In laser-produced high-energy-density plasmas, large-scale strong magnetic fields are spontaneously generated by the Biermann battery effects when temperature and density gradients are misaligned. Saturation of the magnetic field takes place when convection and dissipation balance field generation. While theoretical and numerical modeling provide useful insight into the saturation mechanisms, experimental demonstration remains elusive. In this letter, we report an experiment on the saturation dynamics and scaling of Biermann battery magnetic field in the regime where plasma convection dominates. With time-gated charged-particle radiography and time-resolved Thomson scattering, the field structure and evolution as well as corresponding plasma conditions are measured. In these conditions, the spatially resolved magnetic fields are reconstructed, leading to a picture of field saturation with a scaling of $B\sim 1/L_{\mathrm{T}}$ for a convectively dominated plasma, a regime where the temperature gradient scale ($L_{\mathrm{T}}$) exceeds the ion skin depth.

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• High-energy-density plasmas
• Laboratory studies of space & astrophysical plasmas
• Laser-induced magnetic fields in plasmas