Table 1.
Tetramer | Conductance, pS | Open-state lifetime, ms* | Open-state occupancy | Closed-state occupancy | Median burst duration, ms | Bursts per second |
FL4 | 73 ± 7 | 1.9 ± 0.3 | 4.0 ± 0.4 × 10-2 | 0.9 ± 0.1 | 16 ± 3 | 5 ± 1 |
FL3PM1 | 93 ± 7 | 1.7 ± 0.3 | 5.0 ± 0.5 × 10-2 | 0.7 ± 0.1 | 11 ± 3 | 13 ± 2 |
FL2PM2 | 73 ± 2 | 0.3 ± 0.2† | 2 ± 2 × 10-4 | < < 0.1† | NA | NA |
FL1PM3 | 93 ± 7 | 1.5 ± 0.3 | 2 ± 1 × 10-3 | 0.9 ± 0.1 | 5 ± 0.4 | 0.4 ± 0.3 |
PM4 | 113 ± 7 | 1.4 ± 0.3 | 1.0 ± 0.5 × 10-3 | 0.9 ± 0.1 | 4 ± 0.2 | 0.7 ± 0.3 |
Single-channel properties recorded at V = +150 mV for homotetrameric and heterotetrameric assemblies composed of KvLm-FL and KvLm-PM subunits.
*It is worth noting that fittings of open time distributions of all assemblies but FL4 miss a short-lived component (< 1 ms) (Figs. S2 and S3). The conjecture that all four sensors stabilize the open state is in line with these observations notwithstanding the limitation of our recording system to resolve such brief openings.
†For FL2PM2, open- and closed-state lifetimes are estimates given that the time resolution of the recording prevents rigorous determinations. Open and closed state occupancies do not add up to 1 because the channel resides in a subconductance state(s) for a fraction of the time.