Granted Patent B1

US 12,416,716 · App. 19/075,343 · Granted Sep 16, 2025

Inventors: Stephanie M. Bohaichuk (Waterloo, CA); Vijin Venu (Waterloo, CA); Florian Christaller (Waterloo, CA); Chang Liu (Waterloo, CA); James P. Shaffer (Kitchener, CA)

Assignee: Quantum Valley Ideas Laboratories

G01S13/582G01S7/282G01S7/285G01S13/524

Abstract

Claims (134)

1. A radar method, comprising:

by operation of a transmitter system, transmitting an outgoing series of radio frequency (RF) pulses toward a target region, the outgoing series of RF pulses having a reference phase modulation;

by operation of a receiver system, receiving an incoming series of RF pulses that is based on the outgoing series of RF pulses after passing through the target region, wherein receiving the incoming series of RF pulses comprises:

interacting the incoming series of RF pulses with a vapor of a vapor cell system, the vapor cell system part of the receiver system, and

interacting laser signals with the vapor;

by operation of the vapor cell system, producing output signals that are based on incoming series of RF pulses and the laser signals interacting with the vapor; and

by operation of a signal processing system of the receiver system:

generating, based on the output signals, response data that represents a response of the vapor to the laser signals and the incoming series of RF pulses, the response data comprising transient response data that represents one or more transient responses of the vapor to respective phase changes in the incoming series of RF pulses, the respective phase changes based on the reference phase modulation of the outgoing series of RF pulses, and

determining, based on the transient response data, a Doppler shift in the incoming series of RF pulses, the Doppler shift resulting from the outgoing series of RF pulses interacting with an object in the target region, and

determining a velocity of the object based on the Doppler shift.

2. The radar method of claim 1 ,

wherein the phase changes in the incoming series of RF pulses comprise first and second phase changes, the first phase change occurring before the second phase change;

wherein the transient response data comprises:

a first subset of transient response data that represents a first transient response of the vapor to the first phase change, and

a second subset of transient response data that represents a second transient response of the vapor to the second phase change; and

wherein determining the Doppler shift comprises:

generating first and second values based on, respectively, the first and second subsets of transient response data, the first value representing a degree to which the vapor responds to the first phase change, the second value representing a degree to which the vapor responds to the second phase change, and

calculating a difference between the first and second values, the difference representing a detuning of the incoming series of RF pulses relative to a Rydberg electronic transition of the vapor.

3. The radar method of claim 2 , wherein determining the velocity of the object comprises:

determining a magnitude of the velocity based on a magnitude of the difference between the first and second values; and

determining a direction of the velocity based on a sign of the difference, the direction determined relative to an incoming direction along which the incoming series of RF pulses travels to reach the receiver system.

4. The radar method of claim 1 , wherein the reference phase modulation defines a pattern of phase changes in each of the outgoing series of RF pulses, the pattern of phase changes common to all RF pulses in the outgoing series.

5. The radar method of claim 4 , wherein the pattern of phase changes comprises a pair of phase changes that are equal in magnitude but opposite in sign, the pair of phase changes repeating successively to define the pattern of phase changes.

6. The radar method of claim 1 ,

wherein the incoming series of RF pulses each have a leading pulse edge; and

wherein the one or more transient responses of the vapor occur at respective leading pulse edges of the incoming series of RF pulses.

7. The radar method of claim 1 ,

wherein the outgoing series of RF pulses have a reference amplitude modulation;

wherein the response data comprises steady-state response data that represents one or more steady-state responses of the vapor to respective amplitude changes in the incoming series of RF pulses, the respective amplitude changes based on the reference amplitude modulation of the outgoing series of RF pulses; and

wherein the Doppler shift is determined based on the transient response data and the steady-state response data.

8. The radar method of claim 7 ,

wherein the incoming series of RF pulses each have a trailing pulse edge; and

wherein the one or more steady-state responses of the vapor occur at respective trailing pulse edges of the incoming series of RF pulses.

9. The radar method of claim 1 ,

wherein a laser system of the vapor cell system generates the laser signals, and the laser signals comprise a tunable laser signal;

wherein the radar method comprises:

by operation of the signal processing system, transmitting a control signal to the laser system to alter a frequency of the tunable laser signal from an on-resonance frequency, where the tunable laser signal is on-resonance with an optical electronic transition of the vapor, to a detuned frequency, where the tunable laser signal is detuned relative to the optical electronic transition of the vapor; and

wherein the generating the response data comprises:

generating the transient response data when the tunable laser signal is at the on-resonance frequency, and

generating detuned transient response data when the tunable laser signal is at the detuned frequency.

