IP Library › Granted Patent US 10,763,966
Granted Patent B1
US 10,763,966 · App. 16/363,965 · Granted Sep 1, 2020

Data communications system using an optical antenna

Inventors: Amita Bikram Deb (Dunedin, NZ); Niels Kjaergaard (Dunedin, NZ)
Assignee: Otago Innovation Limited
H04B10/25759
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Quick Facts
Patent No.
US 10,763,966
App. No.
16/363,965
Granted
Sep 1, 2020
Kind
B1
Abstract

In one embodiment, there is provided an apparatus for converting an analogue radio-frequency (RF) signal to an optical signal. The apparatus may include: a vapor cell enclosing a gas of atoms; a probing light source configured to propagate a probing light beam through the vapor cell, a frequency of the probing light beam being tuned across a range in which the atoms transition from a first quantum state to a second quantum state; and, a coupling light source configured to propagate a coupling light beam through the vapor cell, a frequency of the coupling light beam being resonant or off-resonant with transition of the atoms from the second quantum state to a Rydberg state; wherein the vapor cell is configured such that on exposure thereof to an RF field carrying information from the RF signal, the apparatus is configured to encode the RF signal into the probing light beam.

Claims (29)

1. A system for a radio-over-fiber (RoF) information linkage, the system comprising:

a vapor cell enclosing a gas of atoms, the vapor cell configured to be coupled to an information signal source via an RF field, the information signal source configured to generate an information signal of a data transfer protocol, wherein the RF field is a carrier frequency modulated by the information signal;

a probing light source configured to propagate a probing light beam through the vapor cell, a frequency of the probing light beam being fixed within a range in which the atoms transition from a first quantum state to a second quantum state; and,

a coupling light source configured to propagate a coupling light beam through the vapor cell, a frequency of the coupling light beam being either resonant or off-resonant with transition of the atoms from the second quantum state to a Rydberg state;

wherein the vapor cell is configured such that on exposure thereof to the RF field that is the carrier frequency modulated by the information signal, the system is configured to encode the information signal into the probing light beam,

wherein the probing light source is configured to couple the probing light beam to an optical fiber after the probing light beam passes through the vapor cell, wherein the optical fiber is configured to carry the probing light beam to a remote optical detector.

2. The system of claim 1 , wherein the system is configured to encode the information signal into the probing light beam by modulating an amplitude and/or a phase of the probing light beam.

3. The system of claim 1 , wherein the gas of atoms comprises one or more of: atoms from alkali metals; atoms from alkaline metals; rubidium atoms; and, potassium atoms.

4. The system of claim 1 , wherein the vapor cell is configured such that on exposure thereof to a different RF field carrying information from a different RF signal, the apparatus is configured to encode the different RF signal into the probing light beam using a different Rydberg state without reconfiguring the apparatus.

5. The system of claim 1 , wherein the probing and coupling light sources each comprise a laser configured to generate the probing and coupling light beams respectively, and wherein the probing and/or coupling light beam(s) is/are derived from external cavity diode lasers.

6. The system of claim 5 , wherein a wavelength of the probing light beam is about 780 nm and/or a wavelength of the coupling light beam is about 480 nm.

7. The system of claim 1 , further comprising thermal control elements configured to stabilize the gas or vapor cell at a desired temperature.

8. The system of claim 1 , wherein the gas or vapor cell comprises a housing having a first end and a second end, and the probing light beam passes through the housing from the first end to the second end along a first axis.

9. The system of claim 8 , wherein the coupling light beam is counterpropagating to the probing light means.

10. The system of claim 8 , further comprising a retro-reflector configured to re-propagate the probing light beam through the gas or vapor cell such that the probing light beam passes through the gas or vapor cell from the second end to the first end along a second axis.

11. The system of claim 10 , wherein the second axis is the same or substantially the same as the first axis; or is parallel and/or axially separated from the first axis.

12. The system of claim 10 , wherein the retro-reflector comprises a corner cube or a confocal or afocal retro-reflector.

13. The system of claim 12 , wherein the confocal or afocal retroreflector comprises one or more index mismatched surfaces, the one or more index mismatched surfaces comprising non-flat surfaces being aspherical, near-spherical or spherical concave surfaces.

14. A communications system for an RF-to-optical information linkage, the communications system comprising:

a signal source configured to generate an information signal of a data transfer protocol;

an RF source to generate and transmit an RF field, wherein the information signal of the data transfer protocol is encoded in the RF field in the form of a modulation;

an optical antenna comprising:

a vapor cell enclosing a gas of atoms;

a probing light source configured to propagate a probing light beam through the vapor cell, a frequency of the probing light beam being fixed within a range in which the atoms transition from a first quantum state to a second quantum state; and,

a coupling light source configured to propagate a coupling light beam through the vapor cell, a frequency of the coupling light beam being either resonant or off-resonant with transition of the atoms from the second quantum state to a Rydberg state;

wherein the vapor cell is configured such that on exposure thereof to the RF field, the apparatus is configured to encode the information signal from the RF field into the probing light beam;

wherein the probing light beam encoded with the information signal is configured to be coupled through free space to an optical detector at a remote location.

15. The communications system of claim 14 , wherein the apparatus is configured to encode the information signal into the probing light beam by modulating an amplitude and/or a phase of the probing light beam.

16. The communications system of claim 14 , wherein the vapor cell is configured such that on exposure thereof to a different RF field carrying information from a different RF signal, the apparatus is configured to encode the different RF signal into the probing light beam using a different Rydberg state without reconfiguring the apparatus.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 6, 2019
From: DEB, AMITA BIKRAM; KJAERGAARD, NIELS
To: UNIVERSITY OF OTAGO
Reel/Frame 049092/0662 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 6, 2019
From: UNIVERSITY OF OTAGO
To: OTAGO INNOVATION LIMITED
Reel/Frame 049092/0955 →
Cited By (12)
US 12,248,011 US 12,250,025 US 12,267,103 US 12,289,135 US 12,376,216 US 12,399,205 US 12,401,424 US 12,411,162 US 12,449,458 US 12,482,346 US 12,607,661 US 12,656,383