John Clarke (physicist) Created 2026-10-24 Updated 2026-11-05
John Clarke coauthored experiments testing quantum mechanics through a macroscopic superconducting electrical circuit. In 1985, a current-biased Josephson junction exhibited quantized levels of its phase difference, with positions predicted from independently measured classical circuit parameters. The experiment connected precision electrical measurement with the discrete spectrum of a collective circuit coordinate.[ref]
A physicist researching superconducting quantum interference devices and quantum-limited measurements.[ref]
John Clarke | Physics by University of California, Berkeley, Department of Physics. Research Interests: superconducting quantum-interference devices and quantum-limited measurements
Portrait of John Clarke (physicist)
. UC Berkeley. CC BY 4.0, via Wikimedia Commons. Source. 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]
A physicist researching superconducting devices and quantum computers based on Josephson junctions.[ref]
John Martinis by University of California, Santa Barbara. Distinguished Professor; research paragraph on superconducting devices and Josephson-junction quantum bits
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. Martinis-Devoret-Clarke circuit experiments 2026-10-18
The 1985 spectroscopy experiment used niobium-based tunnel Josephson junctions on silicon, thermally anchored with final bias low-pass filters to a dilution refrigerator. Calibrated germanium and cobalt thermometers measured temperature. A filtered coaxial cable injected microwaves; repeated switches to nonzero electric potential difference measured escape with irradiation on and off. Bias scans at fixed microwave frequency resolved separate enhancements matching calculated unequal energy level spacings. Raising temperature merged the structure toward classical response. Junction parameters were calibrated in the classical regime; reducing the superconducting critical current with a magnetic field checked thermal readout. Parameter uncertainties limited absolute resonance positions.[ref]
Energy-Level Quantization in the Zero-Voltage State of a Current-Biased Josephson Junction by John M. Martinis and others. Original paper, pp.1543–1545, apparatus and Figs.2–4; p.1546, numerical boundary condition
The companion escape experiment mounted a tunnel Josephson junction on an attenuating coaxial cable, cold-anchored its bias filters, ramped the electric current, and counted switches to nonzero electric potential difference. Rapid current shutoff limited heating. Classical escape and microwave resonance calibrated the superconducting critical current, capacitance and environmental loading. Low-temperature escape agreed with the quantum prediction using these calibrated parameters. A magnetic field reduced the superconducting critical current to keep the same apparatus thermally activated at lower temperature, testing excess noise. Frequency-dependent loading contributed uncertainty; the predicted damping correction was smaller than combined errors, so the experiment did not resolve that correction.[ref]
Measurements of Macroscopic Quantum Tunneling out of the Zero-Voltage State of a Current-Biased Josephson Junction by Michel H. Devoret and others. Original paper, pp.1909–1910, calibration, Fig.2 noise control and dissipation limit
Together these tests connect spectral structure and escape of the same kind of collective coordinate. They do not constitute a demonstration of coherent gate operations on a qubit, or prove that every macroscopic coordinate retains quantum behavior under arbitrary environmental coupling. The attraction is more concrete: a fabricated electrical circuit admits both an independently measurable classical model and quantitative quantum tests of its phase dynamics.
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