Albertson D G, Thomson J N
Chromosoma. 1982;86(3):409-28. doi: 10.1007/BF00292267.
Light microscopy of the mitotic chromosomes of Caenorhabditis elegans suggests that non-localized kinetochores are present, since the chromosomes appear as stiff rods 1 to 2 micrometers in length and lack any visible constriction. The holokinetic structure was confirmed by reconstructions of electron micrographs of dividing nuclei in serially sectioned embryos. In prophase the kinetochore appears as an amorphous projection approximately 0.18-0.2 micrometer in diameter in cross section and in longitudinal section it appears to be continuous along the chromatin. At prometaphase and metaphase the kinetochore is a convex plaque covering the poleward face of the chromosome and extending the length of the chromosome. In longitudinal section the kinetochore is a trilaminar structure with electron dense inner and outer layers of 0.02 micrometer, and an electron lucent middle layer of 0.03 micrometer. The inner layer is adjacent to a more electron dense region of chromatin. The kinetochore was also seen as a band extending the length of the chromosome in whole mount preparations of chromosomes stained with ethanolic phosphotungstic acid. Most gamma ray induced chromosome fragments segregate normally in embryonic mitoses, but some fragments display aberrant behavior. Similar behavior was seen in embryos carrying a genetically characterized free duplication. It is suggested that mitotic segregation of small fragments may be inefficient because the probability of attachment of microtubules to the kinetochore is proportional to kinetochore length.
秀丽隐杆线虫有丝分裂染色体的光学显微镜观察表明存在非定位的动粒,因为染色体呈现为长度为1至2微米的硬棒状,且没有任何可见的缢缩。通过对连续切片胚胎中正在分裂的细胞核的电子显微镜照片进行重建,证实了全动粒结构。在前期,动粒在横切面上表现为直径约0.18 - 0.2微米的无定形突起,在纵切面上,它似乎沿着染色质是连续的。在前中期和中期,动粒是一个覆盖染色体向极面并延伸染色体长度的凸形斑块。在纵切面上,动粒是一种三层结构,电子致密的内层和外层厚度为0.02微米,电子透明的中间层厚度为0.03微米。内层与染色质中电子密度更高的区域相邻。在用乙醇磷钨酸染色的染色体整装制片中,动粒也被看作是一条延伸染色体长度的带。大多数γ射线诱导的染色体片段在胚胎有丝分裂中正常分离,但一些片段表现出异常行为。在携带经遗传特征鉴定的游离重复片段的胚胎中也观察到了类似行为。有人提出,小片段的有丝分裂分离可能效率低下,因为微管附着到动粒上的概率与动粒长度成正比。