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A simple scheme for universal linear optics quantum computing with constant experimental complexity using fiber-loops
Quantum Physics · Submitted 2 Oct 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Here we show that the same architecture can be modified to implement full, universal linear optics quantum computing, in various incarnations.
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The abstract, sentence by sentence
Recently, Motes, Gilchrist, Dowling & Rohde [Phys. Rev. Lett. 113, 120501 (2014)] presented a scheme for photonic boson-sampling using a fiber-loop architecture. Here we show that the same architecture can be modified to implement full, universal linear optics quantum computing, in various incarnations. The scheme employs two embedded fiber-loops, a single push-button photon source, three dynamically controlled beamsplitters, and a single time-resolved photo-detector. The architecture has only a single point of interference, and thus may be significantly easier to align than other schemes. The experimental complexity of the scheme is constant, irrespective of the size of the computation, limited only by fiber lengths and their respective loss rates.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Recently, Motes, Gilchrist, Dowling & Rohde [Phys. Rev. Lett. 113, 120501 (2014)] presented a scheme for photonic boson-sampling using a fiber-loop architecture. | background 1.00 | 0.03 | 0.03 | asserted 0.99 |
| s1 | Here we show that the same architecture can be modified to implement full, universal linear optics quantum computing, in various incarnations. | contribution 1.00 | 0.91 | 0.84 | asserted 1.00 |
| s2 | The scheme employs two embedded fiber-loops, a single push-button photon source, three dynamically controlled beamsplitters, and a single time-resolved photo-detector. | method 0.96 | 0.75 | 0.09 | asserted 1.00 |
| s3 | The architecture has only a single point of interference, and thus may be significantly easier to align than other schemes. | interpretation 0.87 | 0.64 | 0.07 | hedged possibility 0.99 |
| s4 | The experimental complexity of the scheme is constant, irrespective of the size of the computation, limited only by fiber lengths and their respective loss rates. | result 0.74 | 0.81 | 0.40 | asserted 1.00 |
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Original abstract
Recently, Motes, Gilchrist, Dowling & Rohde [Phys. Rev. Lett. 113, 120501 (2014)] presented a scheme for photonic boson-sampling using a fiber-loop architecture. Here we show that the same architecture can be modified to implement full, universal linear optics quantum computing, in various incarnations. The scheme employs two embedded fiber-loops, a single push-button photon source, three dynamically controlled beamsplitters, and a single time-resolved photo-detector. The architecture has only a single point of interference, and thus may be significantly easier to align than other schemes. The experimental complexity of the scheme is constant, irrespective of the size of the computation, limited only by fiber lengths and their respective loss rates.
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For an elementary introduction to boson-sampling, see Gard et al. [ref] .
An introduction to boson-sampling · Introduction · 1.00
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