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Momentum Dependent Potentials from a Parity Doubling Chiral Mean Field Model in UrQMD: Impact on Flow and Particle Production


المفاهيم الأساسية
The implementation of momentum dependent potentials from a parity doubling chiral mean field (CMF) model in the UrQMD transport simulation significantly improves the description of particle production, especially for hyperons and pions, without significantly affecting the description of flow observables.
الملخص

The authors extend the quantum molecular dynamics (QMD) part of the UrQMD model to allow the implementation of momentum dependent potentials from a parity doubling chiral mean field (CMF) model. This new implementation reproduces qualitatively and quantitatively available data over a wide range of beam energies and improves the description of observables without exception.

The key highlights are:

  1. The CMF model provides a consistent description of the density and momentum dependence of nucleon interactions, as well as baryon-specific potentials and effects of chiral symmetry restoration.

  2. Implementing the momentum dependent potentials from CMF in UrQMD leads to a moderate effect on directed and elliptic flow observables, but a significant impact on hadron multiplicities.

  3. The description of hyperon and pion production at SIS18 energies is improved by the momentum dependent potentials. Compared to HADES data, the present parametrization of the CMF model may lead to a slightly too weak momentum dependence.

  4. The work serves as an important step towards future studies where the properties of dense QCD matter, through parameters of the CMF model, can be constrained using a comparison of the UrQMD model with high precision heavy ion data, allowing direct comparisons with neutron star and neutron star merger observables.

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الإحصائيات
The authors report the following key figures: The relative difference in the available energy between simulations with and without momentum dependent potentials is less than 2.4% for all beam energies considered. The slope of the directed flow v1 of protons at mid-rapidity shows a small effect of the momentum dependence, with the largest impact at the lowest beam energies. The elliptic flow v2 of protons at mid-rapidity also shows a moderate effect of the momentum dependence, with a slightly larger impact in more peripheral collisions. The transverse momentum spectra of pions and hyperons are significantly affected by the inclusion of momentum dependent potentials, with a reduction in the yields.
اقتباسات
"The effect of the momentum dependence is very small for the integrated directed flow and the difference between the two methods is even smaller." "The largest effect can be observed at the lowest beam energies." "The biggest effect of the momentum dependence seems to be therefore an overall reduction of the mid-rapidity yield of the different particles, where those particle closer, or even below their elementary threshold energy are reduced more strongly."

استفسارات أعمق

How can the momentum dependence of the CMF model be further tuned to better match the experimental data on flow and particle production?

To enhance the momentum dependence of the Chiral Mean Field (CMF) model for improved alignment with experimental data on flow and particle production, several strategies can be employed. First, a systematic variation of the scalar coupling parameters within the CMF model could be conducted. By adjusting these parameters, one can increase the strength of the momentum dependence, which may lead to a more pronounced effect on the effective mass of baryons, particularly the nucleons and hyperons. This adjustment could help in capturing the observed discrepancies in particle production rates, especially for hyperons and pions, as indicated by the HADES data. Second, a detailed comparison of the model predictions with a broader range of experimental observables, including flow coefficients and particle multiplicities across different beam energies and collision systems, would provide critical feedback for tuning. This could involve utilizing Bayesian inference techniques to statistically optimize the model parameters based on the fit to experimental data. Lastly, incorporating additional physical effects, such as the influence of resonance production and decay processes, could refine the momentum dependence. By including these dynamics, the model may better account for the complex interactions occurring in heavy-ion collisions, leading to a more accurate description of the flow and particle production phenomena.

What are the implications of the momentum dependent potentials on the equation of state of dense QCD matter and its connection to neutron star properties?

The introduction of momentum dependent potentials in the CMF model has significant implications for the equation of state (EoS) of dense Quantum Chromodynamics (QCD) matter. These potentials allow for a more nuanced description of baryon interactions, which is crucial for understanding the behavior of matter under extreme conditions, such as those found in neutron stars. The momentum dependence reflects the physical reality that baryon interactions are not solely determined by density but also by the momentum of the particles involved. This leads to a more accurate representation of the EoS, particularly in the high-density regime where chiral symmetry restoration occurs. In the context of neutron stars, a well-defined EoS is essential for predicting their mass-radius relationship and understanding phenomena such as gravitational wave emissions from neutron star mergers. The momentum dependent EoS can provide insights into the stability of neutron stars and the conditions under which phase transitions may occur, such as the transition from hadronic to quark matter. This is particularly relevant for understanding the maximum mass of neutron stars and the potential existence of hybrid stars, which contain both hadronic and quark matter. Furthermore, the ability to connect the EoS derived from heavy-ion collision experiments with astrophysical observations enhances our understanding of the fundamental properties of dense QCD matter, bridging the gap between experimental nuclear physics and astrophysical phenomena.

Can the implementation of the fully relativistic equations of motion in the UrQMD model lead to additional insights compared to the current non-relativistic approach?

Implementing fully relativistic equations of motion in the UrQMD model could yield substantial insights compared to the current non-relativistic framework. A relativistic treatment inherently accounts for the effects of Lorentz contraction and time dilation, which become increasingly significant at high energies typical of heavy-ion collisions. This would allow for a more accurate description of the dynamics of the system, particularly during the initial non-equilibrium phase of the collision, where relativistic effects are pronounced. Moreover, a fully relativistic approach would enable the model to incorporate the complete set of momentum-dependent potentials derived from the CMF model more naturally. This could lead to improved conservation of energy and momentum during particle interactions, addressing some of the limitations observed in the non-relativistic implementation, where energy conservation violations were noted. Additionally, the relativistic framework would facilitate a better understanding of the transition between hadronic and quark degrees of freedom, as it would allow for a more seamless integration of the EoS across different density regimes. This is crucial for exploring the properties of dense QCD matter and its implications for neutron star physics. In summary, transitioning to a fully relativistic formulation in the UrQMD model could enhance the accuracy of simulations, provide deeper insights into the dynamics of heavy-ion collisions, and improve the connection between experimental results and theoretical predictions regarding the behavior of dense matter.
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