| 1. | When we were discussing the index of refraction, we saw that an incoming beam of light will make the atoms radiate again .
在讨论折射率时，我们曾看到入射光束使原子再辐射。 |
| 2. | The grating converts the light into a central peak plus side peaks
光栅将入射光束转化成一个中心峰值和一系列副峰值。 |
| 3. | Along with the enlarging of beam size , the effect of walkoff is much smaller and can even be neglected
随着入射光束口径的增大，离散效应的影响相应地减小，甚至可以忽略。 |
| 4. | For example , when the beam waists of both gb and fgb are equal to 10 mm , the width of the sfgb mirror is - 3 . 6 times of the sgb one
研究结果表明，在入射光束的光腰w二10 ~的条件下，平顶高斯光束反射镜面的宽度要比sgb反射镜面的宽度大一3 . 6倍。 |
| 5. | By changing the orientation of the molecules that make up the liquid crystals , the modulators reshape the wavefront of the incoming light beam to display the image encoded in a computer - designed hologram
这种调节器藉著改变液晶分子的方向，重塑入射光束的波前，以显现出电脑设计的全像图中所储存的影像。 |
| 6. | Used arrayed optical receivers to collect laser energy . because of the different between aoa and axes of optical receivers , the energy between each receiver was corresponding different . to contrast with each other can show the aoa
该方法采用阵列光学头接收光能量，利用入射光束与不同光学通道夹角不同，接受的能量则不同的原理，通过对它们的比较来确定入射光束的角度。 |
| 7. | ( 3 ) another method using liquid crystal spatial light modulator can control the small region of incident laser , which can change the intensity distribution and uniform temperature distribution . the related driver circuit of liquid crystal spatial light
( 3 )采用液晶空间光调制器方案实现温度分布均匀化通过液晶空间光调制器对入射光束不同位置的微小局部进行幅度调制,从而改变输出光场分布,达到均匀化的目的。 |
| 8. | This paper insert linear polarized flake in each optical channel to coding the different energy . then put the light come from the different channels together , the polarization of synthesized light would show the aoa . in order to identify the polarization direction , used polarization beamspliting prism
为了减少传统阵列探测中探测器的数量，本论文在各阵列探测通道中加入偏振片，利用偏振片对其出射光束进行偏振方向编码，然后使各通道出射光束叠加，从最后合光的偏振方向中得到入射光束的方位信息。 |
| 9. | Under the same beam parameters , the intensity gradient near the mirror surface of the blue - detune sfgb is the nearly same as that of the sgb , but the intensity distribution of the fgb is a constant within a larger radial range , the width of the sfgb mirror will far greater than one of the sgb mirror
类似地，半束兰失谐平顶高斯光束反射镜和sgb反射镜相比在yoz平面上的衍射强度梯度是近似相同的，也就是说在入射光束参数相同的条件下，在上述二种反射镜表面附近入射原子受到的光偶极排斥力大小是近似相同的。 |
