The present invention relates to measurement of a neural response to a stimulus, and in particular relates to measurement of a compound action potential by using one or more electrodes implanted proximal to the neural pathway.
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 generator, and a power source such as a battery that may be rechargeable by transcutaneous inductive transfer. An electrode array is connected to the pulse generator, and is positioned in the dorsal epidural space above the dorsal column. An electrical pulse applied to the dorsal column by an electrode causes the depolarisation of neurons, and generation of propagating action potentials. The fibres being stimulated in this way inhibit the transmission of pain from that segment in the spinal cord to the brain.
While the clinical effect of spinal cord stimulation (SCS) is well established, the precise mechanisms involved are poorly understood. The DC is the target of the electrical stimulation, as it contains the afferent Aβ fibres of interest. Aβ fibres mediate sensations of touch, vibration and pressure from the skin. The prevailing view is that SCS stimulates only a small number of Aβ fibres in the DC. The pain relief mechanisms of SCS are thought to include evoked antidromic activity of Aβ fibres having an inhibitory effect, and evoked orthodromic activity of Aβ fibres playing a role in pain suppression. It is also thought that SCS recruits Aβ nerve fibres primarily in the DC, with antidromic propagation of the evoked response from the DC into the dorsal horn thought to synapse to wide dynamic range neurons in an inhibitory manner.
Neuromodulation may also be used to stimulate efferent fibres, for example to induce motor functions. In general, the electrical stimulus generated in a neuromodulation system triggers a neural action potential which then has either an inhibitory or excitatory effect. Inhibitory effects can be used to modulate an undesired process such as the transmission of pain, or to cause a desired effect such as the contraction of a muscle.
The action potentials generated among a large number of fibres sum to form a compound action potential (CAP). The CAP is the sum of responses from a large number of single fibre action potentials. The CAP recorded is the result of a large number of different fibres depolarising.
The propagation velocity is determined largely by the fibre diameter and for large myelinated fibres as found in the dorsal root entry zone (DREZ) and nearby dorsal column the velocity can be over 60 ms−1. The CAP generated from the firing of a group of similar fibres is measured as a positive peak potential P1, then a negative peak N1, followed by a second positive peak P2. This is caused by the region of activation passing the recording electrode as the action potentials propagate along the individual fibres.
To better understand the effects of neuromodulation and/or other neural stimuli, it is desirable to record a CAP resulting from the stimulus. 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. Some neuromodulators use monophasic pulses and have capacitors to ensure there is no DC flow to the tissue. In such a design, current flows through the electrodes at all times, either stimulation current or equilibration current, hindering spinal cord potential (SCP) measurement attempts. Moreover, high-pass filter poles in measurement circuitry generate increased electrical artefact with mono-phasic pulses. 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.
A number of approaches have been proposed for recording a CAP. King (U.S. Pat. No. 5,913,882) measures the spinal cord potential (SCP) using electrodes which are physically spaced apart from the stimulus site. To avoid amplifier saturation during the stimulus artefact period, recording starts at least 1-2.5 ms after the stimulus. 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.
Nygard (U.S. Pat. No. 5,758,651) measures the evoked CAP upon an auditory nerve in the cochlea, and aims to deal with artefacts by a sequence which comprises: (1) equilibrating electrodes by short circuiting stimulus electrodes and a sense electrode to each other; (2) applying a stimulus via the stimulus electrodes, with the sense electrode being open circuited from both the stimulus electrodes and from the measurement circuitry; (3) a delay, in which the stimulus electrodes are switched to open circuit and the sense electrode remains open circuited; and (4) measuring, by switching the sense electrode into the measurement circuitry. Nygard also teaches a method of nulling the amplifier following the stimulus. This sets a bias point for the amplifier during the period following stimulus, when the electrode is not in equilibrium. 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.
