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Digital dispersion compensation for ultrabroad-bandwidth single-camera spectral-domain polarization-sensitive OCT

机译:超宽带单相机光谱域偏振敏感OCT的数字色散补偿

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Polarization-sensitive OCT is used to examine tissue microstructure by providing imaging of birefringent properties.[l] Single-camera spectral-domain polarization-sensitive OCT has been of recent interest, whereby a custom spectrometer is employed to simultaneously measure orthogonal polarization states scattered from the sample.[2,3,4] This avoids synchronization and triggering issues associated with multiple-camera setups. It also has the advantage that the optic axis can be extracted without polarization modulating the incident light. However, the disadvantage is that the line camera pixel-to-wavenumber nonlinearity requires either careful spectrometer alignment,[2] or digital compensation.[5]rnIn fact, this problem is further exacerbated in high resolution PSOCT systems as they require compensation over larger bandwidths. Here we report the construction of an ultrabroad-bandwidth PSOCT system using a single camera spectrometer similar to Baumann et al [2]. In order to enjoy the benefits of this instrument, we outline a method for digital dispersion compensation that removes the necessity for special camera alignment. We find that there are three non-negligible types of dispersion to consider: 1) the aforementioned camera pixel-to-wavenumber nonlinearity, 2) the refractive index dispersion in the sample itself, and 3) the dispersion imbalance between the arms of the OCT interferometer. The latter two were previously recognized for time-domain high-resolution OCT, where a digital dispersion compensation method was successfully employed to treat them both. [6] For our SDOCT application, we find that dispersion types 1 and 2 have the same functional effect and can be combined into one compensation step, and as such, much of the previous compensation method can be used. However, we find that it is necessary to add two steps to the analysis technique whereby the relative scaling and positioning of the two polarization images is adjusted to align the scatterers. We also find that better results are achieved by fitting to larger polynomial orders. We show how our technique provides high-resolution PSOCT with precise alignment between the orthogonal polarization images.
机译:偏振敏感型OCT通过提供双折射特性的成像来检查组织的微结构。[1]单相机光谱域偏振敏感型OCT引起了人们的极大兴趣,其中,使用定制光谱仪同时测量从中散射的正交偏振态[2,3,4]这样可以避免同步和触发与多相机设置相关的问题。它还具有可以提取光轴而无需偏振调制入射光的优点。但是,缺点是线相机像素到波数的非线性需要仔细的光谱仪对准[2]或数字补偿。[5]实际上,在高分辨率PSOCT系统中,由于需要更大的补偿,因此这个问题会进一步加剧带宽。在这里,我们报告了使用类似于Baumann等人[2]的单相机光谱仪构建超宽带PSOCT系统的过程。为了享受该仪器的好处,我们概述了一种数字色散补偿方法,该方法消除了特殊摄像机对准的必要性。我们发现要考虑三种不可忽略的色散类型:1)上述相机像素到波数的非线性; 2)样品本身的折射率色散; 3)OCT臂之间的色散不平衡干涉仪。后者在时域高分辨率OCT中得到了公认,其中成功地采用了数字色散补偿方法对其进行了处理。 [6]对于我们的SDOCT应用,我们发现色散类型1和2具有相同的功能效果,可以组合为一个补偿步骤,因此,可以使用许多以前的补偿方法。但是,我们发现有必要在分析技术中增加两个步骤,从而调整两个偏振图像的相对缩放比例和位置以对齐散射体。我们还发现,通过拟合较大的多项式阶数可以获得更好的结果。我们展示了我们的技术如何为高分辨率PSOCT提供正交偏振图像之间的精确对准。

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