Abstract
On the basis of the first principles we argue that self/anti-self charge conjugate states of the (1/2,0) ⊕ (0,1/2) representation can possess the axial charge. Finally, we briefly discuss recent claims of the EquationSource% MathType!MTEF!2!1!+- % feaagCart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn % hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr % 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9 % vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x % fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeSipIOZaa8 % HaaeaacqaHdpWCaiaawEniaiabgwSixpaadmaabaWaa8HaaeaacaWG % bbaacaGLxdcacqGHxdaTdaWhcaqaaiaadgeaaiaawEniaiaacQcaai % aawUfacaGLDbaaaaa!4689!]]</EquationSource><EquationSource Format="TEX"><![CDATA[$$ \sim \overrightarrow \sigma \cdot \left[ {\overrightarrow A \times \overrightarrow A *} \right]$$ interaction term for the particles of this representation.
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Dvoeglazov, V.V. (1998). Chiral Interactions of Massive Particles in the (1/2,0) ⊕ (0,1/2) Representation. In: Hunter, G., Jeffers, S., Vigier, JP. (eds) Causality and Locality in Modern Physics. Fundamental Theories of Physics, vol 97. Springer, Dordrecht. https://doi.org/10.1007/978-94-017-0990-3_32
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DOI: https://doi.org/10.1007/978-94-017-0990-3_32
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