Daly (US Patent Application No. 2007/0225767) utilizes a biphasic stimulus plus a third phase “compensatory” stimulus which is refined via feedback to counter stimulus artefact. As for Nygard, Daly's focus is the cochlea. Daly's measurement sequence comprises (1) a quiescent phase where stimulus and sense electrodes are switched to Vdd; (2) applying the stimulus and then the compensatory phase, while the sense electrodes are open circuited from both the stimulus electrodes and from the measurement circuitry; (3) a load settling phase of about 1 μs in which the stimulus electrodes and sense electrodes are shorted to Vdd; and (4) measurement, with stimulus electrodes open circuited from Vdd and from the current source, and with sense electrodes switched to the measurement circuitry. 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.
Evoked responses are less difficult to detect when they appear later in time than the artifact, or when the signal-to-noise ratio is sufficiently high. The artifact is often restricted to a time of 1-2 ms after the stimulus and so, provided the neural response is detected after this time window, data can be obtained. This is the case in surgical monitoring where there are large distances between the stimulating and recording electrodes so that the propagation time from the stimulus site to the recording electrodes exceeds 2 ms. Because of the unique anatomy and tighter coupling in the cochlea, cochlear implants use small stimulation currents relative to the tens of mA sometimes required for SCS, and thus measured signals in cochlear systems present a relatively lower artifact. However to characterize the responses from the dorsal columns, high stimulation currents and close proximity between electrodes are required, and therefore the measurement process must overcome artifact directly, in contrast to existing “surgical monitoring” techniques.
Any discussion of documents, acts, materials, devices, articles or the like which has been included in the present specification is solely for the purpose of providing a context for the present invention. It is not to be taken as an admission that any or all of these matters form part of the prior art base or were common general knowledge in the field relevant to the present invention as it existed before the priority date of each claim of this application.
Throughout this specification the word “comprise”, or variations such as “comprises” or “comprising”, will be understood to imply the inclusion of a stated element, integer or step, or group of elements, integers or steps, but not the exclusion of any other element, integer or step, or group of elements, integers or steps.
According to a first aspect the present invention provides a method for measuring a neural response to a stimulus, the method comprising:
According to a second aspect the present invention provides an implantable device for measuring a neural response to a stimulus, the device comprising:
It is to be understood herein that open circuiting of an electrode involves ensuring that the electrode is disconnected from other electrodes, the stimulus source, the measurement circuitry and from voltage rails. Ensuring that the sense electrode is disconnected from the stimulus electrodes during the delay period avoids charge transfer onto the sense electrode(s) and associated artefact. The present invention recognizes that connecting the sense electrodes to the stimulus electrodes during a post-stimulus delay period can undesirably give rise to such charge transfer and associated artefact, particularly if the delay is short relative to the time constant of the stimulus electrodes, the latter typically being around 100 μs. The sense electrode is preferably open circuited during the post-stimulus delay so as to be disconnected from all other electrodes of the array, to prevent such charge transfer to the sense electrode from other non-stimulus electrodes. With particular regard to the case of spinal cord response measurement, the present invention recognizes that in the spinal cord, the stimulation electrodes may never reach equilibrium at the stimulation rates used for chronic pain, so that connecting them to the stimulating electrodes at any time would increase artefact. This lack of equilibrium is due to the nature of the Helmholtz layer which causes fractional pole variation in the electrode impedance with frequency, with time constants as long as tens of milliseconds.
The present invention recognizes that it is beneficial to provide for pre-stimulus settling of the measurement circuitry towards a bio-electrically defined steady state. This ensures that charge recovery occurs in the settling stage prior to the stimulus and not during or immediately after the stimulus and thus does not give rise to artefact during or immediately after the stimulus. Thus, the present invention captures the bio-electrically defined steady state as reference point voltage at the end of the measurement cycle, when the system is in its most stable state. The system then amplifies the difference between the captured voltage and the reference point voltage. Where repeated measurement cycles are undertaken, the present invention further permits the measurement amplifier to accumulate a bias point over multiple cycles rather than re-setting the bias point each cycle. The settle period is preferably sufficiently long to permit the electrodes and circuitry to reach an equilibrium, and for example the settle period may be around 1 ms or greater, as permitted by a stimulus rate. For example if therapeutic stimuli are applied to a dorsal column at about 100 Hz and do not give rise to a slow neural response, then after the approximately 2 ms duration of an evoked fast response up to about 8 ms would be available for the settling period. However, this is generally longer than required and the settling period may be substantially less than 8 ms.
