Table 2.
Predicted outcome of the second-born (2nd) CO for the known HM(XR)Bs with BHs.
Source | ![]() |
![]() |
2nd born CO | OUTCOME |
|
---|---|---|---|---|---|
β = 1 | υ = 0.75 | ||||
HD 96670 | 5.23 | 20 | NS | GW merger | unstable MT |
25 | BH | GW merger | unstable MT | ||
M33 X-7 | 3.4522 | 63 | BH | unstable MT | unstable MT |
LMC X-1 | 3.9075 | 32 | BH | GW merger | unstable MT |
Cyg X-1 | 5.5985 | 40 | BH | wide binary | unstable MT |
VFTS 243 | 10.401 | 25 | BH | wide binary | unstable MT |
HD 130298 | 12.407 | 25 | BH | GW merger | unstable MT |
32 | BH | GW merger | unstable MT | ||
HD 215227 | 59.97 | 10 | NS | wide binary | GW merger |
16 | NS | wide binary | GW merger |
Notes. The mass of the systems is assumed to be , where
represents the initial donor’s mass closest to the actual mstar in Ge et al. (2020) tables. Comparison to our results is made using the circularised orbital period
as in Eq. (31), for eccentric systems with e > 0. The estimate of
is reported with the same significant digits as the eccentricities in Table 1. The hypothesized channels of purely isotropic re-emission, β = 1, and mass outflow from L2 with efficiency υ = 0.75 are both considered. The outcomes are also labeled to argue whether the systems have a set of initial properties
that can lead to the evolution into merging double COs via stable MT (GW merger), or are expected to evolve into a wide binary (wide binary) or undergo unstable MT (unstable MT).
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