Abstract

We present magic state factory constructions for producing|CCZ⟩states and|T⟩states. For the|CCZ⟩factory we apply the surface code lattice surgery construction techniques described in \cite{fowler2018} to the fault-tolerant Toffoli \cite{jones2013, eastin2013distilling}. The resulting factory has a footprint of12d×6d(wheredis the code distance) and produces one|CCZ⟩every5.5dsurface code cycles. Our|T⟩state factory uses the|CCZ⟩factory's output and a catalyst|T⟩state to exactly transform one|CCZ⟩state into two|T⟩states. It has a footprint25%smaller than the factory in \cite{fowler2018} but outputs|T⟩states twice as quickly. We show how to generalize the catalyzed transformation to arbitrary phase angles, and note that the caseθ=22.5∘produces a particularly efficient circuit for producing|T⟩states. Compared to using the12d×8d×6.5d|T⟩factory of \cite{fowler2018}, our|CCZ⟩factory can quintuple the speed of algorithms that are dominated by the cost of applying Toffoli gates, including Shor's algorithm \cite{shor1994} and the chemistry algorithm of Babbush et al. \cite{babbush2018}. Assuming a physical gate error rate of10−3, our CCZ factory can produce∼1010states on average before an error occurs. This is sufficient for classically intractable instantiations of the chemistry algorithm, but for more demanding algorithms such as Shor's algorithm the mean number of states until failure can be increased to∼1012by increasing the factory footprint∼20%.

Highlights

  • In fault-tolerant quantum computation based on the surface code, the cost of a quantum algorithm is well approximated by the number of non-Clifford operations

  • We combine the |CCZ factory from Section 2 with the C2T factory from Section 3, producing a |T catalyzed T factory that transforms eight noisy |T states into two |T states with quadratically less noise. Note that this means we achieve a 4:1 ratio of input |T states to output |T state, which is competitive with the 3:1 ratio of block codes [4]

  • In this paper we presented two factories: a |CCZ factory and a catalyzed |T factory

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Summary

Introduction

In fault-tolerant quantum computation based on the surface code (a likely component of future error corrected quantum computers due to the surface code’s comparatively high threshold and planar connectivity requirements [3, 11, 29, 30, 13]), the cost of a quantum algorithm is well approximated by the number of non-Clifford operations. Note that our CCZ factory’s footprint includes an unused 2x4 area, adjacent to where the |CCZ state exits the factory (see Figure 1) This area can be used to hold target qubits waiting for a Toffoli operation, which helps with the routing overhead. We assume that the error rate of the |T0 states doubles while performing a level 0 T gate at distance 7 This increases the effective error of the |T1 states, but this contribution is overshadowed by the large size and proportionally small code distance of the level 1 T factory operating on these states.

Arbitrary-Angle Phase Catalysis
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