The delay may be in the range of substantially zero to 1 ms, and for example may be about 0.3 ms. Such embodiments permit onset of the neural response to be observed, this typically occurring about 0.3 ms after the stimulus for an electrode 3 cm away from the stimulus site. In embodiments in which an amplifier of the measurement circuitry has a very high dynamic range, and/or if using a measurement electrode closer to the stimulus electrode, the delay may be set to a smaller value for example in the range of 50-200 μs. The delay is preferably set to a value which ensures the measurement amplifier is not saturated and therefore performs linearly at all times when connected without experiencing clipping, and for example a feedback loop may be implemented to determine a suitable delay which avoids amplifier saturation for a given stimulus.
In preferred embodiments of the invention, the signal from the or each sense electrode is passed to a sample-and-hold circuit at the input of a measurement amplifier. In such embodiments measurements of a single evoked response may be obtained from a plurality of sense electrodes, even if the measurement circuitry of each electrode is connected to the control unit only by a two wire bus or the like, as is commonly required in implanted electrode arrays.
Additionally or alternatively, a buffer or follower amplifier is preferably provided in some embodiments, between the sense electrode and the measurement amplifier. The buffer is preferably connected to the sense electrode without interposed switches, so that the high reverse impedance of the buffer effectively prevents switching transients from being conveyed to the sense electrode, thereby avoiding artefact which may arise upon the sense electrode if subjected to such transients. The buffer amplifier is also preferably configured to give current gain to drive a storage capacitor of a sample and hold circuit. A series capacitor may be interposed between the sense electrode and the buffer to avoid DC transfer with the tissue in the event where the amplifier malfunctions. This capacitor also allows the bias voltage of the amplifier to equilibrate as the electrode voltage can drift over time periods of several tens of seconds.
In preferred embodiments of the invention, the stimulus and sense electrodes are selected from an implanted electrode array. The electrode array may for example comprise a linear array of electrodes arranged in a single column along the array. Alternatively the electrode array may comprise a two dimensional array having two or more columns of electrodes arranged along the array. Preferably, each electrode of the electrode array is provided with an associated measurement amplifier, to avoid the need to switch the sense electrode(s) to a shared measurement amplifier, as such switching can add to measurement artefact. Providing a dedicated measurement amplifier for each sense electrode is further advantageous in permitting recordings to be obtained from multiple sense electrodes simultaneously.
The measurement may be a single-ended measurement obtained by passing a signal from a single sense electrode to a single-ended amplifier. Alternatively, the measurement may be a differential measurement obtained by passing signals from two sense electrodes to a differential amplifier.
While recovering charge by short circuiting the stimulus electrodes together, it may in some embodiments be advantageous to disconnect the sense electrode from the measurement circuitry, for example by setting a sample-and-hold circuit to “hold”.
Embodiments of the invention may prove beneficial in obtaining a CAP measurement which has lower dynamic range and simpler morphology as compared to systems more susceptible to artefact. Such embodiments of the present invention may thus reduce the dynamic range requirements of implanted amplifiers, and may avoid or reduce the complexity of signal processing systems for feature extraction, simplifying and miniaturizing an implanted integrated circuit. Such embodiments may thus be particularly applicable for an automated implanted evoked response feedback system for stimulus control. Thus, in a further aspect, the present invention provides a method for feedback control of a neural stimulus, the method comprising an implanted control unit obtaining a CAP measurement in accordance with the method of the first aspect, and the implanted control unit using the obtained CAP measurement to control the delivery of subsequent neural stimuli by the implant.
