A Josephson junction can make a collective quantum phase behave as a measurable dynamical coordinate. In current-biased Josephson phase dynamics, the Gauge-invariant Josephson phase moves in a tilted Josephson washboard potential; the junction's capacitance supplies its effective inertia. A trapped phase gives zero mean electric potential difference, while sustained phase advance produces a nonzero mean electric potential difference. Quantized phase levels in a Josephson junction and quantum escape of a current-biased Josephson junction test quantum mechanics for this collective coordinate.
Begin with a stipulated parallel electrical circuit: an ideal sinusoidal Josephson junction, capacitance , and effective electrical resistance . The Kirchhoff node law and Josephson effect give
Here is the constant bias electric current, is a deliberately applied microwave electric current, and represents unwanted fluctuating electric current. Multiplication by puts the undriven equation into the mechanical form
The effective inertia is a coefficient for a dimensionless quantum phase, not a literal material mass moving through the insulating layer. The capacitor's energy, , provides a direct check of that identification. The effective includes loading by the external electrical circuit; a constant parallel is an approximation over the relevant frequency range.
The useful design freedom is that changes the confinement while changes its inertia. The same manufactured device can therefore connect a classical oscillation, discrete energy levels, and escape to an electrical readout. The Martinis-Devoret-Clarke circuit experiments separate these questions experimentally. John Clarke, Michel H. Devoret and John M. Martinis shared the 2025 Nobel Prize in Physics for circuit experiments establishing macroscopic quantum tunnelling and discrete energy levels.[ref]
John M. Martinis Created 2026-10-18 Updated 2026-11-05
John M. Martinis coauthored a 1985 observation of quantized energy levels in a current-biased Josephson junction. The relevant coordinate was the phase difference across an electrical circuit element, rather than the position of one isolated particle. The measured levels agreed with a quantum mechanics calculation using junction parameters measured in the classical regime. This showed that a fabricated superconducting circuit could possess a discrete excitation spectrum suitable for controlled quantum experiments.[ref]
Figure 1.
Portrait of John M. Martinis
. David Orban, Flickr photograph, 13 February 2007; existing Commons crop. Creative Commons Attribution 2.0 Generic., via Wikimedia Commons. Source.