Probing nuclear structure with mean transverse momentum in relativistic isobar collisions
arXiv:2111.14812 · doi:10.1103/PhysRevC.108.L011902
Abstract
Transverse momentum () generation in relativistic heavy ion collisions is sensitive to the initial geometry and the final-state bulk evolution. We demonstrate with hydrodynamic calculations that the mean ratio () between the highly similar isobar Ru+Ru and Zr+Zr collisions is insensitive to the bulk evolution and remains sensitive to the small difference in the initial nuclear structure (neutron skin and deformation) between the Ru and Zr nuclei.We further find that nuclear deformation can produce an anticorrelation between and eccentricity (or elliptic flow) in central collisions. These findings suggest that the between the isobar systems can be used to measure the neutron skin thickness and deformation parameters, which can in turn constrain the nuclear symmetry energy slope parameter.
6 pages, 5 figures
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- Exploring the Nuclear Shape Phase Transition in Ultra-Relativistic Xe+Xe Collisions at the LHC
- Estimate of Background Baseline and Upper Limit on the Chiral Magnetic Effect in Isobar Collisions at GeV at the Relativistic Heavy-Ion Collider
- Impact of initial fluctuations and nuclear deformations in isobar collisions
- Effect of nuclear structure on particle production in relativistic heavy-ion collisions using the AMPT model
- Determining the neutron skin thickness by relativistic semi-isobaric collisions
- Difference between signal and background of the chiral magnetic effect relative to spectator and participant planes in isobar collisions at GeV
- Observation of long-range collective flow in OO and NeNe collisions and implications for nuclear structure studies
- Exploring nuclear structure with multiparticle azimuthal correlations at the LHC
- Benchmarking nuclear matrix elements of decay with high-energy nuclear collisions
- Exploring Rapidity-Even Dipolar Flow in Isobaric Collisions at RHIC
- Impact of the pre-equilibrium phase for the determination of nuclear geometry in high-energy isobar collisions