A GitHub repository has been created on July 27 2021 with a fresh version of the code (https://github.com/tjjlemaire/PySONIC). All future updates will be pushed to this address. However, you can still use the C4Science repository to access older versions along with the code history.
Low-Intensity Focused Ultrasound Stimulation (LIFUS) is emerging as a promising technology for noninvasive brain stimulation, but many questions remain regarding its mechanisms of action as well as optimal stimulation parameters.
One candidate mechanism is that of *intramembrane cavitation*, in which LIFUS induces high-frequency mechanical deflections of the neural membrane to generate depolarizing currents and trigger action potentials. This phernomenon is decribed mathematically by a *Neuronal Intramembrane Cavitation Excitation (NICE)* model [1-3], whose predictions of cell-type-specific LIFUS responses corroborate a wide range of experimental results on LIFUS-evoked brain activity. However, the NICE model is conceptually complex and tedious to simulate, thereby limiting its adoption by the community.
To adress these limitations, we recently developed the *multiScale Optimized Intramembrane Cavitation (SONIC)* model , a computationally efficient variant of the NICE model that also defines a more intuititve frame of interpretation for LIFUS-evoked responses.
The PySONIC package is a Python implementation of the SONIC model, allowing to simulate the responses of various neuron types to ultrasonic (and electrical) stimuli.
The package contains four model classes:
- Model defines the generic interface of a model, including mandatory attributes and methods for simulating it.
- BilayerSonophore defines the underlying biomechanical model of intramembrane cavitation.
- PointNeuron defines an abstract generic interface to conductance-based point-neuron electrical models. It is inherited by classes defining the different neuron types with specific membrane dynamics.
- NeuronalBilayerSonophore defines the full electromechanical model for any given neuron type. To do so, it inherits from BilayerSonophore and receives a specific PointNeuron object at initialization.
All model classes contain a simulate method to simulate the underlying model's behavior for a given set of stimulation and physiological parameters. The NeuronalBilayerSonophore.simulate method contains an additional method argument defining whether to perform a detailed (full), coarse-grained (sonic) or hybrid (hybrid) integration of the differential system.
The default (and fastest) simulation method is the sonic method, and makes use of pre-computed tables that are stored in lookup files within the package architecture (in the lookups subfolder). These large binary files are handled by the git-lfs utility, which sets up dynamic links to these files without storing them physically in the repository, thereby avoiding to store their entire history. Hence, you must install git-lfs in order to download the lookup files together with the repo.
Numerical integration routines are implemented outside the models, in a separate solvers module:
- PeriodicSolver integrates a differential system periodically until a stable periodic behavior is detected.
- EventDrivenSolver integrates a differential system across a specific set of "events" that modulate the stimuluation drive over time.
- HybridSolver inherits from both PeriodicSolverand EventDrivenSolver. It integrates a differential system using a hybrid scheme inside each "ON" or "OFF" period:
- The full ODE system is integrated for a few cycles with a dense time granularity until a periodic stabilization detection
- The profiles of all variables over the last cycle are resampled to a far lower (i.e. sparse) sampling rate
- A subset of the ODE system is integrated with a sparse time granularity, while the remaining variables are periodically expanded from their last cycle profile, until the end of the period or that of an predefined update interval.
- The process is repeated from step 1
Several conductance-based point-neuron models are implemented that inherit from the PointNeuron generic interface.
Among them, several CNS models:
- CorticalRS: cortical regular spiking (RS) neuron
- CorticalFS: cortical fast spiking (FS) neuron
- CorticalLTS: cortical low-threshold spiking (LTS) neuron
- CorticalIB: cortical intrinsically bursting (IB) neuron
- ThalamicRE: thalamic reticular (RE) neuron
- ThalamoCortical: thalamo-cortical (TC) neuron
- OstukaSTN: subthalamic nucleus (STN) neuron
But also some valuable models used in peripheral axon models:
- FrankenhaeuserHuxleyNode: Amphibian (Xenopus) myelinated fiber node (FHnode)
- SweeneyNode: Mammalian (rabbit) myelinated motor fiber node (SWnode)
- MRGNode: Mammalian (human / cat) myelinated fiber node (MRGnode)
- SundtSegment: Mammalian unmyelinated C-fiber segment (SUseg)
- batches: a generic interface to run simulation batches with or without multiprocessing
- parsers: command line parsing utilities
- plt: graphing utilities
- postpro: post-processing utilities (mostly signal features detection)
- constants: algorithmic constants used across modules and classes
- utils: generic utilities
- Python 3.6+
- Git Large File Storage (LFS)
- Package dependencies (numpy, scipy, ...) are installed automatically upon installation of the package.