In some embodiments of the invention, an averaged CAP measurement may be obtained by (i) delivering a first biphasic stimulus which starts with a pulse of a first polarity and then delivers a pulse of a second polarity opposite to the first polarity, and obtaining a first measurement of a CAP evoked by the first stimulus; (ii) delivering a second biphasic stimulus which starts with a pulse of the second polarity and then delivers a pulse of the first polarity, and obtaining a second measurement of a CAP evoked by the second stimulus; and (iii) taking an average of the first measurement and the second measurement to obtain an averaged measurement. Such embodiments exploit the observation that artefact polarity usually reflects the stimulus polarity, whereas the CAP polarity is independent of the stimulus polarity and is instead determined by the anatomy and physiology of the spinal cord membrane, so that averaging the first and second measurements will tend to selectively cancel out artefact. Further noting that for some electrode polarity configurations, such as monopolar, an “anodic first” biphasic stimulus usually has a lower stimulus threshold for neural recruitment than a “cathodic first” biphasic stimulus, the averaged measurement may have a morphology of either (i) a typical CAP of half amplitude if only the anodic-first stimulus exceeds the stimulus threshold; (ii) the average of two CAPs of different amplitude if both stimuli exceed the stimulus threshold but the cathodic first stimulus does not cause saturation recruitment; or (iii) a typical CAP if both stimuli exceed saturation recruitment. Some embodiments may therefore obtain a curve of the averaged measurement vs. stimulus amplitude in order to obtain information regarding the recruitment effected by each stimulus, and such information may be used for feedback control by the implant.
In some embodiments, the method of the present invention may be applied contemporaneously with administration of a drug, in order to gauge efficacy of drug delivery. For example, the implant may comprise or be operatively connected to a drug reservoir and drug delivery pump, with the pump being controlled by feedback based on CAP measurements.
According to another aspect the present invention provides a computer program product comprising computer program code means to make an implanted processor execute a procedure for measuring a neural response to a stimulus, the computer program product comprising computer program code means for carrying out the method of the first aspect.
The present invention recognises that when considering spinal cord stimulation, obtaining information about the activity within the spinal segment where stimulation is occurring is highly desirable. Observing the activity and extent of propagation both above (rostrally of) and below (caudally of) the level of stimulation is also highly desirable. The present invention recognises that in order to record the evoked activity within the same spinal segment as the stimulus requires an evoked potential recording system which is capable of recording an SCP within approximately 3 cm of its source, i.e. within approximately 0.3 ms of the stimulus, and further recognises that in order to record the evoked activity using the same electrode array as applied the stimulus requires an evoked potential recording system which is capable of recording an SCP within approximately 7 cm of its source, i.e. within approximately 0.7 ms of the stimulus.
In preferred embodiments the stimulus comprises a bi-phasic pulse, and the stimulus electrodes have no capacitors. In contrast to a monophasic pulse and capacitor arrangement, such embodiments permit the stimulus electrode current to be interrupted, or forced to zero, at those times where it would interfere with measurement. Omitting capacitors is also desirable in order to minimise the size of the implanted device.
An example of the invention will now be described with reference to the accompanying drawings, in which:
The stimulus 102 induces a voltage on adjacent electrodes, referred to as stimulus crosstalk 104. Where the stimuli 102 are SCP stimuli they typically induce a voltage 104 in the range of about 1-5 V on a SCP sense electrode.
The stimulus 102 also induces electrode artefact, which is a residual voltage on an electrode resulting from uneven charge distribution on its surface. The electrode artefact is indicated in the voltage waveform 104 after cessation of stimulus crosstalk. The stimulus 102 disturbs the galvanic interface between the sense electrode and the tissue, so that after stimulus crosstalk in voltage 104 concludes, a voltage known as the electrode artefact continues on the electrode, as indicated in waveform 104 in
An appropriate stimulus 102 will also induce nerves to fire, and thereby produces an evoked neural response 106. In the spinal cord, the neural response 106 has two major components: a fast response lasting ˜2 ms and a slow response lasting ˜15 ms. The slow response only appears at stimulation amplitudes which are larger than the minimum stimulus required to elicit a fast response. The amplitude of the evoked response seen by epidural electrodes is typically no more than hundreds of microvolts, but in some clinical situations can be only tens of microvolts.
