Methods and apparatus for optically detecting magnetic resonance

Patent metadata

Field	Value
Publication number	US-10648933-B2
Application number	US-201816232137-A
Country	US
Kind code	B2
Filing date	Dec 26, 2018
Priority date	Jan 8, 2014
Publication date	May 12, 2020
Grant date	May 12, 2020

Abstract

A light-trapping geometry enhances the sensitivity of strain, temperature, and/or electromagnetic field measurements using nitrogen vacancies in bulk diamond, which have exterior dimensions on the order of millimeters. In an example light-trapping geometry, a laser beam enters the bulk diamond, which may be at room temperature, through a facet or notch. The beam propagates along a path inside the bulk diamond that includes many total internal reflections off the diamond's surfaces. The NVs inside the bulk diamonds absorb the beam as it propagates. Photodetectors measure the transmitted beam or fluorescence emitted by the NVs. The resulting transmission or emission spectrum represents the NVs' quantum mechanical states, which in turn vary with temperature, magnetic field strength, electric field strength, strain/pressure, etc.

First claim

The invention claimed is:

1. A method for sensing quantum mechanical spin states of color centers in a solid-state host, the method comprising:
coupling an excitation beam into the solid-state host along a propagation path within the solid-state host having a length longer than a longest exterior dimension of the solid-state host;
detecting, with a detector, fluorescence emitted by the color centers in response to the excitation beam; and
determining, from the fluorescence, the quantum mechanical spin states of the color centers.

2. The method of claim 1 , wherein coupling the excitation beam into the solid-state host comprises illuminating a facet of the solid-state host with the excitation beam.

3. The method of claim 2 , wherein illuminating the facet comprises matching a divergence of the excitation beam to a numerical aperture of the facet.

4. The method of claim 1 , wherein coupling the excitation beam into the solid-state host comprises causing the excitation beam to totally internally reflect off an interior surface of the solid-state host.

5. The method of claim 1 , wherein the propagation path is at least 100 times longer than the longest exterior dimension of the solid-state host.

6. The method of claim 1 , wherein the propagation path is about 100,000 times longer than the longest exterior dimension of the solid-state host.

7. The method of claim 1 , wherein the propagation path has a length of about 30 meters.

8. The method of claim 1 , wherein coupling the excitation beam into the solid-state host comprises coupling the excitation beam to a chaotic mode of the solid-state host.

9. The method of claim 1 , wherein coupling the excitation beam into the solid-state host comprises coupling the excitation beam to a non-chaotic mode of the solid-state host.

10. The method of claim 1 , further comprising:
modulating the excitation beam.

11. The method of claim 1 , further comprising:
exciting the color centers with microwave radiation so as to cause the color centers to emit the fluorescence.

12. The method of claim 1 , further comprising:
subjecting the solid-state host to a strain, a temperature, and/or an electromagnetic field; and
determining the strain, the temperature, and/or amplitude of the electromagnetic field based on the quantum mechanical spin states.

13. A method for sensing quantum mechanical spin states associated with color centers in a solid-state host, the method comprising:
matching a divergence angle of an excitation beam to a numerical aperture of a facet of the solid-state host;
coupling the excitation beam into the solid-state host via the facet;
detecting, with a detector, fluorescence emitted by the color centers in response to the excitation beam; and
determining, from the fluorescence, the quantum mechanical spin states of the color centers.

14. The method of claim 13 , wherein coupling the excitation beam into the solid-state host comprises causing the excitation beam to totally internally reflect off an interior surface of the solid-state host.

15. The method of claim 13 , further comprising:
modulating the excitation beam.

16. The method of claim 13 , further comprising:
exciting the color centers with microwave radiation so as to cause the color centers to emit the fluorescence.

17. The method of claim 13 , further comprising:
subjecting the solid-state host to a strain, a temperature, and/or an electromagnetic field; and
determining the strain, the temperature, and/or amplitude of the electromagnetic field based on the quantum mechanical spin states.

18. A method for sensing quantum mechanical spin states associated with color centers in a solid-state host, the method comprising:
coupling an excitation beam to a chaotic mode supported by the solid-state host;
detecting, with a detector, fluorescence emitted by the color centers in response to the excitation beam; and
determining, from the fluorescence, the quantum mechanical spin states of the color centers.

19. The method of claim 18 , further comprising:
subjecting the solid-state host to a strain, a temperature, and/or an electromagnetic field; and
determining the strain, the temperature, and/or amplitude of the electromagnetic field based on the quantum mechanical spin states.

20. The method of claim 18 , wherein the propagation path is from about 100 times longer to about 100,000 times longer than a longest exterior dimension of the solid-state host.

Assignees

• Massachusetts Inst Technology

Inventors

• Clevenson Hannah A
• Englund Dirk Robert

Classifications

• G01N24/006 Primary

  using optical pumping (magnetometers using optical pumping G01R33/26, optical pumping of lasers H01S3/091) · CPC title

• G01R33/323

  Detection of MR without the use of RF or microwaves, e.g. force-detected MR, thermally detected MR, MR detection via electrical conductivity, optically detected MR · CPC title