誤差を許容する普遍的な量子計算への道
Earl T Campbell1, Barbara M Terhal2,3, Christophe Vuillot2
1Department of Physics and Astronomy, University of Sheffield, Sheffield, UK.
Nature
|September 15, 2017
まとめ
研究者たちは 情報を処理できる 容認性のある量子コンピュータを開発しています 現在の取り組みは 騒音に耐える論理量子ビットの作成に焦点を当てています これは複雑な計算のための 信頼性の高い量子プロセッサの構築に向けた重要なステップです
科学分野:
- 量子コンピューティング
- 情報処理
- 欠陥耐性アーキテクチャ
背景:
- 実践的な量子コンピュータには 情報の記憶だけでなく 処理能力も必要です
- 量子システムにおけるノイズによるエラーの拡散を防ぐために欠陥耐性アーキテクチャは不可欠です.
- 現在の研究は 量子計算の基本要素である 騒音に耐える 論理量子ビットへと進んでいます
研究 の 目的:
- 量子デバイスを単なるメモリユニットから機能的なプロセッサに変換するための要件を概説します.
- 論理量子ビットで普遍的な量子ゲートセットを実行するための方法を調査する.
- 既存のゲート導入提案のリソース需要を評価し,代替案を探求する.
主な方法:
- 騒音耐性論理量子ビットの 現在の実験の進展を 検討する
- マジックステート蒸留とカラーコード技術を含む,普遍的なゲート実装の主要な提案を分析する.
- モジュラーアーキテクチャ内の高次元量子コードを使用する代替スキームの探索.
主要な成果:
- 現在の実験では 騒音に耐える論理量子ビットへの 最初のステップが示されています
- 普遍的なゲート実装 (マジックステート蒸留,カラーコード) の主要な提案は,高いリソース要求で注目されています.
- モジュラーアーキテクチャで高次元量子コードを使用する代替アプローチは潜在的ですが,さらなる調査が必要です.
結論:
- 量子デバイスをプロセッサに変換するには,普遍的なゲート操作を定義する必要があります.
- ゲート導入の既存の方法は 重要なリソースの課題に直面しています
- 高次元の量子コードやモジュラーアーキテクチャを含む代替スキームに関するさらなる研究は,実用的な量子コンピューティングの進歩に不可欠です.
関連する概念動画
Ampere-Maxwell's Law: Problem-Solving
1.0K
A parallel-plate capacitor with capacitance C, whose plates have area A and separation distance d, is connected to a resistor R and a battery of voltage V. The current starts to flow at t = 0. What is the displacement current between the capacitor plates at time t? From the properties of the capacitor, what is the corresponding real current?
To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.
For the first part of the...
To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.
For the first part of the...
1.0K
The Quantum-Mechanical Model of an Atom
56.3K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
56.3K
Propagation of Uncertainty from Random Error
1.6K
An experiment often consists of more than a single step. In this case, measurements at each step give rise to uncertainty. Because the measurements occur in successive steps, the uncertainty in one step necessarily contributes to that in the subsequent step. As we perform statistical analysis on these types of experiments, we must learn to account for the propagation of uncertainty from one step to the next. The propagation of uncertainty depends on the type of arithmetic operation performed on...
1.6K
Propagation of Uncertainty from Systematic Error
1.2K
The atomic mass of an element varies due to the relative ratio of its isotopes. A sample's relative proportion of oxygen isotopes influences its average atomic mass. For instance, if we were to measure the atomic mass of oxygen from a sample, the mass would be a weighted average of the isotopic masses of oxygen in that sample. Since a single sample is not likely to perfectly reflect the true atomic mass of oxygen for all the molecules of oxygen on Earth, the mass we obtain from this...
1.2K
Ampere's Law: Problem-Solving
4.2K
Ampere's law states that for any closed looped path, the line integral of the magnetic field along the path equals the vacuum permeability times the current enclosed in the loop. If the fingers of the right hand curl along the direction of the integration path, the current in the direction of the thumb is considered positive. The current opposite to the thumb direction is considered negative.
Specific steps need to be considered while calculating the symmetric magnetic field distribution...
Specific steps need to be considered while calculating the symmetric magnetic field distribution...
4.2K
Fault Types
376
When analyzing a single line-to-ground fault from phase A to ground at a three-phase bus, it is important to consider the fault impedance. This impedance is zero for a bolted fault, equal to the arc impedance for an arcing fault, and represents the total fault impedance for a transmission-line insulator flashover. To derive sequence and phase currents, fault conditions are translated from the phase domain to the sequence domain.
For line-to-line faults occurring between phases B and C, the...
For line-to-line faults occurring between phases B and C, the...
376


