论文标题
斑点斑点
Speckled speckled speckle
论文作者
论文摘要
斑点是当从粗糙的表面反射一致的光线时看到的辐照度的空间波动。这是由于从表面的许多角落和缝隙中反射出的光,这些角落积累了大量的时间延迟,跨越了远远超过光学时期,在通往观察点的途中。尽管众所周知,具有连续波(CW)照明的斑点,但使用Cooherent Light对非线视线(NLOS)成像的新兴兴趣引起了人们的需求,这需要了解高阶斑点,这是由多种粗糙表面反射引起的,即斑点和斑点斑点和斑点的斑点斑点。此外,最近介绍了相曲线($ \ MATHCAL {P} $ - 字段)NLOS成像---依赖于振幅调制的相干照明---需要推动Speckle和高阶Speckle的CW方案。在本文中,我们采用三挡仪传播几何形状来满足上述需求的第一步,该几何形状是三弹性NLOS成像的代理。在小型扩散器的限制中,我们表明CW和调制$ n $ th-tord Speckle的辐照度差异是$(2^n-1)$ - 乘以普通(一阶)Speckle的倍数。但是,NLOS成像的更重要的情况涉及扩展的弥散反射器。对于使用扩展扩散器的传输几何形状,我们处理三阶CW斑点和一阶调制斑点。我们的结果暗示,斑点不太可能阻碍连贯的弹片CW成像器的成功操作,并且他们认为对于$ \ Mathcal {p} $ - field Imagers也可能是正确的。
Speckle is the spatial fluctuation of irradiance seen when coherent light is reflected from a rough surface. It is due to light reflected from the surface's many nooks and crannies accumulating vastly-discrepant time delays, spanning much more than an optical period, en route to an observation point. Although speckle with continuous-wave (cw) illumination is well understood, the emerging interest in non-line-of-sight (NLoS) imaging using coherent light has created the need to understand the higher-order speckle that results from multiple rough-surface reflections, viz., speckled speckle and speckled speckled speckle. Moreover, the recent introduction of phasor-field ($\mathcal{P}$-field) NLoS imaging---which relies on amplitude-modulated coherent illumination---requires pushing beyond cw scenarios for speckle and higher-order speckle. In this paper, we take first steps in addressing the foregoing needs using a three-diffuser transmissive geometry that is a proxy for three-bounce NLoS imaging. In the small-diffusers limit, we show that the irradiance variances of cw and modulated $n$th-order speckle coincide and are $(2^n-1)$-times those of ordinary (first-order) speckle. The more important case for NLoS imaging, however, involves extended diffuse reflectors. For our transmissive geometry with extended diffusers, we treat third-order cw speckle and first-order modulated speckle. Our results there imply that speckle is unlikely to impede successful operation of coherent-illumination cw imagers, and they suggest that the same might be true for $\mathcal{P}$-field imagers.