正入射

We will use the circuit symbol for current source, which is , to model these power injections (which makes sense because, as concluded in Section 3.0, we can treat real power just as we treat currents).

我们为当前来源将使用电路符号，是，塑造(有道理的这些力量射入，因为，如结束在第3.0部分，我们可以对待真正的力量正我们对待潮流)。

I would like to practice, finding a light diffuse reflection principle; easy to fix this problem.

本人在本质处事洋，搜索不入一种诳骗光芒漫不正射道理处置此题目的简便易行的方法。

Then based on the results, the characteristics of radar stealth of a naval vessel were analyzed.

建立以某舰船为参照的艏向与正横向的近似二维模型，基于二维时域有限差分法计算舰船的艏向与正横向在不同频率入射波情况下的雷达散射截面，并根据计算结果对某舰船的雷达隐身特性进行分析。

Fig. 4 Measurement data abo ut echo signal f rom hard target and reference when t he hard target is still , in po sitive , negative rotation c

图 4 是为了矫正参考信号与回波信号入射到法 790 光学学报 28 卷图 4 配合目标静止，正转和反转时回波信号与参考信号的测量数据

It can not eliminate through the unitary transformation or the re\|definition of the wave function.

评述并证明了在场强为零势不为零的复连通区域，规范势沿入射粒子运动闭合路径的不可积积分是贝里几何位相，通过么正变换或重新定义波函数不能除去

In this thesis, we contrived a new experimental device which properties are oblique incidence and perpendicular detecting and a set of formularies of data processing.

设计了新的测量Mueller矩阵的实验装置：斜入射正接收装置，并推导出一组后续数据处理的算法。

However, for the collision processes in He target, a large discrepacy between the CTMC results and experimental measurement is found. As is well known, the microcanonical distributions of bounded electrons in CTMC method is quite different from quantal distributions, we modified the initial microcanonical distribution by using eleven different ionization thresholds of electron bounded in target. With modification, we calculated the collisional process of O~(3+) with He, and the total cross sections of all processess are calculated as a function of the incident energies. The agreement with experiments is improved by the modified distributions.

但由于靶电子的微正则分布与量子分布有很大不同，在计算离子与He靶碰撞时发现结果与实验差距很大，我们基于使用多个系统总能量U值，对初始电子的微正则分布进行了优化，使其更接近于量子力学的径向空间分布，然后计算了O~(3+)与氦原子随入射离子能量变化的各种反应过程截面，发现优化极大地提高了计算精度，特别是我们的模型对于描述单电子、双电子丢失过程非常成功。

For the same reason, the Goos-Hanchen shift is negative for both the TE and TM polarization incident waves as the result of the negative pennittivity and negative permeability nature of NIMs served as the rarer medium when total reflection occurring at a PIM-NIM interface.

对于正—负折射率介质界面处发生全反射时的古斯—汉森位移的研究发现当下半空间的光疏介质为介电常数和磁导率均为负的负折射率介质，不管是对于TE波还是TM入射波，在界面发生全反射时古斯—汉森位移均是负的。

It is symbolically illustrated in the cartoon that a striker is preparing to shoot at the goal defended by a goalkeeper on a football field.

参考译文这幅漫画生动描述了足球场上的一名前锋正准备将球射入守门员把守的球门。

It is symbolically illustrated in the cartoon that a striker is preparing to shoot at the goal defended by a goalkeeper on a football field.

这幅漫画生动描述了足球场上的一名前锋正预备将球射入守门员把守的球门。

The split between the two groups can hardly be papered over.

这两个团体间的分歧难以掩饰。

This approach not only encourages a greater number of responses, but minimizes the likelihood of stale groupthink.

这种做法不仅鼓励了更多的反应，而且减少跟风的可能性。