Radio-frequency receiver pumped to high-azimuthal rydberg states
A radio-frequency receiver achieves high sensitivity by pumping atoms to high-azimuthal ( ≥3) Rydberg states. A vapor cell contains quantum particles (e.g., cesium atoms). A laser system provides probe, dressing, and coupling beams to pump the quantum particles to a first Rydberg state having a high-azimuthal quantum number ≥3. A local oscillator drives an electric field in the vapor cell at a local oscillator frequency, which is imposed on a distribution of quantum particles between the first Rydberg state and a second Rydberg state. An incident RF signal field interferes with the local oscillator field, imposing an oscillation in the distribution at a beat or difference frequency and, consequently, on the intensity of the probe beam. The beat frequency component of the intensity of the probe beam is detected, and the detection signal is demodulated to extract information originally in the RF signal.
1. A radio-frequency receiver comprising:
a vapor cell containing a vapor of quantum particles;
a laser system for pumping the quantum particles to a first Rydberg state, the first Rydberg state being a high-azimuthal Rydberg state with an azimuthal quantum number ≥3, the laser system including a probe laser for transmitting a probe beam through the vapor cell;
an electric field controlling for controlling an electric field within the vapor cell so that a distribution between the first Rydberg state and a second Rydberg state and an intensity of the probe beam vary at a local oscillator frequency ν LO , and so that an incident RF signal having an RF frequency of ν RF interferes to yield a beat frequency Δ RF that is imposed on the distribution between the first Rydberg state and the second Rydberg state and on the intensity of the probe beam;
a photodetector for producing a photodetector signal that tracks the intensity of the probe beam; and
a signal processor for decoding the photodetector signal.
2. The radio-frequency receiver of claim 1 wherein the laser system also includes a coupling laser and at least one dressing laser, the probe laser, the dressing laser and the coupling laser cooperating to pump the quantum particles to the first Rydberg state.
3. The radio-frequency receiver of claim 1 wherein the second Rydberg state is a high-azimuthal Rydberg state with an azimuthal quantum number ≥4.
4. The radio-frequency receiver of claim 1 wherein the second Rydberg state is a low-azimuthal Rydberg state with an azimuthal quantum number ≤2.
5. A radio-frequency receiver process comprising:
selecting a target radio-frequency (RF) frequency ν RF ;
pumping quantum particles to a first Rydberg state, the first Rydberg state being a high-azimuthal Rydberg state with an azimuthal quantum number ≥3, the pumping including exciting the quantum particles with a probe beam;
generating an oscillating electric field having a local oscillator frequency ν LO =ν RF ±Δ RF , wherein Δ RF is a beat frequency resulting from mixing a target radio frequency with the local oscillator frequency, a distribution of the quantum particles between the first Rydberg state and a second Rydberg state and an intensity of the probe beam oscillating at the local oscillator frequency ν LO ;
receiving an RF signal having the target RF frequency ν RF so as to produce the beat frequency Δ RF in the distribution of the quantum particles between the first and second Rydberg states and also in intensity oscillations of the probe beam;
detecting the intensity oscillations in the probe beam so as to produce a detection signal; and
decoding the RF signal by processing the detection signal.
6. The radio-frequency receiver process of claim 5 wherein the pumping also includes using a dressing beam to transition quantum particles from an excited state to a dressed state and using a coupling beam to transition quantum particles from the excited state or another dressed state to the first Rydberg state.
7. The radio-frequency receiver process of claim 5 wherein the second Rydberg state is a high-azimuthal Rydberg state with an azimuthal quantum number ≥4.
8. The radio-frequency receiver process of claim 5 wherein the second Rydberg state is a low-azimuthal Rydberg state with an azimuthal quantum number ≤2.