English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Plus monthly

Global: Zendy Tools annual

Global: Zendy Tools monthly

Global: Zendy Free Plan

Theoretically, in (1+1) dimensions, one can have Klein-Fock-Gordon-Majorana(KFGM) particles. More precisely, these are one-dimensional (1D)Klein-Fock-Gordon (KFG) and Majorana particles at the same time. In principle,the wave equations considered to describe such first-quantized particles arethe standard 1D KFG equation and/or the 1D Feshbach-Villars (FV) equation, eachwith a real Lorentz scalar potential and some kind of Majorana condition. Theaim of this paper is to analyze the latter assumption fully and systematically;additionally, we introduce specific equations and boundary conditions tocharacterize these particles when they lie within an interval (or on a linewith a tiny hole at a point). In fact, we write first-order equations in thetime derivative that do not have a Hamiltonian form. We may refer to theseequations as first-order 1D Majorana equations for 1D KFGM particles. Moreover,each of them leads to a second-order equation in time that becomes the standard1D KFG equation when the scalar potential is independent of time. Additionally,we examine the nonrelativistic limit of one of the first-order 1D Majoranaequations.

Characterizing Klein-Fock-Gordon-Majorana particles in (1+1) dimensions