Precise, subnanosecond, and high-voltage switching enabled by gallium nitride electronics integrated into complex loads

Abstract

In this work, we report the use of commercial gallium nitride (GaN) power electronics to precisely switch complex distributed loads, such as electron lenses and deflectors. This was accomplished by taking advantage of the small form-factor, low-power dissipation, and high temperature compatibility of GaN field effect transistors (GaNFETs) to integrate pulsers directly into the loads to be switched, even under vacuum. This integration reduces parasitics to allow for faster switching and removes the requirement to impedance match the load to a transmission line by allowing for a lumped element approximation of the load even with subnanosecond switching. Depending on the chosen GaNFET and driver, these GaN pulsers are capable of generating pulses ranging from 100 to 650 V and 5 to 60 A in 0.25–8 ns using simple designs with easy control, few-nanosecond propagation delays, and MHz repetition rates. We experimentally demonstrate a simple 250 ps, 100 V pulser measured by using a directly coupled 2 GHz oscilloscope. By introducing resistive dampening, we can eliminate ringing to allow for precise 100 V transitions that complete a −10 to −90 V transition in 1.5 ns, limited primarily by the inductance of the oscilloscope measurement path. The performance of the pulser attached to various load structures is simulated, demonstrating the possibility of even faster switching of internal fields in these loads. We test these circuits under vacuum and up to 120 °C to demonstrate their flexibility. We expect these GaN pulsers to have broad application in fields such as optics, nuclear sciences, charged particle optics, and atomic physics that require nanosecond, high-voltage transitions.

Heat management technology for solid‐state high voltage and high repetitive pulse generators: Towards better effects and reliability

“…High accuracy and stability of pulse form (including rising time, pulse duration, and time base jitter) are required in applications, such as ultrawide band (UWB) radar, mass separation, pulse combination in electromagnetic pulse (EMP) system, irreversible electroporation therapy [30, 31]. Taking the widely used avalanche transistor‐based Marx generator for example, according to Liang et al., the time base jitter σ B is dependent on the trigger transition bias voltage V B and voltage V n , as shown in Equation () [32].…”