高保真度旋转量子位操作和1K以上的算法初始化
Jonathan Y Huang1, Rocky Y Su2, Wee Han Lim2,3
1School of Electrical Engineering and Telecommunications, University of New South Wales, Sydney, New South Wales, Australia. yue.huang6@unsw.edu.au.
Nature
|March 28, 2024
概括
研究人员在1克尔文以上的中展示了自旋量子位的高保真性操作. 这一突破使得可扩展的量子计算能够克服热的限制,为容错的量子计算机铺平了道路.
科学领域:
- 量子计算
- 半导体物理
- 量子信息科学
背景情况:
- 半导体旋转量子比特为量子计算机提供了可扩展的途径.
- 高量子比特数量会产生超过当前冷却能力的热负荷.
- 容错的量子运算需要超过1克尔文以实现可扩展性.
研究的目的:
- 在高于1克尔文的温度下证明中自旋量子位的高保真性运行.
- 克服超出量子比特能量的热能限制,用于高保真性操作.
- 推进可扩展和容错的量子计算.
主要方法:
- 在1克尔文以上的中调整和操作自旋量子位.
- 开发一种用于纯二量子位状态的算法初始化协议.
- 使用射频读取用于量子位初始化和测量.
主要成果:
- 在读取和初始化方面达到99.34%的准确度.
- 一个量子比特的Clifford门的可靠性高达99.85%.
- 达到了98.92%的两位量子比特门忠实度.
结论:
- 高保真度旋转量子比特操作在1克尔文以上是可能的,克服了关键的可扩展性障碍.
- 展示的技术对于实现容错量子计算至关重要.
- 这项工作显著推动了大规模商业可行的量子计算机的开发.
相关概念视频
Atomic Nuclei: Nuclear Spin State Population Distribution
974
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
974
Atomic Nuclei: Nuclear Spin State Overview
938
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of...
938
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
1.0K
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
1.0K
Atomic Nuclei: Nuclear Relaxation Processes
651
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.
651
Atomic Spectroscopy: Effects of Temperature
330
Atomization, converting samples into gas-phase atoms and ions, is essential for atomic spectroscopy. The flame temperature required for atomization affects the efficiency of the atomic spectroscopic methods by increasing the atomization efficiency and the relative population of the excited and ground states.
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature...
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature...
330
Spin–Spin Coupling Constant: Overview
913
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
913