10. The radar method of claim 9 ,

wherein the tunable laser signal is a first tunable laser signal, the detuned frequency is a first detuned frequency, and the control signal is a first control signal;

wherein the laser signals comprise a second tunable laser signal;

wherein the radar method comprises:

by operation of the signal processing system, transmitting a second control signal to the laser system to alter a frequency of the second tunable laser signal from the on-resonance frequency, where the second tunable laser signal is on-resonance with the optical electronic transition of the vapor, to a second detuned frequency, wherein the second tunable laser signal is detuned relative to the optical electronic transition of the vapor; and

wherein the detuned transient response data is generated when the first and second tunable laser signals are at, respectively, the first and second detuned frequencies.

11. The radar method of claim 10 ,

wherein a first difference between the first detuned frequency and the on-resonance frequency defines a first detuning of the first tunable laser signal;

wherein a second difference between the second detuned frequency and the on-resonance frequency defines a second detuning of the second tunable laser signal; and

wherein the first and second detunings are equal in magnitude but opposite in sign to symmetrically detune the first and second tunable laser signals about the optical electronic transition of the vapor.

12. The radar method of claim 1 ,

wherein the outgoing series of RF pulses share a pulse period in common; and

wherein determining the Doppler shift comprises:

generating a sampled portion of response data by sampling the response data over a sampling period that is based on one or more of the pulse periods,

comparing the sampled portion of response data to each of a plurality of response templates to determine respective degrees of fit, each response template having template data that represents a known response of the vapor to one or more reference RF pulses, the one or more reference RF pulses different for each response template,

selecting one of the response templates based on its degree of fit, and

determining the Doppler shift based on the sampled portion of response data and the template data of the selected response template.

13. The radar method of claim 1 ,

wherein each of the outgoing series of RF pulses is divided into a sequence of sub-pulses that have respective phases, the respective phases defined by the reference phase modulation according to a pulse compression protocol; and

wherein the velocity of the object is determined based on the Doppler shift and respective arrival times of one or more target RF pulses in the incoming series of RF pulses.

14. The radar method of claim 13 , comprising:

by operation of the signal processing system:

generating, based on the transient response data over time, correlation values for a target RF pulse in the incoming series of RF pulses, wherein:

the target RF pulse is divided into a sequence of target sub-pulses that have respective target phases,

the correlation values represent a correlation of the target sub-pulses, in time, with one or more reference sub-pulses of a reference RF pulse, and

the one or more reference sub-pulses have respective reference phases that are defined by the reference phase modulation according to the pulse compression protocol; and

determining an arrival time of the target RF pulse based on the correlation values.

15. The radar method of claim 14 , comprising:

assigning, by operation of the signal processing system and based on the transient response data, respective symbols to the target sub-pulses of the target RF pulse, the respective symbols being part of the pulse compression protocol;

wherein the one or more reference sub-pulses are associated with respective symbols of the pulse compression protocol.

16. The radar method of claim 1 , comprising:

by operation of the signal processing system, determining a distance of the object from the receiver system based on the response data.

17. The radar method of claim 1 ,

wherein the vapor cell system comprises a laser system and an optical detector; and

wherein producing the output signals comprises:

generating the laser signals by operation of the laser system,

generating, by operation of the vapor, optical signals in response to the laser signals interacting with the vapor, the vapor having a Rydberg electronic transition that interacts with the incoming series of RF pulses, the optical signals based on a transmission of one of the laser signals through the vapor, and

generating, by operation of the optical detector, the output signals in response to receiving the optical signals at the optical detector, the output signals representing respective intensities of the optical signals.

18. A signal processing method, comprising:

receiving output signals from a vapor cell system, the output signals based on laser signals and an incoming series of radio frequency (RF) pulses interacting with a vapor of the vapor cell system, the incoming series of RF signals received from a target region and based on an outgoing series of RF pulses that have a reference phase modulation;

generating, based on the output signals, response data that represents a response of the vapor to the laser signals and the incoming series of RF pulses, the response data comprising transient response data that represents one or more transient responses of the vapor to respective phase changes in the incoming series of RF pulses, the respective phase changes based on the reference phase modulation of the outgoing series of RF pulses;

determining, based on the transient response data, a Doppler shift in the incoming series of RF pulses, the Doppler shift resulting from the outgoing series of RF pulses interacting with an object in the target region; and

determining a velocity of the object based on the Doppler shift.

19. The signal processing method of claim 18 ,

wherein the phase changes in the incoming series of RF pulses comprise first and second phase changes, the first phase change occurring before the second phase change;

wherein the transient response data comprises:

a first subset of transient response data that represents a first transient response of the vapor to the first phase change, and

a second subset of transient response data that represents a second transient response of the vapor to the second phase change; and

wherein determining the Doppler shift comprises:

generating first and second values based on, respectively, the first and second subsets of transient response data, the first value representing a degree to which the vapor responds to the first phase change, the second value representing a degree to which the vapor responds to the second phase change, and

calculating a difference between the first and second values, the difference representing a detuning of the incoming series of RF pulses relative to a Rydberg electronic transition of the vapor.

