I. Introduction
High stability flat-top pulsed magnetic field (FTPMF) is one of the essential experiment conditions in modern scientific research [1]. Flat-top stability is a key metric for FTPMF [2], [3], [4]. Due to supply voltage fluctuations and magnetic coil temperature increases [5], [6], FTPMFs produced by open-loop discharges from capacitors or batteries require closed-loop controlled active compensation networks for enhanced stability. However, these networks, with their significant power consumption or limited capacitor storage [7], [8], [9], are not only voluminous but also constrain the range of magnetic field adjustments.