IP Library › Granted Patent US 12,289,135
Granted Patent B2
US 12,289,135 · App. 18/863,938 · Granted Apr 29, 2025

Electromagnetic field detector

Inventors: Liam Bussey (London, GB); Amelia Lees (London, GB); Fraser Burton (London, GB); Marco Menchetti (London, GB); Timothy Whitley (London, GB)
Assignee: BRITISH TELECOMMUNICATIONS PUBLIC LIMITED COMPANY
H04B10/70G01R29/0885H04B10/60H04B2210/006
View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 12,289,135
App. No.
18/863,938
Granted
Apr 29, 2025
Kind
B2
Abstract

This invention provides a method of detecting a photon in a first frequency range, the method comprising the steps of: exciting a first transmission medium by a first probe signal at a first probe frequency, wherein the first probe signal excites electrons of the first transmission medium from a ground state of the first transmission medium to a first excited state of the first transmission medium; exciting the first transmission medium by a first coupling signal at a first coupling frequency, wherein the first coupling signal overlaps with the first probe signal in the first transmission medium and excites electrons of the first transmission medium to a predetermined excited state of the first transmission medium such that a first photon in the first frequency range and having a first polarisation incident upon the first transmission medium excites an electron in the predetermined excited state of the first transmission medium to a further excited state of the first transmission medium, wherein a first photon in a second frequency range is emitted as part of a subsequent deexcitation of the electron from the further excited state of the first transmission medium; detecting the first photon in the first frequency range and having the first polarisation by detecting the first photon in the second frequency range; exciting a second transmission medium by a second probe signal at a second probe frequency, wherein the second probe signal excites electrons of the second transmission medium from a ground state of the second transmission medium to a first excited state of the second transmission medium; exciting the second transmission medium by a second coupling signal at a second coupling frequency, wherein the second coupling signal overlaps with the second probe signal in the second transmission medium and excites electrons of the second transmission medium to a predetermined excited state of the second transmission medium such that a second photon in the first frequency range incident upon the second transmission medium and having a second polarisation excites an electron in the predetermined excited state of the second transmission medium to a further excited state of the second transmission medium, wherein a second photon in the second frequency range is emitted as part of a subsequent deexcitation of the electron in the further excited state of the second transmission medium; and detecting the second photon in the first frequency range having the second polarisation by detecting the second photon in the second frequency range. This invention also provides a detector and system for implementing said method.

Claims (31)

1. A method of detecting a photon in a first frequency range, the method comprising the steps of:

exciting a first transmission medium by a first probe signal at a first probe frequency, wherein the first probe signal excites electrons of the first transmission medium from a ground state of the first transmission medium to a first excited state of the first transmission medium;

exciting the first transmission medium by a first coupling signal at a first coupling frequency, wherein the first coupling signal overlaps with the first probe signal in the first transmission medium and excites the electrons of the first transmission medium to a predetermined excited state of the first transmission medium such that a first photon in the first frequency range and having a first polarisation incident upon the first transmission medium excites an electron in the predetermined excited state of the first transmission medium to a further excited state of the first transmission medium, wherein a first photon in a second frequency range is emitted as part of a subsequent deexcitation of the electron from the further excited state of the first transmission medium;

detecting the first photon in the first frequency range and having the first polarisation by detecting the first photon in the second frequency range;

exciting a second transmission medium by a second probe signal at a second probe frequency, wherein the second probe signal excites electrons of the second transmission medium from a ground state of the second transmission medium to a first excited state of the second transmission medium;

exciting the second transmission medium by a second coupling signal at a second coupling frequency, wherein the second coupling signal overlaps with the second probe signal in the second transmission medium and excites the electrons of the second transmission medium to a predetermined excited state of the second transmission medium such that a second photon in the first frequency range incident upon the second transmission medium and having a second polarisation excites an electron in the predetermined excited state of the second transmission medium to a further excited state of the second transmission medium, wherein a second photon in the second frequency range is emitted as part of a subsequent deexcitation of the electron in the further excited state of the second transmission medium; and

detecting the second photon in the first frequency range having the second polarisation by detecting the second photon in the second frequency range.

2. The method as claimed in claim 1 , wherein the method further comprises the steps of:

demodulating data based on detection of the first photon in the first frequency range having the first polarisation corresponding to a first bit value, and detection of the second photon in the first frequency range having the second polarisation corresponding to a second bit value.

