在被困离子量子模拟器中实现的动态拓相
Philipp T Dumitrescu1, Justin G Bohnet2, John P Gaebler2
1Center for Computational Quantum Physics, Flatiron Institute, New York, NY, USA. pdumitrescu@flatironinstitute.org.
Nature
|July 21, 2022
概括
研究人员在被困离子量子位中展示了一个新的动态拓阶段. 这一阶段为量子纠提供了强大的保护,对量子计算和传感应用至关重要.
科学领域:
- 量子信息科学
- 凝聚物质物理学
- 原子,分子和光学物理学
背景情况:
- 可编程的量子模拟器为研究远离平衡的量子动力学提供了新的途径.
- 精确控制量子多体纠对于量子传感和计算至关重要.
- 理论模型预测了纠操纵的拓稳固方法,但实验实现仍然具有挑战性.
研究的目的:
- 通过实验证明一个新兴的动态对称保护的拓阶段.
- 在此阶段研究边缘量子位的性能,
- 将近周期驱动系统与周期驱动系统的稳定性进行比较.
主要方法:
- 在Quantinuum的系统模型H1被困离子量子处理器上使用了十个yterbium-171 (171Yb+) 超细量子位的准周期驱动阵列.
- 设计了一个动态对称保护的拓阶段.
- 在各种扰动下分析边缘量子位的行为.
主要成果:
- 成功证明了一个新兴的动态对称保护的拓阶段.
- 观察到这一阶段内的边缘量子位被动态保护免受控制错误,交叉通话和迷路场.
- 与周期性驱动的边缘状态相比,这些边缘状态的稳定性更高.
结论:
- 由于新出现的动态对称性,演示阶段具有固有的错误弹性,对连贯扰动稳定.
- 与周期性驱动不同,近周期性驱动是实现这些强大的拓性质的关键.
- 这项工作为实施复杂的动态拓顺序的基础,用于对错误有弹性的量子信息处理.
相关概念视频
Phase Transitions
20.0K
Whether solid, liquid, or gas, a substance's state depends on the order and arrangement of its particles (atoms, molecules, or ions). Particles in the solid pack closely together, generally in a pattern. The particles vibrate about their fixed positions but do not move or squeeze past their neighbors. In liquids, although the particles are closely spaced, they are randomly arranged. The position of the particles are not fixed—that is, they are free to move past their neighbors to...
20.0K
Phase Transitions: Vaporization and Condensation
18.1K
The physical form of a substance changes on changing its temperature. For example, raising the temperature of a liquid causes the liquid to vaporize (convert into vapor). The process is called vaporization—a surface phenomenon. Vaporization occurs when the thermal motion of the molecules overcome the intermolecular forces, and the molecules (at the surface) escape into the gaseous state. When a liquid vaporizes in a closed container, gas molecules cannot escape. As these gas phase...
18.1K
The Quantum-Mechanical Model of an Atom
43.1K
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.
43.1K
Mass Analyzers: Common Types
701
The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
701
Fermi Level Dynamics
336
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
336
Atomic Nuclei: Nuclear Relaxation Processes
711
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
711


