To increase the integration scale of superconductor electronics, we are developing a new node, titled SFQ7ee, of the fabrication process at MIT Lincoln Laboratory. In comparison to the existing SFQ5ee node, we increased the number of fully planarized superconducting layers to ten and utilized NbN and NbN/Nb kinetic inductors to increase the possible inductor number density above a hundred million inductors per cm 2 . Increasing the Josephson junction number density to the same level requires implementing self-shunted high- J c Josephson junctions. We investigated the properties of Nb/NbNx/Nb trilayer junctions as a potential replacement of high- J c Nb/Al-AlO x /Nb junctions, where NbN x is a disordered, overstoichiometric, nonsuperconducting nitride deposited by reactive sputtering. Dependences of the IcRn product and Josephson critical current density, Jc on the NbNx barrier thickness and temperature were studied in the thickness range from 5 nm to 20 nm. The fabricated junctions can be well described by the microscopic theory of SNS junctions, assuming no suppression of the energy gap in Nb electrodes near the NbN x interfaces and a Cooper pair decay length in the NbNx barrier, ξ n T c of about 2.3 nm. Current-voltage characteristics of the junctions are well described by the resistively and capacitively shunted junction (RCSJ) model without excess current. In the studied range J c < 10 mA/μm 2 , the Nb/NbN x /Nb junctions have lower values of the specific resistance RnA , lower IcRn products, and a stronger dependence of the IcRn on temperature than the self-shunted or critically damped externally shunted Nb/Al-AlO x /Nb junctions with the same critical current density; A is the junction area, I c the junction critical current, and R n the effective shunting resistance.
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Tolpygo et al. (2024) studied this question.
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