=============================================================================== VMO Feedback Model on ModelDB =============================================================================== ------------------------------------------------------------------------------- Sensory feedback in a multiple oscillator model of place cell activity ------------------------------------------------------------------------------- :Authors: Joseph D. Monaco [1], James J. Knierim [1], Kechen Zhang [2] :Contact: jmonaco@jhu.edu :Organization: [1] Zanvyl Krieger Mind/Brain Institute, Department of Neuroscience, Johns Hopkins University, Baltimore, MD, USA; [2] Department of Biomedical Engineering, Johns Hopkins School of Medicine, Baltimore, MD, USA :Abstract: Mammals navigate by integrating self-motion signals ('path integration') and occasionally fixing on familiar environmental landmarks. The rat hippocampus is a model system of spatial representation in which place cells are thought to integrate both sensory and spatial information from entorhinal cortex. The localized firing fields of hippocampal place cells and entorhinal grid cells demonstrate a phase relationship with the local theta (6-10 Hz) rhythm that may be a temporal signature of path integration. However, encoding self-motion in the phase of theta oscillations requires high temporal precision and is susceptible to idiothetic noise, neuronal variability, and a changing environment. We present a model based on oscillatory interference theory, previously studied in the context of grid cells, in which transient temporal synchronization among a pool of path-integrating theta oscillators produces hippocampal-like place fields. We hypothesize that a spatiotemporally extended sensory interaction with external cues modulates feedback to the theta oscillators. We implement a form of this cue-driven feedback and show that it can restore learned fixed-points in the phase code of position. A single cue can smoothly reset oscillator phases to correct for both systematic errors and continuous noise in path integration. Further, simulations in which local and global cues are rotated against each other reveal a phase-code mechanism in which conflicting cue arrangements can reproduce experimentally observed distributions of 'partial remapping' responses. This abstract model demonstrates that phase-code feedback can provide stability to the temporal coding of position during navigation and may contribute to the context-dependence of hippocampal spatial representations. While the anatomical substrates of these processes have not been fully characterized, our findings suggest several signatures that can be evaluated in future experiments. Installation ------------ Please see the ``INSTALL`` file for details, but you essentially need to have the Enthought EPD python distribution installed. Then you unzip this archive, go into the new directory and run ``sudo python setup.py install``. The model can then be run interactively in an IPython session. Libraries --------- Here is a brief description of the main modules and classes: Top-level Modules ~~~~~~~~~~~~~~~~~ ``vmo`` ``VMOModel``: main model simulation class ``double_rotation`` ``VMODoubleRotation``: subclass that performs double rotation ``session`` ``VMOSession``: container that computes and stores simulation results ``compare`` Functions for comparing remapping responses ``placemap`` ``CirclePlaceMap``: class that computes place fields ``error`` Function definitions for solutions to the phase error integral Subpackages ~~~~~~~~~~~ ``core`` - Base classes for models, analyses, and time-series data ``figures`` - ``PathIntFigure``: basis for Figure 2 - ``RemappingFigure``: basis for Figure 3 - ``FeedbackFigure``: basis for Figure 5 * ``VMOTrackModel``: model subclass that tracks phase information * ``VMOToyModel``: implements idealized linear trajectory - ``PhaseNoiseFigure``: basis for Figure 6 - ``MismatchFigure`` [#ip]_: basis for Figures 7 and 8 ``remapping`` - ``VMOExperiment`` [#ip]_: parallelized double rotation simulations - ``MismatchAnalysis``: comprehensive remapping comparisons - ``MismatchTrends``: remapping trends across mismatch angles ``tools`` - A collection of supporting utility functions ``trajectory`` - ``CircleTrackData``: loads trajectory data, computes laps, etc. .. [#ip] These classes farm simulations out to IPython ipengine instances running on your machine. You must first start them in another terminal:: $ ipcluster local -n C Set ``C`` to the number of cores available on your machine. Example Usage ------------- You can run the model itself, specifying various parameters, or you can run pre-cooked analyses that were used as the basis of figures in the paper. Running the model ~~~~~~~~~~~~~~~~~ Start IPython in ``-pylab`` mode:: $ ipython -pylab Then, import the libraries and create a model instance:: In [0]: from vmo_feedback import * In [1]: model = VMOModel() It will automatically load the trajectory data. To see all the user-settable parameters, you can