Granted Patent B2

US 12,306,234 · App. 18/825,571 · Granted May 20, 2025

Inventors: Stephanie M. Bohaichuk (Waterloo, CA); Harald Kubler (Waterloo, CA); Vijin Venu (Waterloo, CA); James P. Shaffer (Kitchener, CA)

Assignee: Quantum Valley Ideas Laboratories

G01R29/0885G01R29/0892

Abstract

Claims (154)

1. A method, comprising:

generating an optical signal by interacting laser signals with a vapor of a vapor cell sensor, the optical signal based on a transmission of one of the laser signals through the vapor;

altering an intensity of the optical signal by interacting a target RF electromagnetic field with a Rydberg electronic transition of the vapor, the target RF electromagnetic field comprising a time series of RF pulses;

generating, by operation of an optical detection system, a detector signal in response to receiving the optical signal at the optical detection system; and

by operation of a signal processing system:

generating, based on the detector signal, response data that represents a response of the vapor to the laser signals and the target RF electromagnetic field,

determining, based on the response data, an interval during which the vapor experiences a transient response to the target RF electromagnetic field, the interval associated with a phase change in the time series of RF pulses, and

determining a magnitude of the phase change based on a portion of the response data that is generated during the interval.

2. The method of claim 1 , wherein the operations of the signal processing system comprise:

identifying, based on the interval, a transition between two consecutive RF pulses in the time series of RF pulses, the two consecutive RF pulses comprising a target RF pulse and a previous RF pulse;

determining a phase of the target RF pulse based on the magnitude of the phase change and a phase of the previous RF pulse; and

assigning a symbol to the target RF pulse based on the determined phase, the symbol being part of a plurality of symbols of a communication protocol.

3. The method of claim 2 ,

wherein the time series of RF pulses comprise one or more initializing RF pulses that establish a reference phase for the time series of RF pulses;

wherein the one or more initializing RF pulses comprise the previous RF pulse; and

wherein the reference phase defines the phase of the previous RF pulse.

4. The method of claim 1 ,

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

wherein determining the interval comprises:

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

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 a different reference RF pulse,

selecting one of the response templates based on its degree of fit, and determining the interval based on the sampled portion of response data and the template data of the selected response template.

5. The method of claim 4 , wherein determining the magnitude of the phase change comprises determining the magnitude of the phase change based on:

the portion of the response data that is generated during the interval; and

the template data of the selected response template.

6. The method of claim 4 ,

wherein the plurality of response templates are associated with respective symbols of a communication protocol; and

wherein the operations of the signal processing system comprise:

identifying, based on the interval, a transition between two consecutive RF pulses in the time series of RF pulses, the two consecutive RF pulses comprising a target RF pulse and a previous RF pulse, and

assigning the symbol of the selected response template to the target RF pulse.

7. The method of claim 4 ,

wherein comparing the sampled portion of response data comprises generating, for each response template, a difference between the template data of the response template and the sampled portion of response data, the difference defining the degree of fit for the response template; and

wherein selecting one of the response templates comprises identifying an individual response template that has a minimum difference between its template data and the sampled portion of response data, the individual response template defining the selected response template.

8. The method of claim 1 ,

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

wherein the interval is an extended interval during which the vapor experiences two or more transient responses to the target RF electromagnetic field, the extended interval comprising two or more sub-intervals that are associated with respective phase changes in the time series of RF pulses; and

wherein determining the interval comprises:

generating a sampled portion of response data by sampling the response data over a sampling period that is based on a multiple number of 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 a different sequence of reference RF pulses,

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

determining the extended interval based on the sampled portion of response data and the template data of the selected response template.

9. The method of claim 8 , wherein determining the magnitude of the phase change comprises determining a magnitude of each phase change associated with the two or more sub-intervals based on:

an extended portion of the response data that is generated during the extended interval; and

the template data of the selected response template.

10. The method of claim 8 ,

wherein the plurality of response templates are associated with respective sequences of symbols that are part of a communication protocol;

wherein the time series of RF pulses comprises a sequence of RF pulses in the extended interval; and

wherein the operations of the signal processing system comprise assigning the sequence of symbols of the selected response template to the sequence of RF pulses.

