Abstract
Deep brain stimulation (DBS) is used to treat multiple neuropsychiatric disorders, including Parkinson’s disease (PD). Despite widespread clinical use, its therapeutic mechanisms are unknown. Here, we developed a mouse model of subthalamic nucleus (STN) DBS for PD, to permit investigation using cell type–specific tools available in mice. We found that electrical STN DBS relieved bradykinesia, as measured by movement velocity. In addition, our model recapitulated several hallmarks of human STN DBS, including rapid onset and offset, frequency dependence, dyskinesia at higher stimulation intensity, and associations among electrode location, therapeutic benefit, and side effects. We used this model to assess whether high-frequency stimulation is necessary for effective STN DBS and whether low-frequency stimulation can be effective when paired with compensatory adjustments in other parameters. We found that low-frequency stimulation, paired with greater pulse width and amplitude, relieved bradykinesia. Moreover, a composite metric incorporating pulse width, amplitude, and frequency predicted therapeutic efficacy better than frequency alone. We found a similar relationship between this composite metric and movement speed in a retrospective analysis of human data, suggesting that correlations observed in the mouse model may extend to human patients. Together, these data establish a mouse model for elucidating mechanisms of DBS.
Keywords: Neuroscience
Keywords: Mouse models, Parkinson’s disease
Introduction
Parkinson’s disease (PD) is a neurodegenerative disease characterized by motor deficits, including bradykinesia (slowed movement), rigidity, and tremor. Dopamine replacement therapy relieves many motor symptoms, but is often complicated by the development of prominent motor fluctuations and involuntary movements (1). With few effective pharmacological alternatives, patients are often implanted with electrodes in basal ganglia nuclei for chronic stimulation. Deep brain stimulation of the subthalamic nucleus (STN DBS) (2) is highly effective in relieving bradykinesia, rigidity, and tremor (3). Despite several decades of clinical experience, however, the underlying mechanisms and ideal therapeutic parameters for STN DBS remain unclear (4).
The basal ganglia circuit in PD patients exhibits abnormal firing rate, pattern, and synchronization (5); STN DBS may disrupt or correct one or a number of these changes. At present, clinical practice is delivery of continuous pulsatile stimulation at high frequency. Therapeutic benefit depends on the frequency, current amplitude, and pulse width of stimulation (4). One theory postulates that high-frequency stimulation (HFS) (over 90 Hz) disrupts abnormal basal ganglia activity (6), while other parameters (pulse width and current) may allow spread of stimulation through the STN. In fact, HFS provides greater relief of bradykinesia and tremor, whereas very low-frequency stimulation (LFS) (around 10 Hz) can be ineffective or even potentially deleterious (7). However, a less widely held hypothesis is that any manipulation that perturbs neuronal firing may disrupt abnormal activity, and thus clinicians can compensate for a low setting of any one parameter (frequency, pulse width, or current) by increasing the other two; one study found the current amplitude necessary to relieve rigidity varied inversely with the pulse width (8). A better understanding of how individual parameters contribute to STN DBS efficacy would not only improve symptom management in patients, but might also identify potential therapeutic mechanisms of STN DBS.
Though electrical DBS has been demonstrated in both parkinsonian nonhuman primates (9, 10) and rats (11, 12), a mouse model, combined with the extensive mouse genetic toolbox, would permit complementary cellular and circuit investigations of DBS therapeutic mechanisms. Here, we developed a mouse model of STN DBS in hemiparkinsonian mice. Stimulation relieves bradykinesia and recapitulates a number of features of STN DBS in human patients. We used this model to investigate the relationship between stimulation parameters and therapeutic efficacy, as well as adverse effects, and found that a composite metric based on all 3 stimulation parameters predicted STN DBS efficacy. This relationship also holds in a retrospective analysis of human data, suggesting shared therapeutic features in human and mouse STN DBS. Together, our results provide a valuable tool for predicting DBS efficacy as well as a model for further investigation of STN DBS.
Results and Discussion
Parkinsonian mouse models have contributed to our understanding of both disease pathophysiology and the actions of levodopa (5). However, it is not known whether parkinsonian mice respond to electrical STN DBS in ways similar to that of patients. We identified 6 clinical features of STN DBS for PD, which we used as criteria in a mouse model of STN DBS: (i) STN DBS reduces bradykinesia; (ii) motor benefits are time locked to stimulation; (iii) relief of bradykinesia is frequency dependent (13); (iv) increasing stimulation intensity (across multiple parameters) results in dyskinesia (14); (v) dorsal STN stimulation is more effective than ventral stimulation in relieving bradykinesia (15); and (vi) stimulation closer to the pyramidal tract is more likely to evoke motor contractions (16).
