{"@type": "dcat:Dataset", "accessLevel": "public", "bureauCode": ["006:55"], "contactPoint": {"fn": "Noah Schlossberger", "hasEmail": "mailto:noah.schlossberger@nist.gov"}, "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) ? 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 ? 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.", "distribution": [{"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/Fig3a.csv", "mediaType": "text/csv", "title": "Fig3a"}, {"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/Fig3d.csv", "mediaType": "text/csv", "title": "Fig3d"}, {"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/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/Fig5a.csv", "mediaType": "text/csv", "title": "Fig5a"}, {"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/Fig5d.csv", "mediaType": "text/csv", "title": "Fig5d"}, {"downloadURL": "https://data.nist.gov/od/ds/mds2-3102/Fig6a.csv", "mediaType": "text/csv", "title": "Fig6a"}, {"downloadURL": "https://data.nist.gov/od/ds/mds2-3102/Fig6b.csv", "mediaType": "text/csv", "title": "Fig6b"}], "identifier": "ark:/88434/mds2-3102", "issued": "2023-11-16", "keyword": ["Autler-Townes", "Rydberg", "Zeeman", "electrometry", "magnetic field", "quantum sensing", "spectroscopy"], "landingPage": "https://data.nist.gov/od/id/mds2-3102", "language": ["en"], "license": "https://www.nist.gov/open/license", "modified": "2023-11-12 00:00:00", "programCode": ["006:045"], "publisher": {"@type": "org:Organization", "name": "National Institute of Standards and Technology"}, "theme": ["Physics:Atomic, molecular, and quantum", "Physics:Optical physics"], "title": "Data associated with \"Zeeman-resolved Autler-Townes splitting in Rydberg atoms with a tunable RF resonance and a single transition dipole moment\""}