In practical implementation a measurement amplifier used to measure the evoked response does not have infinite bandwidth, and will normally have infinite impulse response filter poles, and so the stimulus crosstalk 104 will produce an output 108 during the evoked response 106, this output being referred to as electrical artefact.
Electrical artefact can be in the hundreds of millivolts as compared to a SCP of interest in the tens of microvolts. Electrical artefact can however be reduced by suitable choice of a high-pass filter pole frequency.
The measurement amplifier output 110 will therefore contain the sum of these various contributions 102-108. Separating the evoked response of interest (106) from the artefacts 104 and 108 is a major technical challenge. For example, to resolve a 10 μV SCP with 1 μV resolution, and have at the input a 5V stimulus, requires an amplifier with a dynamic range of 134 dB. As the response can overlap the stimulus this represents a difficult challenge of amplifier design.
The stimulus and measurement circuitry 200 operates to obtain a SC measurement using five phases. The first phase shown in
In the second phase shown in
In the third phase shown in
The fourth phase shown in
Finally, in the fifth phase shown in
When performing repeated measurement cycles in this fashion, it is noted that the switch positions are the same in the phase 1 “settling” and the phase 5 “measuring” states. Thus, the state of phase 5 is maintained, by virtue of a subsequent phase 1, until the electrodes and circuitry are in equilibrium, even after the time that useful SCP data is no longer present or being captured. Such embodiments thus provide a greater length of the “settle” state.
An advantage of this circuit is that in the phase 2 equilibration, the circuitry around amplifier 210 is a low-pass filter, and is therefore relatively immune to noise and input transients. This also allows the amplifier 210 to accumulate its bias point over successive measurement cycles, as it does not need to be reset for each cycle. Moreover, because of the buffer 206 before the sample/hold 208, the input-referred effect (i.e. the effect upon sense electrode 202) of the charge injection into the sample/hold 208 is lower.
In the embodiment of
The waveforms of
Moreover, it is notable that in this case of a 40 μs pulse width the measurement system is settled and ready to record prior to onset of the evoked CAP. The sense electrode was less than 50 mm from the stimulus electrode, and a post-stimulus delay of 50 μs was observed before the measurement amplifier was switched in to obtain the recordings shown in
In the embodiments of either
In another embodiment of the invention shown in
In contrast, the positive and negative phase stimuli 702, 704 produce SCPs of differing amplitudes, but approximately similar shape and importantly of similar polarity, as this is determined by the anatomy and physiology of the spinal cord nerve fibre membranes. Thus, when the voltages 706, 708 resulting from the positive and negative phase stimuli 702, 704 are recorded, and averaged, the opposite phase stimulation artefacts substantially cancel, leaving the SCP or a combination of the two SCPs 710. Note that in practical situations, the artefact can have much higher amplitude than the SCP, making it much harder to detect the SCP than is apparent from
The response of the spinal cord to these two polarities of stimulation are referred to as the “anodic” and “cathodic” SCP responses, as referred to the electrode considered to be that closest to the recording electrode. I.e. anodic tripolar stimulation makes the central stimulating electrode anodic in the first phase of stimulus. Usually cathodic stimulation has a lower threshold for neural activation than is the case for anodic stimulation. Nevertheless, the SCP polarity is independent of whether the stimulus is anodic 702 or cathodic 704.
