Universal linear components

Patent metadata

Field	Value
Publication number	US-10534189-B2
Application number	US-201314092565-A
Country	US
Kind code	B2
Filing date	Nov 27, 2013
Priority date	Nov 27, 2012
Publication date	Jan 14, 2020
Grant date	Jan 14, 2020

Abstract

Universal linear components are provided. In general, a P input and Q output wave combiner is connected to a Q input and R output wave mode synthesizer via Q amplitude and/or phase modulators. The wave combiner and wave mode synthesizer are both linear, reciprocal and lossless. The wave combiner and wave mode synthesizer can be implemented using waveguide technology. This device can provide any desired linear transformation of spatial modes between its inputs and its outputs. This capability can be generalized to any linear transformation by using representation converters to convert other quantities to spatial mode patterns. The wave combiner and wave mode synthesizer are also useful separately, and can enable applications including self-adjusting mode coupling, optimal multi-mode communication, and add-drop capability in a multi-mode system. Control of the wave combiner and wave mode synthesizer can be implemented with single-variable optimizations.

First claim

The invention claimed is:

1. An N to one coherent integrated optical wave combiner having N≥2 inputs and a single output, the apparatus comprising:
a coherent integrated optical interferometer network that operates substantially on single spatial modes and is substantially linear, reciprocal and lossless, and which includes N−1 2×2 adjustable wave splitters connected in series, configured such that the contribution of each of the N inputs to the output is adjustable in both amplitude and relative phase;
wherein the coherent integrated optical interferometer network provides N−1 control ports at which waves not coupled to the output are emitted, wherein the N−1 control ports are in one to one correspondence with the N−1 2×2 adjustable wave splitters; and
N−1 detectors disposed at the control ports and in one to one correspondence with the N−1 2×2 adjustable wave splitters;
wherein amplitude splits and phase shifts of the coherent integrated optical interferometer network are determined in operation by adjusting them one at a time in a single-pass adjustment sequence to sequentially null signals from the N−1 detectors;
wherein the signals from the N−1 detectors are minimized by adjusting the amplitude splits and phase shifts of the corresponding 2×2 adjustable wave splitter;
wherein each input and the output are substantially single-spatial-mode.

2. The coherent integrated optical wave combiner of claim 1 wherein the 2×2 adjustable wave splitters comprise one or more waveguide Mach-Zehnder interferometers.

3. A P input to Q output coherent integrated optical wave combiner having P≥2 and 2≤Q≤P, the apparatus comprising:
Q combiners indexed by an integer i (1≤i≤Q), wherein each combiner i for 1≤i≤min(Q, P−1) is a P+1−i to one coherent integrated optical wave combiner according to claim 1 ;
wherein inputs of combiner i for i≥2 are provided by the control ports of combiner i −1; and
wherein the detectors of combiner i for i<Q are tap detectors that absorb less than 50% of the incident light and transmit the remainder;
whereby the P input to Q output coherent integrated optical wave combiner includes P(P−1)/2−(P−Q)(P−Q−1)/2 2×2 adjustable wave splitters.

4. The P input to Q output coherent integrated optical wave combiner of claim 3 , wherein the tap detectors absorb less than 10% of the incident light and transmit the remainder.

5. An N to one coherent integrated optical wave combiner having N≥2 inputs and a single output, the apparatus comprising:
a coherent integrated optical interferometer network that operates substantially on single spatial modes and is substantially linear, reciprocal and lossless, and which includes N−1 adjustable 2×2 wave splitters connected in series, configured such that the contribution of each of the N inputs to the output is adjustable in both amplitude and relative phase;
wherein the coherent integrated optical interferometer network provides N−1 control ports at which waves not coupled to the output are emitted, wherein the N−1 control ports are in one to one correspondence with the N−1 2×2 adjustable wave splitters; and
an output detector disposed at the output;
wherein amplitude splits and phase shifts of the coherent integrated optical interferometer network are determined in operation by adjusting them one at a time in a single-pass adjustment sequence to sequentially maximize a signal from the output detector;
wherein each input and the output are substantially single-spatial-mode.

6. The coherent integrated optical wave combiner of claim 5 , wherein the output detector is a tap detector that absorbs less than 50% of the incident light and transmits the remainder.

