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- The phonon polariton is a particle comprised of a photon and a tansverse-optical phonon. 它的物理效应是经典的,不需要用量子力学考虑。
- phonon polariton 声子激子
- Origins of other phonon modes in the spectra are discussed as well. 对光谱中的其他声子模式的起源也进行了讨论;
- The Mechanism of No Phonon Optical Transitions in SiGe Alloy[J]. 引用该论文 董文甫;王启明;杨沁清.
- LO phonon modes in ZnSe-ZnTe strained-layer superlattice[J]. 引用该论文 崔捷;王海龙;干福熹.
- phonon polaritons 声子-极化激元
- RAMAN SPECTRUM STUDY OF PHONON MODES FOR SINGLE WALL CARBON NANOTUBES ? 单层纳米碳管振动模的拉曼光谱研究
- The modulation of SBS pulse shape tends to occur with a short phonon lifetime. 声子寿命越短，SBS波形前沿就越陡，并且越容易出现调制现象。
- A new phonon model of excitation martensitic transformation is presented. 本文提出了一个新的激发马氏体相变的声子模型。
- At zero intensity, the last glimmer of the light vanishes into the atoms, and the polariton comes to a dead stop. 到了控制光强度归零之时，光的最后一丝光芒都消逝到原子里，极化声子就完全停止了。
- As the control beam's intensity ebbs, the remaining signal light is absorbed, and the increasingly atomic polariton slows even more. 一旦控制光的强度逐渐下降，剩馀的讯号光就给吸收了，原子极化愈来愈强的极化声子速度减慢得更多。
- It has nothing to do with special relativity.When light in medium, it is not photon, it is called polariton or so, which has speed change with the medium movement. 以前看过报道，有科学家在某种特殊的介质中，测得的光速非常低，那应该>>可以用来做比较精准的实验了。
- The probability of obtaining a lattice atom displacement via the phonon kick process is evidently small. 很明显，通过声子反冲过程而取得晶格原子位移的几率是不大的。
- Uncertainty Regions for the Vacuum, Number, Coherent, and Squeezed Phonon States. 数量态、相干态及压缩光子态的不确定区域。
- Also, it proved the over passing of the diffusion component with respect to phonon drag component. 热电势以扩散分量为主,声子曳引可以忽略。
- A condensed soft optical phonon mode originates from the triply degenerate symmetric in-plane O-Nb-O bending. 一个软光学声子模来源于在铌-氧平面内的三重简并对称弯曲振动。
- The phonon field and phason field stress intensity factors and stress distribution at the crack tips are also given. 进一步可以求得裂纹尖端的声子场和相位子场的应力强度因子,由这些应力强度因子求解了裂尖处的声子场和相位子场的应力分布。
- The calculated phonon frequencies and polarization of Ag(110) surface are in accord with experimental results. 计算的Ag(110)表面声子谱频率和振动极化方向在全部区间内与实验数据符合得很好。
- On this assumption the phonon density of states has been calculated by the Cluster-Bethe-lattice Method (CBLM). 在此前提下;本文采用 CBLM方法(即 Cluster-Bethe-Lattice Method)计算了a-Si:H的声子态密度.
- This corresponded to a phonon amplification effect.The mechanism of generating the phonon amplification was discussed. 详细讨论了产生这种声子增益效应的机理，给出了产生声子增益的时间间隔。
