Abstract
The standard model of gauge theory for weak and electromagnetic interactions describes fermions as having a definite chirality: left and right chiralities are so different that for example the left handed part of the electron and its right-handed part (each of which is a Weyl fermion) do not have the same quantum numbers (weak hypercharge for example) [1,2], and thus it is natural to try to quantize gauge theories with Weyl fermions.
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© 1987 Plenum Press, New York
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Viallet, CM. (1987). On the Covariant Quantization of Anomalous Gauge Theories. In: Lee, H.C., Elias, V., Kunstatter, G., Mann, R.B., Viswanathan, K.S. (eds) Super Field Theories. NATO Science Series, vol 160. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-0913-0_17
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DOI: https://doi.org/10.1007/978-1-4613-0913-0_17
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