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Phys."],"published-print":{"date-parts":[[2018,7]]},"abstract":"<jats:title>A<jats:sc>bstract<\/jats:sc><\/jats:title><jats:p>We compute the one-loop free energies of the type-A<jats:sub>\u2113<\/jats:sub>and type-B<jats:sub>\u2113<\/jats:sub>higher-spin gravities in (<jats:italic>d<\/jats:italic>+ 1)-dimensional anti-de Sitter (AdS<jats:sub><jats:italic>d<\/jats:italic>+1<\/jats:sub>) spacetime. For large<jats:italic>d<\/jats:italic>and \u2113, these theories have a complicated field content, and hence it is difficult to compute their zeta functions using the usual methods. Applying the character integral representation of zeta function developed in the companion paper [<jats:ext-link xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" xlink:href=\"https:\/\/arxiv.org\/abs\/1805.05646\" ext-link-type=\"uri\">arXiv:1805.05646<\/jats:ext-link>] to these theories, we show how the computation of their zeta function can be shortened considerably. We find that the results previously obtained for the massless theories (<jats:italic>\u2113<\/jats:italic>= 1) generalize to their partially-massless counterparts (arbitrary<jats:italic>\u2113<\/jats:italic>) in arbitrary dimensions.<\/jats:p>","DOI":"10.1007\/jhep07(2018)132","type":"journal-article","created":{"date-parts":[[2018,7,20]],"date-time":"2018-07-20T05:34:29Z","timestamp":1532064869000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":8,"title":["Character integral representation of zeta function in AdSd+1. Part II. 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