Leung A F
J Muscle Res Cell Motil. 1982 Dec;3(4):399-418. doi: 10.1007/BF00712091.
The laser diffraction of single cardiac muscle cells shows distinctive diffraction orders and has the following characteristics. (1) When projected on a screen each diffraction order can be described as an irregular column of fine structures consisting of elliptical spots and short jagged stripes. (2) The fine structures associated with the left and right diffractions of the same diffraction order cannot be correlated according to the plane grating equation, and they do not interchange after the cell has been rotated by 180 degrees around its length. (3) For the same diffraction order, the average diffraction angle of the fine structures as a function of laser incident angle follows the plane grating equation. (4) The meridional diffraction angles of different orders are not related by the plane grating equation. (5) For the same diffraction order, the total intensities of the left and right diffractions are not equal. (6) The left or right intensity of a diffraction column shows a single broad peak as a function of laser incident angle. The incident angles corresponding to the left and right peaks are symmetrical to the axis of normal incidence and are interpreted as the Bragg angles of the Z-discs and the planes formed by the intersections of the A- and I-bands of individual myofibrils. The diffraction measurements are consistent with a model in which the myofibrils are randomly packed in the cell and each myofibril acts as a cylindrical diffractor of one-dimensional order.
单个心肌细胞的激光衍射显示出独特的衍射级次,并具有以下特征。(1) 当投射到屏幕上时,每个衍射级次都可描述为由椭圆形斑点和短锯齿状条纹组成的不规则细结构柱。(2) 同一衍射级次的左右衍射相关的细结构不能根据平面光栅方程相互关联,并且在细胞绕其长度旋转180度后它们不会互换。(3) 对于同一衍射级次,细结构的平均衍射角作为激光入射角的函数遵循平面光栅方程。(4) 不同级次的子午衍射角与平面光栅方程无关。(5) 对于同一衍射级次,左右衍射的总强度不相等。(6) 衍射柱的左或右强度作为激光入射角的函数呈现单个宽峰。左右峰对应的入射角相对于法向入射轴对称,并被解释为Z盘以及单个肌原纤维的A带和I带相交形成的平面的布拉格角。衍射测量结果与一个模型一致,在该模型中,肌原纤维随机排列在细胞中,并且每个肌原纤维充当一维有序的圆柱形衍射体。