“…2.2], and the Lorentz relativistically covariant model which was studied and advanced in [1], [23,Sect. 16], [31], [34], [37,Sects. 2,6], [40], [41, Sects.…”
Section: (T)] = Q E (T R (T)) + 1 C V (T) × B (T R (T))mentioning
confidence: 99%
“…Then using the charge equilibrium equation (15) we eliminate the nonlinearity G in the above equation (34) and obtain the following equation equivalent to it:…”
Section: Accelerated Motion Of Wave-corpuscle In An External Electricmentioning
It is well known that the concept of a point charge interacting with the electromagnetic (EM) field has a problem. To address that problem we introduce the concept of wave-corpuscle to describe spinless elementary charges interacting with the classical EM field. Every charge interacts only with the EM field and is described by a complex valued wave function over the 4-dimensional space time continuum. A system of many charges interacting with the EM field is defined by a local, gauge and Lorentz invariant Lagrangian with a key ingredient-a nonlinear self-interaction term providing for a cohesive force assigned to every charge. An ideal wave-corpuscle is an exact solution to the Euler-Lagrange equations describing both free and accelerated motions. It carries explicitly features of a point charge and the de Broglie wave. Our analysis shows that a system of well separated charges moving with nonrelativistic velocities are represented accurately as wave-corpuscles governed by the Newton equations of motion for point charges interacting with the Lorentz forces. In this regime the nonlinearities are "stealthy" and don't show explicitly anywhere, but they provide for the binding forces that keep localized every individual charge. The theory can also be applied to closely interacting charges as in hydrogen atom where it produces discrete energy spectrum.
“…2.2], and the Lorentz relativistically covariant model which was studied and advanced in [1], [23,Sect. 16], [31], [34], [37,Sects. 2,6], [40], [41, Sects.…”
Section: (T)] = Q E (T R (T)) + 1 C V (T) × B (T R (T))mentioning
confidence: 99%
“…Then using the charge equilibrium equation (15) we eliminate the nonlinearity G in the above equation (34) and obtain the following equation equivalent to it:…”
Section: Accelerated Motion Of Wave-corpuscle In An External Electricmentioning
It is well known that the concept of a point charge interacting with the electromagnetic (EM) field has a problem. To address that problem we introduce the concept of wave-corpuscle to describe spinless elementary charges interacting with the classical EM field. Every charge interacts only with the EM field and is described by a complex valued wave function over the 4-dimensional space time continuum. A system of many charges interacting with the EM field is defined by a local, gauge and Lorentz invariant Lagrangian with a key ingredient-a nonlinear self-interaction term providing for a cohesive force assigned to every charge. An ideal wave-corpuscle is an exact solution to the Euler-Lagrange equations describing both free and accelerated motions. It carries explicitly features of a point charge and the de Broglie wave. Our analysis shows that a system of well separated charges moving with nonrelativistic velocities are represented accurately as wave-corpuscles governed by the Newton equations of motion for point charges interacting with the Lorentz forces. In this regime the nonlinearities are "stealthy" and don't show explicitly anywhere, but they provide for the binding forces that keep localized every individual charge. The theory can also be applied to closely interacting charges as in hydrogen atom where it produces discrete energy spectrum.
“…To see this, we return to the Sommerfeld-Page Eq. (8), which can be written in the following form [9,16]:…”
Section: Runaway and Acausalitymentioning
confidence: 99%
“…This can be seen most easily if Eq. (25) is turned into an integral equation with a Green's function [9,16]: Then the Green's function G(r) vanishes for~<0. Therefore, the motion is causal.…”
Section: Runaway and Acausalitymentioning
confidence: 99%
“…There are several excellent text books [12,13,14] and review articles [15,16,17] on the classical electron theory.…”
ABSTRACT. The current status of understanding of the equation of motion of an electron is summarized. Classically, a consistent, linearized theory exists for an electron of finite extent, as long as the size of the electron is larger than the classical electron radius. Nonrelativistic quantum mechanics seems to offer a tine theory even in the point-particle limit.
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