IP Library Granted Patent US 9,729,152
Granted Patent B2
US 9,729,152 · App. 15/218,548 · Granted Aug 8, 2017

Reducing spontaneous emission in circuit quantum electrodynamics by a combined readout and filter technique

Inventors: Nicholas T. Bronn (Long Island City, NY); Jerry M. Chow (White Plains, NY); Jay M. Gambetta (Yorktown Heights, NY); Nicholas A. Masluk (Putnam Valley, NY); Matthias Steffen (Cortlandt Manor, NY)
Assignee: INTERNATIONAL BUSINESS MACHINES CORPORATION
H03K19/00346H03K19/195
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Quick Facts
Patent No.
US 9,729,152
App. No.
15/218,548
Granted
Aug 8, 2017
Kind
B2
Abstract

A mechanism relates a superconductor circuit. A Δ circuit includes a first node connecting a Purcell capacitor to a qubit coupling capacitor, a second node connecting the Purcell capacitor to a readout coupling capacitor, and a third node connecting the qubit coupling capacitor to the readout coupling capacitor. A qubit is connected to the first node and has a qubit frequency. A readout resonator connects to the third node combining with the Purcell capacitor to form a filter. Capacitance of the Purcell capacitor is determined as a factor of the qubit frequency of the qubit and blocks emissions of the qubit at the qubit frequency. Capacitance of the Purcell capacitor causes destructive interference, between a first path containing Purcell capacitor and a second path containing both the qubit coupling capacitor and readout coupling capacitor, in order to block emissions of the qubit at the qubit frequency to the external environment.

Claims (27)

1. A superconductor circuit comprising:

a circuit comprising a first node connecting a Purcell capacitor (C P ) to a qubit coupling capacitor (C q ), a second node connecting the Purcell capacitor (C P ) to a readout coupling capacitor (C c ), and a third node connecting the qubit coupling capacitor (C q ) to the readout coupling capacitor (C c ), wherein the first node is configured for connection to a qubit having a qubit frequency; and

a readout resonator connected to the third node;

wherein a capacitance of the Purcell capacitor (C P ) is determined as a factor of the qubit frequency of the qubit, such that the capacitance of the Purcell capacitor (C P ) filters emissions of the qubit at the qubit frequency to an external environment.

2. The superconductor circuit of claim 1 , wherein the readout resonator combines with the Purcell capacitor (C P ) to form a filter.

3. The superconductor circuit of claim 1 , wherein the second node is configured for connection to the external environment.

4. The superconductor circuit of claim 3 , wherein the capacitance of the Purcell capacitor (C P ) is set to cause destructive interference, between a first path containing the Purcell capacitor (C P ) and a second path containing both the qubit coupling capacitor (C q ) and the readout coupling capacitor (C c ), at the qubit frequency in order to filter the emissions of the qubit at the qubit frequency to the external environment.

5. The superconductor circuit of claim 1 , wherein the capacitance of the Purcell capacitor (C P ) has a direct relationship to the qubit frequency of the qubit in which the capacitance of the Purcell capacitor (C P ) is to be increased when a value of the qubit frequency is increased in order to filter the qubit frequency to the external environment.

6. The superconductor circuit of claim 1 , wherein the readout resonator further comprises an inductance and a capacitance connected in parallel together.

7. The superconductor circuit of claim 1 , wherein the readout resonator provides dispersive readout of the qubit to the external environment.

8. The superconductor circuit of claim 7 , wherein the readout resonator combined with the Purcell capacitor (C P ) provides filtering, at the qubit frequency, radiation from the qubit to the external environment.

9. The superconductor circuit of claim 1 , wherein the capacitance of the Purcell capacitor (C P ) is determined based on factors which include the qubit frequency of the qubit, an inductance of the readout resonator, and a capacitance of the readout resonator such that the capacitance of the Purcell capacitor (C P ) filters emissions of the qubit at the qubit frequency to the external environment while allowing dispersive readout of a state of the qubit.

10. The superconductor circuit of claim 1 , wherein the qubit includes a Josephson junction.

11. The superconductor circuit of claim 1 , wherein the circuit is a delta (Δ) circuit that has a relationship to a Y circuit; and

wherein the capacitance of the Purcell capacitor (C P ) is determined based on the relationship between the Δ circuit and the Y circuit.

12. A method of providing a superconductor circuit, the method comprising:

providing a circuit comprising a first node connecting a Purcell capacitor (C P ) to a qubit coupling capacitor (C q ), a second node connecting the Purcell capacitor (C P ) to a readout coupling capacitor (C c ), and a third node connecting the qubit coupling capacitor (C q ) to the readout coupling capacitor (C c ), wherein the first node is configured for connection to a qubit having a qubit frequency; and

providing a readout resonator connected to the third node;

wherein a capacitance of the Purcell capacitor (C P ) is determined as a factor of the qubit frequency of the qubit, such that the capacitance of the Purcell capacitor (C P ) filters emissions of the qubit at the qubit frequency to an external environment.

13. The method of claim 12 , wherein the readout resonator combines with the Purcell capacitor (C P ) to form a filter.

14. The method of claim 12 , wherein the second node is configured for connection to the external environment.

15. The method of claim 14 , wherein the capacitance of the Purcell capacitor (C P ) is set to cause destructive interference, between a first path containing the Purcell capacitor (C P ) and a second path containing both the qubit coupling capacitor (C q ) and the readout coupling capacitor (C c ), at the qubit frequency in order to filter the emissions of the qubit at the qubit frequency to the external environment.

16. The method of claim 12 , wherein the capacitance of the Purcell capacitor (C P ) has a direct relationship to the qubit frequency of the qubit in which the capacitance of the Purcell capacitor (C P ) is to be increased when a value of the qubit frequency is increased in order to filter the qubit frequency to the external environment.

17. The method of claim 12 , wherein the readout resonator comprises an inductance and a capacitance connected in parallel together.

18. The method of claim 12 , wherein the readout resonator provides dispersive readout of the qubit to the external environment.

19. The method of claim 18 , wherein the readout resonator combined with the Purcell capacitor (C P ) provides filtering, at the qubit frequency, radiation from the qubit to the external environment.

20. The method of claim 12 , wherein the capacitance of the Purcell capacitor (C P ) is determined based on factors which include the qubit frequency of the qubit, an inductance of the readout resonator, and a capacitance of the readout resonator such that the capacitance of the Purcell capacitor (C P ) filters emissions of the qubit at the qubit frequency to the external environment while allowing dispersive readout of a state of the qubit.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jul 25, 2016
From: BRONN, NICHOLAS T.; CHOW, JERRY M.; GAMBETTA, JAY M.; MASLUK, NICHOLAS A.; STEFFEN, MATTHIAS
To: INTERNATIONAL BUSINESS MACHINES CORPORATION
Reel/Frame 039246/0567 →
Continuity (2)
Continuation 14512489 · Oct 13, 2014
Related Publication 20160329896A1 · Nov 10, 2016