20. The signal processing method of claim 19 ,

wherein the incoming series of RF signals are received by a receiver system; and

wherein determining the velocity of the object comprises:

determining a magnitude of the velocity based on a magnitude of the difference between the first and second values; and

determining a direction of the velocity based on a sign of the difference, the direction determined relative to an incoming direction along which the incoming series of RF pulses travels to reach the receiver system.

21. The signal processing method of claim 18 , wherein the reference phase modulation defines a pattern of phase changes in each of the outgoing series of RF pulses, the pattern of phase changes common to all RF pulses in the outgoing series.

22. The signal processing method of claim 21 , wherein the pattern of phase changes comprises a pair of phase changes that are equal in magnitude but opposite in sign, the pair of phase changes repeating successively to define the pattern of phase changes.

23. The signal processing method of claim 18 ,

wherein the outgoing series of RF pulses have a reference amplitude modulation;

wherein the response data comprises steady-state response data that represents one or more steady-state responses of the vapor to respective amplitude changes in the incoming series of RF pulses, the respective amplitude changes based on the reference amplitude modulation of the outgoing series of RF pulses; and

wherein the Doppler shift is determined based on the transient response data and the steady-state response data.

24. The signal processing method of claim 18 ,

wherein the vapor cell system comprises a laser system that is configured to generate the laser signals, the laser signals comprising a tunable laser signal;

wherein the signal processing method comprises transmitting a control signal to the laser system to alter a frequency of the tunable laser signal from an on-resonance frequency, where the tunable laser signal is on-resonance with an optical electronic transition of the vapor, to a detuned frequency, where the tunable laser signal is detuned relative to the optical electronic transition of the vapor; and

wherein the generating the response data comprises:

generating the transient response data when the tunable laser signal is at the on-resonance frequency, and

generating detuned transient response data when the tunable laser signal is at the detuned frequency.

25. The signal processing method of claim 24 ,

wherein the tunable laser signal is a first tunable laser signal, the detuned frequency is a first detuned frequency, and the control signal is a first control signal;

wherein the laser signals comprise a second tunable laser signal;

wherein the signal processing method comprises transmitting a second control signal to the laser system to alter a frequency of the second tunable laser signal from the on-resonance frequency, where the second tunable laser signal is on-resonance with the optical electronic transition of the vapor, to a second detuned frequency, wherein the second tunable laser signal is detuned relative to the optical electronic transition of the vapor; and

wherein the detuned transient response data is generated when the first and second tunable laser signals are at, respectively, the first and second detuned frequencies.

26. The signal processing method of claim 18 ,

wherein the outgoing series of RF pulses share a pulse period in common; and

wherein determining the Doppler shift comprises:

generating a sampled portion of response data by sampling the response data over a sampling period that is based on one or more of the pulse periods,

comparing the sampled portion of response data to each of a plurality of response templates to determine respective degrees of fit, each response template having template data that represents a known response of the vapor to one or more reference RF pulses, the one or more reference RF pulses different for each response template,

selecting one of the response templates based on its degree of fit, and

determining the Doppler shift based on the sampled portion of response data and the template data of the selected response template.

27. The signal processing method of claim 18 ,

wherein each of the outgoing series of RF pulses is divided into a sequence of sub-pulses that have respective phases, the respective phases defined by the reference phase modulation according to a pulse compression protocol; and

wherein the velocity of the object is determined based on the Doppler shift and respective arrival times of one or more target RF pulses in the incoming series of RF pulses.

28. The signal processing method of claim 27 , comprising:

generating, based on the transient response data over time, correlation values for a target RF pulse in the incoming series of RF pulses, wherein:

the target RF pulse is divided into a sequence of target sub-pulses that have respective target phases,

the correlation values represent a correlation of the target sub-pulses, in time, with one or more reference sub-pulses of a reference RF pulse, and

the one or more reference sub-pulses have respective reference phases that are defined by the reference phase modulation according to the pulse compression protocol; and

determining an arrival time of the target RF pulse based on the correlation values.

29. The signal processing method of claim 28 , comprising:

assigning, based on the transient response data, respective symbols to the target sub-pulses of the target RF pulse, the respective symbols being part of the pulse compression protocol, the one or more reference sub-pulses associated with respective symbols of the pulse compression protocol.

30. The signal processing method of claim 18 ,

wherein the incoming series of RF signals are received by a receiver system; and

wherein the signal processing method comprises determining a distance of the object from the receiver system based on the response data.

Assignments (1)

Continuity (1)

References Cited (47)