Abstract:Black hole (BH) binary mergers formed through dynamical interactions in dense star clusters are believed to be one of the main sources of gravitational waves for Advanced LIGO and Virgo. Here we present a fast numerical method for simulating the evolution of star clusters with BHs, including a model for the dynamical formation and merger of BH binaries. Our method is based on Hénon's principle of balanced evolution, according to which the flow of energy within a cluster must be balanced by the energy productio… Show more
“…The evolution of the BHBs in our cluster models is computed using the fast code cBHBd. While the details of this method are described in Antonini and Gieles [34], here we give a brief summary of the model philosophy, including the full set of differential equations that are used to compute the secular evolution of the cluster models and the merging BHBs they produce.…”
Section: Methodsmentioning
confidence: 99%
“…The decrease in GC population mass by evaporation is K ∆ = K/2 = 16.3 +43.5 −8.87 . Using the approximation for the number of mergers in the observable redshift range from [34], N merge ∝ M 1.6 0 r −0.67…”
Section: B Globular Cluster Mass Functionmentioning
confidence: 99%
“…with t sev ≃ 2 Myr. We include here an additional (mass independent) term which was not present in Antonini and Gieles [34], and that accounts for cluster evaporatioṅ…”
Section: A Clusterbhmentioning
confidence: 99%
“…The main reason for this is that standard numerical techniques such as Nbody and Monte Carlo simulations are still too slow to allow a full parameter space exploration. This is why in this study we employ our new population synthesis code clusterBHBdynamics (hereafter cBHBd) [34] to systematically vary assumptions made for the model parameters and over the full range of initial conditions relevant to real GCs. Thus, we examine the effect of these initial assumptions on the number and properties of merging BHBs using a suite of about 20 million cluster models.…”
Section: Introductionmentioning
confidence: 99%
“…In Section II we compute the GC formation rate density as a function of time using constraints from the present-day GCMF. In Section III we describe our population synthesis model and detail the modifications we made to it with respect to the version used in [34]. Section IV describes our main results.…”
“…The evolution of the BHBs in our cluster models is computed using the fast code cBHBd. While the details of this method are described in Antonini and Gieles [34], here we give a brief summary of the model philosophy, including the full set of differential equations that are used to compute the secular evolution of the cluster models and the merging BHBs they produce.…”
Section: Methodsmentioning
confidence: 99%
“…The decrease in GC population mass by evaporation is K ∆ = K/2 = 16.3 +43.5 −8.87 . Using the approximation for the number of mergers in the observable redshift range from [34], N merge ∝ M 1.6 0 r −0.67…”
Section: B Globular Cluster Mass Functionmentioning
confidence: 99%
“…with t sev ≃ 2 Myr. We include here an additional (mass independent) term which was not present in Antonini and Gieles [34], and that accounts for cluster evaporatioṅ…”
Section: A Clusterbhmentioning
confidence: 99%
“…The main reason for this is that standard numerical techniques such as Nbody and Monte Carlo simulations are still too slow to allow a full parameter space exploration. This is why in this study we employ our new population synthesis code clusterBHBdynamics (hereafter cBHBd) [34] to systematically vary assumptions made for the model parameters and over the full range of initial conditions relevant to real GCs. Thus, we examine the effect of these initial assumptions on the number and properties of merging BHBs using a suite of about 20 million cluster models.…”
Section: Introductionmentioning
confidence: 99%
“…In Section II we compute the GC formation rate density as a function of time using constraints from the present-day GCMF. In Section III we describe our population synthesis model and detail the modifications we made to it with respect to the version used in [34]. Section IV describes our main results.…”
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