Method and System for Controlling Electrical Conditions of Tissue II

Abstract

A method for controlling electrical conditions of tissue in relation to a current stimulus. A first current produced by a first current source is delivered to the tissue via a current injection electrode. A second current drawn by a second current source is extracted from the tissue via a current extraction electrode. The second current source is matched with the first current source so as to balance the first current and the second current. A ground electrode which is proximal to the current injection electrode and the current extraction electrode is grounded, to provide a ground path for any mismatch current between the first current and second current. A response of the tissue to the current stimulus is measured via at least one measurement electrode.

Description

CROSS-REFERENCE TO RELATED APPLICATIONS[0001]This application claims the benefit of Australian Provisional Patent Application No. 2012904838 filed 6 Nov. 2012, which is incorporated herein by reference.TECHNICAL FIELD[0002]The present invention relates to controlling the electrical conditions of tissue, for example for use in suppressing artefact to enable improved measurement of a response to a stimulus, such as measurement of a compound action potential by using one or more electrodes implanted proximal to a neural pathway.BACKGROUND OF THE INVENTION[0003]Neuromodulation is used to treat a variety of disorders including chronic pain, Parkinson's disease, and migraine. A neuromodulation system applies an electrical pulse to tissue in order to generate a therapeutic effect. When used to relieve chronic pain, the electrical pulse is applied to the dorsal column (DC) of the spinal cord or dorsal root ganglion (DRG). Such a system typically comprises an implanted electrical pulse gener...

AI Technical Summary

Benefits of technology

The invention reduces noise in a measurement system by reducing the interaction between the stimulus and the measurement recording through the amplifier. This may be achieved by using a blanking circuit or an unblasted amplifier, which simplifies the signal chain. The electrodes used in the system are selected from an implanted electrode array, which has dedicated amplifiers for each electrode to reduce switching noise. This results in a simpler and more accurate measurement of the cortical activity. Overall, this invention helps achieve lower dynamic range requirements and simplifies the signal processing for feature extraction, making it ideal for an automated implanted evoked response feedback system.

Problems solved by technology

While the clinical effect of spinal cord stimulation (SCS) is well established, the precise mechanisms involved are poorly understood.

However, this can be a difficult task as an observed CAP signal will typically have a maximum amplitude in the range of microvolts, whereas a stimulus applied to evoke the CAP is typically several volts.

Electrode artefact usually results from the stimulus, and manifests as a decaying output of several millivolts throughout the time that the CAP occurs, presenting a significant obstacle to isolating the CAP of interest.

The capacitor recovers charge at the highest rate immediately after the stimulus, undesirably causing greatest artefact at the same time that the evoked response occurs.

To resolve a 10 uV SCP with 1 uV resolution in the presence of an input 5V stimulus, for example, requires an amplifier with a dynamic range of 134 dB, which is impractical in implant systems.

As the neural response can be contemporaneous with the stimulus and / or the stimulus artefact, CAP measurements present a difficult challenge of amplifier design.

In practice, many non-ideal aspects of a circuit lead to artefact, and as these mostly have a decaying exponential appearance that can be of positive or negative polarity, their identification and elimination can be laborious.

At typical neural conduction velocities, this requires that the measurement electrodes be spaced around 10 cm or more away from the stimulus site, which is undesirable as the measurement then necessarily occurs in a different spinal segment and may be of reduced amplitude.

As the bias point is reset each cycle, it is susceptible to noise.

The Nygard measurement amplifier is a differentiator during the nulling phase which makes it susceptible to pickup from noise and input transients when a non-ideal amplifier with finite gain and bandwidth is used for implementation.

However a 1 μs load settling period is too short for equilibration of electrodes which typically have a time constant of around 100 μs.

Further, connecting the sense electrodes to Vdd pushes charge onto the sense electrodes, exacerbating the very problem the circuit is designed to address.

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