With these criteria in mind, we designed and implanted unilateral 6-lead electrodes (divided into 3 bipolar pairs) in the STN of adult hemiparkinsonian mice, using the unilateral 6-hydroxydopamine (6-OHDA) model (Figure 1, A–C). In these mice, parkinsonism was manifest as both ipsilesional rotational bias (Supplemental Figure 1G; supplemental material available online with this article; https://doi.org/10.1172/JCI122390DS1) and decreased movement velocity (Figure 1H). We used the latter indicator as a measure of bradykinesia, though it may also incorporate other parkinsonian features, such as gait dysfunction. We constructed our 6-lead electrodes to span approximately 300–600 μm (covering the approximately 250 μm vertical span of mouse STN) and implanted them in the ipsilesional STN (Figure 1, D and E, and Supplemental Figure 1, A and B). We selected the optimal electrode pair by stimulating at settings mirroring typical human DBS and DBS in rat models (12, 17) (120 Hz, 200 μA, 60 μs with bipolar, biphasic square waves; Supplemental Figure 1C). The stimulated pair eliciting the highest average movement velocity was used for subsequent experiments (Supplemental Figure 1D). Stimulation at these DBS parameters increased movement velocity in mice (Figure 1, F and G, and Supplemental Video 1); velocity changed at short latency from onset (3.19 ± 0.65 seconds) and offset (0.66 ± 0.10 seconds) of stimulation, corroborating clinical features i and ii. We used 1-minute stimulation epochs to efficiently evaluate a wide array of stimulation parameter combinations, but found that longer periods of stimulation (10 minutes) produced similar improvements in movement velocity (Supplemental Figure 1E). These findings suggest that STN DBS in parkinsonian mice and PD patients share core therapeutic features.
We next explored whether STN DBS in hemiparkinsonian mice shows frequency dependence, as has been observed in humans (criterion iii) (7, 13). To address this question, we varied stimulation frequency while holding current amplitude and pulse width constant (200 μA and 60 μs). Movement velocity scaled relatively linearly, with frequency up to approximately 120 Hz (Figure 1H), mirroring observations in patients using hand tapping speed as the outcome measure (13). However, the range of effective frequencies was much wider (as low as 15 Hz) than reported in patients. In addition to absolute velocity, STN DBS also improved other well-established metrics (17), such as percentage of time moving and relative velocity (normalized to prestim period) in a frequency-dependent manner, though rotational bias was not significantly changed (Supplemental Figure 1, F–H). In humans, dyskinesia emerges as a side effect of higher frequency stimulation (14). Likewise, we found that in mice, higher frequency stimulation, as well as increased pulse width and current, evoked dyskinesia (18) (Figure 2A, criterion iv). These findings suggest that in parkinsonian mice, as in humans, both therapeutic and dyskinetic effects of stimulation relate to stimulation frequency.
To assess the relationship of stimulation location to therapeutic efficacy and dyskinesia (criteria v and vi), we determined the location of DBS in postmortem tissue. Following terminal anesthesia, we made electrolytic lesions using the therapeutic leads (Figure 1E and Figure 2B). We correlated dorsoventral location with the relative velocity of each mouse at standard stimulation settings (120 Hz, 200 μA, and 60 s). As in humans, greater improvements in velocity were seen with more dorsal STN stimulation (Figure 2C). This may relate to targeting sensorimotor STN territories (19, 20) or the zona incerta, stimulation of which is also therapeutic (21, 22). We next correlated electrode distance from the pyramidal tract with the dyskinesia score in response to stimulation at 120 Hz, 300 μA, and 120 μs (parameters that reliably evoked dyskinesias in over half of mice). Again, the mouse model mirrored human data: mice with electrodes closer to the pyramidal tract had greater dyskinesia (Figure 2D). Our model fulfilled all 6 clinical criteria, recapitulating key features of human DBS and indicating it may be a useful tool in understanding STN DBS mechanisms.
