{
    "identifier": "ark:\/88434\/mds2-3102",
    "accessLevel": "public",
    "contactPoint": {
        "hasEmail": "mailto:[email protected]",
        "fn": "Noah Schlossberger"
    },
    "programCode": [
        "006:045"
    ],
    "landingPage": "https:\/\/data.nist.gov\/od\/id\/mds2-3102",
    "title": "Data associated with \"Zeeman-resolved Autler-Townes splitting in Rydberg atoms with a tunable RF resonance and a single transition dipole moment\"",
    "description": "Data associated with the publication: \"Zeeman-resolved Autler-Townes splitting in Rydberg atoms with a tunable RF resonance and a single transition dipole moment\"Applying a magnetic field as a method for tuning the frequency of Autler-Townes splitting for Rydberg electrometry has recently been demonstrated. In the corresponding paper, we provide a theoretical understanding of EIT signals in the presence of a large magnetic field, as well as demonstrate some advantages of this technique over traditional Autler-Townes based electrometry. We show that a strong magnetic field provides a well-defined quantization axis regardless of the optical field polarizations, we demonstrate that by separating the $m_J$ levels of the Rydberg state we can perform an Autler-Townes splitting with a single participating dipole moment, and we demonstrate recovery of signal strength by populating a single $m_J$ level using circularly polarized light.Included in this dataset is the data associated with every plot in the paper, separated by figure number, including:FIgure 2: Measured EIT signals in the presence of a strong(1.85(1) mT) magnetic field either aligned with or orthogonalto the polarization axis. Figure 3: Theoretical EIT signals for Cs in the presence ofa 1.85(1) mT magnetic field for light polarizations alignedto or orthogonal to the magnetic field.Figure 4: Measured Autler-Townes splittings in individual mJlevels via the 58D5\/2(mJ = \u00b15\/2) \u2192 59P3\/2(mJ = \u00b13\/2)transitions of Cs in the presence of 2.78(1) mT.Figure 5: Measured Autler-Townes splittings on the Cs58D5\/2 \u2192 59P3\/2 transition with and without mJ selectivityfor various RF fields up to 3.08 V\/m. Figure 6:  EIT in the presence of a large magnetic field using circularly polarized light.EIT signals correspond to voltage traces (collected on an oscilloscope) of a balanced photodiode as laser frequencies are scanned. The x axis is converted from a time series of each voltage to a frequency using a reference cell. The scaling is determined by measuring the difference between the EIT peaks corresponding to the D5\/2 and D3\/2 Rydberg states, and the zero is generally taken to be the location of the D5\/2 EIT peak.",
    "language": [
        "en"
    ],
    "distribution": [
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig5b.csv",
            "mediaType": "text\/csv",
            "title": "Fig5b"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig5c.csv",
            "mediaType": "text\/csv",
            "title": "Fig5c"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/3102_README.txt",
            "mediaType": "text\/plain",
            "title": "3102_README"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig5a.csv",
            "mediaType": "text\/csv",
            "title": "Fig5a"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig3b.csv",
            "mediaType": "text\/csv",
            "title": "Fig3b"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig3a.csv",
            "mediaType": "text\/csv",
            "title": "Fig3a"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig3d.csv",
            "mediaType": "text\/csv",
            "title": "Fig3d"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig5d.csv",
            "mediaType": "text\/csv",
            "title": "Fig5d"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig4b.csv",
            "mediaType": "text\/csv",
            "title": "Fig4b"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig4c.csv",
            "mediaType": "text\/csv",
            "title": "Fig4c"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig4a.csv",
            "mediaType": "text\/csv",
            "title": "Fig4a"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig6b.csv",
            "mediaType": "text\/csv",
            "title": "Fig6b"
        },
        {
            "downloadURL": "https:\/\/data.nist.gov\/od\/ds\/mds2-3102\/Fig6a.csv",
            "mediaType": "text\/csv",
            "title": "Fig6a"
        }
    ],
    "bureauCode": [
        "006:55"
    ],
    "modified": "2023-11-12 00:00:00",
    "publisher": {
        "@type": "org:Organization",
        "name": "National Institute of Standards and Technology"
    },
    "theme": [
        "Physics:Optical physics",
        "Physics:Atomic, molecular, and quantum"
    ],
    "keyword": [
        "spectroscopy",
        "Rydberg",
        "magnetic field",
        "Zeeman",
        "electrometry",
        "quantum sensing",
        "Autler-Townes"
    ]
}