2017
DOI: 10.1103/physrevlett.118.060501
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Unifying Gate Synthesis and Magic State Distillation

Abstract: The leading paradigm for performing computation on quantum memories can be encapsulated as distill-thensynthesize. Initially, one performs several rounds of distillation to create high-fidelity magic states that provide one good T gate, an essential quantum logic gate. Subsequently, gate synthesis intersperses many T gates with Clifford gates to realise a desired circuit. We introduce a unified framework that implements one round of distillation and multi-qubit gate synthesis in a single step. Typically, our m… Show more

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Cited by 49 publications
(52 citation statements)
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“…[45,46]), γγ + 2 jets [47,48,49], γγ + 2 b-jets [50] and γγ + 3 jets [49]. Owing to the computational simplifications of smooth cone isolation (with respect to standard cone isolation), some hadron collider processes with one final-state photon, such as associated Zγ [51,52,53] and W γ [52] production and inclusive single-photon production [54], have also been computed up to the NNLO in QCD perturbation theory.…”
Section: Introductionmentioning
confidence: 99%
“…[45,46]), γγ + 2 jets [47,48,49], γγ + 2 b-jets [50] and γγ + 3 jets [49]. Owing to the computational simplifications of smooth cone isolation (with respect to standard cone isolation), some hadron collider processes with one final-state photon, such as associated Zγ [51,52,53] and W γ [52] production and inclusive single-photon production [54], have also been computed up to the NNLO in QCD perturbation theory.…”
Section: Introductionmentioning
confidence: 99%
“…(b) The integrated lattice 'AC' and (c) the separated lattices 'A' and 'C', after merging and splitting 'A' and 'C', respectively. states is not fault-tolerant and produces states with low fidelity that need to be purified by a non-deterministic procedure called state distillation [45][46][47][48][49]. This distillation procedure is repeated until the measurement results indicate one state is successfully purified.…”
Section: Quantum Error Correctionmentioning
confidence: 99%
“…For fully differential exclusive cross sections, QCD corrections to the second order (next-to-next-to-leading order, NNLO) were computed for the 2 → 1 processes vectorboson production [6,7] and Higgs-boson production [8,9] already about a decade ago. In recent years, NNLO calculations have become available for many 2 → 2 reactions at hadron colliders: pp → γγ [10], pp → V H [11], pp → V γ [12], pp → tt [13,14], pp → H+j [15,16], pp → W + j [17,18], pp → Z + j [19,20], pp → γ + X [21], pp → ZZ [22], pp → WW [23], pp → ZW [24] and pp → 2j [25], as well as for the electron-positron collisions e + e − → 3j [26,27] and lepton-proton processes ep → 1j [28] ep → 2j [29] and for the related 2 → 3 hadron-collider process of Higgs production in vector boson fusion [30,31]. These NNLO calculations of fully differential exclusive cross sections were enabled by substantial methodological developments [31][32][33][34][35][36][37][38] of infrared subtraction methods for the handling of singular contributions that appear in all parton-level subprocesses.…”
Section: Introductionmentioning
confidence: 99%