Table 3.

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

Sample	q (Å−1)	Γ × 10−4 (1/ns)	Γ/q3 (Å3/ns)	t (ns)	$\tilde{\mathit{\kappa }}$ (kBT)**
WT light	0.037	1.59 ± 0.46	3.11 ± 0.94	6261.7 ± 1793.4	—
WT light	0.056	6.10 ± 0.48	3.54 ± 0.53	1638.8 ± 129.2	—
WT light	0.103	8.47 ± 0.11	0.79 ± 0.32	1180.6 ± 155.1	—
WT light at y intercept	—	—	0.73 ± 0.08	—	12250.10 ± 2707.3
WT-DCMU light	0.037	3.08 ± 0.19	5.99 ± 0.61	3249.9 ± 201.1	—
WT-DCMU light	0.056	3.98 ± 0.25	2.31 ± 0.38	2512.6 ± 160.4	—
WT-DCMU light	0.103	14.3 ± 0.99	1.31 ± 0.3	698.8 ± 48.2	—
WT-DCMU light at y intercept	—	—	1.00 ± 0.07	—	6540.62 ± 967.1

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 S3 (Supplementary Information) for comprehensive statistical errors.