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Simulation and evaluation of stimulation scenarios for targeted vestibular nerve excitation

  • Peter Schier EMAIL logo , Michael Handler , Daniel Baumgarten and Christian Baumgartner
Published/Copyright: September 30, 2016

Abstract

Recent studies show that vestibular implants have the potential to compensate the loss of functionality of the organ of equilibrium. The objective of this study was the development of a simulation framework which estimates the capability of various electrode arrangements and stimulation waveforms to selectively excite the ampullary nerves in the vestibular system. The choice of electrode configuration and stimulation waveform shows a significant influence in resulting selectivity, energy expenditure and injected charge in our simulations. This simulation environment could be beneficial in the development of safe and selective stimulation electrode designs.

1 Introduction

A loss of functionality of the vestibular system due to injuries, diseases or toxins can cause a severe detriment to quality of life. Similar to cochlear implants, this functionality can be re-established with neurostimulation prostheses. For the development of these vestibular implants, electrode configurations need to be defined that allow for selective stimulation of the vestibular nerve bundles while not affecting the neighboring facial nerve and cochlear nerve.

This study focuses on the development of a framework for the realistic simulation of the neuronal responses of nerves located in and around the vestibular system during electrical stimulation. Various mono- and multipolar electrode arrangements, stimulation waveforms and stimulus pulse durations are evaluated to find optimal configurations for a selective and efficacious neural excitation of vestibular ampullary nerves. The results of these simulations are planned to be the foundation of innovative vestibular prosthesis designs.

2 Material and methods

2.1 Data pre-processing

Image data from μCT-scans of human inner ears was provided by the Medical University of Innsbruck. The well segmented image data was meshed by a tetrahedral meshing workflow developed at our institute using the free software library CGAL [1] (see Figure 1). As a simplification of the surrounding structure, the meshed geometry of the vestibular system was embedded into a bone sphere with a diameter of 5 cm. The mesh consisted of approximately 2.4 million elements. Stationary potential distributions of various mono- and bipolar electrode arrangements were computed using the finite element method (FEM) and used as an input for the nerve fiber model as previously described in [2].

Figure 1: Meshed vestibular system with the facial nerve (green), the posterior ampullary nerve (blue) and the adjoined anterior and lateral ampullary nerves (red). In the ampullae of the semicircular canals, several electrode configurations (black) are embedded.
Figure 1:

Meshed vestibular system with the facial nerve (green), the posterior ampullary nerve (blue) and the adjoined anterior and lateral ampullary nerves (red). In the ampullae of the semicircular canals, several electrode configurations (black) are embedded.

2.2 Generation of artificial nerve fibers

The nerve volumes had to be populated with a natural distribution of nerve fibers in order to model realistic neural behaviour during stimulation. A method based on the already available FEM-algorithms was developed. The method uses the volume mesh of a nerve and the surface where the nerve is connected to the sensory epithelium as input. The sensory epithelium is considered as the start surface for the fiber generation algorithm. A distance map to this start surface is calculated to find the distal-most portion of the nerve relative to the sensory epithelium. The surface of this portion is then declared as the target surface, that should be reached by the generated nerve fibers starting from the sensory epithelium. In the next step, a direction field is computed by considering the nerve volume as a volume conductor with constant isotropic conductivity. Constant negative and positive potentials are defined at the source and target surfaces, respectively. The potential distribution was calculated by the FEM and the gradient field of the resulting potential distribution serves as a direction field for the artificial nerve fiber growth (see Figure 2).

Figure 2: Adjoined anterior and lateral ampullary nerves. A low potential is applied at the start surfaces (blue) and a high potential at the end surface (red). Vectors represent the potential gradient field and are used as direction for neuron trajectory generation.
Figure 2:

Adjoined anterior and lateral ampullary nerves. A low potential is applied at the start surfaces (blue) and a high potential at the end surface (red). Vectors represent the potential gradient field and are used as direction for neuron trajectory generation.

Subsequently, 400 fiber start points are scattered across the start surface of every nerve and a tracing algorithm determines the paths through the direction fields. Each fiber is assigned a certain diameter depending on its location of origin on the sensory epithelium [3]. Fibers originating from the center of the sensory epithelium are generally thicker than fibers which start from the border regions. Nodes of Ranvier are then distributed along the neurons with respect to their diameters (see Figure 3).

