Abstract: We study the inclusive lifetimes of Ξ<em>bc<sup>+, Ξ</em>bc<sup>0, and Ω<em>bc<sup>0, with emphasis on the mixing between the spin-zero and spin-one bc-diquark configurations. The relevant hadronic matrix elements are evaluated in both the homogeneous bag model (HBM) and the nonrelativistic quark model (NRQM). At the benchmark mixing angles of −23.0<sup>∘ for Ξ</em>bc and −23.5<sup>∘ for Ω<em>bc, the corresponding lifetime triplets are (τ</em>Ξ<em>bc<sup>+,τ</sup></em>Ξ<em>bc<sup>0,τ</sup></em>Ω<em>bc<sup>0)=(0.421<sup>+0.093</sup></sup></em>−0.093,0.075<sup>+0.035<em>−0.010,0.223<sup>+0.074</sup></em>−0.043)ps in the HBM and (τ<em>Ξ</em>bc<sup>+,τ<em>Ξ</em>bc<sup>0,τ<em>Ω</em>bc<sup>0)=(0.367<sup>+0.076<em>−0.070,0.100<sup>+0.032</sup></em>−0.014,0.229<sup>+0.066−0.042)ps in the NRQM. Relative to the unmixed spin-one reference points, the Ξ<em>bc<sup>0 and Ω</em>bc<sup>0 lifetimes decrease by approximately 17%-19%. Neither the minimum nor the maximum of the central lifetime curves occurs at a pure Sbc=0 or Sbc=1 configuration; the extrema instead lie at mixed angles with ∣φB∣≃27<sup>∘-63<sup>∘. The two pure-spin limits alone are therefore insufficient to characterize the full mixing-angle dependence.