IP Library Granted Patent US 10,197,497
Granted Patent B2
US 10,197,497 · App. 15/547,092 · Granted Feb 5, 2019

Sensor for measurements using Johnson noise in materials

Inventors: Shimon Jacob Kolkowitz (Cambridge, MA); Arthur Safira (Somerville, MA); Alexander A. High (Allston, MA); Robert C. Devlin (Abington, PA); Soonwon Choi (Cambridge, MA); Quirin P. Unterreithmeier (Cambridge, MA); David Patterson (Somerville, MA); Alexander S. Zibrov (Cambridge, MA); Vladimir E. Manucharyan (College Park, MD); Mikhail D. Lukin (Cambridge, MA); Hongkun Park (Lexington, MA)
Assignee: President and Fellows of Harvard College
G01N21/6408G01B11/14G01K11/00G01R27/02
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Quick Facts
Patent No.
US 10,197,497
App. No.
15/547,092
Granted
Feb 5, 2019
Kind
B2
Abstract

A method of making measurements includes providing a sensor with at least one solid state electronic spin; irradiating the sensor with radiation from an electromagnetic radiation source that manipulates the solid state electronic spins to produce spin-dependent fluorescence, wherein the spin-dependent fluorescence decays as a function of relaxation time; providing a target material in the proximity of the sensor, wherein, thermally induced currents (Johnson noise) present in the target material alters the fluorescence decay of the solid state electronic spins as a function of relaxation time; and determining a difference in the solid state spins spin-dependent fluorescence decay in the presence and absence of the target material and correlating the difference with a property of the sensor and/or target material.

Claims (27)

1. A method of making measurements, comprising:

providing a sensor with at least one solid state electronic spin;

irradiating the sensor with radiation from an electromagnetic radiation source that manipulates the solid state electronic spins to produce spin-dependent fluorescence,

wherein the spin-dependent fluorescence decays as a function of relaxation time;

providing a target material in the proximity of the sensor,

wherein, thermally induced currents (Johnson noise) present in the target material alters the fluorescence decay of the solid state electronic spins as a function of relaxation time; and

determining a difference in the solid state spins spin-dependent fluorescence decay in the presence and absence of the target material and correlating the difference with a property of the sensor and/or target material.

2. The method of claim 1 , wherein the property of the target material measured is localized at a length scale of 10-100 nm.

3. The method of claim 2 , wherein the property measured is the resistance values within the target material.

4. The method of claim 2 , wherein the property measured is the temperature of the target material.

5. The method of claim 1 , wherein the property measured is the distance of the target material from the surface of the sensor.

6. The method of claim 1 , wherein the property measured is the distance of the solid state electronic spins from the surface of the sensor.

7. The method of claim 1 , wherein, the sensor comprises a diamond crystal lattice.

8. The method of claim 7 , wherein, the solid state electronic spins comprises a defect in the diamond crystal lattice.

9. The method of claim 8 , wherein the defect comprises a nitrogen vacancy center in a diamond crystal lattice.

10. The method of claim 1 , wherein, the electromagnetic radiation source is a laser.

11. The method of claim 1 , wherein, the laser source emits a laser having wavelength of about 532 nanometers.

12. The method of claim 1 , wherein the target material is in contact with the sensor.

13. The method of claim 1 , wherein the target material is not in contact with the sensor.

14. The method of claim 1 , wherein the target material is a conductive material.

15. The method of claim 1 , wherein the target material is a metal.

16. The method of claim 1 , wherein the target material is silver.

17. The method of claim 1 , wherein the target material is copper.

18. The method of claim 1 , wherein the target material is a single crystal.

19. The method of claim 18 , wherein the single crystal is a silver single crystal.

20. The method of claim 1 , wherein the target material is polycrystalline.

21. The method of claim 1 , wherein the target material is a conductive polymer.

Assignments (3)
CONFIRMATORY LICENSE Recorded Feb 26, 2025
From: HARVARD UNIVERSITY
To: NATIONAL SCIENCE FOUNDATION
Reel/Frame 070330/0813 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 25, 2018
From: CHOI, SOONWON; DELVIN, ROBERT C.; HIGH, ALEXANDER; KOLKOWITZ, SHIMON JACOB; LUKIN, MIKHAIL D.; MANUCHARYAN, VLADIMIR E.; PARK, HONGKUN; PATTERSON, DAVID S.; SAFIRA, ARTHUR; UNTERREITHMEIER, QUIRIN P.; ZIBROV, ALEXANDER S.
To: PRESIDENT AND FELLOWS OF HARVARD COLLEGE
Reel/Frame 046960/0685 →
CONFIRMATORY LICENSE Recorded Jul 17, 2018
From: HARVARD UNIVERSITY
To: NATIONAL SCIENCE FOUNDATION
Reel/Frame 046556/0359 →
Continuity (2)
Provisional Application 62109271 · Jan 29, 2015
Related Publication 20180275057A1 · Sep 27, 2018
Cited By (1)
US 12,718,975