Methods, systems, and apparatus for programmable quantum photonic processing

• US 9,354,039 B2
• Filed: 06/05/2015
• Issued: 05/31/2016
• Est. Priority Date: 06/06/2014
• Status: Active Grant

• Current Assignee: Massachusetts Institute of Technology
• Original Assignee: Massachusetts Institute of Technology
• Inventors: Mower, Jacob C., Harris, Nicholas C., Englund, Dirk R., Steinbrecher, Greg
• Primary Examiner(s): PAK, SUNG H
• Application Number:
  US14/732,012
• Publication Number:
  US 20150354938A1
• Time in Patent Office: 361 Days
• Field of Search: 385/14
• US Class Current: 1/1
• CPC Class Codes: B82Y 20/00 Nanooptics, e.g. quantum optics or photonic crystals
• CPC Class Codes: G01B 9/02049 characterised by particular mechanical design details
• CPC Class Codes: G01B 9/02083 characterised by particular signal processing and presentation
• CPC Class Codes: G06N 10/00 Quantum computing, i.e. information processing based on quantum-mechanical phenomena
• CPC Class Codes: G06N 20/00 Machine learning

Abstract

A programmable photonic integrated circuit implements arbitrary linear optics transformations in the spatial mode basis with high fidelity. Under a realistic fabrication model, we analyze programmed implementations of the CNOT gate, CPHASE gate, iterative phase estimation algorithm, state preparation, and quantum random walks. We find that programmability dramatically improves device tolerance to fabrication imperfections and enables a single device to implement a broad range of both quantum and classical linear optics experiments. Our results suggest that existing fabrication processes are sufficient to build such a device in the silicon photonics platform.

Claims

1. A photonic integrated circuit for performing quantum information processing, the photonic integrated circuit comprising:

a semiconductor substrate;

a plurality of interconnected variable beam splitters, fabricated in the semiconductor substrate, to perform at least one linear optical transformation on a plurality of optical modes coupled into the plurality of interconnected variable beam splitters;

a plurality of detectors, in optical communication with the plurality of variable beam splitters, to measure an output state of the plurality of optical modes; and

control circuitry, operably coupled to the plurality of interconnected variable beam splitters and to the plurality of detectors, to determine a fidelity of the output state of the plurality of optical modes to an ideal output state of the plurality of optical modes and to adjust a phase setting of at least one variable beam splitter in the plurality of interconnected variable beam splitters so as to increase the fidelity of the output state of the plurality of optical modes to the ideal output state of the plurality of optical modes.

2. The photonic integrated circuit of claim 1, wherein the plurality of interconnected variable beam splitters comprises a plurality of interconnected Mach-Zehnder interferometers.

3. The photonic integrated circuit of claim 2, wherein the plurality of interconnected Mach-Zehnder interferometers comprises at least 10 interconnected Mach-Zehnder interferometers.

4. The photonic integrated circuit of claim 2, wherein the plurality of interconnected Mach-Zehnder interferometers is configured to implement a quantum optical circuit comprising at least one of a CNOT gate, a CPHASE gate, an iterative phase estimation, a single qubit rotation, and/or a quantum random walk.

5. The photonic integrated circuit of claim 2, wherein the plurality of interconnected Mach-Zehnder interferometers is characterized by a distribution of splitting ratios having a first variance and by a distribution of optical losses having a second variance, the first variance and the second variance reducing the fidelity of the output state of the plurality of optical modes to the ideal output state of the plurality of optical modes.

6. The photonic integrated circuit of claim 5, wherein the plurality of interconnected Mach-Zehnder interferometers comprises at least one waveguide, and

wherein first variance is due at least in part to a variation in a width and/or height of the at least one waveguide.

7. The photonic integrated circuit of claim 5, wherein the second variance is due at least in part to variations in absorption among the plurality of interconnected Mach-Zehnder interferometers.

8. The photonic integrated circuit of claim 2, wherein the control circuitry is configured to adjust the phase setting of the at least one Mach-Zehnder interferometer so as to increase the fidelity to at least about 99% for 10,000 instances of the at least one linear optical transformation.

9. The photonic integrated circuit of claim 2, further comprising:

at least one feedback loop, in optical communication with the plurality of interconnected Mach-Zehnder interferometers, to guide at least one optical mode from an output of the plurality of interconnected Mach-Zehnder interferometers to an input of the plurality of interconnected Mach-Zehnder interferometers.

