Proceedings of Topical Meeting on Optoinformatics (pdf-format, 1.21 ...
Proceedings of Topical Meeting on Optoinformatics (pdf-format, 1.21 ...
Proceedings of Topical Meeting on Optoinformatics (pdf-format, 1.21 ...
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8 OPTOINFORMATICS’05<br />
OPTOELECTRONIC GATES ON BIPHOTONS<br />
Yu. A. Asikritova, I.D. Balatsky, V.N. Gorbachev, A.I Trubilko<br />
Nor'Westerly Institute <str<strong>on</strong>g>of</str<strong>on</strong>g> Printing <str<strong>on</strong>g>of</str<strong>on</strong>g> St.-Petersburg State<br />
University <str<strong>on</strong>g>of</str<strong>on</strong>g> Technology and Design 13, Djambula, St.-Petersburg,<br />
191180, Russia Tel: (+7 812) 164-6556 Fax: (+7 812) 164-6556<br />
Laboratory <str<strong>on</strong>g>of</str<strong>on</strong>g> Quantum In<strong>format</strong>i<strong>on</strong> and Computati<strong>on</strong>, St.-Petersburg<br />
State University <str<strong>on</strong>g>of</str<strong>on</strong>g> AeroSpace Instrumentati<strong>on</strong>, 67, Bolshaya<br />
Morskaya, St.-Petersburg, 190000<br />
E-mail: vn@vg3025.spb.edu<br />
A set <str<strong>on</strong>g>of</str<strong>on</strong>g> the measurement-based gates exploiting bipartite entanglement is<br />
c<strong>on</strong>sidered. These gates allow to perform any operati<strong>on</strong>s <strong>on</strong> given input states<br />
and can be implemented from biphot<strong>on</strong>s.<br />
Biphot<strong>on</strong>s or pairs <str<strong>on</strong>g>of</str<strong>on</strong>g> str<strong>on</strong>g correlated phot<strong>on</strong>s are well known in quantum optics<br />
and there is a significant progress in their generating and manipulating. Because <str<strong>on</strong>g>of</str<strong>on</strong>g> n<strong>on</strong>classical<br />
correlati<strong>on</strong> between phot<strong>on</strong>s their state is entangled and known as EPR (Einstein-<br />
Podolsky-Rosen) pair, that is a main resource <str<strong>on</strong>g>of</str<strong>on</strong>g> quantum in<strong>format</strong>i<strong>on</strong> processing. In our<br />
work we exploit the correlati<strong>on</strong> to achieve a set <str<strong>on</strong>g>of</str<strong>on</strong>g> logical gates with optical input and<br />
output. The gates proceed via measurement <strong>on</strong> the phot<strong>on</strong>s, when the measurement<br />
outcomes or photocurrent <str<strong>on</strong>g>of</str<strong>on</strong>g> detectors carry out the gate operati<strong>on</strong>.<br />
Our gates bel<strong>on</strong>g to the class <str<strong>on</strong>g>of</str<strong>on</strong>g> the measurement based circuits, that perform<br />
computati<strong>on</strong>s using quantum measurement as primitive. This idea has been introduced by<br />
Gottesman and Chuang [1] and developed by many authors. In fact, any gate changes the<br />
input state by transforming it into output. The state <str<strong>on</strong>g>of</str<strong>on</strong>g> the physical system can be changed<br />
by two ways. First is an unitary evoluti<strong>on</strong> due from interacti<strong>on</strong> between physical systems,<br />
sec<strong>on</strong>d is quantum projective measurement. Now there are two models <str<strong>on</strong>g>of</str<strong>on</strong>g> the measurement<br />
based computati<strong>on</strong>. First is teleportati<strong>on</strong> quantum computati<strong>on</strong> (TQC) [1,2] with gates based<br />
<strong>on</strong> teleportati<strong>on</strong>. Sec<strong>on</strong>d is <strong>on</strong>e-way quantum computer (1WQC) introduced Briegel [3] in<br />
which computati<strong>on</strong> proceeds via local single-qubit measurements <strong>on</strong> the multiparticle<br />
entangled states, known as cluster or graph states. An experimental implementati<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
1WQC using four-qubit optical cluster states have been dem<strong>on</strong>strated by Zeilinger [4] .<br />
We c<strong>on</strong>sider a versi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the measurement based gates using biphot<strong>on</strong>s. The key idea<br />
is a str<strong>on</strong>g correlati<strong>on</strong> between pair <str<strong>on</strong>g>of</str<strong>on</strong>g> phot<strong>on</strong>s A and B from biphot<strong>on</strong>. Let phot<strong>on</strong> A is<br />
measured, then the remainder phot<strong>on</strong> B is projected into a state dependent from the<br />
measurement outcome. Therefore there is a str<strong>on</strong>g correlati<strong>on</strong> between the quantum state <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
B phot<strong>on</strong> and the measurement outcomes (or photocurrent <str<strong>on</strong>g>of</str<strong>on</strong>g> detector) which are nice<br />
electr<strong>on</strong>ic replica <str<strong>on</strong>g>of</str<strong>on</strong>g> B.