Controlling a state of a qubit assembly
US-8928391-B2 · Jan 6, 2015 · US
US9509280B1 · US · B1
| Field | Value |
|---|---|
| Publication number | US-9509280-B1 |
| Application number | US-201514952125-A |
| Country | US |
| Kind code | B1 |
| Filing date | Nov 25, 2015 |
| Priority date | Oct 2, 2015 |
| Publication date | Nov 29, 2016 |
| Grant date | Nov 29, 2016 |
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A technique relates to a microwave device. A qubit is connected to a first end of a first coupling capacitor and a first end of a second coupling capacitor. A resonator is connected to a second end of the first coupling capacitor and a second end of the second coupling capacitor. The resonator includes a fundamental resonance mode. A filter is connected to both the qubit and the first end of the first or second coupling capacitor.
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What is claimed is: 1. A method of configuring a microwave device, the method comprising: connecting a qubit to a first end of a first coupling capacitor and a first end of a second coupling capacitor; connecting a resonator to a second end of the first coupling capacitor and a second end of the second coupling capacitor, wherein the resonator has a fundamental resonance mode, the fundamental resonance mode having a fundamental resonance mode frequency; and connecting a filter to both the qubit and the first end of the first coupling capacitor, the filter and the qubit both being connected together on a same side of the first coupling capacitor, such that both the filter and the qubit are on an opposite side of the first coupling capacitor than the resonator. 2. The method of claim 1 , wherein the filter is configured to block microwave signals at the fundamental resonance mode frequency of the resonator, thereby protecting the qubit from the microwave signals applied at the fundamental resonance mode frequency. 3. The method of claim 2 , wherein the fundamental resonance mode frequency of the resonator has a wavelength. 4. The method of claim 3 , wherein the filter is an open-circuited quarter-wavelength stub. 5. The method of claim 4 , wherein a length of the quarter-wavelength stub corresponds to a quarter of the wavelength. 6. The method of claim 2 , wherein the filter comprises an inductor and a capacitor. 7. The method of claim 6 , wherein the inductor is a lumped element. 8. The method of claim 6 , wherein the inductor is a superconducting line. 9. A method of operating a microwave device, the method comprising: receiving, by at least one of a node A and a node B, microwave signals within a frequency band; and protecting, by a filter, a qubit from the microwave signals applied within the frequency band, the qubit being connected to the node A and the node B, wherein the filter is connected to at least one of the node A and the node B, wherein the node A is on an opposite side of a first coupling capacitor than a resonator, and wherein the node B is on an opposite side of a second coupling capacitor than the resonator, the filter and the qubit both being connected together on a same side of at least one of the first coupling capacitor and the second coupling capacitor, such that both the filter and the qubit are on an opposite side of at least one of the first coupling capacitor and the second coupling capacitor than the resonator. 10. The method of claim 9 , wherein the resonator has a resonance frequency; and wherein the frequency band comprises the resonance frequency along with the frequencies above and below the resonance frequency by a predetermined amount. 11. The method of claim 9 , wherein the filter is configured to protect the qubit from microwave signals at one or more frequencies in the frequency band, the microwave signals at the one or more frequencies cause the qubit to at least one of change state, relax, and lose coherence in an absence the filter. 12. The method of claim 9 , wherein the filter is configured to protect the qubit from microwave signals at one or more frequencies in the frequency band, the microwave signals at the one or more frequencies cause the qubit to at least one of change state, relax, and lose coherence faster in an absence the filter.
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