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Hybrid Star Properties with NJL and MFTQCD Model: A Bayesian Approach

Milena Albino, Tuhin Malik, Márcio Ferreira, Constança Providência

TL;DR

This work investigates whether neutron stars can harbor deconfined quark matter by constructing hybrid equations of state (EOS) that couple a hadronic phase described by Relativistic Mean Field theory with two quark-phase models, the Nambu–Jona-Lasinio (NJL) model and Mean Field Theory of QCD (MFTQCD), via a Maxwell construction. A Bayesian framework samples EOS parameters to satisfy NICER X-ray mass–radius constraints and a target phase-transition density around $\rho_{\text{trans}} \approx 0.15$–$0.40\,\mathrm{fm}^{-3}$, with an optional high-density pQCD constraint. The study finds hybrid stars compatible with current observations, but pQCD restrictions lower the maximum mass to about $M_{\max} \sim 2.1$–$2.3\,M_\odot$, with NJL more sensitive to these constraints in the stiff hadronic scenario; MFTQCD can yield smaller radii for moderate-mass stars. Vector interactions are crucial for achieving $M_{\max}>2\,M_\odot$, while multiquark terms can modify indicators of deconfinement, such as the trace anomaly $\Delta$ and conformality-related measures $d_c$; some EOSs even allow a persistently positive renormalized trace anomaly inside the star. Overall, the results support the viability of quark cores under current data and emphasize the role of model details and pQCD guidance in shaping NS properties.

Abstract

The composition of the core of neutron stars (NS) is still under debate. One possibility is that because of the high densities reached in their cores, matter could be deconfined into quark matter. We investigate the existence of hybrid stars, using microscopic models to describe different phases of matter. Within the adopted microscopic models we calculate properties of NS and properties of matter. We want to probe the pQCD calculations influence and analyze properties that identify a transition to deconfined matter. Bayesian approach is applied to generate 8 sets of equations of state (EOS). A Maxwell construction is adopted to describe the deconfinement transition. For the hadron phase, we consider a stiff and a soft EOS obtained from the Relativistic Mean Field model with nonlinear meson terms. For the quark phase, we use 2 different models: the Nambu-Jona-Lasinio model with multiquark interactions and the Mean Field Theory of QCD, a model similar to the vector MIT bag model. Bayesian inference was applied to determine the model parameters that satisfy the X-ray observations from NICER and have phase transition at densities between 0.15 - 0.40 fm$^{-3}$. We also applied restrictions from the pQCD calculations to half of the sets. Hybrid stars are compatible with current observational data. The pQCD restrictions reduce the value of the $M_{max}$. However, even applying this restriction, the models were able to reach values of $2.1 - 2.3 M_\odot$. The conformal limit was still not attained at the center of the most massive stars. The vector interactions are essential to describe hybrid stars with a mass above $2 M_\odot$. The multiquark interactions introduced may affect the limits of some quantities considered as indicators of the presence of a deconfined phase. It is possible to find a set of EOS, that predict that inside NS the renormalized matter trace anomaly is always positive.

Hybrid Star Properties with NJL and MFTQCD Model: A Bayesian Approach

TL;DR

This work investigates whether neutron stars can harbor deconfined quark matter by constructing hybrid equations of state (EOS) that couple a hadronic phase described by Relativistic Mean Field theory with two quark-phase models, the Nambu–Jona-Lasinio (NJL) model and Mean Field Theory of QCD (MFTQCD), via a Maxwell construction. A Bayesian framework samples EOS parameters to satisfy NICER X-ray mass–radius constraints and a target phase-transition density around , with an optional high-density pQCD constraint. The study finds hybrid stars compatible with current observations, but pQCD restrictions lower the maximum mass to about , with NJL more sensitive to these constraints in the stiff hadronic scenario; MFTQCD can yield smaller radii for moderate-mass stars. Vector interactions are crucial for achieving , while multiquark terms can modify indicators of deconfinement, such as the trace anomaly and conformality-related measures ; some EOSs even allow a persistently positive renormalized trace anomaly inside the star. Overall, the results support the viability of quark cores under current data and emphasize the role of model details and pQCD guidance in shaping NS properties.

Abstract

The composition of the core of neutron stars (NS) is still under debate. One possibility is that because of the high densities reached in their cores, matter could be deconfined into quark matter. We investigate the existence of hybrid stars, using microscopic models to describe different phases of matter. Within the adopted microscopic models we calculate properties of NS and properties of matter. We want to probe the pQCD calculations influence and analyze properties that identify a transition to deconfined matter. Bayesian approach is applied to generate 8 sets of equations of state (EOS). A Maxwell construction is adopted to describe the deconfinement transition. For the hadron phase, we consider a stiff and a soft EOS obtained from the Relativistic Mean Field model with nonlinear meson terms. For the quark phase, we use 2 different models: the Nambu-Jona-Lasinio model with multiquark interactions and the Mean Field Theory of QCD, a model similar to the vector MIT bag model. Bayesian inference was applied to determine the model parameters that satisfy the X-ray observations from NICER and have phase transition at densities between 0.15 - 0.40 fm. We also applied restrictions from the pQCD calculations to half of the sets. Hybrid stars are compatible with current observational data. The pQCD restrictions reduce the value of the . However, even applying this restriction, the models were able to reach values of . The conformal limit was still not attained at the center of the most massive stars. The vector interactions are essential to describe hybrid stars with a mass above . The multiquark interactions introduced may affect the limits of some quantities considered as indicators of the presence of a deconfined phase. It is possible to find a set of EOS, that predict that inside NS the renormalized matter trace anomaly is always positive.
Paper Structure (10 sections, 15 equations, 12 figures, 5 tables)

This paper contains 10 sections, 15 equations, 12 figures, 5 tables.

Figures (12)

  • Figure 1: Pressure versus energy density for the soft EOS (left panel) and stiff EOS (right panel). Gray plots show the results from Annala:2019puf.
  • Figure 2: Mass-radius diagram of the 90% of CL stiff sets: MFTQCD (left) and NJL (right). Solid bands represent sets were obtained applying the pQCD constraint. Observational data is show as: PSR J0030+0451 (cyan and purple) Riley:2019ydaMiller:2019cac, PSR J0740+6620 (yellow) Riley:2021pdlMiller:2021qha, HESS J1731-347 (magenta) hess, and GW170817 (light and dark gray) LIGOScientific:2018cki.
  • Figure 3: Corner plots of $\xi_{\omega\omega}$, the maximum mass ($M_\text{max}$) and the speed of sound at $M_\text{max}$ ($c^2_\text{s,max}$) for the NJL stiff sets. Set with (without) pQCD constraint is shown in blue (black).
  • Figure 4: Comparison between models with pQCD constraint. It is shown, from the left to the right: the speed of sound as a function of the baryon density, the mass-radius diagram and the mass by the tidal deformability. The middle panel with the mass-radius curves also includes observational data as specified in Fig. \ref{['fig:graph_TOV']}.
  • Figure 5: 90% CL of the $u,\, d,\,$ and $s$-quark fraction, for MFTQCD (top) and NJL (bottom) and soft (right) and stiff EOS (right). The bands at the low density limit define the region where the deconfinement occurs for the different set EOS, and result from the jump from zero to a finite value of the order of 1/3 for $u$-quarks and $\lesssim2/3$ for the $d$-quark.
  • ...and 7 more figures