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234 Compensation d’électrode sans calibration<br />

A<br />

injected current<br />

200 pA<br />

20 mV<br />

500 ms<br />

bridge compensation<br />

500 ms<br />

calibration-free technique<br />

200 ms<br />

200 ms<br />

Figure 9.1 – Bridge and dynamic electrode compensation methods illustrated on<br />

a patch clamp recording in a pyramidal neuron from mouse auditory cortex. Top :<br />

injected current, starting with a current step for calibrating the bridge compensation method<br />

(left), and followed by a fluctuating current with fast transients (current B, right). Middle :<br />

bridge compensated membrane potential. Bottom : compensated trace using our technique.<br />

Thus it is often necessary to compensate for the electrode bias in single electrode<br />

recordings. The standard compensation technique is bridge balance, and is<br />

generally done directly on the electrophysiological amplifier. It consists in subtracting<br />

Re ·I from the uncompensated recording, where Re is the estimated electrode<br />

resistance (usually manually adjusted using the response to current pulses). There<br />

are two issues with this method. First, even if Re can be accurately estimated,<br />

the electrode is not a pure resistor : it has a non-zero response time, due to capacitive<br />

components. This produces artifacts in the compensated trace, as shown<br />

in Figure 9.1. When a current pulse is injected (top left), the bridge model overcompensates<br />

the trace at the onset of the pulse, resulting in capacitive transients<br />

of amplitude Re · I (Figure 9.1, middle left). These transients become an issue<br />

when fast time-varying currents are injected, such as simulated synaptic inputs<br />

(Figure 9.1, top right). In this case, capacitive transients distort the compensated<br />

trace, which may even make the detection of action potentials difficult (Figure 9.1,<br />

middle right). The second issue is that the capacitive component of the electrode<br />

can make the estimation of Re difficult, given that Re cannot be estimated in the<br />

bath (it changes after impalement).<br />

A recent technique solves this problem by calibrating a model of the electrode<br />

using white noise current (Brette et al. 2008). However, as with other methods,

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