“…In this work, we investigate systematically the possible hadron-quark deconfinement phase transition in dense stellar matter and its influence on compact star structures. For the hadronic phase, we adopt in total ten different EOSs, i.e., eight nuclear EOSs (TM1e [66], TM1 [64], PKDD [74], TW99 [43], DDME2 [75], DD2 [76], VM [49], APR [48]) and two hyperonic EOSs (TM1Λ [70] and VMΛ [83]), which are predicted by relativistic-mean-field model [47] and variational method with realistic baryon interactions [48,49]. For the quark phase, we adopt 46 EOSs predicted by equivparticle model [50][51][52], perturbation model [44,53,54], and NJL model with vector interactions [55,56].…”