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Mixing-angle sensitivity of inclusive ΞbcΞ_{bc} and ΩbcΩ_{bc} lifetimes

Published 1 Sep 2026 in hep-ph and hep-ex | (2609.00660v1)

Abstract: We study the inclusive lifetimes of Ξ<em>bc<sup>+Ξ<em>{bc}<sup>{+}, Ξ</em>bc<sup>0Ξ</em>{bc}<sup>{0}, and Ω<em>bc<sup>0Ω<em>{bc}<sup>{0}, with emphasis on the mixing between the spin-zero and spin-one bcbc-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>-23.0<sup>\circ for Ξ</em>bcΞ</em>{bc} and 23.5<sup>-23.5<sup>\circ for Ω<em>bcΩ<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\left(τ</em>{Ξ<em>{bc}<sup>{+}},τ</sup></em>{Ξ<em>{bc}<sup>{0}},τ</sup></em>{Ω<em>{bc}<sup>{0}}\right)=\left(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}\right)\,\mathrm{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>+0.0660.042)ps\left(τ<em>{Ξ</em>{bc}<sup>{+}},τ<em>{Ξ</em>{bc}<sup>{0}},τ<em>{Ω</em>{bc}<sup>{0}}\right)=\left(0.367<sup>{+0.076}<em>{-0.070},0.100<sup>{+0.032}</sup></em>{-0.014},0.229<sup>{+0.066}_{-0.042}\right)\,\mathrm{ps} in the NRQM. Relative to the unmixed spin-one reference points, the Ξ<em>bc<sup>0Ξ<em>{bc}<sup>{0} and Ω</em>bc<sup>0Ω</em>{bc}<sup>{0} lifetimes decrease by approximately 17%17\%-19%19\%. Neither the minimum nor the maximum of the central lifetime curves occurs at a pure Sbc=0S_{bc}=0 or Sbc=1S_{bc}=1 configuration; the extrema instead lie at mixed angles with φB27<sup>\left|φ_{\mathcal{B}}\right|\simeq27<sup>\circ-63<sup>63<sup>\circ. The two pure-spin limits alone are therefore insufficient to characterize the full mixing-angle dependence.

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