- Open a terminal.
- Install git-lfs if not already done. This step is crucial as it ensures that lookup tables will be downloaded when you clone the repository.
- Activate a Python3 environment if needed, e.g. on the tnesrv5 machine:
source /opt/apps/anaconda3/bin activate
- Check that the appropriate version of pip is activated:
- Clone the repository and install the python package:
git clone https://c4science.ch/diffusion/4670/pysonic.git
pip install -e .
You can easily run simulations of any implemented point-neuron model under both electrical and ultrasonic stimuli with various temporal protocols, and visualize the simulation results, in just a few lines of code. Here's an example:
python import logging import matplotlib.pyplot as plt from PySONIC.utils import logger from PySONIC.neurons import getPointNeuron from PySONIC.core import NeuronalBilayerSonophore, AcousticDrive from PySONIC.core.protocols import * from PySONIC.plt import GroupedTimeSeries logger.setLevel(logging.INFO) # Define point-neuron model and corresponding neuronal bilayer sonophore object nbls = NeuronalBilayerSonophore(32e-9, getPointNeuron('RS')) # Define stimulus drive and time protocol drive = AcousticDrive(500e3, 100e3) pp = PulsedProtocol(100e-3, 100e-3, tstart=10e-3) # Run simulation and plot results data, meta = nbls.simulate(drive, pp) GroupedTimeSeries([(data, meta)]).render() plt.show()
Have a look at the demo.ipynb notebook located in the notebooks folder for more details.
You can easily run simulations of all 3 model types using the dedicated command line scripts. To do so, open a terminal in the scripts directory.
- Use run_mech.py for simulations of the mechanical model upon ultrasonic stimulation. For instance, for a 32 nm radius bilayer sonophore sonicated at 500 kHz and 100 kPa:
python run_mech.py -a 32 -f 500 -A 100 -p Z
- Use run_estim.py for simulations of point-neuron models upon intracellular electrical stimulation. For instance, a regular-spiking (RS) neuron injected with 10 mA/m2 intracellular current for 30 ms:
python run_estim.py -n RS -A 10 --tstim 30 -p Vm
- Use run_astim.py for simulations of point-neuron models upon ultrasonic stimulation. For instance, for a coarse-grained simulation of a 32 nm radius bilayer sonophore within a regular-spiking (RS) neuron membrane, sonicated at 500 kHz and 100 kPa for 150 ms:
python run_astim.py -n RS -a 32 -f 500 -A 100 --tstim 150 --method sonic -p Qm
Additionally, you can run batches of simulations by specifying more than one value for any given stimulation parameter (e.g. -A 100 200 for sonication with 100 and 200 kPa respectively). These batches can be parallelized using multiprocessing to optimize performance, with the extra argument --mpi.
By default, simulation results are neither shown, nor saved.
To view results directly upon simulation completion, you can use the -p [xxx] option, where [xxx] can be all (to plot all resulting variables) or a given variable name (e.g. Z for membrane deflection, Vm for membrane potential, Qm for membrane charge density).
To save simulation results in binary .pkl files, you can use the -s option. You will be prompted to choose an output directory, unless you also specify it with the -o <output_directory> option. Output files are automatically named from model and simulation parameters to avoid ambiguity.
When running simulation batches, it is highly advised to specify the -s option in order to save results of each simulation. You can then visualize results at a later stage.
To visualize results, use the plot_timeseries.py script. You will be prompted to select the output files containing the simulation(s) results. By default, separate figures will be created for each simulation, showing the time profiles of all resulting variables. Here again, you can choose to show only a subset of variables using the -p [xxx] option. Moreover, if you select a subset of variables, you can visualize resulting profiles across simulations in comparative figures wih the --compare option.
Several more options are available. To view them, type in:
python <script_name> -h
You can easily add other neuron types into the package, providing their ion channel populations and underlying voltage-gated dynamics equations are known.
To add a new point-neuron model, follow this procedure:
- Create a new file, and save it in the neurons sub-folder, with an explicit name (e.g. my_neuron.py).
- Copy-paste the content of the template.py file (also located in the neurons sub-folder) into your file.
- In your file, change the class name from TemplateNeuron to something more explicit (e.g. MyNeuron), and change the neuron name accordingly (e.g. myneuron). This name is a keyword used to refer to the model from outside the class. Also, comment out the addSonicFeatures decorator temporarily.