11. The method of claim 1 ,

wherein the interval is a first interval, and the portion of the response data is a first portion of the response data; and

wherein the operations of the signal processing system comprise:

determining, based on the response data, a second interval during which the vapor experiences a steady-state response to the target RF electromagnetic field, and

determining an amplitude of a target RF pulse in the time series of RF pulses based on a second portion of the response data that is generated during the second interval.

12. The method of claim 11 ,

wherein the phase change in the time series of RF pulses occurs between two consecutive RF pulses in the time series of RF pulses, the two consecutive RF pulses comprising the target RF pulse and a previous RF pulse; and

wherein operations of the signal processing system comprise:

determining a phase of the target RF pulse based on the magnitude of the phase change and a phase of the previous RF pulse, and

assigning a symbol to the target RF pulse based on the determined phase and the determined amplitude, the symbol being part of a plurality of symbols of a communication protocol.

13. The method of claim 11 ,

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

wherein determining the second interval comprises:

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

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 a different reference RF pulse,

selecting one of the response templates based on its degree of fit, and determining the second interval based on the sampled portion of response data and the template data of the selected response template.

14. The method of claim 13 , wherein determining the amplitude of the target RF pulse comprises determining the amplitude of the target RF pulse based on:

the second portion of the response data that is generated during the second interval; and

the template data of the selected response template.

15. The method of claim 1 ,

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

wherein the interval is an extended interval during which the vapor experiences one or more transient responses and one or more steady-state responses to the target RF electromagnetic field, the extended interval comprising:

one or more first sub-intervals that are associated with respective phase changes in a target sequence of RF pulses, and

one or more second sub-intervals that are associated with respective amplitudes of the target sequence of RF pulses; and

wherein determining the interval comprises:

generating a sampled portion of response data by sampling the response data over a sampling period that is based on a multiple number of 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 a different sequence of reference RF pulses,

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

determining the extended interval based on the sampled portion of response data and the template data of the selected response template.

16. The method of claim 15 ,

wherein determining the magnitude of the phase change comprises determining a magnitude of each phase change associated with the one or more first sub-intervals based on:

an extended portion of the response data that is generated during the extended interval, and

the template data of the selected response template; and

wherein the operations of the signal processing system comprise determining each amplitude associated with the one or more second sub-intervals based on:

the extended portion of the response data, and

the template data of the selected response template.

17. The method of claim 15 ,

wherein the plurality of response templates are associated with respective sequences of symbols that are part of a communication protocol; and

wherein the operations of the signal processing system comprise assigning the sequence of symbols of the selected response template to the target sequence of RF pulses.

18. The method of claim 1 , wherein generating the response data comprises generating values for respective elements of a density matrix that represents a response of the vapor to the laser signals and the target RF electromagnetic field.

19. The method of claim 1 , comprising:

generating the laser signals by operation of a laser system;

wherein the operations of the signal processing system comprise transmitting a control signal to the laser system to alter a frequency of one of the laser signals, thereby producing a detuned laser signal whose frequency is detuned relative to an optical electronic transition of the vapor;

wherein the optical signal is based on a transmission of the detuned laser signal through the vapor, and the response data comprises detuned response data that represents the response of the vapor when the laser signals comprise the detuned laser signal; and

wherein determining the magnitude of the phase change comprises determining a sign of the phase change based on the detuned response data.

20. The method of claim 19 ,

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

wherein the operations of the signal processing system comprise transmitting a second control signal to the laser system to produce a second detuned laser signal, the second detuned laser signal detuned relative to the optical electronic transition of the vapor; and

wherein the detuned response data represents the response of the vapor when the laser signals comprise the first and second detuned laser signals.

21. The method of claim 20 , wherein the first and second detuned laser signals have respective frequencies that are symmetrically detuned about the optical electronic transition of the vapor.

22. The method of claim 20 , wherein the first and second detuned laser signals have respective frequencies that are asymmetrically detuned about the optical electronic transition of the vapor.

23. The method of claim 1 ,

wherein the laser signals comprise probe and coupling laser signals; and

wherein:

the optical signal is based on a transmission of the probe laser signal through the vapor,

the probe laser signal interacts with a probe optical transition of the vapor, and

the coupling laser signal interacts with a coupling optical transition of the vapor.

