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Merge pull request #2985 from janskaar/sli2py_iaf_psc_exp
Port test_iaf_psc_exp to py
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# -*- coding: utf-8 -*- | ||
# | ||
# test_iaf_psc_exp.py | ||
# | ||
# This file is part of NEST. | ||
# | ||
# Copyright (C) 2004 The NEST Initiative | ||
# | ||
# NEST is free software: you can redistribute it and/or modify | ||
# it under the terms of the GNU General Public License as published by | ||
# the Free Software Foundation, either version 2 of the License, or | ||
# (at your option) any later version. | ||
# | ||
# NEST is distributed in the hope that it will be useful, | ||
# but WITHOUT ANY WARRANTY; without even the implied warranty of | ||
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the | ||
# GNU General Public License for more details. | ||
# | ||
# You should have received a copy of the GNU General Public License | ||
# along with NEST. If not, see <http://www.gnu.org/licenses/>. | ||
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""" | ||
Name: testsuite::test_iaf_psc_exp | ||
Synopsis: (test_iaf_psc_exp) run -> compares response to current step with analytical solution | ||
Description: | ||
A DC current is injected into the neuron using a current generator | ||
device. The membrane potential as well as the spiking activity are | ||
recorded by corresponding devices. | ||
It can be observed how the current charges the membrane, a spike | ||
is emitted, the neuron becomes absolute refractory, and finally | ||
starts to recover. | ||
The timing of the various events on the simulation grid is of | ||
particular interest and crucial for the consistency of the | ||
simulation scheme. | ||
Although 0.1 cannot be represented in the IEEE double data type, it | ||
is safe to simulate with a resolution (computation step size) of 0.1 | ||
ms because by default nest is built with a timebase enabling exact | ||
representation of 0.1 ms. | ||
Author: July 2004, Diesmann | ||
March 2006, Moritz Helias | ||
""" | ||
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import nest | ||
import numpy as np | ||
import numpy.testing as nptest | ||
import pytest | ||
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def test_iaf_psc_exp_dc_input(): | ||
dt = 0.1 | ||
dc_amp = 1000.0 | ||
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nest.ResetKernel() | ||
nest.set(resolution=dt, local_num_threads=1) | ||
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dc_gen = nest.Create("dc_generator", {"amplitude": dc_amp}) | ||
nrn = nest.Create("iaf_psc_exp", 1) | ||
vm = nest.Create("voltmeter", {"interval": 0.1}) | ||
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syn_spec = {"synapse_model": "static_synapse", "weight": 1.0, "delay": dt} | ||
nest.Connect(dc_gen, nrn, syn_spec=syn_spec) | ||
nest.Connect(vm, nrn, syn_spec=syn_spec) | ||
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nest.Simulate(8.0) | ||
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times = vm.get("events", "times") | ||
times -= dt # account for delay to multimeter | ||
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tau_m = nrn.get("tau_m") | ||
R = tau_m / nrn.get("C_m") | ||
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# array for analytical solution | ||
V_m_analytical = np.empty_like(times) | ||
V_m_analytical[:] = nrn.get("E_L") | ||
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# first index for which the DC current is received by neuron. | ||
# DC current will be integrated from this time step | ||
start_index = 1 | ||
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# analytical solution without delay and threshold | ||
vm_soln = nrn.get("E_L") + (1 - np.exp(-times / tau_m)) * R * dc_amp | ||
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# rise until threshold | ||
V_m_analytical[start_index:] = vm_soln[:-start_index] | ||
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# set refractory potential | ||
crossing_ind = (V_m_analytical > nrn.get("V_th")).argmax() | ||
num_ref = int(nrn.get("t_ref") / dt) | ||
V_m_analytical[crossing_ind : crossing_ind + num_ref] = nrn.get("V_reset") | ||
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# rise after refractory period | ||
num_inds = len(times) - crossing_ind - num_ref | ||
V_m_analytical[crossing_ind + num_ref :] = vm_soln[:num_inds] | ||
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nptest.assert_array_almost_equal(V_m_analytical, vm.get("events", "V_m")) |
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