莫特过渡和体积定律与神经量子状态的纠
Chloé Gauvin-Ndiaye1,2, Joseph Tindall2, Javier Robledo Moreno2,3,4
1Université de Sherbrooke, Département de physique, Regroupement québécois sur les matériaux de pointe & Institut quantique, 2500 Boulevard Université, Sherbrooke, Québec J1K2R1, Canada.
Physical review letters
|March 7, 2025
概括
神经网络隐藏的费米子决定性状态 (HFDS) 揭示了无序电子系统中的莫特过渡. 这种先进的方法为有限的系统大小提供比传统方法更准确的波函数洞察力.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子力学就是量子力学.
- 计算物理学的计算物理.
背景情况:
- 莫特过渡意味着电子系统的相变,从金属到绝缘体,由移位和排斥驱动.
- 动态平均场理论 (DMFT) 提供了批量属性的精确解决方案,但仅限于热力学极限.
- 精确模拟有限大小的系统对于理解复杂的电子行为至关重要.
研究的目的:
- 引入和验证神经网络隐藏的费米子决定性状态 (HFDS),用于研究Mott过渡.
- 克服现有方法的局限性,比如精确对角化和有限系统的矩阵产物状态 (MPS).
- 为了获得新的见解,波函数的行为在金属绝缘体过渡附近.
主要方法:
- 实现神经网络隐藏的费米子决定性状态 (HFDS) 来建模无序,完全连接的哈伯德模型.
- 与动态平均场理论 (DMFT) 和矩阵产物状态 (MPS) 相比,HFDS准确性的比较.
- 计算关键的物理可观测值,包括能量,双重占用,准粒子重量和能量差距.
主要成果:
- 与MPS相比,HFDS在金属模式和Mott过渡附近提供了更准确的结果.
- 该方法成功地访问了超出精确的对角化极限的有限系统大小的波函数属性.
- 获得了对波函数幅度的新见解,阐明了过渡机制.
结论:
- HFDS代表了一个强大的新工具,用于模拟强度相关的电子系统.
- 这种方法克服了阻碍MPS等其他方法的纠限制.
- 这项研究开辟了利用神经量子状态在凝聚物质中探索量子现象的新途径.
相关概念视频
Atomic Nuclei: Nuclear Spin State Overview
841
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...
841
Phase Transitions
18.7K
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...
18.7K
Atomic Nuclei: Nuclear Relaxation Processes
598
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.
598
The Quantum-Mechanical Model of an Atom
41.8K
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.
41.8K
Path Between Thermodynamics States
3.0K
Consider the two thermodynamic processes involving an ideal gas that are represented by paths AC and ABC in Figure 1:
3.0K
Entropy Change in Reversible Processes
2.5K
In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
2.5K


