Magnetic fields created in the noncentral heavy-ion collision are studied within a microscopic transport model, namely the Ultrarelativistic Quantum Molecular Dynamics model (UrQMD). Simulations were carried out for different impact parameters within the SPS energy range ($E_{lab} = 10 - 158 A$ GeV) and for highest energies accessible for RHIC. We show that the magnetic field emerging in heavy-ion collisions has the magnitude of the order of $eB_y \sim 10^{-1} m_\pi^2$ for the SPS energy range and $eB_y \sim m_\pi^2$ for the RHIC energies. The estimated value of the magnetic field strength for the LHC energy amounts to $eB_y \sim 15 m_\pi^2$
In off-central heavy-ion collisions, quark-gluon plasma (QGP) is exposed to the strongest magnetic f...
Heavy ion collisions at the LHC facility generate a Quark-Gluon Plasma (QGP) which, for central coll...
When the quark-gluon plasma emerges in the wake of a heavy-ion collision, a magnetic field created b...
The features of magnetic field in relativistic heavy-ion collisions are systematically studied by us...
The electromagnetic fields during relativistic heavy ion collisions are calculated using a simple mo...
At the earliest times after a heavy-ion collision, the magnetic field created by the spectator nucle...
At the earliest times after a heavy-ion collision, the magnetic field created by the spectator nucle...
It is important to understand the strong external magnetic field generated at the very beginning of ...
AbstractIt is important to understand the strong external magnetic field generated at the very begin...
We investigate the effect of large magnetic fields on the (2 + 1)-dimensional reduced-magnetohydrody...
I review the origin and properties of electromagnetic fields produced in heavy-ion collisions. The f...
The energy dependence of the local and violation in Au+Au and Cu+Cu collisions in a large energy ran...
It is expected that the magnetic fields in heavy ion collisions are very high. In this work, we inve...
An extraordinary strong magnetic field, eB0≈1018 Gauss, is expected to be generated in non-central u...
The energy dependence of the local $mathcal{P}$ and $mathcal{CP}$ violation in Au+Au and Cu+Cu colli...
In off-central heavy-ion collisions, quark-gluon plasma (QGP) is exposed to the strongest magnetic f...
Heavy ion collisions at the LHC facility generate a Quark-Gluon Plasma (QGP) which, for central coll...
When the quark-gluon plasma emerges in the wake of a heavy-ion collision, a magnetic field created b...
The features of magnetic field in relativistic heavy-ion collisions are systematically studied by us...
The electromagnetic fields during relativistic heavy ion collisions are calculated using a simple mo...
At the earliest times after a heavy-ion collision, the magnetic field created by the spectator nucle...
At the earliest times after a heavy-ion collision, the magnetic field created by the spectator nucle...
It is important to understand the strong external magnetic field generated at the very beginning of ...
AbstractIt is important to understand the strong external magnetic field generated at the very begin...
We investigate the effect of large magnetic fields on the (2 + 1)-dimensional reduced-magnetohydrody...
I review the origin and properties of electromagnetic fields produced in heavy-ion collisions. The f...
The energy dependence of the local and violation in Au+Au and Cu+Cu collisions in a large energy ran...
It is expected that the magnetic fields in heavy ion collisions are very high. In this work, we inve...
An extraordinary strong magnetic field, eB0≈1018 Gauss, is expected to be generated in non-central u...
The energy dependence of the local $mathcal{P}$ and $mathcal{CP}$ violation in Au+Au and Cu+Cu colli...
In off-central heavy-ion collisions, quark-gluon plasma (QGP) is exposed to the strongest magnetic f...
Heavy ion collisions at the LHC facility generate a Quark-Gluon Plasma (QGP) which, for central coll...
When the quark-gluon plasma emerges in the wake of a heavy-ion collision, a magnetic field created b...