系统状态的动力学在量子力学的概率表示中的系统状态
Vladimir N Chernega1, Olga V Man'ko2
1Institute of Managment and Digital Technologies, Department of Logistics and Transport System Managment, Russian University of Transport (MIIT), Obraztsova Street, 9/9, Moscow 127994, Russia.
Entropy (Basel, Switzerland)
|May 27, 2023
概括
这项研究使用概率分布来澄清量子系统状态,并探索纠的概率结构. 它详细介绍了施罗丁格猫状态对双模振荡器的演变,并连接到基本的量子方程.
科学领域:
- 量子力学就是量子力学.
- 量子信息理论就是量子信息理论.
- 统计力学就是统计力学.
背景情况:
- 量子系统的传统描述通常依赖于抽象的数学形式主义.
- 通过概率分布来理解量子态提供了一个替代的视角.
- 纠,一个关键的量子现象,需要在概率框架内仔细描述.
研究的目的:
- 用传统的概率分布函数来描述量子系统状态.
- 为了澄清纠概率分布的概念和结构.
- 在这种概率框架内,研究特定量子状态 (施罗丁格猫状态) 的时间演变.
主要方法:
- 使用断层图形概率分布来描述量子状态.
- 分析一个反转振荡器的偶数和奇数施罗丁格猫状态的演变.
- 推导和讨论时间依赖概率分布的进化方程.
主要成果:
- 通过概率分布建立了量子态的清晰描述.
- 纠概率分布的结构得到了阐明.
- 成功获得了用于双模振荡器的施罗丁格猫状态的时间演变.
结论:
- 该研究提供了使用概率分布的量子态的新视角.
- 衍生出来的进化方程为量子系统的动态提供了洞察力.
- 阐明了这种概率方法与标准量子形式主义 (施罗丁格方程和·诺曼方程) 之间的联系.
相关概念视频
The Quantum-Mechanical Model of an Atom
42.6K
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.
42.6K
State Space Representation
249
The frequency-domain technique, commonly used in analyzing and designing feedback control systems, is effective for linear, time-invariant systems. However, it falls short when dealing with nonlinear, time-varying, and multiple-input multiple-output systems. The time-domain or state-space approach addresses these limitations by utilizing state variables to construct simultaneous, first-order differential equations, known as state equations, for an nth-order system.
Consider an RLC circuit, a...
Consider an RLC circuit, a...
249
The Uncertainty Principle
23.5K
Werner Heisenberg considered the limits of how accurately one can measure properties of an electron or other microscopic particles. He determined that there is a fundamental limit to how accurately one can measure both a particle’s position and its momentum simultaneously. The more accurate the measurement of the momentum of a particle is known, the less accurate the position at that time is known and vice versa. This is what is now called the Heisenberg uncertainty principle. He...
23.5K
Entropy
30.4K
Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
30.4K
Transfer Function to State Space
318
State-space representation is a powerful tool for simulating physical systems on digital computers, necessitating the conversion of the transfer function into state-space form. Consider an nth-order linear differential equation with constant coefficients, like those encountered in an RLC circuit. The state variables are selected as the output and its n−1 derivatives. Differentiating these variables and substituting them back into the original equation produces the state equations.
In an...
In an...
318
Atomic Nuclei: Nuclear Spin State Overview
1.0K
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...
1.0K


