Circuit assembly, a system and a method for cooling quantum electric devices
US-11210601-B2 · Dec 28, 2021 · US
US11442086B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11442086-B2 |
| Application number | US-201816766152-A |
| Country | US |
| Kind code | B2 |
| Filing date | Nov 22, 2018 |
| Priority date | Nov 23, 2017 |
| Publication date | Sep 13, 2022 |
| Grant date | Sep 13, 2022 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A detector of microwave radiation includes a signal input and a detector output. An absorber element of ohmic conductivity is coupled to said signal input through a first length of superconductor. A variable impedance element, the impedance of which is configured to change as a function of temperature, is coupled to the detector output through a second length of superconductor. The detector also includes a heating input and a heating element coupled to the heating input through a third length of superconductor. The absorber element, the variable impedance element, and the heating element are coupled to each other through superconductor sections of lengths shorter than any of said first, second, and third lengths of superconductor.
Opening claim text (preview).
The invention is claimed as follows: 1. A detector of microwave radiation, comprising: a signal input and a detector output; an absorber element of ohmic conductivity, coupled to said signal input through a first length of superconductor; and a variable impedance element, the impedance of which is configured to change as a function of temperature, coupled to said detector output through a second length of superconductor, wherein: the detector comprises a heating input, the detector comprises a heating element coupled to said heating input through a third length of superconductor, and said absorber element, said variable impedance element, and said heating element are coupled to each other through superconductor sections of lengths shorter than any of said first, second, and third lengths of superconductor to allow hot electron diffusion between said absorber element, said variable impedance element, and said heating element while blocking quasiparticle thermal transport of heat through said first, second, and third lengths of superconductor. 2. The detector according to claim 1 , further comprising microwave filters along at least one of said first and third lengths of superconductor. 3. The detector according to claim 1 , further comprising a low-pass or band-pass microwave filter along said third length of superconductor. 4. The detector according to claim 1 , further comprising a band-pass microwave filter along said first length of superconductor. 5. The detector according to claim 4 , wherein said band-pass microwave filter is controllable with regard to at least one of: middle frequency of its pass band, or width of its pass band. 6. The detector according to claim 1 , wherein: said heating input is a first heating input coupled to a first end of said heating element, and comprises a first heating current lead and a first voltage measurement connection; and said detector comprises a second heating input that is coupled to a second end of said heating element, and comprises a second heating current lead and a second voltage measurement connection. 7. The detector according to claim 1 , wherein: said absorber element and said variable impedance element have a common longitudinal axis; and said heating element runs parallel to at least one of said absorber element and said variable impedance element with a perpendicular displacement therefrom. 8. The detector according to claim 1 , wherein: said variable impedance element has a longitudinal axis; and said absorber element and said heating element form a pattern that is symmetrical with respect to the longitudinal axis of said variable impedance element. 9. A detector arrangement for detecting microwave radiation, comprising: at least one detector; and a resonance measurement circuit configured to measure the resonance frequency of a tank circuit coupled to said detector output, wherein: the detector is a detector of microwave radiation, the detector comprises a signal input, a detector output, an absorber element of ohmic conductivity coupled to said signal input through a first length of superconductor, and a variable impedance element the impedance of which is configured to change as a function of temperature, the variable impedance element is coupled to said detector output through a second length of superconductor, the detector comprises a heating input, the detector comprises a heating element coupled to said heating input through a third length of superconductor, and said absorber element, said variable impedance element, and said heating element are coupled to each other through superconductor sections of lengths shorter than any of said first, second, and third lengths of superconductor to allow hot electron diffusion between said absorber element, said variable impedance element, and said heating element while blocking quasiparticle thermal transport of heat through said first, second, and third lengths of superconductor. 10. The detector arrangement according to claim 9 , further comprising: a heating current controller configured to make a heating current of known magnitude flow through said heating input. 11. The detector arrangement according to claim 10 , wherein: said heating input is a first heating input coupled to a first end of said heating element in said detector, and comprises a first heating current lead and a first voltage measurement connection; said detector comprises a second heating input that is coupled to a second end of said heating element in said detector, and comprises a second heating current lead and a second voltage measurement connection; said heating current controller comprises a series coupling of a voltage source and a ballast resistor, coupled across said first and second heating current leads; and said detector arrangement comprises a voltmeter coupled across said first and second voltage measurement connections. 12. The detector arrangement according to claim 11 , wherein: the detector arrangement is configured to calibrate the detector by making said series coupling feed a calibrating current through said heating element and measuring corresponding change in the resonance frequency of the tank circuit; and the detector arrangement is configured to measure changes in the resonance frequency of the tank circuit during detection of microwave radiation and to produce a measurement signal indicative of such changes. 13. The detector arrangement according to claim 11 , wherein: the detector arrangement is configured to make said series coupling feed a compensating current through said heating element in dependence with a feedback coupling to keep the resonance frequency of the tank circuit constant during detection of microwave radiation; and the detector arrangement is configured to produce a measurement signal indicative of the magnitude of said compensating current.
Compensating for temperature change · CPC title
by thermal methods {, e.g. calorimetric} · CPC title
by means of thermocouples or other heat sensitive elements · CPC title
for measuring the power of light beams, e.g. laser beams · CPC title
Calibrated temperature sources, temperature standards therefor (arrangements with respect to the cold junction of thermo-electric elements G01K7/12) · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.