I. Introduction
The cryogenic current comparator (CCC) bridge is widely used in high-accuracy metrology. It is the chosen system for many national metrology institutes (NMIs) to calibrate standard resistors against the quantum Hall resistance. In this system, a superconducting quantum interference device (SQUID) sensor is used to fix the current ratio. A SQUID can detect extremely small changes of magnetic field, and it is a nonlinear device. This combination of characteristics can produce rectification, flux jumps, or saturation of the SQUID controller. These undesired effects can increase the standard deviation, produce systematic errors [1], or even impede the measurement. Since its origin, the SQUID stabilization and a low null error were obtained using an analog integral controller. Recently, more complex control strategies have been applied. For example, some NMIs have included digital filters in the current sources [2] or have used feedforward techniques [3] to decrease the effect of the time constants difference between the arms of a four-terminal CCC. In addition, an NMI has presented a dynamic model of the CCC and a control strategy [4]. In a more recent publication, a high-frequency control loop has been applied to decrease the effect of noise in the SQUID [5]. Aside from these works, little has been published on the dynamic model of the CCC and its control.