4.8 Article

Heterochromatin drives compartmentalization of inverted and conventional nuclei

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NATURE
卷 570, 期 7761, 页码 395-+

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NATURE PUBLISHING GROUP
DOI: 10.1038/s41586-019-1275-3

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资金

  1. NSF [1504942]
  2. NIH [HG007743, GM114190, HG003143]
  3. Deutsche Forschungsgemeinschaft [SO1054/3, SFB1064]
  4. Department of Defense through the National Defense Science & Engineering Graduate Fellowship (NDSEG) Program
  5. National Institutes of Health Common Fund 4D Nucleome Program [DK107980]
  6. Division Of Physics
  7. Direct For Mathematical & Physical Scien [1504942] Funding Source: National Science Foundation

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The nucleus of mammalian cells displays a distinct spatial segregation of active euchromatic and inactive heterochromatic regions of the genome(1,2). In conventional nuclei, microscopy shows that euchromatin is localized in the nuclear interior and heterochromatin at the nuclear periphery(1,2). Genome-wide chromosome conformation capture (Hi-C) analyses show this segregation as a plaid pattern of contact enrichment within euchromatin and heterochromatin compartments(3), and depletion between them. Many mechanisms for the formation of compartments have been proposed, such as attraction of heterochromatin to the nuclear lamina(2,4), preferential attraction of similar chromatin to each other(1,4-12), higher levels of chromatin mobility in active chromatin(13-15) and transcription-related clustering of euchromatin(16,17). However, these hypotheses have remained inconclusive, owing to the difficulty of disentangling intra-chromatin and chromatin-lamina interactions in conventional nuclei(18). The marked reorganization of interphase chromosomes in the inverted nuclei of rods in nocturnal mammals(19,20) provides an opportunity to elucidate the mechanisms that underlie spatial compartmentalization. Here we combine Hi-C analysis of inverted rod nuclei with microscopy and polymer simulations. We find that attractions between heterochromatic regions are crucial for establishing both compartmentalization and the concentric shells of pericentromeric heterochromatin, facultative heterochromatin and euchromatin in the inverted nucleus. When interactions between heterochromatin and the lamina are added, the same model recreates the conventional nuclear organization. In addition, our models allow us to rule out mechanisms of compartmentalization that involve strong euchromatin interactions. Together, our experiments and modelling suggest that attractions between heterochromatic regions are essential for the phase separation of the active and inactive genome in inverted and conventional nuclei, whereas interactions of the chromatin with the lamina are necessary to build the conventional architecture from these segregated phases.

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