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单根和束状微管的双折射

Birefringence of single and bundled microtubules.

作者信息

Oldenbourg R, Salmon E D, Tran P T

机构信息

Marine Biological Laboratory, Woods Hole, Massachusetts 02543, USA.

出版信息

Biophys J. 1998 Jan;74(1):645-54. doi: 10.1016/S0006-3495(98)77824-5.

Abstract

We have measured the birefringence of microtubules (MTs) and of MT-based macromolecular assemblies in vitro and in living cells by using the new Pol-Scope. A single microtubule in aqueous suspension and imaged with a numerical aperture of 1.4 had a peak retardance of 0.07 nm. The peak retardance of a small bundle increased linearly with the number of MTs in the bundle. Axonemes (prepared from sea urchin sperm) had a peak retardance 20 times higher than that of single MTs, in accordance with the nine doublets and two singlets arrangement of parallel MTs in the axoneme. Measured filament retardance decreased when the filament was defocused or the numerical aperture of the imaging system was decreased. However, the retardance "area," which we defined as the image retardance integrated along a line perpendicular to the filament axis, proved to be independent of focus and of numerical aperture. These results are in good agreement with a theory that we developed for measuring retardances with imaging optics. Our theoretical concept is based on Wiener's theory of mixed dielectrics, which is well established for nonimaging applications. We extend its use to imaging systems by considering the coherence region defined by the optical set-up. Light scattered from within that region interferes coherently in the image point. The presence of a filament in the coherence region leads to a polarization dependent scattering cross section and to a finite retardance measured in the image point. Similar to resolution measurements, the linear dimension of the coherence region for retardance measurements is on the order lambda/(2 NA), where lambda is the wavelength of light and NA is the numerical aperture of the illumination and imaging lenses.

摘要

我们使用新型偏振显微镜在体外和活细胞中测量了微管(MTs)以及基于微管的大分子组装体的双折射。在水悬浮液中、数值孔径为1.4的条件下成像的单根微管,其峰值相位延迟为0.07纳米。一小束微管的峰值相位延迟随束中微管数量线性增加。轴丝(由海胆精子制备)的峰值相位延迟比单根微管高20倍,这与轴丝中平行微管的九联体和两个单联体排列一致。当细丝离焦或成像系统的数值孔径减小时,测得的细丝相位延迟会降低。然而,我们定义为沿垂直于细丝轴的线积分的图像相位延迟的“相位延迟面积”,被证明与焦点和数值孔径无关。这些结果与我们为用成像光学测量相位延迟而开发的理论高度吻合。我们的理论概念基于维纳的混合电介质理论,该理论在非成像应用中已得到充分确立。我们通过考虑由光学装置定义的相干区域,将其应用扩展到成像系统。从该区域内散射的光在像点相干干涉。相干区域内细丝的存在导致与偏振相关的散射截面,并在像点测得有限的相位延迟。与分辨率测量类似,用于相位延迟测量的相干区域的线性尺寸约为λ/(2NA),其中λ是光的波长,NA是照明和成像透镜的数值孔径。

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