scholarly journals Dimension dependence of numerical simulations on gravitational waves from protoneutron stars

2020 ◽  
Vol 102 (2) ◽  
Author(s):  
Hajime Sotani ◽  
Tomoya Takiwaki
2020 ◽  
Vol 102 (8) ◽  
Author(s):  
Alberto Roper Pol ◽  
Sayan Mandal ◽  
Axel Brandenburg ◽  
Tina Kahniashvili ◽  
Arthur Kosowsky

2021 ◽  
Vol 103 (4) ◽  
Author(s):  
Sunil Choudhary ◽  
Nicolas Sanchis-Gual ◽  
Anshu Gupta ◽  
Juan Carlos Degollado ◽  
Sukanta Bose ◽  
...  

Galaxies ◽  
2018 ◽  
Vol 6 (4) ◽  
pp. 119 ◽  
Author(s):  
Antonios Nathanail

In the dawn of the multi-messenger era of gravitational wave astronomy, which was marked by the first ever coincident detection of gravitational waves and electromagnetic radiation, it is important to take a step back and consider our current established knowledge. Numerical simulations of binary neutron star mergers and simulations of short GRB jets must combine efforts to understand such complicated and phenomenologically rich explosions. We review the status of numerical relativity simulations with respect to any jet or magnetized outflow produced after merger. We compare what is known from such simulations with what is used and obtained from short GRB jet simulations propagating through the BNS ejecta. We then review the established facts on this topic, as well as discuss things that need to be revised and further clarified.


2020 ◽  
Vol 498 (3) ◽  
pp. 3503-3512
Author(s):  
Hajime Sotani ◽  
Tomoya Takiwaki

ABSTRACT The ramp up signals of gravitational waves appearing in the numerical simulations could be important signals to estimate parameters of the protoneutron star (PNS) at supernova explosions. To identify the signals with PNS oscillations, we make a linear perturbation analysis and compare the resultant eigenfrequencies with the ramp up signals obtained via the 2D numerical simulations. Then, we find that the ramp up signals correspond well to the g1-mode in the early phase and to the f-mode, to which the g1-mode is exchanged via the avoided crossing. We also confirm that the f- and g1-modes are almost independent of the selection of the PNS surface density in the later phase after core bounce. In addition, we successfully find that the fitting formula of g1- and f-modes, which correspond to the ramp up signals in the numerical simulation, as a function of the PNS average density. That is, via the direct observation of the gravitational waves after supernova explosion, one could extract the time evolution of the PNS average density using our fitting formula.


2014 ◽  
Vol 2014 ◽  
pp. 1-11 ◽  
Author(s):  
David Garrison

Numerical simulations are becoming a more effective tool for conducting detailed investigations into the evolution of our universe. In this paper, we show how the framework of numerical relativity can be used for studying cosmological models. The author is working to develop a large-scale simulation of the dynamical processes in the early universe. These take into account interactions of dark matter, scalar perturbations, gravitational waves, magnetic fields, and turbulent plasma. The code described in this report is a GRMHD code based on the Cactus framework and is structured to utilize one of several different differencing methods chosen at run-time. It is being developed and tested on the University of Houston’s Maxwell cluster.


Author(s):  
H. Rodrigues ◽  
J. A. Rosero-Gil ◽  
A. M. Endler ◽  
S. B. Duarte ◽  
M. Chiapparini

We describe the dynamical behavior of newborn neutron stars modelled as homogeneous rotating spheroids. The dynamical evolution is triggered by the escape of trapped neutrinos, providing the initial equilibrium configuration. It is shown that for a given set of values of the initial angular momentum, a shape transition to a triaxial ellipsoid configuration occurs. Gravitational waves are then generated by the breaking of the axial symmetry, and some aspects of their observation are discussed. We found a narrow window for both, the initial values of the angular frequency and the eccentricity, able to enable a dynamical shape transition, with their upper bound determined by the Kepler frequency. The energy and angular momentum carried away by the gravitational wave are treated consistently with the solution of the equations of motion of the system.


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