A collection of movies visualizing different collision systems and features of the transport approach. ParaView state files are downloadable for some movies to easily recreate them. Please be aware of the ParaView version with which they were created. For a tutorial on how to produce such animations or adapt the provided state files see the Movies Tutorial Page.
Collision of two gold nuclei at a kinetic energy of 1.23A GeV.
Collision of two silver nuclei at a kinetic energy of 1.58A GeV.
Collision of two carbon nuclei at a kinetic energy of 2A GeV.
Collision of an argon projectile with a potassium chloride target at a kinetic energy of 1.76A GeV. For comparison with the experiment, the KCl is represented by an argon with a mass number of 37.
Collision of two gold nuclei at a kinetic energy of 1.23A GeV. The impact parameter is 3.14 fm, which is the mean of the 0-10% centrality bin. Each real particle is represented by 20 test particles.
Collision of two gold nuclei at a kinetic energy of 1.23A GeV. The impact parameter is 5.70 fm, which is the mean of the 10-20% centrality bin. Each real particle is represented by 20 test particles.
Collision of two gold nuclei at a kinetic energy of 1.23A GeV. The impact parameter is 7.38 fm, which is the mean of the 20-30% centrality bin. Each real particle is represented by 20 test particles.
Hadron density and Landau velocity of a gold-gold collision at a kinetic energy of 1.23A GeV. Surfaces of constant density are shown and the direction of the landau velocity is indicated by the arrows in the z=0 plane. The arrows are colored according to the magnitude of the landau velocity.
Pressure anisotropy in a collision of two gold nuclei at a kinetic energy of 1.23A GeV. The pressure anisotropy as defined in D. Oliinychenko et al. Phys.Rev. C93 (2016) no.3 is calculated in the z=0 plane from the energy momentum tensor. After some time the pressure anisotropy starts to vanish, which is a condition for thermalization. The white surface indicates the region with sufficient hadron density.
Visualization of the Landau velocity field in a collision of two gold nuclei at a kinetic energy of 1.23A GeV. The source of each line is the position of a testparticle in the calculation. The lines follow the velocity field until they reach a region with low density. Note that the lines are not the actual trajectories of the particles but reflect the collective velocity.
Hadron density in a collision of two gold nuclei at a kinetic energy of 1.23A GeV with an impact paramter of 3.14 fm.
Infinite matter calculation in a box with periodic boundary conditions.
Sphere calculation. Particles are initialised in a sphere without boundary conditions so that the sphere will expand.
Head on Ar+KCl collision at a kinetic energy of 1.76A GeV. The particle mass is represented by both the coloring and radii of the spheres. In the background plays a catchy and relaxing elevator type of music.
Head on collision of two carbon nuclei at a kinetic energy of 2.0A GeV. The particle mass is represented by both the coloring and radii of the spheres. In the background plays a dramatic tune underlying the journey of a lonesome nucleon.
Collision of two gold nuclei at a kinetic energy of 1.23A GeV. The particle mass is represented by both the coloring and the radii of the spheres. In the background plays a shredded guitar, use headphones.
Collision of two silver nuclei. Before the collision, the camera rotates around the nuclei to give a better picture of the initial state. The spectators are highlighted in red while for the other particles the number of binary interactions is encoded in the color.
Collision of two silver nuclei. Before the collision, the camera rotates around the nuclei to give a better picture of the initial state. The spectators are highlighted in red while for the other particles the number of binary interactions is encoded in the color. [Extended version with explanations]
Collision of two gold nuclei at top RHIC energy (center of mass energy of 200 GeV). The particles are colored according to their species.
Collision of two gold nuclei at a kinetic energy of 1.23A GeV.
Collision of two silver nuclei at a kinetic energy of 1.58A GeV.
Collision of two carbon nuclei at a kinetic energy of 2A GeV.
Collision of an argon projectile with a potassium chloride target at a kinetic energy of 1.76A GeV. For comparison with the experiment, the KCl is represented by an argon with a mass number of 37.
Nucleons and energy density of a gold nucleus with potentials and Fermi motion at rest.
Gold nucleus with potentials and Fermi motion at rest.
Comparison of a nucleus with and without nuclear potentials.
Gold nucleus with fermi motion but without potentials. The nucleons themselves and the density are shown side by side.