2025A&A...693A.104B


Query : 2025A&A...693A.104B

2025A&A...693A.104B - Astronomy and Astrophysics, volume 693A104 (2025/1-1)

New constraints on the central mass contents of Omega Centauri from combined stellar kinematics and pulsar timing.

BANARES-HERNANDEZ A., CALORE F., MARTIN CAMALICH J. and READ J.I.

Abstract (from CDS):

Aims. We performed a combined analysis of stellar kinematics with line-of-sight accelerations of millisecond pulsars (MSPs) to probe the mass content of Omega Centauri (ω Cen). Our mass model includes the stellar mass distribution, a more concentrated mass component linked to the observed MSP population, a generic cluster of stellar remnants (assumed to be more concentrated than the stars and MSPs), and an intermediate-mass black hole (IMBH), allowing us to determine which of these is statistically preferred to account for these observations.
Methods. We mass-modeled ω Cen using the package GravSphere to solve the Jeans equations, including constraints in the form of proper motions, line-of-sight velocities, the surface density profile of the stars, the spatial distribution of MSPs, and the recently measured line-of-sight accelerations of a subset of these MSPs, self-consistently modeling their intrinsic spin-down. We explore the impact of different assumed centers of ω Cen on our results and we infer the posterior distributions of the model parameters from the combined likelihood using the nested sampling package dynesty.
Results. Our analysis favors an extended central mass of ∼2-3 × 105 M⊙ over an IMBH, setting a 3σ upper limit on the IMBH mass of 6 × 103 M⊙. We find that pulsar timing observations are an important additional constraint, favoring a central mass distribution that is ∼20% more massive and extended than implied by models that are constrained by the stellar kinematics alone. Finally, we find a 3σ confidence level (CL) upper bound of 6 × 104 M⊙ on the total mass traced by the MSPs, with the density profile following ρp(r) ∝ ρ⋆(r)^γ^/σ(r), with γ = 1.9 ± 0.3, where ρ⋆(r) is the stellar mass density and σ(r) is the stellar velocity dispersion profile. This favors models in which MSPs form via stellar encounters, as in the leading paradigm whereby MSPs are the progeny of low-mass X-ray binaries.
Conclusions. Our analysis demonstrates how combining stellar kinematics with MSP accelerations produces new constraints on mass models, shedding light on the presence or absence of IMBHs at the centers of globular clusters. Further, we provide the first validation of its kind where MSP positions are linked to their place of formation in globular clusters, which is in excellent agreement with the expectations of stellar encounter models of MSP formation. This sets a promising precedent amid the rapid growth in the number of observations and discoveries currently taking place in this field.

Abstract Copyright: © The Authors 2025

Journal keyword(s): stars: black holes - stars: kinematics and dynamics - pulsars: general - galaxies: kinematics and dynamics - galaxies: star clusters: general - globular clusters: individual: ω Centauri

Simbad objects: 9

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Number of rows : 9
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NGC 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 4158 0
2 PSR J1326-4728D Psr 13 26 32.7130 -47 28 40.053           ~ 5 0
3 PSR J1326-4728A Psr 13 26 39.670 -47 30 11.64           ~ 7 0
4 PSR J1326-4728E Psr 13 26 42.67844 -47 27 23.9990           ~ 5 0
5 NGC 5139 GlC 13 26 47.28 -47 28 46.1           ~ 3677 0
6 PSR J1326-4728B Psr 13 26 49.563 -47 29 24.62           ~ 10 0
7 PSR J1326-4728C Psr 13 26 55.2219 -47 30 11.753           ~ 5 0
8 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
9 Cl Terzan 5 Cl* 17 48 05.00 -24 46 48.0           ~ 948 1

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