This embodiment of the invention further recognises that the averaged waveform of
When the stimulus amplitude is in the range 902 such that only the cathodic stimulus produces an SCP, then the averaged SCP waveform would have a normal SCP morphology but would be half the amplitude compared to a true cathodic SCP due to the averaging. In the region 904 where both the anodic and cathodic responses contribute to the averaged SCP, the resultant averaged SCP waveform will have morphology in between the two measurements. It would not directly represent an SCP, but rather the average of two different SCPs. Nevertheless, this waveform could still be valuable for example in implementing an automatic control loop for stimulation adjustment, as it gives a value proportional to neural recruitment.
It is further to be noted that the principle portrayed by
Some embodiments of the invention, such as the embodiment of
Differential amplifiers are often used because they provide a means to reduce electrode artefact, when other means have been insufficient. However,
With the measurement sequence of the present invention, the artefact is reduced so that some embodiments may instead use a single-ended amplifier, even in situations where previously they would have suffered from too much electrode artefact. Moreover, trials to date show that recording can be initiated with an extremely short time interval from cessation of the stimulus, permitting the same electrode array to be used for recording and stimulation, and even permitting recordings to be made on the electrode immediately adjacent to the stimulus electrode in an electrode array with electrode spacings of less than 10 mm.
Single ended amplifiers have the further advantage that they consist of fewer capacitors and amplifier components than differential amplifiers, so will take up less space on a silicon chip, which is a significant benefit when intended for use in an implanted system with many electrodes and where the silicon area for each amplifier is limited.
Preferred embodiments of the invention may comprise a separate amplifier chain (e.g. 206, 208, 210, see
Further embodiments of the invention may employ divisible electrodes, as discussed below with reference to
A similar effect happens when current flows between two electrodes, as shown in
The model of
The evoked response telemetry of the present invention may in some embodiments be used to monitor the effect of a delivered compound. The administration of compounds (drugs or other chemical therapeutics) to effect a change in the nervous system is common for treatment of a wide number of diseases and disorders. Anaesthetics of various types are administered to the spinal cord for the relief of pain. Perhaps the most common form is administration of anaesthetics in the epidural space for pain relief during child birth.
In such embodiments, a catheter comprising a drug delivery tube may be fitted with electrode elements and configured to obtain neural response measurements in accordance with the present invention in order to monitor drug-induced effects on the neural response. Alternatively an electrode array may be temporarily or permanently implanted and used to apply neural stimuli and monitor the neural response. The neural response measurements may be obtained repeatedly during administration of the drug in order to directly measure the effect of the administered drug and control the dosage delivered.
The plots of
It will be appreciated by persons skilled in the art that numerous variations and/or modifications may be made to the invention as shown in the specific embodiments without departing from the spirit or scope of the invention as broadly described. For example in the measurements stages of charge recovery (
Number | Date | Country | Kind |
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2011901817 | May 2011 | AU | national |
This application is a continuation of U.S. application Ser. No. 17/729,158, filed Apr. 26, 2022, which is a continuation of U.S. application Ser. No. 16/391,181, filed Apr. 22, 2019 and issued on May 10, 2022 as U.S. Pat. No. 11,324,427, which is a continuation of U.S. application Ser. No. 15/184,787, filed Jun. 16, 2016 and issued on May 7, 2019 as U.S. Pat. No. 10,278,600, which is a continuation of U.S. application Ser. No. 14/117,144, filed Nov. 12, 2013 and issued on Jul. 12, 2016 as U.S. Pat. No. 9,386,934, which application is a national stage of Application No. PCT/AU2012/000511, filed May 11, 2012, which application claims the benefit of Australian Provisional Patent Application No. 2011901817, filed May 13, 2011, the disclosures of which are incorporated herein by reference in their entirety.
Number | Date | Country | |
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Parent | 17729158 | Apr 2022 | US |
Child | 18738925 | US | |
Parent | 16391181 | Apr 2019 | US |
Child | 17729158 | US | |
Parent | 15184787 | Jun 2016 | US |
Child | 16391181 | US | |
Parent | 14117144 | Nov 2013 | US |
Child | 15184787 | US |