Fig. 4

Real-time observation of strand transfer and apical interface stability in STCs. a Scheme depicting signatures of strand transfer. Top: binding and reaction near plectoneme end loops minimally affect σz but enables supercoil release through apical interface unbinding (green arrow) and rotational relaxation (black arrow). Bottom: binding near the origin of the plectoneme suppresses σz, strand transfer quenches dynamic bridging by intasome-target anchoring. b, c Extension time-traces of supercoiled target DNA reacting with intasome, depicting stepwise extension increments (b) and extension hopping followed by a stable extension level (c). d Extension time-trace of supercoiled target DNA reacting with WT intasome. External magnets introduce supercoils that are released in steps due to transient apical interface unbinding. Extension plateaus quantify dwell times ΔtApicSTC, step sizes Δz quantify extension increments. e In the plectonemic regime, the number of turns released per unbinding event ΔLk is proportional to Δz. f ΔLk distribution (kernel density estimate; bandwidth 0.2 turns). Inset: Fourier transformation after subtracting an exponential background. g Dependence of step size ΔLk distribution on the sign of ΔLkTCC in TCCs and on the sign of the torque ΓSTC applied to STCs (red data points are mean <ΔLk> and error bars are 95% CI as obtained from an exponential fit; Supplementary Fig. 7). h Dependence of dwell times ΔtApicSTC on ΔLkTCC and ΓSTC (red data points are mean lifetime τApicSTC and error bars are 95% CI as obtained from an exponential fit; Supplementary Fig. 7). Significance calculated using two-sample Kolmogorov–Smirnov test (nTCC+STC+ = 227; nTCC+STC‒ = 288; nTCC−STC+ = 412; nTCC‒STC‒ = 444). Source data are provided as a Source Data file