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1 slope conductance of Gmax congruent with 690 picosiemens.
2 d a unitary slope conductance of 3.9 +/- 0.2 picosiemens.
3 ngle channel conductance of approximately 13 picosiemens.
4 the channel has a unitary conductance of 5-7 picosiemens.
5 conductance states of 47 +/- 8 and 200 +/- 9 picosiemens.
6 range of conductivities from microsiemens to picosiemens.
7 e with their pore diameter, ranging from 110 picosiemens (~0.5 nanometer pore diameter) to 430 picosi
9 tances were 110 picosiemens at -40 mV and 68 picosiemens at +40 mV, and the mean open time was 0.9 ms
10 Cl, the single-channel conductances were 110 picosiemens at -40 mV and 68 picosiemens at +40 mV, and
13 K(+) ions with a unitary conductance of 113 picosiemens, fivefold larger than the conductance of sev
14 conductances of 161 +/- 7.9 and 67.5 +/- 6.9 picosiemens in symmetric 300 and 150 mm KCl, respectivel
18 onductance of these homomeric receptors (sub-picosiemens) is too small to be resolved directly, and c
19 ncreased membrane conductance from 10 to 260 picosiemens/picofarads due to activation of Ca(2+)-depen
23 ibited a larger K(+) conductance (489 +/- 13 picosiemens (pS) for V2548I versus 364 +/- 5 pS for wild
25 , approximately 700, and approximately 1,000 picosiemens (pS) in symmetrical 150 mm CsCl were observe
26 curve, with a slope conductance of 80 +/- 3 picosiemens (pS) in the +/- 100 mV range of holding pote
27 m: there was a nearly constitutively open 13-picosiemens (pS) state and a second 40-pS level that was
28 exclusively exhibits a main transition to 39 picosiemens (pS) with very rare 13 pS step transitions t
34 e found with large conductances (hundreds of picosiemens), suggesting a major disruption of the membr