2020
DOI: 10.1103/physrevc.101.025807
|View full text |Cite
|
Sign up to set email alerts
|

First-order phase transition from hypernuclear matter to deconfined quark matter obeying new constraints from compact star observations

Abstract: We reconsider the problem of the hyperon puzzle and its suggested solution by quark deconfinement within the two-phase approach to hybrid compact stars with recently obtained hadronic and quark matter equations of state. For the hadronic phase we employ the hypernuclear equation of state from the lowest order constrained variational method and the quark matter phase is described by a sufficiently stiff equation of state based on a color superconducting nonlocal Nambu-Jona-Lasinio model with constant (model A) … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
42
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
7
1

Relationship

1
7

Authors

Journals

citations
Cited by 50 publications
(44 citation statements)
references
References 78 publications
0
42
0
Order By: Relevance
“…Systems with isospin and chiral imbalance are completely different systems and it is remarkable that some phenomena in these systems are entirely equivalent. Additionally, one can notice that the dualities D M and D ∆ are themselves dual to each other with respect to the D duality (10). So one can conclude that there exists only one independent additional duality and one can get the other duality by making use of the main duality (10).…”
Section: Other Dualitiesmentioning
confidence: 94%
See 2 more Smart Citations
“…Systems with isospin and chiral imbalance are completely different systems and it is remarkable that some phenomena in these systems are entirely equivalent. Additionally, one can notice that the dualities D M and D ∆ are themselves dual to each other with respect to the D duality (10). So one can conclude that there exists only one independent additional duality and one can get the other duality by making use of the main duality (10).…”
Section: Other Dualitiesmentioning
confidence: 94%
“…However, one can show dynamically (at least in the framework of NJL model) that pions do not condense in the system with just chiral or chiral isospin imbalance and the condition of zero pion condensate holds in this case. So we can use the dualities (18), (10) and argue that (µ 5 , T) and (µ I /2, T) phase diagrams are dual to each other if one performs the transformation PC ↔ CSB. Thus one can use the duality to get the critical temperature of chiral symmetry breaking phase as a function of chiral chemical potential T c (µ 5 ) from the phase structure at µ I .…”
Section: Predicting the Catalysis Of Chiral Symmetry Breakingmentioning
confidence: 99%
See 1 more Smart Citation
“…David has been successfully using quark models all over his career, including applications to dense matter where the otherwise usually confined quarks may be de-confined and give rise to stars with a quark core [1,2]. In this talk we focus on other aspects of chiral quark models, such as the Nambu-Jona-Lasinio (NJL) model, applied to the domain where they were originally designed for, namely the soft limit in the vacuum.…”
Section: Introductionmentioning
confidence: 99%
“…This provokes a larger jump in n s from the previous transition, and moves it towards lower chemical potentials. In summary, decreasing the vector interaction causes the transition to superconducting matter to occur at lower chemical potentials, but at the cost of deconfining more s quarks.The fact that the color superconducting phase occurs before or after the decoupling of the s quark from its chiral condensate is currently a matter of debate[101], and as we have just seen it strongly depends on the model parameters used. Furthermore, changing the diquarks coupling ζ D = G D G S also competes by moving the phase transition to higher (or lower) chemical potentials.…”
mentioning
confidence: 96%