“…This is the case of longitudinal potentials for which several exact solutions of the Dirac equation were found [10].…”
Section: Splitting the Dirac Equation In Longitudinal External Fieldsmentioning
confidence: 99%
“…In what follows we shall work with external fields of special configuration, so-called crossed and longitudinal fields, non-standard but Lorentz covariant, see [10]. We shall also need elements of spinor calculus.…”
Section: Relativistic Wave Equationsmentioning
confidence: 99%
“…It is possible to separate variables in Equations (33) and (34) following procedures described in [10]. Substituting ξ 1…”
Section: Separation Of Variables In Subequationsmentioning
confidence: 99%
“…where λ 2 1 is the separation constant and we note that Equations (46a) and (46b) are analogous to Equations (12.15) and (12.19) in [10].…”
Section: Separation Of Variables In Subequationsmentioning
confidence: 99%
“…Substituting first two equations into the third one in Equation (61), we get the Klein-Gordon equation π µ π µ ψ = m 2 ψ, which can be solved via separation of variables for the case of crossed fields, see Chapter 3 in [10] (the same can be done in Equation (62)). …”
Section: Splitting the Spin 0 Duffin-kemmer-petiau Equations In Crossmentioning
Abstract:In the present paper we study subsolutions of the Dirac and Duffin-Kemmer-Petiau equations in the interacting case. It is shown that the Dirac equation in longitudinal external fields can be split into two covariant subequations (Dirac equations with built-in projection operators). Moreover, it is demonstrated that the Duffin-Kemmer-Petiau equations in crossed fields can be split into two 3 × 3 subequations. We show that all the subequations can be obtained via minimal coupling from the same 3 × 3 subequations which are thus a supersymmetric link between fermionic and bosonic degrees of freedom.
“…This is the case of longitudinal potentials for which several exact solutions of the Dirac equation were found [10].…”
Section: Splitting the Dirac Equation In Longitudinal External Fieldsmentioning
confidence: 99%
“…In what follows we shall work with external fields of special configuration, so-called crossed and longitudinal fields, non-standard but Lorentz covariant, see [10]. We shall also need elements of spinor calculus.…”
Section: Relativistic Wave Equationsmentioning
confidence: 99%
“…It is possible to separate variables in Equations (33) and (34) following procedures described in [10]. Substituting ξ 1…”
Section: Separation Of Variables In Subequationsmentioning
confidence: 99%
“…where λ 2 1 is the separation constant and we note that Equations (46a) and (46b) are analogous to Equations (12.15) and (12.19) in [10].…”
Section: Separation Of Variables In Subequationsmentioning
confidence: 99%
“…Substituting first two equations into the third one in Equation (61), we get the Klein-Gordon equation π µ π µ ψ = m 2 ψ, which can be solved via separation of variables for the case of crossed fields, see Chapter 3 in [10] (the same can be done in Equation (62)). …”
Section: Splitting the Spin 0 Duffin-kemmer-petiau Equations In Crossmentioning
Abstract:In the present paper we study subsolutions of the Dirac and Duffin-Kemmer-Petiau equations in the interacting case. It is shown that the Dirac equation in longitudinal external fields can be split into two covariant subequations (Dirac equations with built-in projection operators). Moreover, it is demonstrated that the Duffin-Kemmer-Petiau equations in crossed fields can be split into two 3 × 3 subequations. We show that all the subequations can be obtained via minimal coupling from the same 3 × 3 subequations which are thus a supersymmetric link between fermionic and bosonic degrees of freedom.
The dynamics of relativistic particles of spin 0 and 1/2, interacting with an external electromagnetic field and a quantized plane wave, is studied using the path integral framework. We take advantage of the existing properties of the interaction to introduce a delta functional in order to calculate Green's functions. This simply reduces the problem to two coupled oscillators. The energy spectrum and wave functions are calculated for the spin 0 case and the analogy with Jaynes‐Cummings model is made to derive the energy spectrum for the spin 1/2 case.
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