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散射角

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The angular distribution of the transmission coefficient of HH polarization are obtained by numerical implementation, the influence of the permittivity and the mean layer thickness of intermediate medium, friction velocity and the frequency of the incident wave on the transmission coefficient is discussed.

通过数值计算得到了HH极化透射系数随散射角的变化曲线,讨论了中间介质介电常数和厚度、摩擦风速和入射波频率对透射系数的影响,得到改进的一维分形分层海面透射系数的基本特征、分区特征和随频率变化的特征,结果表明透射系数近似具有"量子化"特征。

The angular distribution of stimulated Raman scattering energy has been measured.

报道了采用PIN探测器阵列测量大角度受激Raman散射角分布和采用激光卡计对背向SRS光能量积分测量的实验结果。

Decreasing the apex angle appropriately of the transmitter helps the signal detection when the scattering angle remains unchanged.

计算结果还表明,在散射角和传输距离一定的情况下,适当地降低发射机的仰角可以提高接收机探测到的信号功率和信噪比。

The inelastic scattering angular distributions of discrete levels and double differential cross sections were calculated and analyzed by using the distorted wave Born approximation theory ,the unified Hauser-Feshbach model and the exciton model.

应用得到的光学模型势参量,根据光学模型、统一的Hauser-Feshbach和激子模型理论以及扭曲波玻恩近似理论,系统计算和分析了中子与58,60Ni反应的非弹散射角分布和双微分截面,理论结果与实验很好地一致。

The absolute differential cross section of e-Ar scattering with one-, two-, and three-photon exchange at scatering angles 1°~26° are calculated.

利用第二玻恩近似方法对激光场中e-Ar的散射进行了研究,计算了散射角为1°~26°,交换多个光子的微分散射截面。

The scattering and absorption coefficient values measured by the D-OPC were compared with that measured by an Aethalometre and an Integrating Nephelometer.

与TSI公司黑炭仪和浊度计测量的吸收系数和散射系数对比表明,双散射角光学粒子计数器测量气溶胶折射率和谱分布结果合理,测量误差0%,可以满足同时测量气溶胶粒子谱分布和折射率的需要。

Overwatch weapon scatter tuning adjusted - angle reduced, area reduced marginally.

英军皇家炮兵支援的观测炮击技能散射效果调整-减少散射角以略微减小落弹散步范围。

Finally, the variation of polarization degree of scattering laser with particle size and scattering angle.

最后分析了散射光的偏振度对粒子尺度和散射角的变化关系。

Scattering angle is the angle between the scattered and incident directions.

散射角是散射方向与入射方向之间的夹角。

The results show that the angular distribution of the total differential cross section at zero degree increases and the position of oscillation minimum of the same order gradually shift towards small scattering angle along with the increase of the incident isotope He atom mass at identical collision energy. And crossing angle between the elastic and total inelastic DCS gradually decreases and the total inelastic DCS gradually increases.

结果表明:在相同碰撞能量时,随着同位素氦原子质量的增加,总微分截面在0°时的角分布逐渐增大,同一级衍射振荡极小值位置逐渐向小散射角方向移动;弹性与总非弹性截面交界角逐渐减小,总非弹性截面逐渐增加。

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