Figure 3: Start points of different fiber types scattered across the sensory epithelium (A) and artificially generated neural trajectories originating from these start points in the posterior ampullary nerve (B). Black dots along the neurons indicate nodes of Ranvier.
Figure 3:

Start points of different fiber types scattered across the sensory epithelium (A) and artificially generated neural trajectories originating from these start points in the posterior ampullary nerve (B). Black dots along the neurons indicate nodes of Ranvier.

2.3 Mathematical neuron model

A mathematical neuron model is used to predict the behavioural pattern of nerve fibers during electrical stimulation. Hayden’s modified SENN model [2] was used in a first attempt and further elaborated to fit human anatomy. Morphologic data of human nerve fibers [4], [5] were introduced into the nerve model and parameters for afterhyperpolarization effects were adapted accordingly. Different types of neurons based on clinical studies [3] are considered in the simulations. The previously computed potential distribution of a given electrode configuration is scaled proportionally to the stimulus amplitude and interpolated at the nodes of Ranvier for every nerve fiber and serves as an input for the neuron model as described in [6].

2.4 Electrode configurations and stimulation protocols

One monopolar and four bipolar electrode arrangements were simulated for all ampullary nerves using the electrode configurations as shown in Figure 4. In bipolar arrangements one electrode is set active with a current outflow of 1 A and the other is set as reference with a constant potential of 0 V. Since active and reference electrode are also switched, each bipolar configuration has to be computed twice. For the monopolar configuration, the boundary surface of the model was set to a constant reference potential of 0 V.

Figure 4: Spherical electrode configurations in the posterior ampulla. Nerve axial (magenta), nerve tip parallel (cyan) and perpendicular (red) arrangements are oriented orthogonally to each other. The ampullary axial configuration (yellow and brown) is roughly oriented along the axis of the semicircular canal. In case of monopolar stimulation only the yellow electrode is active.
Figure 4:

Spherical electrode configurations in the posterior ampulla. Nerve axial (magenta), nerve tip parallel (cyan) and perpendicular (red) arrangements are oriented orthogonally to each other. The ampullary axial configuration (yellow and brown) is roughly oriented along the axis of the semicircular canal. In case of monopolar stimulation only the yellow electrode is active.

Since it is known that stimulation of proximal neurons mostly depends on the cathodic phase while anodic pulses affect distal parts of the nerve fibers [7], a number of clinical neurostimulation devices targeting tissue in close proximity use pseudo-monophasic, cathodic stimulation. These pulses consist of a short cathodic phase with a high amplitude and a long refractory anodic phase with low amplitude. To avoid tissue damage, it is required that the stimulus is charge balanced [8].

The influence of stimulus shape variation of the cathodic phase was tested by exciting the nerves with the same rectangular, sinusoidal, linearly increasing and decreasing as well as exponentially increasing and decreasing pulses as described by Sahin [9]. Instead of a gaussian pulse a centered triangular pulse was used. Stimulus durations were initially short (10 μs) and systematically increased up to 500 μs to evaluate the influence of different pulse spans.

2.5 Evaluation

A binary search algorithm is used to determine the excitation current strength threshold. The scaling factor of the potential distribution is varied until the lower and upper search boundary differ < 0.1% from each other. The selectivity of electrode configurations is determined via receiver operating characteristic (ROC) curves. The true positive rate is defined as the ratio between excited targeted nerve fibers and all targeted nerve fibers. The false positive rate is computed correspondingly for non-targeted neurons. The area under the ROC-curve (AUC) is considered as evaluation criterion for selectivity efficiency. Higher AUC-values indicate a better selectivity.

3 Results

Variations regarding electrode configurations and stimulation protocols were simulated in order to maximize fiber recruitment in the targeted nerve while minimizing the excitation of non-targeted nerves.

3.1 Influence of different electrode arrangements

In a first step, the ampullary nerve with the lowest overall selectivity was determined. It was assumed that the effect of an alteration of the electrode arrangement would be easier to detect in this nerve. Therefore, improvements in selectivity would also be more visible. Fiber recruitment patterns and their corresponding AUC were computed using monopolar stimulation in each ampulla. The interpolated external potential in each node was scaled by a biphasic, symmetric, cathodic-phase-first stimulus protocol with 200 μs phase duration. The lateral ampullary nerve exhibited the lowest AUC in these simulations. Because of the central position of the lateral ampulla and the proximity to the facial nerve, this outcome was expected.

