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Matches in SemOpenAlex for { <https://semopenalex.org/work/W2127747745> ?p ?o ?g. }

• W2127747745 endingPage "B966" @default.
• W2127747745 startingPage "B959" @default.
• W2127747745 abstract "Assuming that the strong interaction ${H}_{mathrm{st}}$ is invariant under the particle-antiparticle conjugation $C$, it is shown that all possible $C$-noninvariant electromagnetic interactions ${H}_{ensuremath{gamma}}$ can be classified according to the anticommutator between $C$ and the charge operator $Q$ into two types: (1) ${C, Q}=0$ and (2) ${C, Q}ensuremath{ne}0$. Discussions of the first type $C$-noninvariant minimal electromagnetic interaction have already been given in a previous paper. If ${C, Q}ensuremath{ne}0$, then the operator $C$ must be different from what is normally called the charge-conjugation operator ${C}_{ensuremath{gamma}}$ which, by definition, changes any state of charge $Q$ to that of $ensuremath{-}Q$. Thus, ${{C}_{ensuremath{gamma}}, Q}=0$ and $Censuremath{ne}{C}_{ensuremath{gamma}}$. As a consequence, there must exist, at least, a charged particle ${a}^{+}$ which is an eigenstate of $C$; its eigenvalue can always be chosen to be +1. Furthermore, in the framework of a Lorentz-invariant local-field theory, ${H}_{mathrm{st}}$ and ${H}_{ensuremath{gamma}}$ are invariant under ${C}_{ensuremath{gamma}}mathrm{PT}$, but not $mathrm{CPT}$. The ${C}_{ensuremath{gamma}}mathrm{PT}$ invariance requires the existence of another charged particle ${a}^{ensuremath{-}}$ which has the same mass as ${a}^{+}$ but the opposite charge. The ${a}^{ensuremath{-}}$ is also an eigenstate of $C$. The existence of such ${a}^{ifmmodepmelsetextpmfi{}}$ particles necessitates not only the $C$ nonconservation of ${H}_{ensuremath{gamma}}$, but also the $T$ noninvariance of ${H}_{mathrm{st}}$. The general algebraic relations between ${H}_{mathrm{st}}$, ${H}_{ensuremath{gamma}}$, and these symmetry operators are studied, and the properties of the particles ${a}^{ifmmodepmelsetextpmfi{}}$ are discussed. An explicit spin-textonehalf{} model of ${a}^{ifmmodepmelsetextpmfi{}}$ based on the principle of minimal electromagnetic interaction is given. A possible unifying view connecting the present $C$, $T$ noninvariance with the well-known $C$, $P$ nonconservation of the weak interaction is discussed." @default.
• W2127747745 created "2016-06-24" @default.
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• W2127747745 date "1965-11-22" @default.
• W2127747745 modified "2023-09-25" @default.
• W2127747745 title "Classification of All<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>C</mml:mi></mml:math>-Noninvariant Electromagnetic Interactions and the Possible Existence of a Charged, but<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>C</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mn /></mml:math>, Particle" @default.
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• W2127747745 doi "https://doi.org/10.1103/physrev.140.b959" @default.
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