Quantum information processing
US-2016300155-A1 · Oct 13, 2016 · US
US10496932B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10496932-B2 |
| Application number | US-201816039186-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jul 18, 2018 |
| Priority date | Jul 18, 2017 |
| Publication date | Dec 3, 2019 |
| Grant date | Dec 3, 2019 |
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.
Aspects of the present disclosure describe a compact RF driver circuit for Paul traps in trapped ion quantum computers and methods, and structures including same.
Opening claim text (preview).
The invention claimed is: 1. A compact RF driver circuit for a Paul trap in a trapped ion quantum computer system comprising: the trapped ion quantum computer system including the compact RF driver circuit having an inductive-capacitive tank circuit; an unmatched, low-output-impedance amplifier (<4 Ω) that electrically drives the tank circuit; and the Paul trap electrically connected to an output of the tank circuit. 2. The driver circuit for the quantum computer Paul trap of claim 1 wherein the amplifier exhibits an output impedance of 1 ohm or less. 3. The driver circuit for the quantum computer Paul trap of claim 1 wherein the circuit is operated under cryogenic conditions. 4. The driver circuit for the quantum computer Paul trap of claim 3 wherein the tank circuit includes a superconducting inductor and the Paul trap is driven at a trap frequency >10 MHz. 5. The driver circuit for the quantum computer Paul trap of claim 1 configured such that it does not include a tuning circuit. 6. The driver circuit for the quantum computer Paul trap of claim 1 configured such that it does not include a helical resonator. 7. A method of operating a Paul trap in a trapped ion quantum computer, said method comprising: providing a quantum computer system including: a compact RF driver circuit having an inductive-capacitive tank circuit; an unmatched, low-output-impedance amplifier (<4 ohm) electrically connected to the tank circuit; providing a load to the driver circuit, said load comprising the Paul trap; and operating the driver circuit such that the Paul trap is operational to trap sample ions. 8. The method of claim 7 wherein the unmatched, low-output-impedance amplifier exhibits an output impedance of 1 ohm or less. 9. The method of claim 7 further comprising providing cryogenic conditions for the Paul trap and the driver circuit. 10. The method of claim 7 wherein the tank circuit includes a superconducting inductor. 11. The method of claim 10 wherein the Paul trap is driven at a frequency >10 MHz. 12. The method of claim 10 wherein the Paul trap is driven at a frequency from 30 MHz to 500 MHz. 13. The method of claim 7 wherein the quantum computer system does not include a helical resonator. 14. The method of claim 7 wherein the driver circuit does not include a tuning circuit.
Multipole linear ion traps, e.g. quadrupoles, hexapoles · CPC title
Impedance-matching networks · CPC title
by the use, as active elements, of superconductive devices · CPC title
Quantum computing, i.e. information processing based on quantum-mechanical phenomena · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.