A dominant theory is that HFS and LFS produce qualitatively different changes in basal ganglia activity, and thus only HFS is efficacious (7). Alternatively, any combination of frequency, current, and pulse width that sufficiently disrupts STN–basal ganglia circuit activity may be therapeutic. To test these theories using our model, we first assessed the relationship of each of the 3 variables (current, frequency, and pulse width) to movement velocity, while holding the other two constant. As we previously observed, movement velocity showed a strong linear correlation with frequency when pulse width and current were held at constant (Figure 3A). However, we also observed strong linear relationships when only varying pulse width (Figure 3B) or current (Figure 3C), suggesting each variable individually contains linear predictive value. These individual parameters can also be combined in a metric cited in the clinical DBS literature: total electrical energy delivered (TEED) (23). TEED is calculated as follows: [current2 × frequency × pulse width]/impedance. We found that current2, one term in this metric, was also linearly correlated with movement velocity (Figure 3D). Together, these results support the idea that many parameter combinations can provide therapeutic benefit.
While within the limited range tested, all 3 parameters correlated with therapeutic benefit, we wondered whether a combined metric might predict benefit across a wider set of parameters. If so, such a metric might prove a useful tool for clinicians. To explore this possibility, we stimulated STN using 31 different parameter combinations (Supplemental Figure 2A and Supplemental Table 1) and measured the resulting movement velocity. We collapsed each parameter combination into a single value (picombo, where the i subscript indicates constant-current stimulation), calculated as current2 × frequency × pulse width. picombo is based on TEED, but we ascribe no physical meaning to this composite metric and use it only to compare different parameter combinations. We found that the effectiveness of DBS, as measured by movement velocity, scaled linearly with picombo (Figure 3E). This relationship held across stimulation bouts when parameter combinations were grouped into 3 picombo levels (Supplemental Figure 2B). These results also indicate that many different parameter combinations may be effective.
In PD patients, optimal stimulation parameters often change over the first few months of DBS use; typically, one or more parameters must be increased to maintain efficacy (24). This phenomenon may relate to changes in both the electrodes and the surrounding tissue (25). To test for this phenomenon in mice, we performed STN DBS in the same 9 mice at 50 new parameter combinations approximately 2 months later (Supplemental Figure 2A and Supplemental Table 2). Consistent with human data, mice showed less benefit from stimulation at later time points (Supplemental Figure 2C, comparing slopes of solid and dotted lines), but DBS efficacy again scaled linearly with picombo (Supplemental Figure 2C). With these parameters, we also manually scored dyskinesia and found severity scaled linearly with picombo (Supplemental Figure 2D). These findings are consistent with the idea that a composite metric incorporating stimulation pulse width, amplitude, and frequency consistently explains much of the variance in both the therapeutic and dyskinetic effects of STN DBS.
We next generated a model for DBS efficacy, using the regression between stimulation parameters and movement velocity in early DBS testing. This model was based on picombo (Supplemental Figure 3, A–D) and predicts that when current and pulse width are held at levels mimicking standard human stimulation, DBS efficacy will show frequency dependence (Supplemental Figure 3, B and C). However, a more comprehensive exploration of parameter space revealed that increased pulse width and current amplitude can be used to compensate for reduced frequency, extending the range of effective DBS parameters. Similar results were observed when a model was created based on the regression from late DBS testing (Supplemental Figure 3, E and H), though due to the shallower slope of the late DBS regression, the same combination of any 3 parameters produced less therapeutic benefit than in the early model. These models not only explain previous clinical observations, but may provide valuable individualized visualizations of effective parameters for future PD patients.
To determine whether the picombo metric could be used with individual stimulation site data to predict relationships between stimulation site and therapeutic efficacy and/or dyskinesia, we calculated a metric for therapeutic efficacy. We calculated the slope of the correlation between picombo and movement velocity (Supplemental Figure 4A), representing the additional benefit derived from unit increases in picombo. We found that electrode location along the dorsoventral axis showed a modest correlation with vel slope (Supplemental Figure 4B), consistent with human observations and our data at a single stimulation setting (Figure 2C). We next calculated a similar metric for dyskinesia: the slope of the correlation between picombo and the dyskinesia score (dysk slope), an indicator of tendency toward stimulation-induced dyskinesia. In line with our data from a single stimulation setting (Figure 2D), we observed that electrodes closer to the internal capsule tended to have higher dysk slopes (Supplemental Figure 4C). Finally, and perhaps most excitingly, we found no correlation between vel slope and dysk slope (Supplemental Figure 4D). These findings suggest that despite a shared correlation with picombo, improved DBS efficacy and the vulnerability to dyskinesias may be dissociable.
