We compute tree-level n-point scattering amplitudes in scalar field theories in terms of geometric invariants on a fiber bundle. All 0- and 2-derivative interactions are incorporated into a metric on this bundle. The on-shell amplitudes can be efficiently pieced together from covariant Feynman rules, and we present a general closed formula for obtaining the n-point amplitude in this way. The covariant Feynman rules themselves can be derived using a generalization of the normal coordinate expansion of the fiber bundle metric. We demonstrate the efficiency of this approach by computing the covariant Feynman rules up to n ¼ 10 points, from which one can obtain the full amplitudes using our general formula. The formalism offers a prototype for obtaining geometric amplitudes in theories with higher-derivative interactions, by passing from the fiber bundle to its jet bundles.
Alminawi, M., Brivio, I., Davighi, J. (2026). Scalar amplitudes from fiber bundle geometry. PHYSICAL REVIEW D, 113(7), 076005-076019 [10.1103/qxwr-1vs6].
Scalar amplitudes from fiber bundle geometry
Brivio, Ilaria;
2026
Abstract
We compute tree-level n-point scattering amplitudes in scalar field theories in terms of geometric invariants on a fiber bundle. All 0- and 2-derivative interactions are incorporated into a metric on this bundle. The on-shell amplitudes can be efficiently pieced together from covariant Feynman rules, and we present a general closed formula for obtaining the n-point amplitude in this way. The covariant Feynman rules themselves can be derived using a generalization of the normal coordinate expansion of the fiber bundle metric. We demonstrate the efficiency of this approach by computing the covariant Feynman rules up to n ¼ 10 points, from which one can obtain the full amplitudes using our general formula. The formalism offers a prototype for obtaining geometric amplitudes in theories with higher-derivative interactions, by passing from the fiber bundle to its jet bundles.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.



