Abstract
The intended unification of electromagnetic, weak, strong, and gravitational interactions within the geometric concept of gauge invariance is still flawed by one essential shortcoming that cannot be disregarded.
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- 1.
(Weyl 1924, p. 609), “eine dynamische Theorie der Materie am aussichtsreichsten: die Materie ein felderregendes Agens, das Feld ein extensives Medium, das die Wirkungen von Körper zu Körper überträgt.”
- 2.
Fermions with a higher half-integer spin are not to be considered here.
- 3.
- 4.
This restriction is to be explained later on.
- 5.
In compliance with our previous conventions, we denote the covariant derivative in a vector bundle by the same symbol D, since it is always possible to infer from the field in question which representation of the structure group or its covering group is meant.
- 6.
A corresponding conservation law is also valid for the axial vector current \(j_{n+1}:=i\overline{\psi }{}^{*}\gamma \gamma ^{n+1}\psi \) of a Dirac field without mass. However, a quantum-theoretic treatment by means of a functional integral, due to an anomaly, results in (cf., for instance, Jackiw 1977)
$$ \langle - \infty | D \tau _{A}| \infty \rangle ^{\overset{(+)}{-}} = \frac{1}{(4.) 8\pi ^{2}} \mathrm {Tr} (\varOmega ^{g} \wedge \varOmega ^{g(*)}) . $$Thus in quantum field theory, the conservation of the axial current is violated by topological contributions of the Pontryagin class, and this in dependence on the asymptotic helicity states concerning \(\gamma ^{n+1}\). This is the physical content of the celebrated Atiyah–Singer index theorem (Römer 1981a, b; Eguchi et al. 1980).
- 7.
At an earlier stage, this was described as a “mixed” theory, since the affine connection and the tetrad field occur as independent variables in the variation procedure.
- 8.
The Heisenberg–Pauli–Weyl spinor equation within two dimensions serves as the starting point for the quantum-field-theoretic Thirring model (1958). This equation has solutions not only exhibiting quark confinement (Chang et al. 1975; Hortaçsu 1977), but also with particle characteristics (Yamamoto 1977; Rañada & Rañada 1984).
- 9.
- 10.
- 11.
...ferner der Grund, warum wir an der Energie oder trägen Masse eines zusammengesetzten Körpers die nicht auflösbare Energie seiner letzten materiellen Elementarbestandteile der auflösbaren Energie ihrer wechselseitigen Bindung gegenüberstellen.” (Weyl 1924, p. 592).
- 12.
Hermann Weyl’s still valid admonitory statement is to be remembered here:
The formulation of Dirac’s theory of the electron in the frame of general relativity has to its credit one feature that should be appreciated even by the atomic physicist who feels safe in ignoring the role of gravitation in the building up of the elementary particles: its explanation of the quantum-mechanical principle of “gauge invariance” that connects Dirac’s \(\psi \) with the electromagnetic potentials
(Weyl 1950).
- 13.
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Mielke, E.W. (2017). Spinor Bundles. In: Geometrodynamics of Gauge Fields. Mathematical Physics Studies. Springer, Cham. https://doi.org/10.1007/978-3-319-29734-7_11
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