Local oscillator port embedded field enhancement resonator for Rydberg atomic heterodyne technique

Abstract

Rydberg atom-based sensors using the atomic heterodyne technique demonstrate prominent performance on sensing sensitivity and thus have significant potential for radar, electronic reconnaissance, and communication applications. Here, we propose a local oscillator (LO) embedded field enhancement resonator to improve the sensitivity and integration of Rydberg atomic heterodyne sensors. In this approach, a vapor cell filled with cesium atoms is placed into the resonance structure for electric (E) field measurements. By integrating parallel-plate waveguide (PPWG) antennas and the resonator, the LO signal can be directly guided to the resonator using coaxial cable instead of the use of external antennas radiating through free space, allowing for a more flexible and practical Rydberg atom-based heterodyne technique. Based on the off-resonant Rydberg atomic heterodyne approach, for a radio frequency (RF) signal at 638 MHz, it is found that the sensitivity is 43 μV/cm$\sqrt{\text{Hz}}$ Hz in the absence of the resonator, while in the presence of our resonator, the sensitivity is down to 854.36 nV/cm$\sqrt{\text{Hz}}$ Hz , indicating 50 times or 34 dB improvement capacity of the proposed resonator. This type of enhancement resonator is expected to benefit Rydberg atomic heterodyne applications in practical environments.

Eliminating sensing blind spots of field-enhanced Rydberg atomic antenna via an asymmetric parallel-plate resonator

“…We utilize cesium 50S 1/2 m j = 1/2 state EIT to detect about 2 GHz microwave field. Because α 0 (ω RF ) polarizability only factor to effect the electric field in the far off-resonant of the Stark shift regime, we have not used 50D state EIT [32], where different m j = 1/2, 3/2, 5/2 have different polarizability [33]. We use a numerical Floquet theory [34] to calculate the |50S 1/2 ⟩ Rydberg α 0 = 53.7 MHz • cm 2 /V 2 by fitting a quadratic relationship of the AC shift of the 50S 1/2 level at an microwave frequency of 2 GHz as shown in Fig.…”