Electrometer with radio frequency tuning signal

Patent metadata

Field	Value
Publication number	US-12379406-B2
Application number	US-202318357867-A
Country	US
Kind code	B2
Filing date	Jul 24, 2023
Priority date	Jan 17, 2023
Publication date	Aug 5, 2025
Grant date	Aug 5, 2025

Abstract

One example includes an electrometer system. The system includes a sensor cell comprising alkali metal atoms within, and an optical beam system configured to provide at least one optical beam through the sensor cell to provide a first Rydberg energy state of the alkali metal atoms, the at least one optical beam exiting the sensor cell as a detection beam. The system also includes a radio frequency (RF) tuning field generator configured to generate an RF tuning signal having a tuning frequency that is equal to an energy difference between the first Rydberg energy state and a second Rydberg energy state of the alkali metal atoms. The system further includes a detection system configured to monitor the detection beam to detect an external signal having a frequency that is between the first and second Rydberg energy states.

First claim

What is claimed is:

1. An electrometer system comprising:
a sensor cell comprising alkali metal atoms within;
an optical beam system configured to provide at least one optical beam through the sensor cell to provide a first Rydberg energy state of the alkali metal atoms, the at least one optical beam exiting the sensor cell as a detection beam;
a radio frequency (RF) tuning field generator configured to generate an RF tuning signal having a tuning frequency that is equal to an energy difference between the first Rydberg energy state and a second Rydberg energy state of the alkali metal atoms; and
a detection system configured to monitor the detection beam to detect an external signal having a frequency that is between the first and second Rydberg energy states.

2. The system of claim 1 , wherein the at least one optical beam is provided through the sensor cell along a length of the sensor cell, wherein the tuning frequency has a wavelength that is greater than twice the length of the sensor cell.

3. The system of claim 1 , further comprising a waveguide extending along a length of the sensor cell, the waveguide being configured to propagate the RF tuning signal in the sensor cell.

4. The system of claim 3 , wherein the waveguide extends within the sensor cell from a first end of the sensor cell through the sensor cell to a second end of the sensor cell opposite the first end.

5. The system of claim 1 , wherein the RF tuning field generator is configured to adjust a power of the RF tuning signal, wherein the detection system is configured to determine the frequency of the external signal based on the power of the RF tuning signal.

6. The system of claim 5 , wherein the power of the RF tuning signal is adjusted to relate a detuning of the external signal with respect to the energy difference between the first and second Rydberg energy states to a Rabi frequency of the RF tuning signal.

7. The system of claim 5 , wherein the detection system is configured to determine the frequency of the external signal based on a Hamiltonian matrix associated with the power and frequency of the RF tuning signal.

8. The system of claim 1 , wherein the RF tuning signal generator is configured to provide the tuning frequency of the RF tuning signal equal to the energy difference between the first and second Rydberg energy states of the alkali metal atoms, such that the detection system is configured to detect the external signal having the frequency that is less than the energy difference between the first and second Rydberg energy states, in response to the frequency of the external signal being less than a threshold,
wherein the RF tuning signal generator is configured to provide the tuning frequency of the RF tuning signal equal to the energy difference between the first Rydberg energy state and a third Rydberg energy state of the alkali metal atoms to adjust the energy difference between the first and second Rydberg energy states, such that the detection system is configured to detect the external signal having the frequency that is between the energy difference of the first and second Rydberg energy states, in response to the frequency of the external signal being greater than the threshold.

9. The system of claim 1 , wherein the optical beam system comprises:
a probe laser configured to generate a probe beam directed through the sensor cell in a first direction, the probe beam exiting the sensor cell as the detection beam; and
a coupling laser configured to generate a coupling beam directed through the sensor cell collinearly and anti-parallel with the probe beam to provide the first Rydberg energy state of the alkali metal atoms.

10. The system of claim 9 , further comprising optics configured to collimate the probe beam and the coupling beam to provide the probe beam and the coupling beam to be collinear and anti-parallel with respect to each other, such that the detection system is configured to monitor the detection beam along an axis through the sensor cell to detect the external signal.

11. A method for detecting an external signal via an electrometer system, the method comprising:
directing a probe beam through a sensor cell comprising an alkali metal atoms in a first direction, the probe beam exiting the sensor cell as a detection beam;
directing a coupling beam through the sensor cell to provide a first Rydberg energy state of the alkali metal atoms based on the probe beam and the coupling beam;
providing a radio frequency (RF) tuning signal through the sensor cell, the RF tuning signal having a tuning frequency that is equal to an energy difference between the first Rydberg energy state and a second Rydberg energy state of the alkali metal atoms; and
monitoring the detection beam to detect the external signal having a frequency that is between the first and second Rydberg energy states.

12. The method of claim 11 , wherein the probe and coupling beams are provided through the sensor cell along a length of the sensor cell, wherein the tuning frequency has a wavelength that is greater than twice the length of the sensor cell.

13. The method of claim 11 , wherein the sensor cell comprises a waveguide extending along a length of the sensor cell, the waveguide being configured to propagate the RF tuning signal in the sensor cell.

14. The method of claim 11 , further comprising adjusting a power of the RF tuning signal to relate a detuning of the external signal with respect to the energy difference between the first and second Rydberg energy states to a Rabi frequency of the RF tuning signal, the method further comprising determining the frequency of the external signal based on a Hamiltonian matrix associated with the power and frequency of the RF tuning signal.

15. The method of claim 11 , wherein providing the RF tuning signal comprises:
providing the RF tuning signal having the tuning frequency that is equal to the energy difference between the first Rydberg energy state and the second Rydberg energy state of the alkali metal atoms in response to the frequency of the external signal being less than a threshold; and
providing the RF tuning signal having the tuning frequency that is equal to an energy difference between the first Rydberg energy state and a third Rydberg energy state of the alkali metal atoms to adjust the energy difference between the first and second Rydberg energy states in response to the frequency of the external signal being greater than the threshold.

16. An electrometer system comprising:
a sensor cell comprising alkali metal atoms within;
a probe laser configured to provide a probe beam through the sensor cell in a first direction along a length of the sensor cell, the probe beam exiting the sensor cell as a detection beam;
a coupling laser configured to provide a coupling beam through the sensor cell to provide a first Rydberg energy state of the alkali metal atoms based on the probe beam and the coupling beam;
a radio frequency (RF) tuning field generator configured to generate an RF tuning signal having a tuning frequency that is equal to an energy difference between the first Rydberg energy state and a second Rydberg energy state of the alkali metal atoms and has a wavelength that is greater than twice the length of the sensor cell; and
a detection system configured to monitor the detection beam to detect an external signal having a frequency that is between the first and second Rydberg energy states.

17. The system of claim 16 , further comprising a waveguide extending along the length of the sensor cell, the waveguide being configured to propa

Assignees

• Northrop Grumman Systems Corp

Inventors

• Imhof Eric A
• Jefferts Steven Ryan

Classifications

• G01R29/14 Primary

  Measuring field distribution · CPC title

• G01R29/0885 Primary

  using optical probes, e.g. electro-optical, luminescent, glow discharge, or optical interferometers · CPC title