3. The method as claimed in claim 2 , further comprising the step of:

determining a cryptographic key based on the demodulated data.

4. The method as claimed in claim 1 , wherein the first frequency range is lower than the second frequency range.

5. The method as claimed in claim 1 , wherein the first frequency range is in the Radio Frequency (RF), microwave or infrared ranges of the electromagnetic spectrum.

6. A non-transitory computer readable carrier medium storing a computer program, which upon execution by a computer, causes the steps of the method of claim 1 to be performed.

7. A device for detecting a photon in a first frequency range, the detector comprising:

a first transmission medium excitable by a first probe signal at a first probe frequency and an overlapping first coupling signal at a first coupling frequency, wherein the first probe frequency excites electrons of the first transmission medium from a ground state of the first transmission medium to a first excited state of the first transmission medium and the first coupling frequency excites the electrons of the first transmission medium to a predetermined excited state of the first transmission medium such that a first photon in a first frequency range and having a first polarisation incident upon the first transmission medium excites an electron in the predetermined excited state of the first transmission medium to a further excited state of the first transmission medium, wherein a first photon in a second frequency range is emitted as part of a subsequent deexcitation of the electron in the further excited state of the first transmission medium;

a first detector configured to detect the first photon in the first frequency range having the first polarisation by detecting the first photon in the second frequency range;

a second transmission medium excitable by a second probe signal at a second probe frequency and an overlapping second coupling signal at a second coupling frequency, wherein the second probe frequency excites electrons of the second transmission medium from a ground state of the second transmission medium to a first excited state of the second transmission medium, wherein the second coupling frequency excites the electrons of the second transmission medium to a predetermined excited state of the second transmission medium such that a second photon in the first frequency range having a second polarisation incident upon the second transmission medium excites an electron in the predetermined excited state of the second transmission medium to a further excited state of the second transmission medium, wherein a second photon in the second frequency range is emitted as part of a subsequent deexcitation of the electron in the further excited state of the second transmission medium; and

a second detector configured to detect the second photon in the first frequency range having the second polarisation by detecting the second photon in the second frequency range.

8. The device as claimed in claim 7 , further comprising:

a housing configured to permit passage of the first photon in the first frequency range to the first transmission medium when arriving in a predetermined direction.

9. The device as claimed in claim 7 , further comprising:

a processor configured to demodulate data based on detection of the first photon in the first frequency range having the first polarisation corresponding to a first bit value and detection of the second photon in the first frequency range having the second polarisation corresponding to a second bit value.

10. The device as claimed in claim 9 , wherein the processor is further configured to determine a cryptographic key based on the demodulated data.

11. The device as claimed in claim 7 , wherein the first frequency range is lower than the second frequency range.

12. The device as claimed in claim 7 , wherein the first frequency range is in the Radio Frequency (RF), microwave or infrared ranges of the electromagnetic spectrum.

13. A system comprising:

a first transmission medium excitable by a first probe signal at a first probe frequency and an overlapping first coupling signal at a first coupling frequency, wherein the first probe frequency excites electrons of the first transmission medium from a ground state of the first transmission medium to a first excited state of the first transmission medium and the first coupling frequency excites the electrons of the first transmission medium to a predetermined excited state of the first transmission medium such that a first photon in a first frequency range and having a first polarisation incident upon the first transmission medium excites an electron in the predetermined excited state of the first transmission medium to a further excited state of the first transmission medium, wherein a first photon in a second frequency range is emitted as part of a subsequent deexcitation of the electron in the further excited state of the first transmission medium;

a first detector configured to detect the first photon in the first frequency range and having the first polarisation by detecting the first photon in the second frequency range;

a second transmission medium excitable by a second probe signal at a second probe frequency and an overlapping second coupling signal at a second coupling frequency, wherein the second probe frequency excites electrons of the second transmission medium from a ground state of the second transmission medium to a first excited state of the second transmission medium, wherein the second coupling frequency excites the electrons of the second transmission medium to a predetermined excited state of the second transmission medium such that a second photon in the first frequency range and having a second polarisation incident upon the second transmission medium excites an electron in the predetermined excited state of the second transmission medium to a further excited state of the second transmission medium, wherein a second photon in the second frequency range is emitted as part of a subsequent deexcitation of the electron in the further excited state of the second transmission medium; and

