I. Introduction
Following the successful implementation of Programmable Josephson Voltage Standards at 10 V [1], [2], it is foreseeable that systems based on stable quantum voltage steps will in the future progressively replace the conventional Josephson voltage standard (CJVS) systems based on metastable, zero-crossing quantum voltage steps. PJVS systems have the potential to bring to the field of voltage metrology accuracy equivalent to CJVS, improved ease of use, and new measurement capabilities that exploit the intrinsic stability and programmability of their voltages. However, a number of precautions need to be followed in order to limit the magnitude of errors at the output of the probe [3].