
Section: Introductionmentioning
confidence: 60%
“…Therefore, we shall base our theory on the 7 × 7 formulation, see Eqs. (18), (19) in [1] and Subsection 6 ii) in [19]. These equations violate parity P , where P :…”
Section: Generalized Solutions Of the Dirac Equation In The Interactimentioning
confidence: 99%
“…Recently, we have shown that in the free case covariant solutions of the s = 0 and s = 1 Duffin-Kemmer-Petiau (DKP) equations are generalized solutions of the Dirac equation [1]. These wavefunctions are non-standard since they involve higher-order spinors.…”
Section: Introductionmentioning
confidence: 99%
“…Several classes of potentials were used in DKP equations to investigate interactions of spin 1 particles [6][7][8][9][10][11][12][13][14][15]. However, we shall apply the 7 × 7 Hagen-Hurley equations [16][17][18] in spinor form [1,19,20]. Our motivation stems from the observation that these equations violate parity and thus should describe weakly interacting particles.…”
Section: Introductionmentioning
confidence: 99%
“…We have shown recently that, in the non-interacting case, solutions of the s = 0 and s = 1 DKP equations are generalized solutions of the Dirac equation [1].…”
We study the 7×7 Hagen-Hurley equations describing spin 1 particles. We split these equations, in the interacting case, into two Dirac equations with non-standard solutions. It is argued that these solutions describe decay of a virtual W boson in beta decay. *
“…In the next Section we transform the Hagen-Hurley equations, in the interacting case, into two Dirac equations with non-standard solutions involving higher-order spinors, extending our earlier results described in [1]. These generalized solutions bear some analogy to generalized solutions of the Dirac equation argued to describe a lepton and three quarks [21].…”
Section: Introductionmentioning
confidence: 60%
“…Therefore, we shall base our theory on the 7 × 7 formulation, see Eqs. (18), (19) in [1] and Subsection 6 ii) in [19]. These equations violate parity P , where P :…”
Section: Generalized Solutions Of the Dirac Equation In The Interactimentioning
confidence: 99%
“…Recently, we have shown that in the free case covariant solutions of the s = 0 and s = 1 Duffin-Kemmer-Petiau (DKP) equations are generalized solutions of the Dirac equation [1]. These wavefunctions are non-standard since they involve higher-order spinors.…”
Section: Introductionmentioning
confidence: 99%
“…Several classes of potentials were used in DKP equations to investigate interactions of spin 1 particles [6][7][8][9][10][11][12][13][14][15]. However, we shall apply the 7 × 7 Hagen-Hurley equations [16][17][18] in spinor form [1,19,20]. Our motivation stems from the observation that these equations violate parity and thus should describe weakly interacting particles.…”
Section: Introductionmentioning
confidence: 99%
“…We have shown recently that, in the non-interacting case, solutions of the s = 0 and s = 1 DKP equations are generalized solutions of the Dirac equation [1].…”
We study the 7×7 Hagen-Hurley equations describing spin 1 particles. We split these equations, in the interacting case, into two Dirac equations with non-standard solutions. It is argued that these solutions describe decay of a virtual W boson in beta decay. *
We carry out a constructive review of non-standard solutions of relativistic wave equations. Such solutions are obtained via splitting of relativistic wave equations written in spinor form. All these solutions are also solutions of the Dirac equation and are non-standard because they involve higher-order spinors. The main finding is that non-standard solutions describe decaying states.
In the present work a transition from the spin-0 Duffin-Kemmer-Petiau equation to the Dirac equation is described. This transformation occurs when a crossed field changes into a certain longitudinal field. An experimental setup to carry out the transition is proposed.
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