Nature, Volume 427Sir Norman Lockyer Macmillan Journals Limited, 2004 - Electronic journals |
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Page 330
... potential hill in the limit of strong B. This energy is intermediate between the bottom and top of the disorder potential , and therefore leads to a non- quantized asymptotic slope whose value is between = O and v = 1. The scatter of ...
... potential hill in the limit of strong B. This energy is intermediate between the bottom and top of the disorder potential , and therefore leads to a non- quantized asymptotic slope whose value is between = O and v = 1. The scatter of ...
Page 549
... potential - dependent shift characteristic of the Q - V curve1o . Finally , the time course of R362H proton channel opening ( Fig . 1b ) is similar to the time course of the gating - charge movement recorded from the non - conducting ...
... potential - dependent shift characteristic of the Q - V curve1o . Finally , the time course of R362H proton channel opening ( Fig . 1b ) is similar to the time course of the gating - charge movement recorded from the non - conducting ...
Page 802
... potential of each ion , Ex , is Ex RT zxF Ini [ X ] ex ( 3 ) where zx is ionic valence , R is universal gas constant , T is tempera- ture , F is Faraday's constant and where brackets denote ionic activity . This secondary active ...
... potential of each ion , Ex , is Ex RT zxF Ini [ X ] ex ( 3 ) where zx is ionic valence , R is universal gas constant , T is tempera- ture , F is Faraday's constant and where brackets denote ionic activity . This secondary active ...
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