相关实验视频
Updated: Sep 18, 2025

06:42
Generation and Coherent Control of Pulsed Quantum Frequency Combs
Published on: June 8, 2018
9.1K
高维量子力学的波束和低密度方法:适用于非线性光谱的非对称的光采集构件
Joachim Galiana1, Michèle Desouter-Lecomte2, Benjamin Lasorne1
1ICGM, Univ Montpellier, CNRS, ENSCM, Montpellier, France.
The Journal of chemical physics
|June 23, 2025
概括
使用先进的量子方法模拟聚乙烯 (聚乙烯) 树突中的激发能量转移,揭示了超快的电子道. 高频振动模式对于这种能量传输过程至关重要.
科学领域:
- * 量子力学模拟. 量子力学模拟.
- * 有机材料的光物理.
背景情况:
- * 聚乙烯 (PPE) 树突是光采集应用的关键构建块.
- * 了解刺激能量转移 (EET) 和放松对于优化它们的性能至关重要.
研究的目的:
- * 模拟EET和放松在光学激发的PPE树状分子构建块.
- *使用先进的计算方法研究超高速电子道动态.
主要方法:
- *多层多配置时间依赖的哈特树 (ML-MCTDH) 方法使用波包.
- * 带有低密度矩阵的等级运动方程 (HEOM) 方法.
- * Ab initio振动合汉密尔顿 (VCH) 模型 (93维),包括线性,双线性和二次数项.
主要成果:
- * 模拟特定PPE寡合体中前两个激发状态之间的超快电子道.
- * 通过使用线性VCH模型,在一个非扰动的非马科夫体制中校准了一个开放的量子系统.
- * 模拟的线性响应吸收和发射光谱.
- * 探索了非线性模式,走向二维光谱学.
- * 确定了高频乙和状振动模式的重要作用.
结论:
- *最小的VCH模型可以提供成本效益高的极化敏感信号,用于监测早期EET动态.
- *这项研究证实了PPE树状体内ET过程中特定振动模式的关键重要性.
相关概念视频
¹H NMR: Interpreting Distorted and Overlapping Signals
1.1K
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
1.1K
The de Broglie Wavelength
27.3K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
27.3K
UV–Vis Spectroscopy of Conjugated Systems
7.4K
Organic compounds with conjugated double bonds show strong absorption features in the UV–visible region of the electromagnetic spectrum attributed to π → π* electronic excitations. Generally, a UV–vis absorption spectrum is recorded as a plot of absorbance vs wavelength. The wavelength of maximum absorbance, which manifests as a peak in the absorption spectrum, is denoted as λmax.
One of the factors influencing λmax is the extent...
One of the factors influencing λmax is the extent...
7.4K
IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration
1.7K
A covalently bonded heteronuclear diatomic molecule can be modeled as two vibrating masses connected by a spring. The vibrational frequency of the bond can be expressed using an equation derived from Hooke's law, which describes how the force applied to stretch or compress a spring is proportional to the displacement of the spring. In this case, the atoms behave like masses, and the bond acts like a spring.
According to Hooke's law, the vibrational frequency is directly proportional to...
According to Hooke's law, the vibrational frequency is directly proportional to...
1.7K
UV–Vis Spectroscopy: Molecular Electronic Transitions
1.8K
In Ultraviolet–Visible (UV–Vis) spectroscopy, the absorption of electromagnetic radiation is used to probe the electronic structure of molecules. This technique provides insights into molecular electronic transitions, particularly the movement of electrons between different molecular orbitals. Radiation is absorbed if the energy of the electromagnetic radiation passing through the molecule is precisely equal to the energy difference between the excited and ground states. During this...
1.8K
Molecular Spectroscopy: Absorption and Emission
3.4K
Molecules possess discrete energy levels called quantum states. Unlike atoms, which have simpler energy levels, molecules possess additional rotational and vibrational energy levels. Each energy level is separated by an energy gap, with the gaps between adjacent electronic, vibrational, and rotational levels varying significantly. The three types of energy levels in a diatomic molecule are shown in Figure 1.
3.4K

