Table 1.

Relaxation and bending properties with statistical errors (1σ) of native WT and inhibited WT-DCMU membranes during the dark cycle.

Sample	q (Å−1)	Γ × 10−4 (1/ns)	Γ/q3 (Å3/ns)	t (ns)	$\tilde{\mathit{\kappa }}$ (kBT)**
WT dark	0.037	2.58 ± 0.38	5.02 ± 0.85	3880.5 ± 564.8	—
WT dark	0.056	10.3 ± 0.83	5.79 ± 0.68	969.9 ± 78.2	—
WT dark	0.103	14.5 ± 0.96	1.29 ± 0.29	688.2 ± 45.4	—
WT dark at y intercept	—	—	1.08 ± 0.14	—	5654.85 ± 1420.5
WT-DCMU dark	0.037	2.68 ± 0.36	5.07 ± 0.82	3729.9 ± 491.7	—
WT-DCMU dark	0.056	4.26 ± 0.28	2.46 ± 0.41	2349.6 ± 156.9	—
WT-DCMU dark	0.103	9.83 ± 0.91	0.89 ± 0.29	1016.6 ± 94.3	—
WT-DCMU dark at y intercept	—	—	0.87 ± 0.06	—	8712.69 ± 1283.8

The relaxation parameters are calculated according to Eq. (1). The effective bending coefficient is calculated according to Eq. (3) from the y intercept of the Lorentz fit in Fig. 2a. **The value 0.00125 kg (m s)⁻¹ is used as the D₂O viscosity at 20 °C in the calculation of the bending modulus. Please see extended Table S1 (Supplementary Information) for comprehensive statistical errors.