Wireless Josephson bifurcation amplifier
US-9948254-B2 · Apr 17, 2018 · US
US11277107B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11277107-B2 |
| Application number | US-201916685753-A |
| Country | US |
| Kind code | B2 |
| Filing date | Nov 15, 2019 |
| Priority date | Feb 6, 2015 |
| Publication date | Mar 15, 2022 |
| Grant date | Mar 15, 2022 |
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A traveling wave parametric amplifier involving a series of Josephson junctions is disclosed. Devices and systems incorporating traveling wave parametric amplifiers, and methods of using and fabricating traveling wave parametric amplifiers are also disclosed.
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The invention claimed is: 1. A traveling wave parametric amplifier, comprising: a first port configured to receive a weak signal and a pump signal; a transmission line in communication with the first port and configured to transmit the weak signal and the pump signal, wherein the transmission line comprises a plurality of coupled asymmetric SQUIDS configured to amplify the weak signal to provide an amplified signal; and a second port from which the amplified signal exits. 2. The amplifier of claim 1 , further comprising: a magnetic flux adjuster configured to adjust a magnetic flux, the magnetic flux being produced by an external source, an adjustment of the magnetic flux by the magnetic flux adjuster providing an in situ optimization of a performance of the amplifier. 3. The amplifier of claim 2 , wherein the magnetic flux adjuster includes a mutual coupled inductance DC bias line. 4. The amplifier of claim 2 , wherein the optimization of the performance includes a tuning of a nonlinear inductance to realize phase matching conditions in a degenerate four-wave mixing process. 5. The amplifier of claim 4 , wherein each of the plurality of coupled asymmetric SQUIDS includes at least one of a smaller Josephson energy junction and more than one of a larger Josephson energy junction, wherein the larger Josephson energy junction has a higher critical current than the smaller Josephson junction. 6. The amplifier of claim 5 , wherein an in situ tuning of the nonlinear inductance causes the nonlinear inductance to change sign from negative to positive. 7. The amplifier of claim 5 , wherein adjacent coupled asymmetric SQUIDs of the plurality of coupled asymmetric SQUIDs are coupled through a larger Josephson energy junction of the more than one larger Josephson energy junction. 8. The amplifier of claim 5 , wherein each of the plurality of coupled asymmetric SQUIDs includes one smaller Josephson energy junction and two to three larger Josephson energy junctions. 9. The amplifier of claim 1 , wherein the plurality of coupled asymmetric SQUIDs is configured to allow for a mixing process between the weak signal, generated idler, and the pump signal traveling along the transmission line, the mixing process resulting in a parametric gain of the weak signal. 10. The amplifier of claim 1 , wherein the plurality of coupled asymmetric SQUIDs is configured to amplify the weak signal in a transmission mode. 11. The amplifier of claim 1 , wherein the plurality of coupled asymmetric SQUIDs is configured to amplify the weak signal by providing an exponential gain of the weak signal as a function of a length of the transmission line. 12. A method, comprising: receiving a weak signal and a pump signal at a first port of a traveling wave parametric amplifier, the traveling wave parametric amplifier including a transmission line in communication with the first port and a second port, the transmission line including a plurality of coupled asymmetric SQUIDs; transmitting the weak signal and the pump signal along the transmission line, the plurality of coupled asymmetric SQUIDs amplifying the weak signal as the weak signal is transmitted along the transmission line to produce an amplified signal; and transmitting the amplified signal through the second port. 13. The method as in claim 12 , wherein each of the plurality of coupled asymmetric SQUIDs includes a plurality of Josephson energy junctions. 14. The method as in claim 12 , wherein the plurality of coupled asymmetric SQUIDs defines a ladder-like structure. 15. The method as in claim 12 , wherein transmitting the weak signal and the pump signal along the transmission line includes: adjusting a magnetic flux to provide an in situ optimization of a performance of the traveling wave parametric amplifier, the magnetic flux being produced by an external source. 16. The method as in claim 15 , wherein the adjustment of the magnetic flux is performed using a DC bias line. 17. The method of claim 15 , wherein the optimization of the performance of the traveling wave parametric amplifier includes a tuning of inductance to realize phase matching conditions in a degenerate four-wave mixing process. 18. The method of claim 17 , wherein each of the plurality of coupled asymmetric SQUIDs includes at least one of a smaller Josephson energy junction and more than one of a larger Josephson energy junction, wherein the larger Josephson energy junction has a higher critical current than the smaller Josephson energy junction.
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