QUANTUM PROCESSING DEVICE

• US 20140291490A1
• Filed: 10/12/2012
• Published: 10/02/2014
• Est. Priority Date: 10/14/2011
• Status: Active Grant

• Current Assignee: Element Six Technologies US Corporation (Anglo American PLC)
• Original Assignee: Element Six Technologies US Corporation (Anglo American PLC)
• Inventors: Markham, Matthew Lee, Twitchen, Daniel James, Hanson, Ronald, Bernien, Hannes
• Granted Patent: US 9,335,606 B2
• Time in Patent Office: Days
• US Class Current: 250/214.R
• CPC Class Codes: B82Y 10/00 Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic
• CPC Class Codes: B82Y 20/00 Nanooptics, e.g. quantum optics or photonic crystals
• CPC Class Codes: G02B 6/00 Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
• CPC Class Codes: G02F 3/00 Optical logic elements; Optical bistable devices
• CPC Class Codes: G06N 10/00 Quantum computing, i.e. information processing based on quantum-mechanical phenomena
• CPC Class Codes: H01L 29/127 Quantum box structures
• CPC Class Codes: H01L 29/66977 Quantum effect devices, e.g. using quantum reflection, diffraction or interference effects, i.e. Bragg- or Aharonov-Bohm effects
• CPC Class Codes: H01L 29/66984 Devices using spin polarized carriers

Abstract

A device for achieving multi-photon interference, said device comprising: at least two solid state photon emitters, each solid state photon emitter comprising nuclear and electron spin states coupled together, each solid state photon emitter being configured to produce photon emission comprising a photon emission peak, wherein the photon emission peaks from different solid state photon emitters have a first frequency difference between peak intensities, and wherein the electron spin states of each solid state photon emitter are resolvable; an excitation arrangement configured to individually address the at least two solid state photon emitters; a plurality of optical out coupling structures wherein each solid state photon emitter is provided with an associated optical out coupling structure; a tuning arrangement configured to reduce the first frequency difference between the peak intensities of the photon emission peaks from the at least two solid state photon emitters to a second frequency difference which is smaller than the first frequency difference; a photon interference arrangement configured to overlap photon emissions from the at least two solid state emitters after tuning; and a detector arrangement configured to detect photon emissions from the at least two solid state emitters after tuning and passing through the photon interference arrangement, wherein the detector arrangement is configured to resolve sufficiently small differences in photon detection times that tuned photon emissions from the at least two solid state emitters are quantum mechanically indistinguishable resulting in quantum interference between indistinguishable photon emissions from different solid state photon emitters.

Claims

1. A device for achieving multi-photon interference, said device comprising:

at least two solid state photon emitters, each solid state photon emitter comprising nuclear and electron spin states coupled together, each solid state photon emitter being configured to produce photon emission comprising a photon emission peak, wherein the photon emission peaks from different solid state photon emitters have a first frequency difference between peak intensities, and wherein the electron spin states of each solid state photon emitter are resolvable;

an excitation arrangement configured to individually address the at least two solid state photon emitters;

a plurality of optical outcoupling structures wherein each solid state photon emitter is provided with an associated optical outcoupling structure;

a tuning arrangement configured to reduce the first frequency difference between the peak intensities of the photon emission peaks from the at least two solid state photon emitters to a second frequency difference which is smaller than the first frequency difference;

a photon interference arrangement configured to overlap photon emissions from the at least two solid state emitters after tuning; and

a detector arrangement configured to detect photon emissions from the at least two solid state emitters after tuning and passing through the photon interference arrangement, wherein the detector arrangement is configured to resolve sufficiently small differences in photon detection times that tuned photon emissions from the at least two solid state emitters are quantum mechanically indistinguishable resulting in quantum interference between indistinguishable photon emissions from different solid state photon emitter;

wherein the at least two solid state photon emitters are formed by photon emissive defects in a diamond material, and

wherein the photon emissive defects are nitrogen vacancy (NV) defects.

2. A device according to claim 1, wherein each photon emission peak has a bandwidth which is no more than a factor of 100, 80, 60, 40, 20, 10, 5, or 1 times a natural linewidth of its associated solid state emitter.

4. A device according to claim 1, wherein the first frequency difference between two photon emission peaks from different solid state photon emitters is no more than a factor of 10000, 5000, 3000, 1000, 750, or 500 times a natural line width of each of the two photon emission peaks.

6. A device according to claim 1, wherein the second frequency difference between two photon emission peaks from different solid state photon emitters after tuning is no more than a factor of 100, 75, 50, 25, 10, 5, or 1 times a natural line width of each of the two photon emission peaks.

8. A device according to claim 1, wherein the detector is configured to resolve differences in photon detection times smaller than:

1/(a natural linewidth of each solid state photon emitter);

10/(200 times a natural linewidth of each solid state photon emitter);

1/(200 times a natural linewidth of each solid state photon emitter);

1/(500 times a natural linewidth of each solid state photon emitter);

1/(1000 times a natural linewidth of each solid state photon emitter);

or 1/(2000 times a natural linewidth of each solid state photon emitter).

9. A device according to claim 1, wherein the detector has a frequency resolution in a range 0.1 to 25 GHz, 0.5 to 20 GHz, 1 to 15 GHz, 1 to 10 GHz, or 1 to 5 GHz.

10. A device according to claim 1, wherein each solid state photon emitter is configured to produce photon emission having a larger bandwidth than its associated photon emission peak, the quantum interference device further comprising a filtering arrangement configured to reduce the bandwidth of photon emission from each solid state photon emitter by filtering out photons not associated with the photon emission peak of each solid state photon emitter.

11. A device according to claim 10, wherein the filtering arrangement is configured whereby after filtering the photon emission from each solid state photon emitter has a bandwidth which is no more than a factor of 100, 80, 60, 40, 20, 10, 5, or 1 times a natural linewidth of its associated solid state emitter.

13. A device according to claim 10, wherein the filtering arrangement comprises a filtering element configured to separate a zero phonon line emission from a phonon side band emission.

14. A device according to claim 13, further comprising a detector configured to measure the separated phonon side band emission and an adjustment configuration for realigning and/or refocusing components of the quantum processing device if a reduction in intensity of the phonon side band emission is detected to thereby increase the intensity of the phonon side band emission.

17. A device according to claim 1, wherein the quantum processing device further comprises a polarization filtering arrangement configured to selectively filter photons of a common polarization.

21. A device according claim 1, wherein the photon emissive defects are preferentially oriented relative to a crystallographic orientation of the diamond material.

22. A device according to claim 21, wherein the diamond material is oriented in a {111} crystallographic orientation and the photon emissive defects each have dipoles corresponding to E_x and E_y transitions lying in a surface plane and orthogonal to each other.

24. A device according to claim 1, wherein the excitation arrangement is configured to adjust polarization of the excitation to selectively excite E_x or E_y emission.

25. A device according to claim 1, wherein the tuning arrangement is configured to apply an electric field to one or more of the at least two solid state photon emitters to compensate for frequency differences between the at least two solid state photon emitters and bring the photon emission peaks into resonance.

27. A device according to claim 17, wherein the polarization filtering arrangement is configured to compensate for changes in dipole orientation as a result of the applied electric field of the tuning arrangement.

28. A device according to claim 1, wherein a switching device is provided to alter emission modes between parallel and orthogonal polarization.

33. A device according to claim 1, comprising a time resolved multi-photon interference contrast no less than 50%, 60%, 65%, 70% or 75%.

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