- Modify/add biophysical parameters of your model (resting parameters, reversal potentials, channel conductances, ionic concentrations, temperatures, diffusion constants, etc...) as class attributes. If some parameters are not fixed and must be computed, assign them to the class inside a __new__ method, taking the class (cls) as sole attribute.
- Specify a dictionary of names:descriptions of your different differential states (i.e. all the differential variables of your model, except for the membrane potential).
- Modify/add gating states kinetics (alphax and betax methods) that define the voltage-dependent activation and inactivation rates of the different ion channnels gates of your model. Those methods take the membrane potential Vm as input and return a rate in s-1. Alternatively, your can use steady-state open-probabilties (xinf) and adaptation time constants (taux) methods.
- Modify the derStates method that defines the derivatives of your different state variables. These derivatives are defined inside a dictionary, where each state key is paired to a lambda function that takes the membrane potential Vm and a states vector x as inputs, and returns the associated state derivative (in <state_unit>/s).
- Modify the steadyStates method that defines the steady-state values of your different state variables. These steady-states are defined inside a dictionary, where each state key is paired to a lambda function that takes the membrane potential Vm as only input, and returns the associated steady-state value (in <state_unit>). If some steady-states depend on the values of other-steady states, you can proceed as follows:
- define all independent steady-states functions in a dictionary called lambda_dict
- add dependent steady-state functions to the dictionary, calling lambda_dict[k](Vm) for each state k whose value is required.
- Modify/add membrane currents (iXX methods) of your model. Those methods take relevant gating states and the membrane potential Vm as inputs, and must return a current density in mA/m2. You also need to modify the docstring accordingly, as this information is used by the package.
- Modify the currents method that defines the membrane currents of your model. These currents are defined inside a dictionary, where each current key is paired to a lambda function that takes the membrane potential Vm and a states vector x as inputs, and returns the associated current (in mA/m2).
- Add the neuron class to the package, by importing it in the __init__.py file of the neurons sub-folder:
python from .my_neuron import MyNeuron
- Verify your point-neuron model by running simulations under various electrical stimuli and comparing the output to the neurons's expected behavior. Implement required corrections if any.
- Uncomment the addSonicFeatures decorator on top of your class. This decorator will automatically parse the derStates, steadyStates and currents methods in order to adapt your neuron model to US stimulation. For this to work, you need to make sure to:
- keep them as class methods
- check that all calls to functions that depend solely on Vm appear directly in the methods' lambda expressions and are not hidden inside nested function calls.
- Pre-compute lookup tables required to run coarse-grained simulations of the neuron model upon ultrasonic stimulation. To do so, go to the scripts directory and run the run_lookups.py script with the neuron's name as command line argument, e.g.:
python run_lookups.py -n myneuron --mpi
If possible, use the --mpi argument to enable multiprocessing, as lookups pre-computation greatly benefits from parallelization.
That's it! You can now run simulations of your point-neuron model upon ultrasonic stimulation.
Code written and maintained by Theo Lemaire (firstname.lastname@example.org).
This project is licensed under the MIT License - see the LICENSE file for details.
If PySONIC contributes to a project that leads to a scientific publication, please acknowledge this fact by citing Lemaire, T., Neufeld, E., Kuster, N., and Micera, S. (2019). Understanding ultrasound neuromodulation using a computationally efficient and interpretable model of intramembrane cavitation. J. Neural Eng.
-  B. Krasovitski, V. Frenkel, S. Shoham, and E. Kimmel, “Intramembrane cavitation as a unifying mechanism for ultrasound-induced bioeffects,” Proc. Natl. Acad. Sci. U.S.A., vol. 108, no. 8, pp. 3258–3263, Feb. 2011, DOI.
-  M. Plaksin, S. Shoham, and E. Kimmel, “Intramembrane Cavitation as a Predictive Bio-Piezoelectric Mechanism for Ultrasonic Brain Stimulation,” Physical Review X, vol. 4, no. 1, Jan. 2014, DOI.
-  M. Plaksin, E. Kimmel, and S. Shoham, “Cell-Type-Selective Effects of Intramembrane Cavitation as a Unifying Theoretical Framework for Ultrasonic Neuromodulation,” eNeuro, vol. 3, no. 3, Jun. 2016, DOI.
-  T. Lemaire, E. Neufeld, N. Kuster, and S. Micera, “Understanding ultrasound neuromodulation using a computationally efficient and interpretable model of intramembrane cavitation,” J. Neural Eng., vol. 16, no. 4, p. 046007, Jul. 2019, DOI.