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Compared with 3, 6-carbazo derivatives, the OPA wavelengths of 2, 7-carbazole derivatives are bathochromic shift and the oscillator strength increased; the TPA wavelengths are red-shifted and the TPA cross-section increased.

与3, 6-咔唑衍生物相比,2, 7-咔唑衍生物的单光子吸收波长红移,振子强度增大;双光子吸收波长红移,双光子吸收截面增加。

All these characteristics can extend frequency band , reduce antennaelectric size and improve impedance characteristics. In order to miniaturization ofantenna, impedance complete compensate and matching optimization of electricallysmall antenna are brought forward, and this method is applied to the discage antennas.

从阻抗特性和辐射特性的实测数据表明,水加载单极振子天线的谐振频率能很好地向低端下移,局部水加载单极圆锥天线在保持原有宽频带特性的前提下,以较少的效率损失实现了较大范围向低频区扩展,即天线小型化,这将为短波超短波波段天线进一步的小型化设计提供很好的思路。

Simulation results of the Duffing oscillator and qubit measurement will be presented.

并在最后提出一些 Duffing 振子和量子位元测量的模拟结果。

During theoretic analysis and experimentation,the feasibility of weak signal detection based on Duffing Oscillators is proved.

结合理论分析和大量的仿真试验,表明了Duffing振子检测微弱正弦信号的可行性。

So we focus on the properties of the quantum Duffing oscillator and present the operation principles of the JBA.

因此,我们著重於量子 Duffing 振子的性质和介绍 JBA 的运作原理。

As an example, two Duffing oscillators coupled with linear and nonlinear stiffness terms are investigated.

作为例子,考察了两自由度线性与非线性刚度耦合的Duffing振子,证明了其响应的非高斯特性依赖于脉冲平均到达率和系统弛豫时间的乘积,并用Monte Carlo模拟验证了该方法的可行性。

Based on calculating the first-order corrections to the energy from relativistic and mass-polarization effects, we estimate the higher-order relativistic contribution and QED correction to the energy under a hydrogenic approximation. The transition energies, wavelengths and oscillator strengths for the 1s23s-1s2np transitions of this ion are calculated.

在计算相对论效应和质量极化效应对体系能量的一级修正的基础上,通过引入价电子的有效核电荷,在类氢近似下,估算了对能量的高阶相对论修正和QED修正,计算了该离子1s23s-1s2np的跃迁能,波长和在三种规范下的振子强度。

In chapter 4, by AREELS, the Generalized Oscillator Strength Density Spectra were measured in the energy region from 56 to 66eV, with the incident energy 2. 5 keV and energy resolution 80 meV, at scattering angles from 0°to 6°, corresponding to the momentum transfer K〓=0.03~2. 01 a. u. The Fano profile parameters f〓 and q for the optically allowed transition 〓(0, 1)〓P°and the optically forbidden transitions 〓(1, 0)〓S〓and 〓(1, 0)〓D〓 were obtained as a function of K〓. With the hyperspherical coordinate wavefunctions, the dynamical correlation are discussed qualitatively. So, a new experimental way to study dynamical electron correlation effect is opened.In chapter 5, the widely used R-matrix theory was introduced. Then, the GOSDS for the optically allowed excitation series (1s〓)〓S〓→〓(0, 1)〓P°(n=2-4) were calculated by this method, and the Fano profile parameters f〓 and q were obtained sequently. So the electron correlation effect can be described by these parameters quantitatively, and the theoretical results were compared with our AREELS experimental results.

在第四章中,实验上,同样使用角分辨的高能量分辨快电子能量损失谱仪,在2.5keV电子入射能量和80meV的能量分辨下,测量了0°到6°散射角下的He原子双电子激发态在56~66eV的广义振子强度密度谱,这种情况,0°~6°对应的动量转移范围K〓=0.03~2.01a.u。,得到了光学允许跃迁的双电子激发态〓(0,1)〓P〓和光学禁戒跃迁的双电子激发态〓(1,0)〓S〓、〓(1,0)〓D〓的Fano线形参数f〓,q等随动量转移变化的曲线;观测到了几个强度很弱、能级很窄的光学允许和禁戒跃迁双电子激发态,用前人准确的理论结果进行了标识;通过比较弱共振〓(1,0)〓S〓和〓(-1,0)〓S〓的强度随动量转移K〓的变化规律,结合超球坐标理论计算的波函数,定性地阐述了在电子碰撞散射过程中它们各自不同的动力学电子关联效应,发展了一套在实验上研究电子关联效应的新方法。

In addition, there exists the high dimensional oscillator in physics, In its Hamiltonian coordinates and momenta are coupled. For instance, quantumHall system does so.

另外,物理问题中有一类型振子是高维的,在其哈密顿量中动量和坐标是相互耦合的,比如量子霍尔系统就是如此。

Moreover,the mechanismunderlying the transition to nonlocal synchronization has been made clear,i.e.,that the oscillators between the nonlocal synchronized sites can transferthe synchronous components,although they stay in nonsynchronous status.

针对这一奇怪的时空动力学行为,我们详细研究了其机制,发现处于非局域混沌相同步中间位置的振子虽然没被锁相,但它们的运动中包含有相同步的元素起到了传递相同步信号的作用。

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在对危险的南部地区访问时,他斥责什叶派民兵领导人对中央集权的挑衅行为。

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