Electromagnetic Interaction in the Presence of Isotopic Field-Charges and a Kinetic Field

Darvas, György

doi:10.1007/s10773-013-1781-2

Cited by 5 publications

(8 citation statements)

References 30 publications

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“…Earlier publications by the author [3] showed that this D field is subject to an invariance under rotations of an SU(2) isomorphic group that characterises hypersymmetry. We demonstrated that the (isotopic field-charge spin) transformation in the D field must be coupled with a SM interaction field, and also that the transformation leaves the mediating bosons of the respective SM field intact [10]. The derived formula confirms that the D field causes no observable effects at low velocities, but it should be taken into account at relativistic high velocities: it extends the SM but does not influence it in the range of its validity.…”

Section: Discussionmentioning

confidence: 68%

“…The absence of such precise high-velocity considerations led to anomalies that -among others -formulated the demand for extending the Standard Model (SM) in the nineties. In contrast to other models proposed for the extension of the SM, hypersymmetry (HySy) 1 offered an alternative by the application of a strongly relativistic model [6], [7], [8], [9], [10], [11], [12], [13], [3]. This model includes (among others) a velocity-dependent field (D), which proved to be a gauge field, and should be added to the SM fields.…”

Section: Introductionmentioning

confidence: 99%

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Hypersymmetry field rotation angle

Darvas

2020

Chinese Journal of Physics

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The paper determines a limit energy under which hypersymmetry (HySy) is broken. According to gauge theories, interaction mediating spin-0 bosons must be massless. The theory of HySy predicted massive intermediate bosons. Hypersymmetry field rotation, described in this paper, justifies the mass of the HySy mediating boson. The mass of intermediate bosons must arise from dynamical spontaneous breaking of the group of HySy. HySy rotation is performed in the velocity-dependent D field. The derived rotation of the field is defined by the spontaneous symmetry breaking and precession of the velocity v around its third projection in the D field (that produced the mass of the field's bosons). The latter represents the real-and effective velocities of a boson-emitting particle in the direction towards a target particle. The mass of the discussed (fictitious) Goldstone bosons can be removed by the unitarity gauge condition through Higgs (BEH) mechanism. According to the simultaneous presence of a Standard Model (SM) interaction's symmetry group and the (beyond SM) HySy group, their bosons should be transformed together. Spontaneous breakdown of HySy may allow performing a transformation that does not influence the SM physical state of the investigated system. The paper describes a field transformation that eliminates the mass of the intermediate bosons, rotates the SM-and HySy bosons' masses together while leaving the SM bosons intact. The result is an angle that characterises the HySy by a precession mechanism of the velocity that generates the field. In contrast to the known SM intermediate bosons, the HySy intermediate bosons have no fixed mass. The mass of the HySy intermediate bosons (that appear as quanta of a velocity-dependent gauge field D) depends on the relative velocity of the particles whose interaction they mediate. So, the derived precession angle is a function of that velocity.

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Section: Discussionmentioning

confidence: 68%

Section: Introductionmentioning

confidence: 99%

Hypersymmetry field rotation angle

Darvas

2020

Chinese Journal of Physics

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“…5 In contrast to the Pauli-Dirac treatment [27], this moment is a measurable quantity. Further conclusions are discussed in [22].…”

Section: The Electro-kinetic Momentmentioning

confidence: 96%

“…Otherwise, these minor alterations do not influence the conslusions (cf., e.g., (20a) in sec. 7 of [22]).…”

Section: Introductionmentioning

confidence: 97%

“…To restore the broken invariance, the paper refers to the conservation of the isotopic field-charge spin, proven in [14], so that the two transformations applied together ensure the invariance, and save the physical relevance of the theory. Secondly, the author introduces the isotopic electric charges in the classical Dirac equation [20]. At third, he extends the Dirac equation with a kinetic 1 Electromagnetic field theories were related with anisotropic geometries in, at least, two terms.…”

Section: Introductionmentioning

confidence: 99%

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The Isotopic Field-Charge Assumption Applied to the Electromagnetic Interaction

Darvas¹

2013

Int J Theor Phys

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This paper applies the isotopic field-charge spin theory (Darvas, IJTP 2011) to the electromagnetic interaction. First there is derived a modified Dirac equation in the presence of a velocity dependent gauge field and isotopic field charges (namely Coulomb and Lorentz type electric charges, as well as gravitational and inertial masses). This equation is compared with the classical Dirac equation. There is shown that, since the presence of isotopic fieldcharges would distort the Lorentz invariance of the equation, there is a transformation, which together with the Lorenz transformation restores the invariance of the equation, in accordance with the conservation of the isotopic field-charge spin (Darvas, 2009). The paper discusses the conclusions derived from the extensions of the Dirac equation. It is shown that in semiclassical approximation the model provides the original Dirac equation, and at significantly relativistic velocities it approaches to the Schrödinger equation. Among other conclusions, the clue gives physical meaning to the electric moment. The closing section summarises a few further conclusions and shows a few developments to be discussed in detail in a next paper (Darvas, 2013). A J J A J A what demonstrates an analogy with our formula derived in [22] based on the findings in this paper. Note also that the potential (Coulomb) charges behave like corpuscles, while the kinetic (Lorentz type) charges like waves [16]. This complementary double behaviour (formulated first by Bohr in 1927, then discussed in 1937 [5]) became subject of studies again (cf., [41]).

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Giving mass to the mediating boson of HyperSymmetry by a field transformation applying Higgs mechanism beyond the Standard Model

Darvas¹

2020

J. Phys.: Conf. Ser.

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According to gauge theories, interaction mediating spin-0 bosons must be massless. Theory of hypersymmetry (HySy) predicted massive intermediate bosons. Hypersymmetry field rotation, to be described in this paper, gives mass to the HySy mediating boson. Hysy rotation is performed in the velocity dependent D field – a gauge field defined beyond the Standard Model (SM). Its angle is something similar to the weak mixing Weinberg angle that explains the surplus mass to the neutral weak vector boson; as well as it is similar to the fermion flavour mixing Cabibbo-Kobayashi-Maskawa angles that justify the mass change under weakly interacting quarks’ mixing, respectively. Mass of intermediate bosons must arise from dynamical spontaneous breaking of the group of HySy. The mass of the discussed (fictitious) Goldstone bosons can be removed by the unitarity gauge condition through the Higgs (BEH) mechanism. According to the simultaneous presence of a SM interaction’s symmetry group and the HySy group, their bosons should be transformed together. Spontaneous breakdown of HySy may allow to perform a transformation that does not influence the SM physical state of the investigated system. The paper describes a field transformation that eliminates the mass of the intermediate bosons by the application of the BEH mechanism, rotates the SM and HySy bosons’ masses together, while leaves the SM bosons intact. The result is an angle of precession inclination that characterises the HySy mechanism. In contrast to the known SM intermediate bosons, the HySy intermediate bosons have no fix mass. The mass of the HySy intermediate bosons (that appear as quanta of a velocity dependent gauge field D) depends on the relative velocity of the particles whose interaction they mediate, therefore the derived transformation angle is a function of that velocity.

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Electromagnetic Interaction in the Presence of Isotopic Field-Charges and a Kinetic Field

Cited by 5 publications

References 30 publications

Hypersymmetry field rotation angle

Hypersymmetry field rotation angle

The Isotopic Field-Charge Assumption Applied to the Electromagnetic Interaction

Giving mass to the mediating boson of HyperSymmetry by a field transformation applying Higgs mechanism beyond the Standard Model

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