量子信息对于另一个类型的新提议的超级波动潜能
R Santana-Carrillo1, Roberto de J León-Montiel2, Guo-Hua Sun1
1Centro de Investigación en Computación, Instituto Politécnico Nacional, UPALM, Mexico City 07738, Mexico.
Entropy (Basel, Switzerland)
|September 28, 2023
概括
这项研究探讨了过度波动潜能中的香农,发现单井潜能比双井潜能更能定位波函数. 度满足了潜在深度的BBM不平等.
科学领域:
- 量子力学就是量子力学.
- 数学物理 数学物理
背景情况:
- 香农度量化了量子系统中的不确定性.
- 在各种物理模型中,超标潜能是相关的.
- 了解波函数局部化是关键.
研究的目的:
- 调查香农的四个新的过度波动潜力.
- 分析位置和动量输入.
- 检查Bialynicki-Birula和Mycielski (BBM) 不等式的情况.
主要方法:
- 计算过的位置和动量对于过度波动的潜力.
- 研究了波函数局部化.
- 评估了不同潜能深度 (u ̄) 的行为.
主要成果:
- 单井电位 (U0,3) 显示出比双井 (U1,2) 更大的波函数局部化.
- 位置密度对于单井潜力更为局部化;动量密度更为局部化.
- 双井潜能表现出逆局部化行为.
- 香农值满足了所有测试深度的BBM不等式.
- 位置和动量输入的总和在U1,2,3时随着u ̄增加,但在U0.0时随着u ̄减少.
- 费舍尔 (F ̄x) 随着u的增加而增加,而F ̄p则减少.
结论:
- 过度波动的潜在深度会影响波函数局部化和分布.
- 对于这些潜能,BBM不等式是正确的.
- 的行为在单井和双井潜力之间有明显的差异.
相关概念视频
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
Entropy and the Second Law of Thermodynamics
2.9K
The second law of thermodynamics can be stated quantitatively using the concept of entropy. Entropy is the measure of disorder of the system.
The relation between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
The relation between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
2.9K
Thermodynamic Potentials
870
Thermodynamic potentials are state functions that are extremely useful in analyzing a thermodynamic system. They have dimensions of energy. The four important thermodynamic potentials are internal energy, enthalpy, Helmholtz free energy, and Gibbs free energy. These thermodynamic potentials can be expressed using two of the following variables: pressure, volume, temperature, and entropy. These two variables are expressed as the rate of change of the thermodynamic potential with respect to other...
870
Maxwell's Thermodynamic Relations
2.8K
Maxwell's thermodynamic relations are very useful in solving problems in thermodynamics. Each of Maxwell's relations relates a partial differential between quantities that can be hard to measure experimentally to a partial differential between quantities that can be easily measured. These relations are a set of equations derivable from the symmetry of the second derivatives and the thermodynamic potentials.
All thermodynamic potentials are exact differentials. Therefore, their second-order...
All thermodynamic potentials are exact differentials. Therefore, their second-order...
2.8K
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
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


