精确的封闭式表达式为单元自旋适应费米离子单元双激励运算符
Erik Rosendahl Kjellgren1, Karl Michael Ziems2,3, Peter Reinholdt1
1Department of Physics, Chemistry and Pharmacy, University of Southern Denmark, Campusvej 55, 5230 Odense, Denmark.
The Journal of chemical physics
|October 3, 2025
概括
研究人员开发了针对反赫米蒂安自旋适应单元双激励费米离子运算子的精确公式. 这使得高效的量子计算方法成为可能,并保证了量子设备的特定自旋对称性.
科学领域:
- 量子计算是一种量子计算.
- 量子化学是一种量子化学.
- 理论物理学的理论物理.
背景情况:
- 对于量子化学模拟来说,费米离子运算符的有效实施至关重要.
- 保持旋转对称性对于准确的量子力学计算至关重要.
研究的目的:
- 为了获得准确的封闭式表达式,对抗赫密斯旋转适应单元双激发费米子运算符的矩阵指数.
- 为了促进这些运算符在量子计算框架中的有效实施.
- 为了实现能够保证对特定旋转对称性趋同的设想.
主要方法:
- 对矩阵指数的精确封闭式表达式的导数.
- 在单一产品状态框架内的应用.
- 开发用于量子设备的自旋适应电路.
主要成果:
- 获得了特定费米子运算符的矩阵指数的精确闭式表达式.
- 在传统量子硬件上实现了高效的实现.
- 确保接近所需的旋转对称性.
结论:
- 衍生的表达式为分子性质的高效量子计算提供了一条途径.
- 这些方法可用于构建量子计算机的强大的自旋适应电路.
- 这项工作促进了化学和材料科学量子算法的发展.
相关概念视频
The Pauli Exclusion Principle
58.9K
The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
58.9K
Valence Bond Theory
11.2K
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
11.2K
Atomic Nuclei: Nuclear Spin State Overview
1.9K
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 one, the...
1.9K
Crystal Field Theory - Tetrahedral and Square Planar Complexes
48.1K
Tetrahedral Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
48.1K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
1.6K
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...
1.6K
Atomic Nuclei: Nuclear Spin State Population Distribution
2.3K
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.
2.3K


