Granted Patent B2

US 12,267,103 · App. 18/005,318 · Granted Apr 1, 2025

Inventors: Fraser Burton (London, GB); Liam Bussey (London, GB)

Assignee: British Telecommunications Public Limited Company

H04B10/073G01R29/0885H04B1/16H04B2210/006

Abstract

Claims (28)

1. A method of controlling an electromagnetic field detector comprising a first optical transmitter and a second optical transmitter, a transmission medium, and an optical receiver, wherein the first optical transmitter is configured to transmit a probe signal to the optical receiver via the transmission medium at a probe frequency and the second transmitter is configured to transmit a coupling signal via the transmission medium at a coupling frequency, wherein the probe frequency is set to excite electrons of the transmission medium from a ground state to a first excited state and the coupling frequency is set to excite electrons of the transmission medium to a predetermined excited state so as to induce an Electromagnetic Induced Transparency (EIT) effect in the electromagnetic field detector such that an incident electromagnetic field at the transmission medium causes a detectable change in power of the probe signal at the optical receiver, the method comprising:

varying one or both of an intensity value and the coupling frequency of the coupling signal so as to cause a variation in the change in power of the probe signal at the optical receiver due to the incident electromagnetic field at the transmission medium;

monitoring the variation in the change in power of the probe signal due to the incident electromagnetic field at the transmission medium; and

based on the monitoring of the variation in the change in power of the probe signal, setting at least one of the intensity value or the coupling frequency of the coupling signal so as to increase the change in power of the probe signal.

2. The method as claimed in claim 1 , wherein a variation in the coupling frequency causes a greater variation in the change in power of the probe signal at the optical receiver than a variation in the intensity value, and the method further comprises:

varying the coupling frequency of the coupling signal so as to cause the variation in the change in power of the probe signal at the optical receiver due to the incident electromagnetic field at the transmission medium;

monitoring the variation in the change in power of the probe signal due to the incident electromagnetic field at the transmission medium in response to the variation of the coupling frequency;

based on the monitoring of the variation in the change in power of the probe signal in response to the variation of the coupling frequency, setting the coupling frequency of the coupling signal so as to increase the change in power of the probe signal; and then,

varying the intensity value of the coupling signal so as to cause the variation in the change in power of the probe signal at the optical receiver due to the incident electromagnetic field at the transmission medium;

monitoring the variation in the change in power of the probe signal due to the incident electromagnetic field at the transmission medium in response to the variation of the intensity value; and

based on the monitoring of the variation in the change in power of the probe signal in response to the variation of the intensity value, setting the intensity value of the coupling signal so as to increase the change in power of the probe signal.

3. The method as claimed in claim 1 , wherein a variation in the intensity value causes a greater variation in the change in power of the probe signal at the optical receiver than a variation in the coupling frequency, and the method further comprises:

varying the intensity value of the coupling signal so as to cause the variation in the change in power of the probe signal at the optical receiver due to the incident electromagnetic field at the transmission medium;

monitoring the variation in the change in power of the probe signal due to the incident electromagnetic field at the transmission medium in response to the variation of the intensity value;

based on the monitoring of the variation in the change in power of the probe signal in response to the variation of the intensity value, setting the intensity value of the coupling signal so as to increase the change in power of the probe signal; and then,

varying the coupling frequency of the coupling signal so as to cause the variation in the change in power of the probe signal at the optical receiver due to the incident electromagnetic field at the transmission medium;

monitoring the variation in the change in power of the probe signal due to the incident electromagnetic field at the transmission medium in response to the variation of the coupling frequency; and

based on the monitoring of the variation in the change in power of the probe signal in response to the variation of the coupling frequency, setting the coupling frequency of the coupling signal so as to increase the change in power of the probe signal.

4. The method as claimed in claim 1 , wherein varying the intensity value or the coupling frequency of the coupling signal, monitoring the variation in the change in power of the probe signal, and setting the coupling frequency based on the monitoring of the variation in the change in power of the probe signal are performed iteratively until a termination condition is met.

5. The method as claimed in claim 4 , wherein the termination condition is that the power of the probe signal following the change in power of the probe signal is less than or equal to the power of the probe signal before the change in power of the probe signal.

6. The method as claimed in claim 1 , wherein the transmission medium includes a metal vapor.

7. The method as claimed in claim 6 , wherein the metal vapor is of an alkali metal.

8. The method as claimed in claim 7 , wherein the alkali metal vapor is one of: Rubidium, Cesium or Strontium.

9. The method as claimed in claim 1 , wherein the electromagnetic field is a Radio Frequency (RF) field and the electromagnetic field detector is an RF detector.

10. An electromagnetic field detector controller comprising a processor configured to implement the method of claim 1 .

11. A system comprising an electromagnetic field detector and the electromagnetic field detector controller as claimed in claim 10 .

12. A non-transitory computer-readable storage medium storing a computer program product comprising instructions that, when executed by a computer, cause the computer to carry out the method of claim 1 .

13. A system comprising at least one processor and memory configured to carry out the method of claim 1 .

Assignments (1)

Priority Claims (1)

Continuity (1)

References Cited (140)