Fig. 3: Probing biomolecular structures in living cells with STARSS. | Nature Biotechnology

Fig. 3: Probing biomolecular structures in living cells with STARSS.

From: Extending fluorescence anisotropy to large complexes using reversibly switchable proteins

Fig. 3

a, Live human U2OS cells expressing rsEGFP2 targeted to the mitochondrial outer membrane (OM) with different linker sizes were measured using STARSS method 1. A short rigid helical linker (blue, integrated over n = 9 cells) resulted in higher anisotropy values compared with a longer flexible linker (orange, integrated over n = 7 cells). b, Cartoon of histone H2B fused with rsEGFP2 via a prolonged terminal alpha-helix (upper left) as a unit of chromatin filaments of size of ~30 nm (bottom). c, Anisotropy recorded in the rigid and flexible constructs of H2B-rsEGFP2 in U2OS cells with STARSS method 1, in live cells and fixed cells (integrated over n = 3 cells). d, Representative fluorescence intensity image and segmentation map of nucleoli/nucleus (left, scale bar 4 μm) used to split the anisotropy measured with STARSS method 1 in blue and orange datasets (right, integrated over n = 8 cells). e, Anisotropy decays recorded with STARSS method 1 in HeLa cells expressing rigid H2B-rsEGFP2 for interphase chromatin (integrated over n = 8 cells), mitotic chromosomes (integrated over n = 18 cells), treatment of interphase chromatin with TSA (integrated over n = 8 cells) and treatment and recovery of interphase chromatin for ATP depletion (ATPd, both integrated over n = 8 cells). f, Fluorescence count maps (left) and fluorescence anisotropy maps (right) for two representative fields of view of chromatin in an interphase nucleus after ATPd (top), and mitotic chromosomes (bottom). Scale bars, 4 μm. In all relevant panels, error bars and shaded regions of anisotropy values are 95% confidence intervals evaluated from detector noise according to Supplementary Information 20.

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