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Table 2.

Predicted outcome of the second-born (2nd) CO for the known HM(XR)Bs with BHs.

Source (days) 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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