Fig. 4From: Super-resolution visualization and modeling of human chromosomal regions reveals cohesin-dependent loop structuresMulti-scale whole nucleus simulations of chromosomes with compartments and loops. a Multi-scale whole nucleus simulation approach. Shown are simulation snapshots, where each of the 46 chromosomes is modeled as a polymer chain with a distinct color. Chromosome 1 is highlighted in blue, chromosome 2 in red. Simulations proceed in three consecutive phases. In phase 1, all chromosome chains are coarse grained, with 1 bead for every megabase of DNA, and tā=ā3āĆĀ 106 iterations of Langevin dynamics are computed. In phase 2, chromosome 1 is fine-grained progressively in five successive stages. At each stage, beads of chromosome 1 are replaced by 2 or 5 smaller beads, each representing 2 or 5 times smaller DNA segments, until each bead corresponds to 5Ā kb of DNA. All other 45 chromosomes are kept coarse-grained (1āMb beads), and tā=ā105 iterations are computed at each stage. In phase 3, a specified number of loops can be formed by creating bonds between non-consecutive bead pairs, and tā=ā105 iterations are computed. Insets to either side of the green rectangle show a polymer segment featuring 3 loops in different colors (right) or no loops (left). The simulations in all three phases also include energy potentials to model the formation of A/B compartments. See āMethodsā for details. b Contact frequency matrices for chromosome 1 as predicted by a simulation with compartments and 15 loops/MbĀ (logarithmic scale). Left: entire chromosome 1 with bins of 1āMb. Alternating A/B compartments are clearly visible. Right: a 2.5-Mb region on chromosome 1 with bins of 25Ā kb. BlocksĀ of enriched contact frequencies consistent with TADs are clearly seen along the diagonal. Color bar indicates the natural logarithm ofĀ counts per binBack to article page