24. The method of claim 23 ,

wherein the vapor has electronic states that comprise:

first and second electronic states, and

first and second Rydberg electronic states;

wherein the first electronic state, the second electronic state, and the first Rydberg electronic state are progressively higher in energy; and

wherein:

the probe optical transition is defined by the first and second electronic states,

the coupling optical transition is defined by the second electronic state and the first Rydberg electronic state, and

the Rydberg electronic transition is defined by the first and second Rydberg electronic states.

25. The method of claim 23 ,

wherein the coupling laser signal is a first coupling laser signal, and the coupling optical transition is a first coupling optical transition; and

wherein the laser signals comprise a second coupling laser signal that interacts with a second coupling optical transition of the vapor.

26. The method of claim 25 ,

wherein the vapor has electronic states that comprise:

first, second, and third electronic states, and first and second Rydberg electronic states;

wherein the first electronic state, the second electronic state, the third electronic state, and the first Rydberg electronic state are progressively higher in energy; and

wherein:

the probe optical transition is defined by the first and second electronic states,

the first coupling optical transition is defined by the second electronic state and the third electronic state,

the second coupling optical transition is defined by the third electronic state and the first Rydberg electronic state, and

the Rydberg electronic transition is defined by the first and second Rydberg electronic states.

27. The method of claim 1 ,

wherein the laser signals comprise a probe laser signal having comb lines at respective comb frequencies, the comb lines representing different respective detunings of the probe laser signal relative to a probe optical transition of the vapor;

wherein the optical signal is based on a transmission of the probe laser signal through the vapor;

wherein the detector signal represents an intensity of the optical signal at two or more comb frequencies that are associated with respective target comb lines of the probe laser signal; and

wherein generating response data comprises generating a subset of response data for each target comb line of the probe laser signal.

28. The method of claim 27 ,

wherein the respective target comb lines of the probe laser signal comprise first and second target comb lines;

wherein determining the interval comprises:

determining a first interval for the first target comb line based on a first subset of response data that is generated for the first target comb line, the first interval associated with a first phase change in the time series of RF pulses, and

determining a second interval for the second target comb line based on a second subset of response data that is generated for the second target comb line, the second interval associated with a second phase change in the time series of RF pulses; and

wherein determining the magnitude of the phase change comprises:

determining a magnitude of the first phase change based on a portion of the first subset of response data that is generated during the first interval, and

determining a magnitude of the second phase change based on a portion of the second subset of response data that is generated during the second interval.

29. The method of claim 1 ,

wherein the laser signals comprise a probe laser signal and a coupling laser signal, the coupling laser signal having comb lines at respective comb frequencies, the comb lines representing different respective detunings of the coupling laser signal relative to a coupling optical transition of the vapor;

wherein the optical signal comprises optical sub-signals that are associated with respective comb lines of the coupling laser signal, the optical sub-signals based on a transmission of the probe laser signal through the vapor as the respective comb lines of the coupling laser signal interact with the vapor;

wherein two or more of the optical sub-signals are associated with respective target comb lines of the coupling laser signal, the two or more optical sub-signals each having an intensity;

wherein the detector signal represents the intensities of the two or more optical sub-signals; and

wherein generating response data comprises generating a subset of response data for each target comb line of the coupling laser signal.

30. The method of claim 29 ,

wherein the time series of RF pulses is a first time series of RF pulses, and the target RF electromagnetic field comprises a second time series of RF pulses, the first and second time series of RF pulses having different carrier frequencies;

wherein the respective target comb lines of the coupling laser signal comprise first and second target comb lines that are associated with, respectively, the first and second time series of RF pulses;

wherein determining the interval comprises:

determining a first interval for the first target comb line based on a first subset of response data that is generated for the first target comb line, the first interval associated with a first phase change in the first time series of RF pulses, and

determining a second interval for the second target comb line based on a second subset of response data that is generated for the second target comb line, the second interval associated with a second phase change in the second time series of RF pulses; and

wherein determining the magnitude of the phase change comprises:

determining a magnitude of the first phase change based on a portion of the first subset of response data that is generated during the first interval, and

determining a magnitude of the second phase change based on a portion of the second subset of response data that is generated during the second interval.

Assignments (1)

Continuity (2)

References Cited (48)