Wireless josephson bifurcation amplifier
US-2018198427-A1 · Jul 12, 2018 · US
US11737376B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11737376-B2 |
| Application number | US-201816770942-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 11, 2018 |
| Priority date | Dec 11, 2017 |
| Publication date | Aug 22, 2023 |
| Grant date | Aug 22, 2023 |
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A superconducting device includes two nodes and a Josephson junction coupled between the two nodes, wherein the Josephson junction is characterized by a superconducting phase difference, φ, wherein the superconducting device has a potential that varies as a function of the superconducting phase difference, φ, and has a single potential well. The potential has a non-zero cubic term and quartic term is zero. The Josephson junction may be a single small Josephson junction. The superconducting device may include a superconducting ring connected between the two nodes. The superconducting ring may include a first ring portion with a plurality of large Josephson junctions connected in series. The superconducting ring may also include a second ring portion that includes the single small Josephson junction in parallel with the plurality of large Josephson junctions between the two nodes.
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What is claimed is: 1. A superconducting device comprising: two nodes; and a Josephson junction coupled between the two nodes, wherein the Josephson junction is characterized by a superconducting phase difference, φ wherein the superconducting device has a potential that varies as a function of the superconducting phase difference, φ and has a single potential well, wherein the potential has a non-zero φ 3 term and a φ 4 term that is equal to zero. 2. The superconducting device of claim 1 , wherein the Josephson junction is a first Josephson junction and the superconducting device further comprises: a superconducting ring connected between the two nodes, the superconducting ring comprising: a first ring portion comprising a plurality of second Josephson junctions connected in series, wherein each second Josephson junction of the plurality of second Josephson junctions has the same tunneling energy; and a second ring portion comprising the first Josephson junction in parallel with the plurality of second Josephson junctions between the two nodes. 3. The superconducting device of claim 2 , further comprising a magnetic flux generation device positioned in proximity to the superconducting ring and configured to generate an external DC magnetic flux through the superconducting ring. 4. The superconducting device of claim 3 , wherein the plurality of second Josephson junctions consists of three second Josephson junctions. 5. The superconducting device of claim 4 , wherein the three second Josephson junctions are formed from two Dolan bridges. 6. The superconducting device of claim 4 , wherein a tunneling energy of the first Josephson junction is less than a tunneling energy of each of the second Josephson junctions. 7. The superconducting device of claim 6 , wherein the tunneling energy of each second Josephson junction is E J , and the tunneling energy of the first Josephson junction is αE J , where α is less than 0.50 and greater than 0.20. 8. The superconducting device of claim 7 , wherein α is approximately equal to 0.29 and the external DC magnetic flux is 0.41Φ 0 , where (Φ 0 is the magnetic flux quantum.
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