Jorge L. Cervantes-Cota
Interactive Intelligence
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Jorge L. Cervantes-Cota.
Astronomy and Astrophysics | 2006
Ruslan Gabbasov; Mario A. Rodríguez-Meza; Jaime Klapp; Jorge L. Cervantes-Cota
The joint influence of numerical parameters such as the number of particlesxa0 N , the gravitational softening lengthxa0 e and the time-step
Classical and Quantum Gravity | 1999
Jorge L. Cervantes-Cota
Delta t
General Relativity and Gravitation | 2001
Jorge L. Cervantes-Cota; Marcos Nahmad
is investigated in the context of galaxy simulations. For isolated galaxy models we have performed a convergence study and estimated the numerical parameters ranges for which the relaxed models do not deviate significantly from its initial configuration. By fixingxa0 N , we calculate the range of the mean interparticle separationxa0
Archive | 2002
Mario A. Rodríguez-Meza; Jaime Klapp; Jorge L. Cervantes-Cota; Heinz Dehnen
lambda(r)
arXiv: General Physics | 2015
Alejandro Aviles; Jorge L. Cervantes-Cota; Jaime Klapp; Orlando Luongo; Hernando Quevedo
along the disc radius. Uniformly spaced values ofxa0 λ are used asxa0 e in numerical tests of disc heating. We have found that in the simulations with
arXiv: Cosmology and Nongalactic Astrophysics | 2014
Jorge L. Cervantes-Cota; Jaime Klapp
N=1,310,720
Archive | 2002
Jorge L. Cervantes-Cota; Mario A. Rodríguez-Meza; Marcos Nahmad
particlesxa0 λ varies by a factor ofxa06, and the corresponding final Toomres parameters Q change by only aboutxa05xa0perxa0cent. By decreasingxa0 N , the λ and Q ranges broaden. Largexa0 e and smallxa0 N cause an earlier bar formation. In addition, the numerical experiments indicate, that for a given set of parameters the disc heating is smaller with the Plummer softening than with the spline softening. For galaxy collision models we have studied the influence of the selected numerical parameters on the formation of tidally triggered bars in galactic discs and their properties, such as their dimensions, shape, amplitude and rotational velocity. Numerical simulations indicate that the properties of the formed bars strongly depend upon the selection ofxa0 N andxa0 e . Large values of the gravitational softening parameter and a small number of particles result in the rapid formation of a well defined, slowly rotating bar. On the other hand, small values ofxa0 e produce a small, rapidly rotating disc with tightly wound spiral arms, and subsequently a weak bar emerges. We have found that by increasingxa0 N , the bar properties converge and the effect of the softening parameter diminishes. Finally, in some cases short spiral arms are observed at the ends of the bar that change periodically from trailing to leading and vice-versa – the wiggle.
Revista Mexicana De Fisica | 2007
Jorge L. Cervantes-Cota; M. A. Rodríguez-Meza; R.F. Gabbasov; J. Klapp
It is shown some exact solutions in the Brans-Dicke (BD) theory for a Bianchi V metric having the property of inflationary expansion, graceful exit, and asymptotic evolution to a Friedmann-Robertson-Walker (FRW) open model. It is remarkable that an inflationary behaviour can occur, even without a cosmological potential or constant. However, the horizon and flatness problems cannot be solve within the standard BD theory because the inflationary period is severely restricted by the value of the BD parameter
Revista Mexicana De Fisica | 2007
R.F. Gabbasov; M.A. Rodrı́guez-Meza; Jorge L. Cervantes-Cota; J. Klapp
omega
Revista Mexicana De Fisica | 2003
Marcos Nahmad; Jorge L. Cervantes-Cota; M. A. Rodríguez-Meza
.Some exact solutions in the Brans-Dicke (BD) theory are shown for a Bianchi V metric having the properties of inflationary expansion, graceful exit and asymptotic evolution to a Friedmann-Robertson-Walker open model. It is remarkable that inflationary behaviour can occur, even without a cosmological potential or constant. However, the horizon and flatness problems cannot be solved within the standard BD theory because the inflationary period is severely restricted by the value of the BD parameter .