Searcharxiv⌕ Search

arXiv subjects

G. I. Nápoles-Cañedo

Publications and source records attributed to G. I. Nápoles-Cañedo.

3 recordsLinked to original sources

Diphoton Higgs signal strength in universal extra dimensions

The signal strength of the $gg \to H \to γγ$ reaction in $pp$ collisions at the LHC is studied within the context of the SM with UED. The impact of an arbitrary number $n$ of UED on both the $gg\to H$ and $H\to γγ$ subprocesses is studied. The 1-loop contributions of Kaluza-Klein excitations to these subprocesses are proportional to discrete and continuous sums, which can diverge. By implementing dimensional regularization, it is shown that discrete regularized sums can naturally be expressed as multidimensional Epstein functions, and that divergences, if exist, emerge through the poles of these functions. It is found that continuous sums converge, but the discrete ones diverge, with the exception of the $n=1$ case, in which the 1-dimensional Epstein function converges. It is argued that divergences that arise from discrete sums for $n\geq 2$ are genuine UV divergences, since they correspond to short-distance effects in the compact manifold. Then, the amplitudes are renormalized in a modern sense by incorporating interactions of canonical dimension higher than four that allow us to generate the required counterterms, which are determined using a $\overline{\rm MS}$-like renormalization scheme. We find that the $gg\to H$ subprocess is quite sensitive to both the size and the dimension of the compact manifold, but the SM prediction for $H\to γγ$ subprocess is practically unchanged. In the $n=1$ case, it is found that the experimental constraint on the compactification scale $R^{-1}\geq 1.5$ TeV allow us to reproduce the experimental limit on the signal strength $1.01\leq μ^{(1)}_{γγ}\leq 1.2$. In the $n\geq 2$ cases, it is found that the experimental limit on $μ^{(n)}_{γγ}$ leads to stronger lower bounds for the compactification scale given by $R^{-1}\geq 1.55, 2.45, 3.57, 5.10, 7.25$ TeVs for $n=2, 4, 6, 8, 10$, respectively.

hep-ph↗

One-loop order effects from one universal extra dimension on $λϕ^{4}$ theory

The self-interacting $λϕ^{4}$ scalar field theory is a warhorse in quantum field theory. Here we explore the one-loop order impact from one universal extra dimension, $S^{1}/\mathbb{Z}_{2}$, to the self-energy and four point vertex functions associated to this theory. Such effects come as an infinite number of UV divergences corresponding to an infinite superposition of excited KK particles around the loop. We show that dimensional regularisation is adequate enough to control them in terms of the product of the one dimensional inhomogenous Epstein zeta function times the gamma function. From the analytical properties of these functions, the UV divergences are extracted and the counterterms defined; the latter turn out to be of canonical dimension four at the Lagrangian level. We use both, the MS-scheme and a mass-dependent subtraction scheme to remove divergences. Only the latter manifestly satisfy the decoupling theorem.

hep-th↗

The Standard Model in extra dimensions and its Kaluza-Klein effective Lagrangian

We construct an effective theory for the SM with extra dimensions. We start from a theory governed by the extra-dimensional groups ISO$(1,3+n)$ and $G_{\rm SM}({\cal M}^{4+n})=SU_C(3,{\cal M}^{4+n})\times SU_L(2,{\cal M}^{4+n})\times U_Y(1,{\cal M}^{4+n})$, characterized by an unknown energy scale $Λ$ and valid at energies far below this scale. Assuming that the extra dimensions are much larger than the distance scale of this theory, we construct an effective theory with symmetry groups ISO(1,3), $G_{\rm SM}({\cal M}^{4})$. The theories are connected by a canonical transformation that hides ISO$(1,3+n)$, $G_{\rm SM}({\cal M}^{4+n})$ into ISO(1,3), $G_{\rm SM}({\cal M}^{4})$; KK fields receive mass. Using a set of orthogonal functions $\{f^{(\underline{0})},f^{(\underline{m})}\}$, generated by the Casimir invariant $\bar{P}^2$ associated with the translations subgroup $T(n)\subset$ISO$(n)$, we expand the degrees of freedom of ISO$(1,3+n)$, $G_{\rm SM}({\cal M}^{4+n})$ in general Fourier series, whose coefficients are the degrees of freedom of ISO(1,3), $G({\cal M}^{4})$. These functions, which correspond to the projection on $\{|\bar{x}\big>\}$ of the discrete basis $\{|0\big>,|p^{(\underline{m})}\big>\}$ of $\bar{P}^2$, are central to define the effective theory. Components along the ground state $f^{(\underline{0})}=\big <\bar x|0\big>$ do not receive mass at the compactification scale, so they are the SM fields; components along excited states $f^{(\underline{m})}=\big<\bar x|p^{(\underline{m})}\big>$ get mass at this scale, so they are KK excitations. For any direction $|p^{(\underline{m})}\neq0\big>$ there are a massive gauge field and a pseudo-Goldstone boson. We stress resemblances of this mass-generating mechanism with the Englert-Higgs mechanism and discuss physical implications. We include a full catalog of Lagrangian terms that can be used to calculate Feynman rules.

hep-ph↗