施罗丁格猫在热环境中的脆弱性
Sandip Bera1, Kenny L S Yip1, Sajeev John2
1Department of Physics, University of Toronto, 60 St. George Street, Toronto, ON, M5S 1A7, Canada.
Scientific reports
|November 1, 2023
概括
施罗丁格猫在斯-哈巴德模型中的状态变得不稳定,由于热波动导致粒子数量增加. 对于小的Cat状态来说,存在一个狭窄的参数制度,以生存脱凝.
科学领域:
- 量子力学就是量子力学.
- 凝聚物质物理学 凝聚物质物理学
- 原子物理 原子物理
背景情况:
- 施罗丁格猫状态是量子力学中的叠加状态.
- 斯-哈巴德模型描述了互动的玻色子在一个格子上.
- 有吸引力的现场相互作用可以在零温度下稳定这些状态.
研究的目的:
- 为了研究施罗丁格猫状态的脱凝不稳定性.
- 确定这些状态可以在物理环境中生存的条件.
主要方法:
- 分析了具有吸引力的现场交互的两站式Bose-Hubbard模型.
- 多体哈密尔顿数的精确数值对角化.
- 对热波动和粒子数波动的研究.
主要成果:
- 随着粒子数 (N) 的增加,施罗丁格猫状态对热波动变得不稳定.
- 对于较大的N,脱凝度温度下降.
- 基和兴奋状态的热混合主导着连贯性损失.
- 粒子数的波动也会降低连贯性,但不那么显著.
结论:
- 为了小猫状态的生存,确定了一个狭窄的参数模式 (粒子数,温度,U/t).
- 不连贯性限制了大型施罗丁格 Cat 状态的实际实现.
相关概念视频
Atomic Spectroscopy: Effects of Temperature
343
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...
343
Atomic Nuclei: Nuclear Spin State Population Distribution
988
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.
988
The Quantum-Mechanical Model of an Atom
42.4K
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.
42.4K
Third Law of Thermodynamics
19.0K
A pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K) may be described by a single microstate, as its purity, perfect crystallinity,and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.
19.0K
Entropy
30.3K
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...
30.3K
Diversity of Archaea IV
35
Hyperthermophilic archaea are a group of extremophiles thriving at temperatures above 80°C, often in hydrothermal vents and volcanic soils where conditions surpass the boiling point of water. At such temperatures, proteins, membranes, and DNA in most organisms degrade, but hyperthermophiles have evolved remarkable adaptations to maintain stability and function.Unique Cellular FeaturesHyperthermophilic membranes are composed of a monolayer of biphytanyl tetraether lipids, which resist...
35


