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Covariant quantization of totally antisymmetric tensor-spinor field in AdSd

A. O. Barvinsky1,2,*, I. L. Buchbinder3,4,5,†, V. A. Krykhtin6,‡, and D. V. Nesterov1,§

  • *Contact author: barvin@lpi.ru
  • †Contact author: buchbinder@theor.jinr.ru
  • ‡Contact author: krykhtin@tpu.ru
  • §Contact author: nesterov@lpi.ru

Phys. Rev. D 113, 045022 – Published 24 February, 2026

DOI: https://doi.org/10.1103/1f2m-wg1p

Abstract

We develop the quantization of a recently proposed model describing a totally antisymmetric rank-p tensor-spinor field (a fermionic p-form theory) in d-dimensional anti–de Sitter (AdS) space. The model provides a new nontrivial example of a reducible gauge theory, in which gauge transformations are linearly dependent and the degree of reducibility increases with p. It is well-known that in such cases the standard Faddeev-Popov-DeWitt prescription for the generating functional is not applicable. We quantize the fermionic p-form theory using the general Batalin-Vilkovisky formalism, employing two distinct gauge fermions associated with gauge-fixing functions of different admissible ranks, confirming the independence from the gauge choice. As a result, we obtain the quantum effective action in terms of a sequence of functional determinants corresponding to specific Dirac-like operators on AdS space.

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