Optimizing patient DBS parameters is common, but extensive controlled testing is challenging in a clinical setting. Indeed, few studies have explored parameter space while measuring quantitative outcomes. However, one human study tested a subset of the parameter space (voltage, frequency, and pulse width) described here, using hand tapping as a measure of bradykinesia (13). We reanalyzed this data to determine whether a similar relationship between stimulation parameters and therapeutic effects governs STN DBS in PD patients. Based on parameter combinations tested in all 12 patients within a range equivalent to those tested in mice (Supplemental Figure 2B and Supplemental Table 3), we calculated a constant-voltage version of picombo (pvcombo = voltage2 × frequency × pulse width) and estimated efficacy. We found that tapping speed was strongly correlated with pvcombo (Figure 3F). These human results are consistent with our findings in parkinsonian mice: STN DBS efficacy for bradykinesia (as measured by locomotor velocity) scales linearly with a combined metric incorporating all 3 stimulation parameters.
Though STN DBS has provided symptomatic relief to PD patients for over 2 decades, ideal parameters for DBS, as well as their underlying therapeutic mechanisms, are still unclear. We used a set of custom-built tools to create a model of STN DBS in hemiparkinsonian mice and leveraged this model to rigorously explore the parameter space for effective DBS. We found that STN DBS is not only effective in restoring near-normal levels of locomotion in parkinsonian mice, but that it recapitulates many key features of STN DBS in PD patients. We found low-frequency DBS could be effective, provided pulse width and current amplitude were adjusted to compensate. Indeed, behavioral effectiveness depended linearly on a combination of all 3 parameters, picombo, suggesting a much larger and more predictable parameter space than previously assumed. Finally, we found that a similar metric strongly predicted relief of bradykinesia in a human DBS data set; however, due to differences in brain size, parkinsonism features, and the stimulation devices used between humans and mice, further human studies are clearly needed.
Our findings support the hypothesis that stimulation frequency does not uniquely predict DBS efficacy; indeed, multiple recent human studies also report low-frequency DBS is effective (26, 27). This relationship may not have been detected previously due to practical clinical barriers to systematic study of parameter space as well as outcome measures used. Utilizing a model such as ours facilitates a wider and more standardized exploration of parameter space, which can be used to generate new hypotheses for optimal human treatment.
We hope the STN DBS mouse model presented here can serve as a platform, allowing the use of the powerful mouse genetic toolbox to investigate how STN DBS modifies activity patterns in basal ganglia–thalamocortical circuits. These tools, such as genetically encoded calcium and voltage sensors, as well as optical and chemical manipulators of neural activity, will allow causal investigation of DBS therapeutic mechanisms in the future, complementing ongoing groundbreaking work in patients, nonhuman primates, and rat models.
Methods
For complete information, see Supplemental Methods.
Statistics.
All behavioral data recorded with video tracking (Noldus Ethovision) was exported to MATLAB (MathWorks) for offline analysis. Statistical differences between stimulation parameters were assessed using 1-way repeated-measures ANOVA, followed by post hoc comparisons using Tukey’s honest significant difference procedure. P adjusted values reported for ANOVAs are P values with the most conservative lower bound adjustment, as calculated by MATLAB. Linear correlations and adjusted R2 values were calculated in MATLAB by fitting data to a linear model. The generalized linear model was created in MATLAB using a normal distribution.
Study approval.
All the animal studies were approved by the Institutional Animal Care and Use Committee of the University of California, San Francisco.
Author contributions
JSS and ABN designed experiments. JSS built all experimental components (commutator, stimulation electrodes) and performed all experiments and analyses. JSS and ABN wrote the manuscript.
Supplementary Material
Acknowledgments
The authors would like to acknowledge P. Starr, J. Ostrem, K. Bender, D. Ron, K. Kay, A.L. Benabid, L. Ptacek, and members of the Nelson lab for providing advice and feedback on the manuscript. We thank R. Brakaj and C. Bair-Marshall for technical support. This work was supported by the National Institute of Neurological Disorders and Stroke (K08 NS081001 to ABN) and UCSF startup funds (to ABN). ABN is the Richard and Shirley Cahill Endowed Chair in Parkinson’s Disease Research.
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Footnotes
Conflict of interest: The authors have declared that no conflict of interest exists.
Copyright: © 2019, American Society for Clinical Investigation.
Reference information: J Clin Invest. 2019;129(9):3833–3838.https://doi.org/10.1172/JCI122390.
Contributor Information
Jonathan S. Schor, Email: Jonathan.Schor@ucsf.edu.
Alexandra B. Nelson, Email: Alexandra.Nelson@ucsf.edu.
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