Further simulations using various bipolar electrode arrangements (see Figure 4) with the same stimulus protocol were conducted in the lateral ampulla. Every bipolar configuration yielded at least one active-reference electrode combination which was superior to monopolar stimulation in terms of selectivity (see Table 1). However, the current strength threshold required for excitation of targeted neurons was significantly higher in all bipolar cases. The best selectivity was achieved by the nerve tip perpendicular arrangement with its active electrode located further inside the SCC than the reference electrode. This is in accordance with the simulation results performed by Hayden et al. [2].

Table 1:

AUC values for monopolar and bipolar electrode arrangements. For bipolar arrangements only the better active-reference electrode combination is depicted.

ArrangementLocation of active electrodeAUC
Monopolar0.680
Ampullary axialProximal to target nerve0.687
Nerve axialProximal to target nerve0.785
Nerve tip perpendicularMedial to target ampulla0.810
Nerve tip parallelDistal to anterior ampulla0.764

3.2 Influence of stimulus shape variation

After determining the best electrode arrangement, the shape and duration of stimulus protocols were varied (see section 2.4). Although there were no significant differences between the pulse shapes in terms of selectivity, it was apparent throughout all stimulus patterns that shorter pulses exhibit better selectivity than longer pulses.

Injected charge and expended energy are indicators for tissue damage and battery life. In order to calculate these two parameters for each waveform, the current strength required for excitation of 80% of targeted nerve fibers was computed for every simulation. Charge and energy are plotted against pulse duration and against each other to determine optimal waveform shapes (see Figure 5). The simulation results exhibit high accordance with similar studies from existing literature [9], [10]. Injected charge and energy consumption show identical behaviour for the same waveforms.

Figure 5: Injected charge and required energy strongly depend on the choice of stimulus shape and -duration. For short pulse durations, the least energy is expended by the centered triangular waveform. For longer pulses the exponentially increasing and decreasing waveforms are a reasonable choice.
Figure 5:

Injected charge and required energy strongly depend on the choice of stimulus shape and -duration. For short pulse durations, the least energy is expended by the centered triangular waveform. For longer pulses the exponentially increasing and decreasing waveforms are a reasonable choice.

4 Discussion

A computer simulation framework for the generation of artificial nerve fibers and the estimation of their excitation thresholds was developed. Based on image data of the human inner ear, several electrode arrangements and stimulation pulse waveforms were tested to evaluate their selectivity, injected charge and energy expenditure.

Bipolar electrode configurations yielded a better selectivity at the cost of higher energy expenditure than monopolar stimulation. In terms of waveform shapes, sinusoidal and especially centered triangular pulses showed promising results with regards to reduced charge injection and lower required energy thresholds.

5 Outlook

As further progress of the study, the current spherical electrodes will be replaced by an elaborated design. Utricular and saccular nerves are planned to be embedded in the model to simulate undesirable side effects on the otolith organs. An implementation of the auditory nerve is considered as well. In our future studies the tool will contribute to the analysis of novel electrode configurations and stimulus patterns. This could eventually pave the way for a safer and more selective stimulation electrode design.

Acknowledgement

This work was supported by the Standortagentur Tirol within the K-Regio project VAMEL. The authors would like to thank MED-EL and the K-Regio Project partners for their support as well as the Medical University of Innsbruck for their highly detailed image data.

Author’s Statement

Research funding: The author state no funding involved. Conflict of interest: Authors state no conflict of interest. Material and Methods: Informed consent: Informed consent has been obtained from all individuals included in this study. Ethical approval: The conducted research is not related to either human or animal use.

References

[1] The CGAL Project. CGAL User and Reference Manual. Edition 4.8. CGAL Editorial Board.Search in Google Scholar

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[3] Fernández C, Baird RA, Goldberg JM. The vestibular nerve of the chinchilla. I. Peripheral innervation patterns in the horizontal and superior semicircular canals. J Neurophysiol. 1988;60:167–81.10.1152/jn.1988.60.1.167Search in Google Scholar PubMed

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Published Online: 2016-9-30
Published in Print: 2016-9-1

©2016 Peter Schier et al., licensee De Gruyter.

This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License.

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