Mitigating baseband pulse dispersion via radiofrequency-to-baseband conversion

Patent metadata

Field	Value
Publication number	US-2023198555-A1
Application number	US-202117552580-A
Country	US
Kind code	A1
Filing date	Dec 16, 2021
Priority date	Dec 16, 2021
Publication date	Jun 22, 2023
Grant date	—

Abstract

Systems and techniques that facilitate mitigation of baseband pulse distortion via radiofrequency-to-baseband conversion are provided. In various embodiments, a system can comprise a qubit. In various aspects, the system can further comprise a signal generator that can produce a radiofrequency signal. In various instances, the system can further comprise a signal converter coupled between the qubit and the signal generator. In various cases, the signal converter can convert the radiofrequency signal into a baseband signal. In various aspects, such radiofrequency-to-baseband conversion can reduce a dispersion-induced distortion associated with driving the qubit.

First claim

What is claimed is:

1 . A system, comprising:
a qubit; a signal generator producing a radiofrequency signal; and a signal converter coupled between the qubit and the signal generator, wherein the signal converter converts the radiofrequency signal into a baseband signal.

2 . The system of claim 1 , further comprising:
a non-superconducting cable located in a first signal path between the signal generator and the signal converter; and a superconducting cable located in a second signal path between the signal converter and the qubit.

3 . The system of claim 1 , wherein the signal converter is an envelope detector.

4 . The system of claim 1 , further comprising:
a bias-tee coupled between the signal converter and the qubit, wherein the bias-tee combines the baseband signal with a constant baseband signal.

5 . The system of claim 1 , wherein the radiofrequency signal is a rectangular radiofrequency pulse, and wherein the baseband signal is a baseband pulse defined by an envelope of the rectangular radiofrequency pulse.

6 . The system of claim 1 , wherein the radiofrequency signal is a rectangular radiofrequency offset pulse that is a result of superimposition of a constant radiofrequency signal onto a rectangular radiofrequency pulse that is 180 degrees out of phase with the constant radiofrequency signal, and wherein the baseband signal is a baseband offset pulse defined by an envelope of the rectangular radiofrequency offset pulse.

7 . The system of claim 1 , further comprising:
a second qubit, a second signal generator producing a second radiofrequency signal, and a second signal converter coupled between the second qubit and the second signal generator; a multiplexer located at an end of a non-superconducting cable, wherein the multiplexer combines the radiofrequency signal with the second radiofrequency signal, thereby yielding a multiplexed radiofrequency signal; and a demultiplexer coupled to another end of the non-superconducting cable and that separates the multiplexed radiofrequency signal into the radiofrequency signal and the second radiofrequency signal, wherein the second signal converter converts the second radiofrequency signal to a second baseband signal.

8 . The system of claim 1 , wherein the signal converter is implemented at a cryogenic temperature.

9 . A method, comprising:
generating, by a signal generator, a radiofrequency signal; and converting, by a signal converter that is coupled between a qubit and the signal generator, the radiofrequency signal into a baseband signal.

10 . The method of claim 9 , wherein a non-superconducting cable is located in a first signal path between the signal generator and the signal converter, and wherein a superconducting cable is located in a second signal path between the signal converter and the qubit.

11 . The method of claim 9 , wherein the signal converter is an envelope detector.

12 . The method of claim 9 , further comprising:
combining, by a bias-tee that is coupled between the signal converter and the qubit, the baseband signal with a constant baseband signal.

13 . The method of claim 9 , wherein the radiofrequency signal is a rectangular radiofrequency pulse, and wherein the baseband signal is a baseband pulse defined by an envelope of the rectangular radiofrequency pulse.

14 . The method of claim 9 , wherein the radiofrequency signal is a rectangular radiofrequency offset pulse that is a result of superimposition of a constant radiofrequency signal onto a rectangular radiofrequency pulse that is 180 degrees out of phase with the constant radiofrequency signal, and wherein the baseband signal is a baseband offset pulse defined by an envelope of the rectangular radiofrequency offset pulse.

15 . The method of claim 9 , further comprising:
generating, by a second signal generator, a second radiofrequency signal; combining, by a multiplexer, the radiofrequency signal with the second radiofrequency signal, thereby yielding a multiplexed radiofrequency signal; separating, by a demultiplexer, the multiplexed radiofrequency signal into the radiofrequency signal and the second radiofrequency signal; and converting, by a second signal converter coupled between the second signal generator and a second qubit, the second radiofrequency signal into a second baseband signal.

16 . The method of claim 9 , wherein the signal converter is implemented at a cryogenic temperature.

17 . An apparatus, comprising:
a qubit; a signal generator operable to produce a radiofrequency signal; and a signal converter coupled between the qubit and the signal generator, wherein the signal converter is operable to convert the radiofrequency signal into a baseband signal.

18 . The apparatus of claim 17 , wherein the signal generator is implemented at a non-cryogenic temperature, and wherein the qubit and the signal converter are implemented at cryogenic temperatures.

19 . The apparatus of claim 17 , further comprising:
a bias-tee coupled between the signal converter and the qubit, wherein the bias-tee is operable to combine the baseband signal with a constant baseband signal, and wherein the bias-tee is implemented at a cryogenic temperature.

20 . The apparatus of claim 17 , further comprising:
a second qubit, a second signal generator operable to produce a second radiofrequency signal, and a second signal converter coupled between the second qubit and the second signal generator; a multiplexer operable to combine the radiofrequency signal with the second radiofrequency signal, thereby yielding a multiplexed radiofrequency signal; and a demultiplexer operable to separate the multiplexed radiofrequency signal into the radiofrequency signal and the second radiofrequency signal, wherein the second signal converter is operable to convert the second radiofrequency signal to a second baseband signal; wherein the multiplexer is implemented at a non-cryogenic temperature, and wherein the demultiplexer is implemented at a cryogenic temperature.

Assignees

• IBM

Inventors

• Phung Timothy
• Underwood Devin
• Stehlik Jiri
• Zajac David

Classifications

• H04B1/0096 Primary

  where a full band is frequency converted into another full band · CPC title

• H04B1/0028 Primary

  wherein the AD/DA conversion occurs at baseband stage · CPC title

• G06N10/40

  Physical realisations or architectures of quantum processors or components for manipulating qubits, e.g. qubit coupling or qubit control · CPC title

• G06N10/00

  Quantum computing, i.e. information processing based on quantum-mechanical phenomena · CPC title