The dc-Josephson effect with more than four superconducting leads
R. Mélin · arXiv (Cornell University) · 2021
By definition, the $p$-terminal dc-Josephson current is sensitive to the superconducting phase variables of $p$ terminals. In the paper, we establish protocol for direct detection of the $p$-terminal dc-Josephson effect with $p\ge 3$ in a device containing $N$ superconducting leads $S_1,\,S_2,\,...,\,S_N$ having the phase variables $φ_1,\,φ_2,\,...,\,φ_N$. The calculated signal $χ^{(N)}$ can be probed in microwave experiments, and it corresponds to the higher-order nonlocal inverse inductance obtained from differentiating the current $I_1$ through $S_1$ with respect to the remaining $N-2$ independent phase differences $φ_2-φ_N,\,φ_3-φ_N,\, ...,φ_{N-1}-φ_N$. We find that the values $p\le N-2$ do not contribute to $χ^{(N)}$, and that $χ^{(N)} e 0$ implies evidence for the $p=N-1$ or the $p=N$-terminal dc-Josephson currents. For $N=4$ superconducting leads, we demonstrate that $χ^{(4)} e 0$ implies evidence for the $p=3$ or $p=4$ dc-Josephson effect, irrespective of the $p=2$-terminal dc-Josephson current. Thus, we provide a way to demonstrate the dc-Josephson effect with more than three terminals (i.e. with $p\ge 3$) in a device containing more than four superconducting leads (i.e. with $N\ge 4$). The predicted $χ^{(4)}$ is "yes or no" answer to the $p\ge 3$ dc-Josephson effect, i.e. for $N=4$, nonvanishingly small $χ^{(4)} e 0$ implies the $p=3$ or $p=4$-terminal dc-Josephson effect and vanishingly small $χ^{(4)}=0$ implies absence of the $p=3$ and $p=4$-terminal dc-Josephson effect. The paper can be viewed as generalizing the recently considered $φ$-junctions in Andreev molecules to arbitrary number $N$ of the superconducting leads, and it relies on basic properties of the dc-Josephson effect that are not directly related to nontrivial topology and Weyl point singularities.