Voltage biasing of a single superconducting weak link results in coherent electromagnetic oscillation at the frequency ν=VΦ₀; simultaneous voltage biasing of two weak links in a superconducting ring produces two strongly coupled oscillators at the same frequency. The electromagnetic phase difference is the difference in the gauge-invariant quantum phases across the two contacts. Because of the quantization of the superconducting ring, this phase difference is 2π〈Φ〉Φ₀, where 〈Φ〉 is the time-averaged magnetic flux in the superconducting circuit and Φ₀ is the flux quantum. We can characterize the coupled system in terms of normal modes, and we have experimentally observed these modes of oscillation at 30 MHz. This provides a means of understanding the earlier observations of quantum interference in the resistive state.
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Silver et al. (1967) studied this question.
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