Granted Patent B2

US 12,287,201 · App. 17/759,599 · Granted Apr 29, 2025

Inventor: Michael Stern (Givat Shmuel, IL)

G01C17/32G01R33/26

Abstract

Claims (49)

1. A magnetometer that finds a magnitude of an ambient magnetic field, comprising:

a) a crystal having a diamond cubic structure, with four tetrahedral axes, with an ensemble of paramagnetic defects, some of the defects oriented along each of the crystal's four tetrahedral axes;

b) a microwave source that produces a microwave field at the crystal, of controllable frequency over a range that includes microwave resonance frequencies, in the presence of the ambient magnetic field, for paramagnetic defects oriented along all four axes;

c) a light source that illuminates the paramagnetic defects with light of a wavelength to cause fluorescent emission;

d) a light detector that measures a total detected fluorescent emission power of the paramagnetic defects; and

e) a controller configured to:

1) measure the detected fluorescent emission power at each of a plurality of different selected microwave frequencies within the range, over a spectrum acquisition time, to obtain a spectrum of the paramagnetic defect ensemble;

2) calculate a variance property of the spectrum; and

3) calculate the magnitude of the ambient magnetic field from the variance property.

2. A magnetometer according to claim 1 , wherein the light source comprises a light emitting diode.

3. A magnetic navigation device comprising:

a) a magnetometer according to claim 1 ;

b) a data storage medium containing magnetic map data about the magnitude of the ambient magnetic field as a function of position; and

c) a navigation controller, the same as or different from the controller of the magnetometer, configured to use the magnitude of the ambient magnetic field found by the magnetometer at one or more locations, together at least with the magnetic map data, to find a location of the navigation device.

4. A magnetic navigation device according to claim 3 also comprising an accelerometer, wherein the navigation controller is configured to obtain the magnitude of the ambient magnetic field at more than one location, and to use the accelerometer to obtain information about a relative spatial configuration of the locations, and finding the location of the navigation device comprises using the magnitude of the ambient magnetic field at the locations and information about the relative spatial configuration of the locations.

5. A magnetometer according to claim 1 , wherein the crystal comprises a diamond crystal, and the paramagnetic defects comprise NV centers.

6. A magnetometer according to claim 5 , wherein the light detector has a noise level, a level of consumed power of the light source less than 250 milliwatts, the spectrum acquisition time is less than 200 milliseconds, and in a uniform constant magnetic field of 0.5 gauss oriented in any direction, has an expected random error of the magnitude of the magnetic field due to the noise level of the light detector that is less than 50 nanotesla.

7. A magnetometer that finds a magnitude of an ambient magnetic field or of one or more components of the magnetic field or both, comprising:

a) a crystal having a diamond cubic structure with four tetrahedral axes, with an ensemble of paramagnetic defects, some of the defects oriented along each of the crystal's four tetrahedral axes;

b) a microwave source that produces a microwave field at the crystal of controllable frequency over a range that includes microwave resonance frequencies, in the presence of the ambient magnetic field, for paramagnetic defects oriented along all four axes;

c) a light source with a light emitting surface that illuminates the paramagnetic defects with light of a wavelength to cause fluorescent emission;

d) a light detector with a light detecting surface, that measures a total detected power of fluorescent emission light of the paramagnetic defects; and

e) a controller configured to:

1) measure the detected fluorescent emission power at each of a plurality of different selected microwave frequencies within the range, over a spectrum acquisition time, to obtain a spectrum of the paramagnetic defect ensemble; and

2) calculate the magnitude of the magnetic field or the one or more components of the magnetic field or both, from the spectrum;

wherein all of the crystal is closer to the light emitting surface than a largest transverse dimension of the light emitting surface, and closer to the light detecting surface than a largest transverse dimension of the light detecting surface.

8. A magnetometer according to claim 7 , wherein the light source comprises a light emitting diode.

9. A magnetometer according to claim 7 , wherein the controller is configured to calculate the magnitude of the magnetic field by obtaining a variance property of the spectrum, and calculating the magnitude of the magnetic field from the variance property.

10. A magnetometer according to claim 7 , wherein the light emitting surface and the light detecting surface are substantially planar and substantially parallel to each other, and are situated on opposite sides of the crystal.

11. A magnetometer according to claim 10 , also comprising a filter situated between the crystal and the light detecting surface that substantially filters out the illuminating light from the light emitting surface and substantially passes the fluorescent emission light to the light detecting surface.

