Further Compactifying Linear Optical Unitaries
About
Quantum integrated photonics requires large-scale linear optical circuitry, and for many applications it is desirable to have a universally programmable circuit, able to implement an arbitrary unitary transformation on a number of modes. This has been achieved using the Reck scheme, consisting of a network of Mach Zehnder interferometers containing a variable phase shifter in one path, as well as an external phase shifter after each Mach Zehnder. It subsequently became apparent that with symmetric Mach Zehnders containing a phase shift in both paths, the external phase shifts are redundant, resulting in a more compact circuit. The rectangular Clements scheme improves on the Reck scheme in terms of circuit depth, but it has been thought that an external phase-shifter was necessary after each Mach Zehnder. Here, we show that the Clements scheme can be realised using symmetric Mach Zehnders, requiring only a small number of external phase-shifters that do not contribute to the depth of the circuit. This will result in a significant saving in the length of these devices, allowing more complex circuits to fit onto a photonic chip, and reducing the propagation losses associated with these circuits. We also discuss how similar savings can be made to alternative schemes which have robustness to imbalanced beam-splitters.
Related benchmarks
| Task | Dataset | Result | Rank | |
|---|---|---|---|---|
| Image Classification | MNIST (test) | Accuracy97.6 | 882 | |
| Image Classification | MNIST (val) | Accuracy96.06 | 55 | |
| Classification | DIGITS (test) | -- | 49 | |
| Image Classification | MNIST (train) | Training Loss0.0634 | 12 | |
| Classification | Iris (test) | Accuracy96 | 10 | |
| Classification | Iris (train) | Training Loss0.0896 | 4 | |
| Classification | Iris (val) | Accuracy98.75 | 4 | |
| Classification | Digits (val) | Accuracy94.72 | 4 | |
| Classification | Olivetti (train) | Training Loss0.2648 | 4 | |
| Classification | Olivetti (test) | Accuracy70.5 | 4 |