研究目的
Extending the approach to measurements of high-intensity RF electric fields above 1 kV/m and continuous-frequency RF measurement capability.
研究成果
Measurements of RF fields exceeding 1 kV/m have been demonstrated. Continuous-frequency measurements of RF fields in the strong-field regime have been discussed.
研究不足
The atomic response becomes nonlinear due to increasing AC shifts from a multitude of other Rydberg levels, as well as due to multi-photon and higher-order couplings in the high-field regime.
1:Experimental Design and Method Selection:
The experimental setup involves a small (3 mm inner-diameter) rubidium (Rb) vapor cell and two counter-propagating lasers at wavelengths of 780 nm and 480 nm for EIT spectroscopy on field-sensitive Rydberg states. The 780 nm laser is frequency stabilized to the Rb 5S1/2 to 5P3/2 transition, while the 480 nm laser frequency is scanned linearly across a range of 5P3/2 to Rydberg-state transitions.
2:Sample Selection and Data Sources:
The range of states / energy ranges scanned is adapted to the field-strength and frequency ranges of the RF fields to be measured.
3:List of Experimental Equipment and Materials:
A small rubidium vapor cell, two lasers (780 nm and 480 nm), and RF field generation equipment.
4:Experimental Procedures and Operational Workflow:
The transmission peaks of the 780 nm light through the vapor cell serve to locate the energy levels of the RF-field-perturbed Rydberg levels. The RF-field-induced frequency shifts of the Rydberg levels as well as the measured splitting patterns of the spectroscopic lines provide a measure for the RF field strength.
5:Data Analysis Methods:
Floquet theory is used as a non-perturbative method to quantify the atomic response in the high-field regime.
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