Tunable transmon circuit assembly

Patent metadata

Field	Value
Publication number	US-9685935-B2
Application number	US-201414485129-A
Country	US
Kind code	B2
Filing date	Sep 12, 2014
Priority date	Sep 12, 2014
Publication date	Jun 20, 2017
Grant date	Jun 20, 2017

Abstract

Systems and methods are provided for a tunable transmon qubit. The qubit includes a first Josephson junction on a first path between a transmission line and a circuit ground and second and third Josephson junctions arranged in parallel with one another on a second path between the transmission line and the circuit ground to form a direct current superconducting quantum interference device (DC SQUID). The DC SQUID is in parallel with the first Josephson junction. A capacitor is arranged in parallel with the first Josephson junction and the DC SQUID on a third path between the transmission line and the circuit ground as to form, in combination with the first path, an outer loop of the tunable transmon qubit. A bias circuit is configured to provide a constant bias flux to one of the DC SQUID and the outer loop of the tunable transmon qubit.

First claim

Having described the invention, we claim:

1. A tunable transmon qubit comprising:
a first Josephson junction on a first path between a transmission line and a circuit ground;
second and third Josephson junctions arranged in parallel with one another on a second path between the transmission line and the circuit ground to form a direct current superconducting quantum interference device (DC SQUID), the DC SQUID being in parallel with the first Josephson junction;
a capacitor in parallel with the first Josephson junction and the DC SQUID on a third path between the transmission line and the circuit ground as to form, in combination with the first path, an outer loop of the tunable transmon qubit; and
a bias circuit configured during an operation of the tunable transmon qubit to provide a first constant bias flux to one of the DC SQUID and the outer loop of the tunable transmon qubit and to provide a second constant bias flux to another of the DC SQUID and the outer loop of the tunable transmon qubit.

2. The tunable transmon qubit of claim 1 , wherein the bias circuit is configured to provide the first constant bias flux to the DC SQUID.

3. The tunable transmon qubit of claim 1 , wherein the bias circuit is configured to provide the first constant bias flux the outer loop of the tunable transmon qubit.

4. The tunable transmon qubit of claim 1 , wherein the bias circuit is a first bias circuit configured to provide the first constant bias flux to the one of the DC SQUID and the outer loop of the tunable transmon qubit, the system further comprising a second bias circuit configured to provide the second constant bias flux to another of the DC SQUID and the outer loop of the tunable transmon qubit.

5. The tunable transmon qubit of claim 4 , the DC SQUID comprising at least one inductor, such that a bias current within the DC SQUID can be induced in response to the first constant bias flux, such that a frequency of a transition between a ground state of the qubit and a first excited state of the qubit is a function of the provided first constant bias flux.

6. The tunable transmon qubit of claim 5 , the outer loop comprising at least one inductor, such that a bias current can be induced in the outer loop in response to the second constant bias flux, such that a frequency of a transition between a ground state of the qubit and a first excited state of the qubit is a function of both of the first constant bias flux and the second constant bias flux.

7. The tunable transmon qubit of claim 4 , the outer loop comprising at least one inductor, such that a bias current can be induced in the outer loop in response to the second constant bias flux, such that a frequency of a transition between a ground state of the qubit and a first excited state of the qubit is a function of the provided second constant bias flux.

8. The tunable transmon qubit of claim 1 , further comprising a fourth Josephson junction arranged in series with the first Josephson junction on the first path.

9. A system comprising:
the tunable transmon qubit of claim 1 ; and
a classical control configured to provide a control flux to the tunable transmon qubit.

10. The system of claim 9 , further comprising a transmission line resonator coupled to the tunable transmon qubit.

11. The system of claim 9 , wherein the classical control comprises a reciprocal quantum logic (RQL) driver providing current to a current loop inductively coupled to the tunable transmon qubit.

12. The system of claim 11 , wherein the bias circuit is configured to provide current to a current loop inductively coupled to the tunable transmon qubit.

13. A system comprising:
a plurality of tunable transmon qubits, wherein a given transmon qubit of the plurality of tunable transmon qubits comprises:
a first Josephson junction on a first path between a transmission line and a circuit ground;
second and third Josephson junctions arranged in parallel with one another on a second path between the transmission line and the circuit ground to form a direct current superconducting quantum interference device (DC SQUID), the DC SQUID being in parallel with the first Josephson junction;
a capacitor in parallel with the first Josephson junction and the DC SQUID on a third path between the transmission line and the circuit ground as to form, in combination with the first path, an outer loop of the tunable transmon qubit; and
a bias circuit configured to provide a constant bias flux to one of the DC SQUID and the outer loop of the tunable transmon qubit; and

a classical control associated with each of the plurality of tunable transmon qubits and coupled to a digital-to-analog converter (DAC) to receive a control signal, each classical control comprising a respective a reciprocal quantum logic (RQL) driver that provides current to a current loop inductively coupled to a respective tunable transmon qubit to deliver a control flux to the respective tunable transmon qubit in response to the control signal from the DAC.

14. The system of claim 9 , further comprising a system control operatively connected to the classical control, the system control being operative to control respective magnitudes of the control flux to transition the tunable transmon qubit among energy states associated with the qubit.

15. A method for constructing a tunable transmon qubit, the method comprising:
fabricating a transmon qubit comprising a first Josephson junction on a first path between a transmission line and a circuit ground, second and third Josephson junctions arranged in parallel with one another on a second path between the transmission line and the circuit ground to form a direct current superconducting quantum interference device (DC SQUID) in parallel with the first Josephson junction, and a capacitor in parallel with first Josephson junction and the DC SQUID on a third path between the transmission line and the circuit ground as to form, in combination with the first path, an outer loop of the transmon qubit;
determining a frequency curve of the transmon qubit; and
providing during operation of the tunable transmon qubit a first constant bias flux to one of the DC SQUID and the outer loop of the transmon qubit and a second constant bias flux to another of the DC SQUID and the outer loop of the transmon qubit to adjust the frequency curve of the transmon qubit, the frequency curve representing a frequency of a first energy level transition as a function of a control flux.

16. The method of claim 15 , wherein during operation of the tunable transmon qubit a first constant bias flux to one of the DC SQUID and the outer loop of the transmon qubit and a second constant bias flux to another of the DC SQUID and the outer loop of the transmon qubit to adjust the frequency curve of the transmon qubit comprises providing the first constant bias flux to the outer loop as to translate the frequency curve, such that a substantially constant value is added or subtracted from the frequency of a first energy level transition across a range of control fluxes.

17. The method of claim 16 , wherein providing the first constant bias flux to the outer loop comprises adding the constant bias flux to a control flux provided to the transmon qubit.

18. The method of claim 16 , wherein providing the first constant bias flux to the outer loop comprises providing the first constant bias flux independently of a control flux provided to the transmon qubit.

19. The method of claim 15 , wherein during an operation of the tunable transmon qubit a first constant bias flux to

Assignees

• Strand Joel D
• Pesetski Aaron A
• Northrop Grumman Systems Corp

Inventors

• Strand Joel D
• Pesetski Aaron A

Classifications

• G06N99/002

  Physics · mapped topic

• H03K3/012

  Modifications of generator to improve response time or to decrease power consumption · CPC title

• H03K3/38 Primary

  by the use, as active elements, of superconductive devices · CPC title

• H01L39/2493

  Electricity · mapped topic

• B82Y10/00

  Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic · CPC title