U.S. flag

An official website of the United States government

Dot gov

Official websites use .gov
A .gov website belongs to an official government organization in the United States.

Https

Secure .gov websites use HTTPS
A lock () or https:// means you’ve safely connected to the .gov website. Share sensitive information only on official, secure websites.

Breadcrumb

  1. Home

Superconducting Qubit Control Using Cryogenic Frequency Conversion

Dataset for the APL paper "Superconducting Qubit Control Using Cryogenic Frequency Conversion".

Abstract:
Expanding to higher qubit frequencies introduces the challenge of routing > 20 GHz signals into a dilution refrigerator without adding excess thermal load or frequency-dependent loss. In this work, we demonstrate a solution to this problem by using a frequency multiplier to drive the qubit with room-temperature control pulses at half or one third of the qubit frequency fQB. The control pulses are up-converted inside the cryogenic environment using a frequency multiplier based on a high-kinetic inductance nonlinear transmission line. We evaluated the success of the up-conversion technique by comparing the randomized benchmarking error-per-gate metrics to that of a standard direct qubit driving technique. The fQB/2 drive technique achieved error rates consistent with the direct drive, with a minimum error-per-gate of 3.5x10−3±0.4x10−3. The fQB/3 drive technique resulted in a minimum error per gate of 7.6x10−3±0.81x10−3. While this demonstration is based around a fQB = 4.836 GHz qubit so that a direct drive comparison is possible, this technique will allow higher-frequency qubits to be tested using existing radio-frequency (RF) infrastructure.

About this Dataset

Updated: 2026-09-04
Metadata Last Updated: 2026-02-26 00:00:00
Date Created: N/A
Data Provided by:
Dataset Owner: N/A

Access this data

Contact dataset owner Landing Page URL
Download URL
Table representation of structured data
Title Superconducting Qubit Control Using Cryogenic Frequency Conversion
Description Dataset for the APL paper "Superconducting Qubit Control Using Cryogenic Frequency Conversion". Abstract: Expanding to higher qubit frequencies introduces the challenge of routing > 20 GHz signals into a dilution refrigerator without adding excess thermal load or frequency-dependent loss. In this work, we demonstrate a solution to this problem by using a frequency multiplier to drive the qubit with room-temperature control pulses at half or one third of the qubit frequency fQB. The control pulses are up-converted inside the cryogenic environment using a frequency multiplier based on a high-kinetic inductance nonlinear transmission line. We evaluated the success of the up-conversion technique by comparing the randomized benchmarking error-per-gate metrics to that of a standard direct qubit driving technique. The fQB/2 drive technique achieved error rates consistent with the direct drive, with a minimum error-per-gate of 3.5x10−3±0.4x10−3. The fQB/3 drive technique resulted in a minimum error per gate of 7.6x10−3±0.81x10−3. While this demonstration is based around a fQB = 4.836 GHz qubit so that a direct drive comparison is possible, this technique will allow higher-frequency qubits to be tested using existing radio-frequency (RF) infrastructure.
Modified 2026-02-26 00:00:00
Publisher Name National Institute of Standards and Technology
Contact mailto:[email protected]
Keywords Superconductors , kinetic inductance , Frequency conversion.
{
    "identifier": "ark:\/88434\/mds2-4118",
    "accessLevel": "public",
    "contactPoint": {
        "hasEmail": "mailto:[email protected]",
        "fn": "Nathan Flowers-Jacobs"
    },
    "programCode": [
        "006:045"
    ],
    "landingPage": "https:\/\/data.nist.gov\/od\/id\/mds2-4118",
    "title": "Superconducting Qubit Control Using Cryogenic Frequency Conversion",
    "description": "Dataset for the APL paper \"Superconducting Qubit Control Using Cryogenic Frequency Conversion\".\n\nAbstract:\nExpanding to higher qubit frequencies introduces the challenge of routing > 20 GHz signals into a dilution refrigerator without adding excess thermal load or frequency-dependent loss. In this work, we demonstrate a solution to this problem by using a frequency multiplier to drive the qubit with room-temperature control pulses at half or one third of the qubit frequency fQB. The control pulses are up-converted inside the cryogenic environment using a frequency multiplier based on a high-kinetic inductance nonlinear transmission line. We evaluated the success of the up-conversion technique by comparing the randomized benchmarking error-per-gate metrics to that of a standard direct qubit driving technique. The fQB\/2 drive technique achieved error rates consistent with the direct drive, with a minimum error-per-gate of 3.5x10\u22123\u00b10.4x10\u22123. The fQB\/3 drive technique resulted in a minimum error per gate of 7.6x10\u22123\u00b10.81x10\u22123. While this demonstration is based around a fQB = 4.836 GHz qubit so that a direct drive comparison is possible, this technique will allow higher-frequency qubits to be tested using existing radio-frequency (RF) infrastructure.",
    "language": [
        "en"
    ],
    "distribution": [
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/4118_README.txt",
            "mediaType": "text\/plain",
            "title": "4118_README"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/fig6_tripler.txt",
            "mediaType": "text\/plain",
            "title": "fig6_tripler"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/fig6_doubler.txt",
            "mediaType": "text\/plain",
            "title": "fig6_doubler"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/fig7.json",
            "mediaType": "application\/json",
            "title": "fig7"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/fig6_direct_drive.txt",
            "mediaType": "text\/plain",
            "title": "fig6_direct_drive"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/fig5_left.txt",
            "mediaType": "text\/plain",
            "title": "fig5_left"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/fig2.json",
            "mediaType": "application\/json",
            "title": "fig2"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/fig3.json",
            "mediaType": "application\/json",
            "title": "fig3"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/fig5_right.txt",
            "mediaType": "text\/plain",
            "title": "fig5_right"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-4118\/fig8.json",
            "mediaType": "application\/json",
            "title": "fig8"
        }
    ],
    "bureauCode": [
        "006:55"
    ],
    "modified": "2026-02-26 00:00:00",
    "publisher": {
        "@type": "org:Organization",
        "name": "National Institute of Standards and Technology"
    },
    "theme": [
        "Electronics:Superconducting electronics"
    ],
    "keyword": [
        "Superconductors",
        "kinetic inductance",
        "Frequency conversion."
    ]
}