Elizalde, E. (Emili), 1950-Romeo, A.2010-05-062010-05-0619890556-2821https://hdl.handle.net/2445/12532The proof of $\ensuremath{\zeta}$-function regularization of high-temperature expansions, a technique which provides correct results for many field-theoretical quantities of interest, is known to fail, however, in the case of "Epstein-type" expressions such as $\ensuremath{\Sigma}{{n}_{1},\dots{},{n}_{N}=1}^{\ensuremath{\infty}}{(\ensuremath{\Sigma}{j=1}^{N}{a}_{j}{n}_{j}^{\ensuremath{\alpha}})}^{\ensuremath{-}s}$, $\ensuremath{\alpha}=2, 4, \dots{}$. After showing where precisely the existing demonstration breaks down, we provide a new proof of this regularization valid for a wider range of the parameter $\ensuremath{\alpha}$. The extra terms are calculated explicitly for any value of $\ensuremath{\alpha}\ensuremath{\le}2$. As an application, we provide the finite results corresponding to the $\ensuremath{\zeta}$-function regularization of expressions associated with field theories evaluated in partially compactified, toroidal spacetimes of the form ${\mathrm{T}}^{p}\ifmmode\times\else\texttimes\fi{}{\mathrm{R}}^{q+1}$.8 p.application/pdfeng(c) The American Physical Society, 1989Teoria de camps (FĂsica)Funcions zetaField theory (Physics)Zeta functionsRigorous extension of the proof of zeta-function regularizationinfo:eu-repo/semantics/article73462info:eu-repo/semantics/openAccess