Shunting inhibition

ID: shunting-inhibition

Shunting inhibition is suppression of another input's effect through increased synaptic conductance: opening additional ion channels lowers effective electrical resistance, reducing the voltage response to a given added electric current. When the added reversal potential equals the resting membrane potential, there can be no voltage change at rest and still be inhibition of a simultaneous input. See 1.4 Limitations of the Leaky Integrate-and-Fire Model.
Use the passive synaptic potential model below with leak , and capacitance . A sustained inward test electric current of alone gives a steady voltage increase of , so . Effective electrical resistance is and the time constant is .
Now hold a shunting conductance open with . With no test electric current, rest stays at . With the same test electric current, total conductance becomes , so the steady voltage increase is only : . Effective electrical resistance is and the time constant is . A faster response can therefore be smaller. At the original rest the shunting electric current is zero; at it is , opposing the voltage excursion.
The factor of three reduction applies to this constant-electric current, constant-conductance example. A finite pulse, conductance-driven input or spatially extended dendrite need not have the same reduction. The interesting feature is conditional action: the shunt can leave a quiet neuron's voltage unchanged yet reshape its response when another input arrives. A model that represents all inhibition as a fixed outward electric current misses this behavior.

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