2022
DOI: 10.1016/j.cjph.2022.04.010
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Degenerate solutions to the massless Dirac and Weyl equations and a proposed method for controlling the quantum state of Weyl particles

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Cited by 5 publications
(9 citation statements)
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“…Furthermore, in [1] we have shown that all solutions to the Weyl equation are degenerate, corresponding to an infinite number of electromagnetic 4potentials, explicitly calculated in Theorem 3.1 in [1]. Some very interesting properties of Weyl particles, mainly regarding their control and localization, are discussed in [2,3].…”
Section:      =+mentioning
confidence: 90%
“…Furthermore, in [1] we have shown that all solutions to the Weyl equation are degenerate, corresponding to an infinite number of electromagnetic 4potentials, explicitly calculated in Theorem 3.1 in [1]. Some very interesting properties of Weyl particles, mainly regarding their control and localization, are discussed in [2,3].…”
Section:      =+mentioning
confidence: 90%
“…[10][11][12][13][14][15] Furthermore, the state of Weyl and massless Dirac particles described by degenerate spinors, will not be affected by the presence of a plane electromagnetic wave, e.g., a laser beam of arbitrary polarization, propagating along the direction of motion of the particles. [3] Thus, particles in degenerate states, as well as electromagnetic waves can propagate along the same direction without interacting with each other, which obviously is not the case for charged particles in nondegenerate states.…”
Section: On the Experimental Detection Of Degenerate Statesmentioning
confidence: 99%
“…In the latter case, the corresponding electromagnetic 4‐potentials are calculated using Theorem 3.1. [ 1 ] In recent articles [ 2–5 ] we have extended these results providing several classes of degenerate solutions to the Dirac and Weyl equations for massive [ 2,5 ] and massless [ 3,4 ] particles, and describing their physical properties and potential applications. Furthermore, we discuss some very interesting properties of Weyl particles, mainly regarding their localization.…”
Section: Introductionmentioning
confidence: 99%
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“…In a recent work, [ 2 ] we have shown that all spinors of the form ψbadbreak=()cosθ()t2normaleiφtsinθ()t2exp[]normalih()boldr,t\begin{equation}\hspace*{8pc}\psi = \left( { \def\eqcellsep{&}\begin{array}{@{}*{1}{c}@{}} {\cos \left( {\frac{{\theta \left( t \right)}}{2}} \right)}\\ {{{\rm{e}}^{{\rm{i}}\varphi \left( t \right)}}\sin \left( {\frac{{\theta \left( t \right)}}{2}} \right)} \end{array} } \right){\rm{exp}}\left[ {{\rm{i}}h\left( {{\bf{r}},t} \right)} \right]\end{equation}…”
Section: Introductionmentioning
confidence: 99%