3 research outputs found

    Magic state distillation with punctured polar codes

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    We present a scheme for magic state distillation using punctured polar codes. Our results build on some recent work by Bardet et al. (ISIT, 2016) who discovered that polar codes can be described algebraically as decreasing monomial codes. Using this powerful framework, we construct tri-orthogonal quantum codes (Bravyi et al., PRA, 2012) that can be used to distill magic states for the TT gate. An advantage of these codes is that they permit the use of the successive cancellation decoder whose time complexity scales as O(Nlog⁡(N))O(N\log(N)). We supplement this with numerical simulations for the erasure channel and dephasing channel. We obtain estimates for the dimensions and error rates for the resulting codes for block sizes up to 2202^{20} for the erasure channel and 2162^{16} for the dephasing channel. The dimension of the triply-even codes we obtain is shown to scale like O(N0.8)O(N^{0.8}) for the binary erasure channel at noise rate 0.010.01 and O(N0.84)O(N^{0.84}) for the dephasing channel at noise rate 0.0010.001. The corresponding bit error rates drop to roughly 8×10−288\times10^{-28} for the erasure channel and 7×10−157 \times 10^{-15} for the dephasing channel respectively.Comment: 18 pages, 4 figure

    Algebraic Properties of Polar Codes From a New Polynomial Formalism

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    Polar codes form a very powerful family of codes with a low complexity decoding algorithm that attain many information theoretic limits in error correction and source coding. These codes are closely related to Reed-Muller codes because both can be described with the same algebraic formalism, namely they are generated by evaluations of monomials. However, finding the right set of generating monomials for a polar code which optimises the decoding performances is a hard task and channel dependent. The purpose of this paper is to reveal some universal properties of these monomials. We will namely prove that there is a way to define a nontrivial (partial) order on monomials so that the monomials generating a polar code devised fo a binary-input symmetric channel always form a decreasing set. This property turns out to have rather deep consequences on the structure of the polar code. Indeed, the permutation group of a decreasing monomial code contains a large group called lower triangular affine group. Furthermore, the codewords of minimum weight correspond exactly to the orbits of the minimum weight codewords that are obtained from (evaluations) of monomials of the generating set. In particular, it gives an efficient way of counting the number of minimum weight codewords of a decreasing monomial code and henceforth of a polar code.Comment: 14 pages * A reference to the work of Bernhard Geiger has been added (arXiv:1506.05231) * Lemma 3 has been changed a little bit in order to prove that Proposition 7.1 in arXiv:1506.05231 holds for any binary input symmetric channe

    Magic state distillation with punctured polar codes

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    We present a scheme for magic state distillation using punctured polar codes. Our results build on some recent work by Bardet et al. [1] who discovered that polar codes can be described algebraically as decreasing monomial codes. Using this powerful framework, we construct tri-orthogonal codes [2] that can be used to distill magic states for the T gate. An advantage of these codes is that they permit the use of the successive cancellation decoder whose time complexity scales as O(N log(N)). We supplement this with numerical simulations for the erasure channel and dephasing channel. We obtain estimates for the dimensions and error rates for the resulting codes for block sizes up to 2 20 for the erasure channel and 2 16 for the dephasing channel. The dimension of the triply-even codes we obtain is shown to scale like O(N 0.8) for the binary erasure channel at noise rate 0.01 and O(N 0.84) for the dephasing channel at noise rate 0.001. The corresponding bit error rates drop to roughly 8 × 10 −28 for the erasure channel and 7 × 10 −15 for the dephasing channel respectively
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