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Electronics and Communications in Japan (Part III Fundamental Electronic Science)

On a construction of a nonstabilizer clifford quantum code for 2h(2j+1)‐level states

Manabu Hagiwara, Hideki Imai

Published Dec 13, 2006• 0 citations
Publisher

Abstract

Abstract The construction of an infinite number of nonstabilizer codes of Clifford type was given for the first time by the authors. However, the method of construction was restricted to encoding from odd prime p‐level quantum states to 2p‐level states. In this paper, the result is extended to the construction of nonstabilizer‐type quantum codes which encode quantum states of arbitrary odd 2j+1‐level to quantum states of 2h(2j+1)‐level, where h are mutually prime 2j+1. © 2006 Wiley Periodicals, Inc. Electron Comm Jpn Pt 3, 90(4): 63 – 68, 2007; Published online in Wiley InterScience ( www.interscience.wiley.com ). DOI 10.1002/ecjc.20222

DOI
10.1002/ecjc.20222

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Abstract The construction of an infinite number of nonstabilizer codes of Clifford type was given for the first time by the authors. However, the method of construction was restricted to encoding from odd prime p‐level quantum states to 2p‐level states. In this paper, the result is extended to the construction of nonstabilizer‐type quantum codes which encode quantum states of arbitrary odd 2j+1‐level to quantum states of 2h(2j+1)‐level, where h are mutually prime 2j+1. © 2006 Wiley Periodicals, Inc. Electron Comm Jpn Pt 3, 90(4): 63 – 68, 2007; Published online in Wiley InterScience ( www.interscience.wiley.com ). DOI 10.1002/ecjc.20222
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Recent work has shown that quantum double models can be used to circumvent the Bravyi-Koenig bound. In particular, this is achieved through code-switching protocols in which non-Pauli stabilizer phases appear as intermediate codes. We introduce the XCd(k)X\mathcal C^{(k)}_dXCd(k)​ stabilizer formalism, which generalizes the Pauli stabilizer formalism by combining Pauli-XXX operators with diagonal operators drawn from a fixed level kkk of the Clifford hierarchy on prime-dimensional qudits. This yields a natural class of beyond-Pauli stabilizer models, including many twisted quantum double phases. We classify a large class of these XCd(k)X\mathcal C^{(k)}_dXCd(k)​ stabilizer states, showing that they are uniform superpositions over affine-linear subspaces with diagonal phases. In particular, when the stabilizers of a state require operators from level kkk of the Clifford hierarchy, we show that the diagonal gates required to produce the phases in the wavefunction sit one level higher. We further show that every 2D twisted quantum double Dω(Zpn){\cal D}^ω(\mathbb{Z}_p^n)Dω(Zpn​) with ωωω a product of type-III cocycles and ppp an odd prime admits a realization using only Clifford (k=2k=2k=2) stabilizers, and we conjecture that phases where ωωω contains a type-I or type-II cocycle require level-ppp Clifford-hierarchy stabilizers for ppp-dimensional qudits. Finally, we demonstrate that a pair of qudit toric codes may be deterministically prepared in a logical magic state by measuring XCd(k)X\mathcal C^{(k)}_dXCd(k)​ stabilizers. Together, these results provide a concrete stabilizer framework for topological codes beyond Pauli stabilizer models and their logical gates.
This paper is motivated by the computer-generated nonadditive code described in Rains et al\cite{rains97nonadditive}. We describe a theory of non-stabilizer codes of which the nonadditive code of Rains et al is an example. Furthermore, we give a general strategy of constructing good nonstabilizer codes from good stabilizer codes and give some explicit constructions and asymptotically good nonstabilizer codes. Like in the case of stabilizer codes, we can design fairly efficient encoding and decoding procedures.