7. A P input to Q output coherent integrated optical wave combiner having P≥2 and 2≤Q≤P, the apparatus comprising:
Q combiners indexed by an integer i (1≤i≤Q), wherein each combiner i for 1≤i≤min(Q, P−1) is a P+1−i to one coherent integrated optical wave combiner according to claim 5 ;
wherein inputs of combiner i for i≥2 are provided by the control ports of combiner i−1;
whereby the P input to Q output coherent integrated optical wave combiner includes P(P−1)/2−(P−Q)(P−Q−1)/2 2×2 adjustable wave splitters.

8. A one to N coherent integrated optical wave mode synthesizer having one input and N≥2 outputs, the apparatus comprising:
a coherent integrated optical interferometer network that operates substantially on single spatial modes and is substantially linear, reciprocal and lossless, and which includes 2×2 adjustable wave splitters connected in series, configured such that the contribution of the input to each of the N outputs is adjustable in both amplitude and relative phase;
wherein the coherent integrated optical interferometer network provides N−1 control ports at which waves incident on the outputs can be emitted, wherein the N−1 control ports are in one to one correspondence with the N−1 2×2 adjustable wave splitters; and
N−1 detectors disposed at the control ports and in one to one correspondence with the N−1 2×2 adjustable wave splitters;
wherein amplitude splits and phase shifts of the coherent integrated optical interferometer network are determined in operation by adjusting them one at a time in a single-pass adjustment sequence to sequentially null signals from the N−1 detectors when the N outputs are illuminated with a phase-conjugated version of a desired output mode;
wherein the signals from the N−1 detectors are minimized by adjusting the amplitude splits and phase shifts of the corresponding 2×2 adjustable wave splitter;
wherein the input and each output are substantially single-spatial-mode.

9. The coherent integrated optical wave mode synthesizer of claim 8 wherein the 2×2 adjustable wave splitters comprise one or more waveguide Mach-Zehnder interferometers.

10. A Q input to R output coherent integrated optical wave mode synthesizer having Q≥2 and 2≤Q≤R, the apparatus comprising:
Q mode synthesizers indexed by an integer i (1≤i≤Q), wherein each mode synthesizer i for 1≤i≤min(Q, R−1) is a one to R+1−i coherent integrated optical wave mode synthesizer according to claim 8 ;
wherein outputs of mode synthesizer i for i≥2 are provided to the control ports of mode synthesizer i −1 as inputs; and
wherein the detectors of mode synthesizer i for i<R are tap detectors that absorb less than 50% of the incident light and transmit the remainder;
whereby the Q input to R output coherent integrated optical wave mode synthesizer includes R(R−1)/2−(R−Q)(R−Q−1)/2 2×2 adjustable wave splitters.

11. The coherent integrated optical wave mode synthesizer of claim 10 , wherein the tap detectors absorb less than 10% of the incident light and transmit the remainder.

12. A one to N coherent integrated optical wave mode synthesizer having one input and N≥2 outputs, the apparatus comprising:
a coherent integrated optical interferometer network that operates substantially on single spatial modes and is substantially linear, reciprocal and lossless, and which includes N−1 2×2 adjustable wave splitters connected in series, configured such that the contribution of the input to each of the N outputs is adjustable in both amplitude and relative phase;
wherein the coherent integrated optical interferometer network provides N−1 control ports at which waves incident on the outputs can be emitted, wherein the N−1 control ports are in one to one correspondence with the N−1 2×2 adjustable wave splitters; and
an input detector disposed at the input and capable of detecting radiation incident on the outputs that is coupled to the input;
wherein amplitude splits and phase shifts of the coherent integrated optical interferometer network are determined in operation by adjust

Assignees

• Univ Leland Stanford Junior

Inventors

• Miller David A B

Classifications

• G02B27/145 Primary

  having sequential partially reflecting surfaces · CPC title

• G02F1/0136

  for the control of polarisation, e.g. state of polarisation [SOP] control, polarisation scrambling, TE-TM mode conversion or separation (G02F1/0353 takes precedence) · CPC title

• G02F1/31

  Digital deflection, {i.e. optical switching}(G02F1/33 takes precedence) · CPC title

• G02F2001/212

  Physics · mapped topic

• G06F40/45

  Example-based machine translation; Alignment · CPC title