print the model:: In [2]: print model VMOModel(Model) object -------------------------------- Parameters: C_W : 0.050000000000000003 N_cues : 3 N_cues_distal : 3 N_cues_local : 3 N_outputs : 500 N_theta : 1000 cue_offset : 0.0 cue_std : 0.15707963267948966 distal_cue_std : 0.15707963267948966 distal_offset : 0.0 done : False epsilon : 0.050000000000000003 gamma_distal : 0.46101227797811462 gamma_local : 0.46101227797811462 init_random : True lambda_range : (100, 200) local_cue_std : 0.15707963267948966 local_offset : 0.0 monitoring : True omega : 7 pause : False refresh_fixed_points : True Tracking: C_distal, C_local, I, active_distal_cue, x, y, alpha, active_local_cue, vel In parameter names above, parameters with ``local`` and ``distal`` control one of the two cue sets (local rotate CCW, distal CW) to allow for independent manipulation:: C_W feedforward connectivity and N_theta number of theta oscillators N_outputs the number of output units; each receives input from C_W*N_theta oscillators N_cues number of cues per cue set cue_offset starting point on the track for laying out cues cue_std cue size (s.d.) in radians epsilon error tolerance lambda_range the range of spatial scales (multiplied by 2PI) gamma peak cue gains; if not specified, these gains are set automatically based on epsilon init_random whether each trial gets randomized initial phases omega frequency of the carrier signal. The values shown are the defaults used for the paper (aside from cue manipulations, etc.). The tracked variables are time-series data that are saved from the simulation:: C_* cue interaction coefficients I summed oscillatory inputs for each output x, y trajectory position vel instantaneous velocity vector alpha track angle active_*_cue index number of the currently active cue Parameters can be changed by passing them as keyword arguments to the constructor. To simulate only 200 oscillators, you would call ``VMOModel(N_theta=200)``. Run the simulation:: In [3]: model.advance() Look at the tracked data:: In [4]: data = model.post_mortem() In [5]: print data.tracking In [6]: subplot(221) In [7]: plot(data.x, data.y, 'k-') Plot cue coefficients for the local and distal cue sets:: In [8]: subplot(222) In [9]: scatter(x=data.x, y=data.y, c=data.C_local, s=1, linewidths=0) In [10]: subplot(224) In [11]: scatter(x=data.x, y=data.y, c=data.C_distal, s=1, linewidths=0) Now compute the output responses based on the amplitude envelope of excitation. These are computed and stored in ``VMOSession`` objects based on the simulation results:: In [12]: session = VMOSession(model) Get the population response matrix and plot the place fields:: In [13]: subplot(223) In [14]: R = session.get_population_matrix() In [15]: plot(R.T, 'k-') In [16]: xlim(0, 360) The ``VMODoubleRotation`` is a subclass that automatically performs double rotations across a series of mismatch angles. Running double rotation and computing the responses is as easy as:: In [17]: drmodel = VMODoubleRotation() In [18]: drmodel.advance_all() In [19]: drsessions = VMOSession.get_session_list(drmodel) The analysis subclasses in the remapping subpackage encapsulate double rotation experiment simulations and various remapping analyses. Running figure analyses ~~~~~~~~~~~~~~~~~~~~~~~ To run the figure analyses, you simply create an analysis object and run it by calling it with analysis parameters. The single-cue feedback analysis is performed by the ``FeedbackFigure`` analysis class:: In [20]: fig = FeedbackFigure(desc='test') In [21]: fig.collect_data? The first command creates an analysis object with the description 'test'. The second command (with the ``?``) tells IPython to print out meta-data about the ``collect_data`` method. This is the method that actually performs the analysis when you call the object, so this tells you the available parameters along with their descriptions. We could run the analysis with different cue sizes:: In [22]: fig(cue_sizes=[5, 25]) This performs the simulations, collects data for the figures, and stores data, statistics, and an *analysis.log* file in the analysis directory. When that completes, you can bring up the resulting figure and save it:: In [23]: fig.view() In [24]: fig.save_plots() Running the ``view`` method renders the figures, outputs RGB image files, and saves a *figure.log* file in the analysis directory. Some of the figures have parameter arguments to change the figure. You will have to use the ``create_plots`` method, as this is what the ``view`` method actually calls. To see the figure parameters and make changes:: In [25]: fig.create_plots? In [26]: fig.create_plots(...) The same process can be used for the other figure analysis classes. You can create your own analyses by subclassing from ``core.analysis.BaseAnalysis`` and implementing the ``collect_data`` and ``create_plots`` methods. ---- Please explore the code, and let me know at `jmonaco@jhu.edu <mailto:jmonaco@jhu.edu>`_ if there are any major issues. There are no guarantees that this code will work perfectly everywhere. Enjoy.