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Table A.1.

Summary of the new direct N-body evolutionary models of star clusters and their GR-merger yields in this work.

No. Mcl/Msamp rh/pc W0 Z fbin Tevol/Myr remnant model SN kick BH spin Nmrg, in Nmrg, out
1 17.5 × 104 2.0 7.0 0.0002 0.052 300.0 rapid+B16 mom. cons.3 FM194 0 3
2 0 1
3 0 1
4 2 2

5 7.5 × 104 2.0 7.0 0.001 0.05 300.0 rapid+B16 mom. cons. FM19 1 3
6 2 1
7 0 1
8 1 0

9 7.5 × 104 2.0 7.0 0.005 0.05 300.0 rapid+B16 mom. cons. FM19 0 1
10 0 0
11 0 1
12 0 0

13 7.5 × 104 2.0 7.0 0.01 0.05 300.0 rapid+B16 mom. cons. FM19 0 0
14 1 0
15 0 0
16 0 0

17 7.5 × 104 2.0 7.0 0.02 0.05 300.0 rapid+B16 mom. cons. FM19 0 1
18 0 0
19 1 0
20 0 0

21 7.5 × 104 2.0 9.0 0.0002 0.05 300.0 rapid+B16 mom. cons. FM19 1 2
22 2 3
23 0 0
24 0 1

25 7.5 × 104 2.0 9.0 0.001 0.05 300.0 rapid+B16 mom. cons. FM19 1 0
26 1 1
27 0 1
28 0 1

29 7.5 × 104 2.0 9.0 0.005 0.05 300.0 rapid+B16 mom. cons. FM19 2 1
30 1 1
31 0 0
32 1 1

Notes.

1

Initial number of stars N ≈ 1.28 × 105.

2

The binary fraction is defined as fbin = 2Nbin/N, with Nbin being the total number of binaries and N being the total number of members. Notably, the initial binary fraction among the O stars, considered separately, is fObin = 1.0 as opposed to the smaller overall binary fraction, fbin.

3

Momentum conserving natal kick as in Ba20.

4

Vanishing BH natal spins (Fuller & Ma 2019).

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