极化子

结果证明，钢中的C含量对成品磁性有着重要的影响。磁场中强耦合表面极化子的性质

C. magnetic properties were measured . PROPERTIES OF STRONG-COUPLING SURFACE POLARON IN MAGNETIC FIELD

GaAs中与施主高激发态有关的共振极化子效应

Resonant polaron effect related with high excited states of donors in GaAs

Zn（1-x）CdxSe/ZnSe异质结中的界面极化子

The Interface Polarons in a Zn_ ( 1-x ) Cd_xSe / ZnSe Heterojunction

GaAs晶体膜中弱耦合极化子的自陷能

Self - Trapping Energy of the Weak - Coupling Polaron in GaAs Crystal Slab

三元混晶AxB（1-x）C中极化子回旋质量

Cyclotron mass of polaron in ternary mixed crystal A_xB_ ( 1-x ) C

多支LO模对极化子基态能量的影响

Effect of LO Modes on the Ground State Energy of Polaron

柱形量子线中极化子的电子与LO声子之间相互作用能

Electron-phonon Interaction Energies of Polaron in Cylindrical Quantum Wires

GaAs／AlxGa（1－x）As异质界面极化子的温度效应

Temperature Effect of Polarons on a GaAs / Al_xGa_ ( 1-x ) As Heterointerface

极化子动力学被划分为两类，弱耦合动力学（weak-couplingdynamics）和强耦合动力学（strong-couplingdynamics）。

Two types of polaron dynamics are classified : the weak-coupling dynamics and the strong-coupling dynamics .

三元混晶AxB（1-x）C中强束缚极化子激发态能量

The Excited State Energies of the Strong Bound Polaron in Ternary Mixed Crystal A_xB_ ( 1-x ) C

极化子效应对Morse势阱中三次谐波产生的影响

Polaron effects on the third-harmonic generation in Morse quantum well

Holstein极化子能带和有效质量的温度依赖性

Temperature Dependence of Energy-band Width and Effective Mass for the Holstein Polaron

GaAs-Ga（1x）AlxAs多层极性膜中的束缚极化子

A Research on The Bound Polaron in GaAs-Ga_ ( 1_x ) Al_xAs Multiple Polar Crystal Slab

GaAs-Ga（1-x）AlxAs量子阱中极化子的结合能

Binding energy of dressed charged particles in gaas-ga_ ( 1-x ) al_xas quantum well

电子与双声子相互作用对Holstein极化子的影响

The influence of the electron and one pair of phonons interaction on Holstein polaron

Wu等人利用非绝热的分子动力学方法研究了金属/聚合物/金属三明治结构中极化子形成的动力学过程。

Using a nonadiabatic dynamic method , Wu et al . studied the dynamic process of polaron formation in a metal / polymer / metal sandwich structure .

数值计算结果表明：抛物量子线中强耦合极化子的基态能量Eo随约束强度ω0的增强而增大，而随电场强度F和量子线长Z的增大而单调减小。

Numerical calculation illustrated that the ground state energy increases with the increasing confinement strength , and decreases with increasing of electric field strength and wire length .

一维环Aharonov－Bohm势对极化子的影响

Effect of Aharonov Bohm Potential on the Polaron in 1D Ring

与中性态相比，带电态下其分子结构表现在C-C键键长发生显著改变，单电荷掺杂导致极化子元激发；

Comparing with the neutral states , the changes of the bond lengths of the charged states are very evident .

Aharonov－Bohm磁通对&维分子环中局域极化子的影响

Local Polarons in a one-dimensional molecular ring affected by an Aharonov-Bohm flux

在考虑电子与LO声子相互作用和加电场的情况下，计算了抛物量子线中强耦合极化子的基态能量。

The ground state energy of strong-coupling polaron in parabolic quantum wires is calculated for the case where the electron interacted with bulk LO phonon and added electric field .

GaAs-GaAlAs量子阱中极化子的尺度效应

The width effect of the polaron in GaAs-GaAlAs quantum well

并对CdF2、CsI、ZnS和GaAs晶体进行了数值计算，结果表明：两种情况下抛物量子线中极化子的基态能量E0都随约束强度ω0的增大而增大。

Numerical calculation for crystals CdF_2 ? CsI ? ZnS and GaAs indicated that the ground state energy E_0 will increases with the increasing of confinement strength ω _0 .

实验结果表明，是双交换作用和小极化子效应的共同作用决定了CMR效应的特性。

The experimental evidences show that both actions of double exchange interaction and small polarons are responsible for the variation of the CMR effect .

并对KCl材料进行了数值计算。结果表明，振动频率λ随膜厚的增加而减少，极化子自陷能随着膜厚的增加而减少；

And the numerical calculations for KCl crystal show that the variation frequent contacts λ and the self-trapping energy are all reduce with the increase of the slab thickness .

GaAs-GaAlAs量子阱中光极化子

Localized Optical Polaron in a GaAs-GaAlAs Quantum Well

随着掺杂程度的增大，两种极化子都是载流子，同样经历了由Curie自旋到Pauli自旋的转变。

With increasing doping level , the two polarons underwent similar transfer from Curie spin to Pauli spin and both polarons were charge carriers in the conducting polymer .

弱电场对激子没有明显影响：当静电场超过临界值150kVcm，激子解离为电子型极化子和空穴型极化子，与共轭聚合物不同，极化和解离同时发生；

But in the critical electric field 150 kV / cm , an exciton is directly split into an electron polaron and a hole polaron . The polarization and dissociation happen at the same time , which differs from that in conjugated polymers .

我们发现在150MPa至600MPa的高压条件下，均可以合成出具有纳米网状结构的PANI薄膜样品，而且样品的极化子吸收峰随压力增加出现红移现象。

Between 150 MPa and 600 MPa high-pressure ranges , it is easy to synthesize PANI film with nano-network .

一维小极化子模型的代数Bethe-Ansatz方程

Algebraic Bethe-Ansatz equations for a small - polaron model