We propose an all-optical, single-laser-pulse scheme for generating a dense relativistic strongly magnetized electron–positron pair plasma. The scheme involves the interaction of an extremely intense (I ≳ 1024 W/cm2) circularly polarized laser pulse with a solid-density target containing a conical cavity. Through full-scale three-dimensional particle-in-cell simulations that account for quantum electrodynamic effects, it is shown that this interaction results in two significant outcomes: first, the generation of quasi-static magnetic fields reaching tens of gigagauss, and, second, the production of large quantities of electron–positron pairs (up to 1013) via the Breit–Wheeler process. The e−e+ plasma becomes trapped in the magnetic field and remains confined in a small volume for hundreds of femtoseconds, far exceeding the laser timescale. The dependence of pair plasma parameters, as well as the efficiency of plasma production and confinement, is discussed in relation to the properties of the laser pulse and the target. Realizing this scheme experimentally would enable the investigation of physical processes relevant to extreme astrophysical environments.
Samsonov et al. (2025) studied this question.