Searcharxiv⌕ Search

arXiv subjects

Pedro González

Publications and source records attributed to Pedro González.

5 recordsLinked to original sources

The ${^{3}\!}P_{0}$ model reloaded

We revisit the phenomenological ${^{3}\!}P_{0}$ model for the decay of quarkonium $\left( Q\bar{Q}\right) $ into two open flavor mesons ($\bar{\mathfrak{M}}\mathfrak{M}% $). We take the heavy-quark limit and derive a transition rate between $Q\bar{Q}$ and $\bar{\mathfrak{M}}\mathfrak{M}$ to be compared with the one calculated in studies of string breaking using lattice QCD. This comparison allows to fit the creation amplitude of a light quark-antiquark pair in the ${^{3}\!}P_{0}$ model to the string-breaking transition rate in QCD.

hep-ph↗

Strong decays of the lowest bottomonium hybrid within an extended Born-Oppenheimer framework

We analyze the decays of the theoretically predicted lowest bottomonium hybrid $H(1P)$ to open bottom two-meson states. We do it by embedding a quark pair creation model into the Born-Oppenheimer framework which allows for a unified, QCD-motivated description of bottomonium hybrids as well as bottomonium. A new $^{1}\!P_{1}$ decay model for $H(1P)$ comes out. The same analysis applied to bottomonium leads naturally to the well-known $^{3}\!P_{0}$ decay model. We show that $H(1P)$ and the theoretically predicted bottomonium state $Υ(5S)$, whose calculated masses are close to each other, have very different widths for such decays. A comparison with data from $Υ(10860)$, an experimental resonance whose mass is similar to that of $Υ(5S)$ and $H(1P)$, is carried out. Neither a $Υ(5S)$ nor a $H(1P)$ assignment can explain the measured decay widths. However, a $Υ(5S)$-$H(1P)$ mixing may give account of them supporting previous analyses of dipion decays of $Υ(10860)$ and suggesting a possible experimental evidence of $H(1P)$.

hep-ph↗

A Population-based Hybrid Approach to Hyperparameter Optimization for Neural Networks

In recent years, large amounts of data have been generated, and computer power has kept growing. This scenario has led to a resurgence in the interest in artificial neural networks. One of the main challenges in training effective neural network models is finding the right combination of hyperparameters to be used. Indeed, the choice of an adequate approach to search the hyperparameter space directly influences the accuracy of the resulting neural network model. Common approaches for hyperparameter optimization are Grid Search, Random Search, and Bayesian Optimization. There are also population-based methods such as CMA-ES. In this paper, we present HBRKGA, a new population-based approach for hyperparameter optimization. HBRKGA is a hybrid approach that combines the Biased Random Key Genetic Algorithm with a Random Walk technique to search the hyperparameter space efficiently. Several computational experiments on eight different datasets were performed to assess the effectiveness of the proposed approach. Results showed that HBRKGA could find hyperparameter configurations that outperformed (in terms of predictive quality) the baseline methods in six out of eight datasets while showing a reasonable execution time.

cs.LG↗

Quark model description of $ψ(4260)$

From lattice indications we follow a Born-Oppenheimer approximation to build a quark-antiquark static potential for $J^{PC}=1^{--}$ charmonium states below their first S- wave meson-meson threshold. We show that a good description of the mass and decay properties of the experimentally well established $ψ(4260)$ resonance is feasible.

hep-ph↗

A plausible explanation of $Υ(10860)$

We show that a good description of the $Υ(10860)$ properties, in particular the mass, the $e^+ e^-$ leptonic widths and the $π^{+}π^{-}Υ(ns)$$\ (n=1,2,3)$ production rates, can be obtained under the assumption that $Υ(10860)$ is a mixing of the conventional $Υ(5s)$ quark model state with the lowest $P-$ wave hybrid state.

hep-ph↗