10. The photonic integrated circuit of claim 9, further comprising:

at least one variable coupler, in optical communication with the at least one feedback loop, to vary a power of the at least one optical mode guided from the output of the plurality of interconnected Mach-Zehnder interferometers to the input of the plurality of interconnected Mach-Zehnder interferometers.

11. A method of performing quantum information processing, the method comprising:

(A) coupling a plurality of optical modes into a plurality of interconnected variable beam splitters fabricated in a semiconductor substrate so as to perform at least one linear optical transformation on the plurality of optical modes;

(B) detecting the plurality of optical modes at an output of the plurality of interconnected variable beam splitters;

(C) determining a fidelity of the output state of the plurality of optical modes to an ideal output state of the plurality of optical modes; and

(D) adjusting at least one phase of at least one variable beam splitter in the plurality of interconnected variable beam splitter so as to increase the fidelity of the output state of the plurality of optical modes to the ideal output state of the plurality of optical modes.

12. The method of claim 11, wherein (A) comprises coupling the plurality of optical modes into a plurality of interconnected Mach Zehnder interferometers.

13. The method of claim 12, wherein (A) comprises coupling at least 10 optical modes into the plurality of interconnected Mach-Zehnder interferometers.

14. The method of claim 12, wherein (A) comprises implementing at least one of a CNOT gate, a CPHASE gate, an iterative phase estimation, and a quantum random walk.

15. The method of claim 12, wherein the plurality of interconnected Mach-Zehnder interferometers is characterized by a distribution of splitting ratios having a first variance and by a distribution of optical losses having a second variance, the first variance and the second variance reducing the fidelity of the output state of the plurality of optical modes to the ideal output state of the plurality of optical modes.

16. The method of claim 15, wherein (A) comprises coupling the plurality of optical modes into at least one waveguide, and

wherein first variance is due at least in part to a variation in a width and/or height of the at least one waveguide.

17. The method of claim 15, wherein the second variance is due at least in part to variations in absorption among the plurality of interconnected Mach-Zehnder interferometers.

18. The method of claim 12, wherein (D) comprises adjusting the at least one phase setting of the at least one Mach-Zehnder interferometer so as to increase the fidelity to at least about 99% for 10,000 instances of the at least one linear optical transformation.

19. The method of claim 18, further comprising:

guiding at least one optical mode from an output of the plurality of interconnected Mach-Zehnder interferometers to an input of the plurality of interconnected Mach-Zehnder interferometers.

20. The method of claim 19, further comprising:

varying a power of the at least one optical mode guided from the output of the plurality of interconnected Mach-Zehnder interferometers to the input of the plurality of interconnected Mach-Zehnder interferometers.

21. A photonic integrated circuit for performing quantum information processing, the photonic integrated circuit comprising:

a semiconductor substrate;

a plurality of interconnected Mach-Zehnder interferometers, fabricated in the semiconductor substrate, to perform at least one linear optical transformation on a plurality of optical modes coupled into the plurality of interconnected Mach-Zehnder interferometers, the plurality of interconnected Mach-Zehnder interferometers being characterized by a distribution of splitting ratios having a first variance and by a distribution of optical losses having a second variance;

a plurality of detectors, in optical communication with the plurality of Mach-Zehnder interferometers, to measure an output state of the plurality of optical modes; and

control circuitry, operably coupled to the plurality of interconnected Mach-Zehnder interferometers and to the plurality of detectors, to determine a fidelity of the output state of the plurality of optical modes to an ideal output state of the plurality of optical modes and to adjust a phase setting of at least one Mach-Zehnder interferometer in the plurality of interconnected Mach-Zehnder interferometers so as to increase the fidelity of the output state of the plurality of optical modes to the ideal output state of the plurality of optical modes; and

at least one feedback loop, in optical communication with the plurality of interconnected Mach-Zehnder interferometers, to guide at least one optical mode from an output of the plurality of interconnected Mach-Zehnder interferometers to an input of the plurality of interconnected Mach-Zehnder interferometers,

wherein the first variance and the second variance reduce the fidelity of the output state of the plurality of optical modes to the ideal output state of the plurality of optical modes.

22. The photonic integrated circuit of claim 21, further comprising:

at least one variable coupler, in optical communication with the at least one feedback loop, to vary a power of the at least one optical mode guided from the output of the plurality of interconnected Mach-Zehnder interferometers to the input of the plurality of interconnected Mach-Zehnder interferometers.