a second detector configured to detect the second photon in the first frequency range and having the second polarisation by detecting the second photon in the second frequency range.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Nov 7, 2024
From: BUSSEY, LIAM; LEES, AMELIA; BURTON, FRASER; MENCHETTI, MARCO; WHITLEY, TIMOTHY
To: BRITISH TELECOMMUNICATIONS PUBLIC LIMITED COMPANY
Reel/Frame 069188/0926 →
Priority Claims (1)
EP 22173349 · May 13, 2022 · regional
Continuity (1)
Related Publication 20250112709A1 · Apr 3, 2025
References Cited (32)
US 4024396A · Hill et al. · 1977 [cited by applicant]
US 10256917B2 · Dolgin · 2019 [cited by examiner]
US 10763966B1 · Deb · 2020 [cited by examiner]
US 11349569B2 · Graceffo · 2022 [cited by examiner]
US 12028111B1 · Bussey · 2024 [cited by examiner]
US 20140210473A1 · Campbell · 2014 [cited by examiner]
US 20150042327A1 · Bulatowicz · 2015 [cited by examiner]
US 20220196716A1 · Anderson · 2022 [cited by examiner]
US 20220196719A1 · Walker · 2022 [cited by examiner]
US 20220294619A1 · Menchetti · 2022 [cited by examiner]
US 20230261743A1 · Burton · 2023 [cited by examiner]
US 20240094275A1 · Burton · 2024 [cited by examiner]
CN 110401492A · 2019 [cited by examiner]
CN 111490825A · 2020 [cited by applicant]
CN 112867934A · 2021 [cited by applicant]
CN 110231332B · 2022 [cited by examiner]
GB 2588754 · 2021 [cited by applicant]
GB 2588754A · 2021 [cited by examiner]
WO WO2020192153A1 · 2020 [cited by examiner]
Nina et al; Controlled multi-photon subtraction with cascaded Rydberg super atoms as single-photon absorbers; 2021; pp. 1-8. (Year: 2021). [cited by examiner]
International Preliminary Report on Patentability dated Nov. 28, 2024, issued for International Application No. PCT/EP2023/059390 (7 pages). [cited by applicant]
International Search Report and Written Opinion of the ISA for PCT/EP2023/059390 dated Jul. 18, 2023, 12 pages. [cited by applicant]
Extended European Search Report for Application No. 22173349.6 dated Nov. 16, 2022, 11 pages. [cited by applicant]
Combined Search Report and Abbreviated Examination Report for GB Application No. 2207032.0 dated Nov. 11, 2022, 6 pages. [cited by applicant]
Intention to Grant under Section 18(4) for GB Application No. 2207032.0 dated Feb. 21, 2024, 2 pages. [cited by applicant]
Adams C S et al., “Rydberg atom quantum technologies”, Journal of Physics B, Atomic Molecular and Optical Physics, vol. 53, No. 1, 2019, 24 pages. [cited by applicant]
J. Sedlacek et al., “Atom Based Vector Microwave Electrometry Using Rubidium Rydberg Atoms in a Vapor Cell”, ResearchGate, University of Oklahoma, Apr. 15, 2013, 6 pages. [cited by applicant]
Christopher L. Holloway et al., “Detecting and Receiving Phase-Modulated Signals With a Rydberg Atom-Based Receiver”, IEEE Antennas and Wireless Propagation Letters, vol. 18, No. 9, Sep. 2019, 5 pages. [cited by applicant]
Philippe Torchio et al., “High-reflectivity HfO2/SiO2 ultraviolet mirrors”, Applied Optics, vol. 41, No. 16, Jun. 1, 2002, 7 pages. [cited by applicant]
Lucy A. Downes et al., “Ultra-high-speed Terahertz Imaging using Atomic Vapour”, Durham University, Mar. 18, 2019, 9 pages. [cited by applicant]
Hamamatsu, Photomultiplier tubes (PMTs) dated Oct. 19, 2021 (4 pages). [cited by applicant]
First Notification of Office Action dated Jan. 17, 2025, issued for Chinese Application No. 202380037718.5 (9 pages). [cited by applicant]