Maikel Yusat Ballester

Prof. Maikel Yusat Ballester

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Research Focus & Metrics

Academic Career Length

22Years (2005-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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19 April 2019 in Astronomy & Astrophysics
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Journal Article
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AFA. Fuente
A. Fuente
DND. G. Navarro
D. G. Navarro
PCP. Caselli
P. Caselli
MGM. Gerin
M. Gerin
CKC. Kramer
C. Kramer
MBMaikel Yusat Ballester
Maikel Yusat Ballester
GEMS is an IRAM 30 m Large Program whose aim is determining the elemental depletions and the ionization fraction in a set of prototypical star-forming regions. This paper presents the first results from the prototypical dark cloud Taurus molecular cloud (TMC) 1. Extensive millimeter observations have been carried out with the IRAM 30 m telescope (3 and 2 mm) and the 40 m Yebes telescope (1.3 cm and 7 mm) to determine the fractional abundances of CO, HCO+, HCN, CS, SO, HCS+, and N2H+ in three cuts which intersect the dense filament at the well-known positions TMC 1-CP, TMC 1-NH3, and TMC 1-C, covering a visual extinction range from AV ~ 3 to ~20 mag. Two phases with differentiated chemistry can be distinguished: (i) the translucent envelope with molecular hydrogen densities of 1−5 × 103 cm−3; and (ii) the dense phase, located at AV > 10 mag, with molecular hydrogen densities >104 cm−3. Observations and modeling show that the gas phase abundances of C and O progressively decrease along the C+/C/CO transition zone (AV ~ 3 mag) where C/H ~ 8 × 10−5 and C/O ~ 0.8−1, until the beginning of the dense phase at AV ~ 10 mag. This is consistent with the grain temperatures being below the CO evaporation temperature in this region. In the case of sulfur, a strong depletion should occur before the translucent phase where we estimate an S∕H ~ (0.4−2.2) × 10−6, an abundance ~7–40 times lower than the solar value. A second strong depletion must be present during the formation of the thick icy mantles to achieve the values of S/H measured in the dense cold cores (S∕H ~ 8 × 10−8). Based on our chemical modeling, we constrain the value of ζH2 to ~(0.5–1.8) × 10−16 s−1 in the translucent cloud.

27 August 2021 in International Journal of Quantum Chemistry
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JAJudith P. Araújo
Judith P. Araújo
MBMaikel Yusat Ballester
Maikel Yusat Ballester
Interatomic potentials laid at the heart of molecular physics. They are a bridge between the spectroscopic and structural properties of molecular systems. In this paper, a century‐old review from 1920 to 2020, of functional forms used to analytically represent potential energy as a function of interatomic distance for diatomic systems is presented. With such a purpose 50 functions were selected. For all of them, motivation and the main mathematical features are discussed. Our goal is to provide a chronological pathway to the reader, even with little knowledge on the subject, to understand how to calculate each parameter that composes the interatomic potentials, as well as obtain spectroscopic constants from them. Comparative evaluation for the N2, CO, and HeH+ systems in their ground electronic states are also presented.

4 May 2005 in Physical Chemistry Chemical Physics
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MBMaikel Yusat Ballester
Maikel Yusat Ballester
AVAntónio J. C. Varandas
António J. C. Varandas
A global potential energy surface is reported for the ground electronic state of HSO2 by using the double many-body expansion (DMBE) method. It employs realistic DMBE functions previously reported from accurate ab initio calculations (in some cases, fine tuned to spectroscopic data) for the triatomic fragments, and four-body energy terms that were modelled by fitting novel ab initio FVCAS/AVTZ calculations for the tetratomic system. In some cases, FVCAS/AVDZ energies have been employed after being scaled to FVCAS/AVTZ ones. To assess the role of the dynamical correlation, exploratory single-point Rayleigh–Schrödinger perturbation calculations have also been conducted at one stationary point. All reported calculations are compared with previous ab initio results for the title system. The potential energy surface predicts HOSO to be the most stable configuration, in good agreement with other theoretical data available in the literature. In turn, the HSO2 isomer with H bonded to S is described as a local minimum, which is stable with respect to the H + SO2 dissociation asymptote.

12 January 2007 in Chemical Physics Letters
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MBMaikel Yusat Ballester
Maikel Yusat Ballester
AVAntónio J. C. Varandas
António J. C. Varandas

16 February 2011 in The Journal of Physical Chemistry A
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Journal Article
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JGJuan D. Garrido
Juan D. Garrido
MBMaikel Yusat Ballester
Maikel Yusat Ballester
YOYoelvis Orozco-González
Yoelvis Orozco-González
SCSylvio Canuto
Sylvio Canuto

1 January 2019 in Proceedings of the Combustion Institute
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Journal Article
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JCJ.M. Colom-Díaz
J.M. Colom-Díaz
MAM. Abián
M. Abián
MBMaikel Yusat Ballester
Maikel Yusat Ballester
ÁMÁ. Millera
Á. Millera
RBR. Bilbao
R. Bilbao
MAM.U. Alzueta
M.U. Alzueta