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The Role of the Hadron-Quark Phase Transition in Core-Collapse Supernovae

Published 21 Apr 2022 in astro-ph.HE, astro-ph.SR, and nucl-th | (2204.10397v2)

Abstract: The hadron-quark phase transition in quantum chromodyanmics has been suggested as an alternative explosion mechanism for core-collapse supernovae. We study the impact of three different hadron-quark equations of state (EoS) with first-order (DD2F_SF, STOS-B145) and second-order (CMF) phase transitions on supernova dynamics by performing 97 simulations for solar- and zero-metallicity progenitors in the range of 14-100 M<em>⊙14\texttt{-}100\,\text{M}<em>\odot. We find explosions only for two low-compactness models (14M</em>⊙14 \text{M}</em>\odot and 16 M<em>⊙16\,\text{M}<em>\odot) with the DD2F_SF EoS, both with low explosion energies of ∼10<sup>50 erg\mathord{\sim}10<sup>{50}\,\mathrm{erg}. These weak explosions are characterised by a neutrino signal with several mini-bursts in the explosion phase due to complex reverse shock dynamics, in addition to the typical second neutrino burst for phase-transition driven explosions. The nucleosynthesis shows significant overproduction of nuclei such as <sup>90Zr<sup>{90}\mathrm{Zr} for the 14 M</em>⊙14\,\text{M}</em>\odot zero-metallicity model and <sup>94Zr<sup>{94}\mathrm{Zr} for the 16 M<em>⊙16\,\text{M}<em>\odot solar-metallicity model, but the overproduction factors are not large enough to place constraints on the occurrence of such explosions. Several other low-compactness models using the DD2F_SF EoS and two high-compactness models using the STOS EoS end up as failed explosions and emit a second neutrino burst. For the CMF EoS, the phase transition never leads to a second bounce and explosion. For all three EoS, inverted convection occurs deep in the core of the proto-compact star due to anomalous behaviour of thermodynamic derivatives in the mixed phase, which heats the core to entropies up to 4k</em>B/baryon4k</em>\text{B}/\text{baryon} and may have a distinctive gravitational wave signature, also for a second-order phase transition.

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