Methods, systems, and apparatus for programmable quantum photonic processing

• US 9,791,258 B2
• Filed: 04/29/2016
• Issued: 10/17/2017
• 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:
  US15/143,450
• Publication Number:
  US 20160245639A1
• Time in Patent Office: 536 Days
• Field of Search: None
• 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 Mach-Zehnder interferometers, fabricated in the semiconductor substrate, to perform an arbitrary unitary optical transformation on at least one optical mode, the plurality of interconnected Mach-Zehnder interferometers having a plurality of input waveguides to receive the at least one optical mode and a plurality of output waveguides to output the at least one optical mode after the arbitrary unitary optical transformation;

a plurality of detectors, in optical communication with the plurality of output waveguides, to measure the at least one optical mode after the arbitrary unitary optical transformation; and

control circuitry, operably coupled to the plurality of Mach-Zehnder interferometers and to the plurality of detectors, to determine a density distribution of the at least one optical mode at the plurality of output waveguides and to adjust a phase setting of at least one Mach-Zehnder interferometer in the plurality of interconnected Mach-Zehnder interferometers so as to change the density distribution of the at least one optical mode at the plurality of output waveguides.

2. The photonic integrated circuit of claim 1, wherein the at least one Mach-Zehnder interferometer in the plurality of interconnected Mach-Zehnder interferometers comprises a phase shifter operably coupled to an output arm of the at least one Mach-Zehnder interferometer.

3. The photonic integrated circuit of claim 1, wherein the phase shifter comprises a heater.

4. The photonic integrated circuit of claim 1, wherein the plurality of interconnected Mach-Zehnder interferometers comprises at least 10 interconnected Mach-Zehnder interferometers.

5. The photonic integrated circuit of claim 1, 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.

6. The photonic integrated circuit of claim 1, wherein the control circuitry is configured to adjust the phase setting of the at least one Mach-Zehnder interferometer so as to decrease Anderson localization of the at least one optical mode at the plurality of output waveguides.

7. The photonic integrated circuit of claim 1, wherein the control circuitry is configured to apply a random phase settings along a propagation direction of the at least one optical mode in the plurality of interconnected Mach-Zehnder interferometers so as to create a time-dependent disorder in the plurality of interconnected Mach-Zehnder interferometers.

8. The photonic integrated circuit of claim 1, wherein the at least one optical mode comprises a single optical mode and the arbitrary unitary optical transformation distributes the single optical mode across at least 40 output waveguides.

9. The photonic integrated circuit of claim 1, wherein the at least one optical mode comprises a plurality of optical modes and the arbitrary unitary optical transformation distributes the plurality of optical modes across the plurality of output waveguides.

10. The photonic integrated circuit of claim 1, further comprising:

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

11. The photonic integrated circuit of claim 1, further comprising:

at least one variable coupler, in optical communication with the at least one feedback loop, to vary a power of the output guided from the at least one output waveguide to the at least one input waveguide.

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

(A) coupling at least one optical mode into a plurality of input waveguides of a plurality of interconnected Mach-Zehnder interferometers fabricated in a semiconductor substrate so as to perform an arbitrary unitary optical transformation on the at least one optical mode;

(B) detecting the at least one optical mode at a plurality of output waveguides of the plurality of interconnected Mach-Zehnder interferometers;

(C) determining a density distribution of the at least one optical mode across the plurality of the output waveguides; and

(D) adjusting a phase setting of at least one Mach-Zehnder interferometers in the plurality of interconnected Mach-Zehnder interferometers so as to change the density distribution of the at least one optical mode.

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 (A) comprises coupling a single optical mode into the plurality of interconnected Mach-Zehnder interferometers, and further comprising:

transmitting the single optical mode via at least 40 output waveguides after the arbitrary unitary optical transformation.

16. The method of claim 12, wherein (D) comprises adjusting a temperature of a heater operably coupled to an output arm of the at least one Mach-Zehnder interferometer.

17. The method of claim 12, wherein (D) comprises applying a random phase setting along a propagation direction of the at least one optical mode in the plurality of interconnected Mach-Zehnder interferometers so as to create a time-dependent disorder in the plurality of interconnected Mach-Zehnder interferometers.

18. The method of claim 12, wherein (D) comprises adjusting the phase setting of the at least one Mach-Zehnder interferometer so as to reduce Anderson localization of the at least one optical mode at the plurality of output waveguides.

19. The method of claim 12, further comprising:

guiding output from at least one output waveguide in the plurality of output waveguides to an input waveguide in the plurality of input waveguides.

20. The method of claim 12, further comprising:

varying a power of the output guided from the at least one output waveguide of the plurality of interconnected Mach-Zehnder interferometers to the at least one input waveguide 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, at least one Mach-Zehnder interferometer in the plurality of interconnected Mach-Zehnder interferometers comprising a heater operably coupled to an output arm of the at least one Mach-Zehnder interferometer;

a plurality of detectors, in optical communication with the plurality of Mach-Zehnder interferometers, to measure the plurality of optical modes at a plurality of output waveguides of the plurality of interconnected Mach-Zehnder interferometers;

control circuitry, operably coupled to the plurality of interconnected Mach-Zehnder interferometers and to the plurality of detectors, to determine a density distribution of the plurality of optical modes at the plurality of output waveguides and to adjust a temperature of the heater in the at least one Mach-Zehnder interferometer so as to change the density distribution of the plurality of optical modes at the plurality of output waveguides; 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 at least one output waveguide in the plurality of output waveguides to an input of the plurality of interconnected Mach-Zehnder interferometers.