12. A magnetometer according to claim 10 , also comprising a filter situated between the light emitting surface and the crystal that substantially filters out any light emitted from the light emitting surface in a range of wavelengths corresponding to predominant wavelengths of the fluorescent emission light, and substantially passes light emitted from the light emitting surface at wavelengths that excite the fluorescent emission.

13. A magnetometer according to claim 7 , wherein the crystal comprises diamond, and the paramagnetic defects comprise NV centers.

14. A magnetometer according to claim 13 , wherein the light detector has a noise level, and wherein the light source consumes less than 250 milliwatts of power, the spectrum acquisition time that the controller is configured to use is less than 200 milliseconds, and for a magnetic field of 0.5 gauss, for any orientation of the magnetic field relative to the crystal's four tetrahedral axes, for all of the components or magnitude of the magnetic field that the controller is configured to calculate, using the selected microwave frequencies that the controller is configured to use, there is an expected random error in the calculated value of the magnitude or component of the magnetic field of less than 50 nanotesla, due to random errors in the spectrum at each selected frequency due to the noise level of the light detector.

15. A magnetometer according to claim 7 , wherein the total detected power of the fluorescent emission light is at least 3 percent of a power of light emitted by the light source.

16. A method of determining a magnitude of an ambient magnetic field, using an ensemble of paramagnetic defects in a crystal having a diamond cubic structure with four tetrahedral axes, some of the defects oriented along each of the crystal's four tetrahedral axes, the defects having a zero-field splitting resonant frequency Do, the method comprising:

a) exposing the paramagnetic defect ensemble to microwave radiation at a selected frequency;

b) illuminating the paramagnetic defects with light, from a light source, of a wavelength to cause fluorescent emission;

c) measuring a total detected fluorescent emission power from the paramagnetic defect ensemble with a light detector;

d) repeating (a), (b) and (c), using different selected frequencies of the microwave radiation to obtain a microwave absorption spectrum of the paramagnetic defect ensemble over frequencies that include Zeeman splitting of the zero-field splitting resonant frequency Do, due to the ambient magnetic field, for paramagnetic defects oriented along all four tetrahedral axes;

e) calculating a variance property of the microwave absorption spectrum; and

f) calculating a magnitude of the ambient magnetic field from the variance property.

17. A method according to claim 16 , wherein the crystal comprises a diamond crystal, and the paramagnetic defects comprise nitrogen vacancy (NV) centers.

18. A method according to claim 17 , wherein the light detector has an output voltage that includes a noise level, wherein illuminating with light from a light source comprises illuminating with light from a light source that consumes less than 250 milliwatts of power, and wherein measuring the total fluorescent emission power at each selected frequency comprises measuring an emission power, for a measurement time, so that a total of all the measurement times is less than 200 milliseconds, and there is an expected random error in the calculated value of the magnitude of the magnetic field of less than 50 nanotesla (nT), that corresponds to random errors in the spectrum at each selected frequency due to the noise level of the output voltage of the light detector, when the variance property is calculated from the spectrum, and the variance property is used to calculate the magnitude of the magnetic field.

19. A method according to claim 16 , wherein the ambient magnetic field is dominated by the earth's magnetic field, with only smaller contributions, or no contributions, from man-made structures or magnetic field sources.

20. A method of determining a magnitude of an ambient magnetic field, using the method of claim 16 , during a time interval, wherein the crystal is located in a device that generates a self magnetic field in the crystal due to one or more independently changeable device currents, one or more permanent magnets, or both, the method comprising:

a) determining a direction and a ratio of magnitude of self magnetic field to device current, in the crystal, for each of the device currents, if any, and direction and magnitude of the self magnetic field in the crystal due to the permanent magnets, if any;

b) measuring each of the device currents, if any, as a function of time during the time interval;

c) during the time interval, passing field-cancelling currents through each of a set of field-cancelling coils surrounding the crystal, the coils configured and the currents selected to substantially cancel the self magnetic field in the crystal, using the measured device currents if any, the ratios of self magnetic field and device current, if any, and the self magnetic field due to the permanent magnets, if any; and

d) using the method of claim 16 to measure the magnitude of the ambient magnetic field during the time interval, while the self magnetic field in the crystal is substantially cancelled by the field-cancelling currents in the field-cancelling coils.

Continuity (2)

References Cited (81)