Generators and Relations for Real Stabilizers
dc.contributor.author | Makary, Justin J. | |
dc.contributor.copyright-release | Not Applicable | en_US |
dc.contributor.degree | Master of Science | en_US |
dc.contributor.department | Department of Mathematics & Statistics - Math Division | en_US |
dc.contributor.ethics-approval | Not Applicable | en_US |
dc.contributor.external-examiner | n/a | en_US |
dc.contributor.graduate-coordinator | Dr. David Iron | en_US |
dc.contributor.manuscripts | Not Applicable | en_US |
dc.contributor.thesis-reader | Dr. Dorette Pronk | en_US |
dc.contributor.thesis-reader | Dr. Peter Selinger | en_US |
dc.contributor.thesis-supervisor | Dr. Neil J. Ross | en_US |
dc.date.accessioned | 2020-09-02T11:14:51Z | |
dc.date.available | 2020-09-02T11:14:51Z | |
dc.date.defence | 2020-08-20 | |
dc.date.issued | 2020-09-02T11:14:51Z | |
dc.description.abstract | Real stabilizer operators, which are also known as real Clifford operators, are generated, through composition and tensor product, by the Hadamard gate, the Pauli Z gate, and the controlled-Z gate. We introduce a normal form for real stabilizer circuits and show that every real stabilizer operator admits a unique normal form. Moreover, we give a finite set of relations that suffice to rewrite any Clifford circuit to its normal form. This yields a presentation by generators and relations of the strict spatial monoidal category of real stabilizer operators. | en_US |
dc.identifier.uri | http://hdl.handle.net/10222/79798 | |
dc.language.iso | en | en_US |
dc.subject | Quantum Computation | en_US |
dc.subject | Quantum Circuits | en_US |
dc.subject | Clifford Circuits | en_US |
dc.subject | Stabilizer Circuits | en_US |
dc.subject | Generators and Relations | en_US |
dc.title | Generators and Relations for Real Stabilizers | en_US |
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