Weyl, Pontryagin, Euler, Eguchi and Freund

Abstract

In a September 1976 PRL Eguchi and Freund considered two topological invariants: the Pontryagin number $P\sim \int d^{4}x\sqrt{g}{R}^{\ast }R$ and the Euler number $\chi \sim \int d^{4}x\sqrt{g}{R}^{\ast }{R}^{\ast }$ and posed the question: to what anomalies do they contribute? They found that $P$ appears in the integrated divergence of the axial fermion number current, thus providing a novel topological interpretation of the anomaly found by Kimura in 1969 and Delbourgo and Salam in 1972. However, they found no analogous role for $\chi$. This provoked my interest and, drawing on my April 1976 paper with Deser and Isham on gravitational Weyl anomalies, I was able to show that for Conformal Field Theories the trace of the stress tensor depends on just two constants: \[ g^{μν}\langle T_{μν}\rangle=\frac{1}{(4π)^2}(cF-aG)\] where $F$ is the square of the Weyl tensor and $\int d^{4}x\sqrt{g}G/(4\pi {)}^2$ is the Euler number. For free CFTs with $N_s$massless fields of spin $s$ \[ 720c=6N_0 + 18N_{1/2} + 72 N_1~~~~ 720a=2N_0 + 11N_{1/2} + 124N_1 \]

arXiv commentPublished version, minor corrections and improvements, added references

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Cited by in corpus (8)

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• Curvature Invariants for accelerating Kerr-Newman black holes in (anti-)de Sitter spacetime
• Trace anomaly for Weyl fermions using the Breitenlohner-Maison scheme for ${\gamma }_{\ast }$
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• Dynamical 4-D Gauss-Bonnet action from matter-graviton interaction at one-loop
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