Use of nuclear spin impurities to suppress electronic spin fluctuations and decoherence in composite solid-state spin systems

Patent metadata

Field	Value
Publication number	US-9720067-B2
Application number	US-201214361626-A
Country	US
Kind code	B2
Filing date	Nov 30, 2012
Priority date	Nov 30, 2011
Publication date	Aug 1, 2017
Grant date	Aug 1, 2017

Abstract

A solid state electronic spin system contains electronic spins disposed within a solid state lattice and coupled to an electronic spin bath and a nuclear spin bath, where the electronic spin bath composed of electronic spin impurities and the nuclear spin bath composed of nuclear spin impurities. The concentration of nuclear spin impurities in the nuclear spin bath is controlled to a value chosen so as to allow the nuclear spin impurities to effect a suppression of spin fluctuations and spin decoherence caused by the electronic spin bath. Sensing devices such as magnetic field detectors can exploit such a spin bath suppression effect, by applying optical radiation to the electronic spins for initialization and readout, and applying RF pulses to dynamically decouple the electronic spins from the electronic spin bath and the nuclear spin bath.

First claim

What is claimed is:

1. A system comprising
a solid state electronic spin system containing one or more electronic spins disposed within a solid state lattice and coupled to an electronic spin bath and a nuclear spin bath, the electronic spin bath composed of electronic spin impurities and the nuclear spin bath composed of nuclear spin impurities;
wherein concentration of the nuclear spin impurities in the nuclear spin bath is chosen so that the nuclear spin impurities effect a suppression of spin fluctuations and spin decoherence of the one or more electronic spins caused by the electronic spin bath;
an optical source configured to generate optical excitation radiation for initialization and readout of the electronic spins in the solid state lattice;
an RF source configured to generate RF pulse sequences configured to dynamically decouple the electronic, spins from the electronic spin bath and the nuclear spin bath; and
a detector configured to detect output optical radiation correlated with the electronic spins, after the electronic spins have been subject to the optical excitation radiation and the RF pulse sequences, so as to detect a variable of interest.

2. The system of claim 1 , wherein the solid state lattice comprises diamond, the electronic spins comprise NV centers in the diamond, the electronic spin impurities comprise N atoms in the diamond, and the nuclear spin impurities comprise 13 C isotopes within the diamond.

3. The system of claim 2 , wherein the electronic spins of the N atoms are configured to magnetically interact with each other and with the electronic spins of the NV centers, so as to cause spin flipping and spin decoherence of the N atom electronic spins and the NV center electronic spins; and
wherein the nuclear spins of the 13 C isotopes are configured to magnetically interact with the N atom electronic spins and with the NV center electronic spins thereby reducing spin flipping and increasing spin coherence of the electronic spins of the NV centers.

4. The system of claim 2 , wherein the concentration of the 13 C isotopes within the diamond lattice is chosen so that the magnetic interactions between the 13 C nuclear spins and the N atom electronic spins shift the energy levels of the N atom electronic spins relative to each other and remove the degeneracy in these energy levels, thereby substantially suppressing the spin flipping and spin decoherence of the N atom electronic spins and the NV center electronic spins.

5. The system of claim 2 , wherein a ratio of single substitutional nitrogen to 13 C given by [N](ppm)/ 13 C(%) is in a range 1 to 500, 10 to 400, 20 to 300, 30 to 200, 40 to 150, or 50 to 150.

6. The system of claim 2 , wherein a single substitutional nitrogen concentration is equal to or greater than 150 ppm, 200 ppm, 300 ppm, 500 ppm, 750 ppm, or 1000 ppm.

7. The system of claim 6 , wherein the single substitutional nitrogen concentration is equal to or less than 10000 ppm, 5000 ppm, 2000 ppm, or 1000 ppm.

8. The system of claim 6 , wherein a 13 C concentration is equal to or greater than 1.5%, 2%, 3%, 5%, 7%, or 10%.

9. The system of claim 7 , wherein the 13 C concentration may be equal to or less than 100%, 75%, 50%, 30%, 20%, or 15%.

10. The system of claim 2 , wherein a single substitutional nitrogen concentration is equal to or greater than greater than 1 ppm, 5 ppm, 10 ppm, 20 ppm, 50 ppm, or 70 ppm.

11. The system of claim 10 , wherein the single substitutional nitrogen concentration is equal to or less than 80 ppm, 60 ppm, 40 ppm, 20 ppm, or 10 ppm.

12. The system of claim 2 , wherein a 13 C concentration is equal to or greater than 0.02%, 0.05%, 0.10%, 0.2%, 0.3%, 0.5% or 0.7%.

13. The system of claim 12 , wherein the C concentration is equal to or less than 0.8%, 0.6%, 0.4%, 0.25%, 0.15%, 0.10% or 0.75%.

14. The system of claim 2 , wherein a ratio of [NV](ppm)/[N](ppm) is equal to or greater than 1×10 −3 , 5×10 −3 , 1×10 −2 , or 5×10 −2 .

15. The system of claim 14 , wherein the ratio of [NV](ppm)/[N](ppm) is equal to or less than 1, 5×10 −1 , or 1×10 −1 .

16. The system according to claim 1 , wherein T 2 (n) scales with the number of pulses n according to the equation:
T 2 ( n )= T 2 (1)× n (SF)

where T 2 (n) is the T 2 for an n pulse RF sequence, T 2 (1) is the T 2 for one RF pulse, and SF is a scaling factor, wherein the scaling factor SF is equal to or greater than 0.55 or 0.6.

17. The system according to claim 1 , wherein a figure of merit (FOM) given by NV×T 2 (n) [ms/cm 3 ] is equal to or greater than 5×10 14 , 1×10 15 , 5×10 15 , 1×10 16 , 5×10 16 , or 1×10 17 using an RF pulse sequence with a number of pulses it less than or equal to 1000, 800, 600, 400, 200, 100, 80 or 60.

18. The system of claim 17 , wherein NV×T 2 (n) is equal to or greater than 1×10 16 with a number of pulses n less than or equal to 400, 200, 100, 80, Or 60.

19. The system according to claim 1 , wherein NV×T 2 (n)>5×10 15 ×n (0.55) .

20. The system according, to claim 1 , wherein the RF pulse sequences comprise at least one of: a Halm-echo sequence; and a CPMG sequence.

21. The system according to claim 1 , wherein the variable of interest an external magnetic field, and the system a magnetometer.

22. The system according to claim 1 , wherein the variable of interest is an external electric field, and the system is an electric field detector.

Assignees

• Walsworth Ronald L
• Bar-Gill Nir
• Belthangady Chinmay
• Pham Linh My
• Harvard College

Inventors

• Walsworth Ronald L
• Bar-Gill Nir
• Belthangady Chinmay
• Pham Linh My

Classifications

• G01R33/4616

  using specific RF pulses or specific modulation schemes, e.g. stochastic excitation, adiabatic RF pulses, composite pulses, binomial pulses, Shinnar-le-Roux pulses, spectrally selective pulses not being used for spatial selection · CPC title

• G01R33/60

  using electron paramagnetic resonance (G01R33/24, G01R33/62 take precedence) · CPC title

• G01R33/24

  for measuring direction or magnitude of magnetic fields or magnetic flux · CPC title

• G01R33/58 Primary

  Calibration of imaging systems, e.g. using test probes {, Phantoms; Calibration objects or fiducial markers such as active or passive RF coils surrounding an MR active material} · CPC title

• G01R33/1284 Primary

  Spin resolved measurements; Influencing spins during measurements, e.g. in spintronics devices · CPC title