SpineML The Spiking Neural Mark-up Language

Tutorials

We have three tutorials to help new users get used to working with the idea of creating components. Components are used to specify the mathematical rules for the neural elements in a model. These components are used as the basis for the populations which are connected together in a network. Once you have a network, you can then create an experiment which allows you to simulate the model for a given amount of time and with a given set of inputs.

Creating a component in the component editor

Creating a network in the network editor

Creating experiments and graphing

More about data input to a model

Creating a new connectivity using a Python Script

Python scripts for generating connectivity are added to SpineCreator through the Settings/Preferences dialog, and once added appear in the list of connection types.

To allow non-programmers to use and configure extended connectivity types a set of formatted comments is added to the top of the Python script: these specify parameters to pass to the script, and define how SpineCreator should provide a graphical interface for these parameters. For example, this connectionFunc gives a 2-D Gaussian connection like the one shown in James et al. 2018, Fig 1(c):

#PARNAME=sigma #LOC=1,1
#PARNAME=min_w #LOC=2,1
#HASWEIGHT

# sigma is the 2-D Gaussian width
# min_w is the minimum weight for which to add a
# connection to 'out' which is returned by
# connectionFunc

def connectionFunc(srclocs,dstlocs,sigma,min_w):
  import math
  # normterm is a normalisation term used in the loop.
  normterm = 1/(sigma*math.sqrt(2*math.pi))
  # out is a list in which to return the connection
  # weights.
  out = []
  # Iterate through the source and destination locations:
  i = 0
  for srcloc in srclocs:
    j = 0
    for dstloc in dstlocs:
      # Compute Euclidean distance between src and dst:
      dist = math.sqrt(math.pow((srcloc[0] - dstloc[0]),2) + \
        math.pow((srcloc[1] - dstloc[1]),2) + \
        math.pow((srcloc[2] - dstloc[2]),2))
      # Compute the Gaussian weight:
      gauss_weight = normterm*math.exp(-0.5*math.pow(dist/sigma,2))
      # If the weight exceeds the min_w cutoff weight,
      # then add to out. Having a cutoff means that we
      # keep out fairly small; without this, it would
      # contain many infinitessimally small weights.
      if gauss_weight > min_w:
        conn = (i,j,0,gauss_weight)
        out.append(conn)
      j = j + 1
    i = i + 1
  return out

Adding parameters to the SpineCreator GUI is performed using the #PARNAME comment, which gives a name used as a label for the parameter, and a #LOC which describes the row and column where the parameter should be added in a grid for laying out the parameters. The order of the parameters in the code denotes the order they have in the corresponding Python function call, and allows the label to have a more descriptive name than the variable used in the function. In addition there are two more comments that are parsed; #HASWEIGHT and #HASDELAY, which inform SpineCreator if the script needs to generate a weight and/or a delay. If a weight is generated SpineCreator will provide a drop-down list of the corresponding Properties in the WeightUpdate Component, and the selected Property will have the weight values inserted when the connectivity is generated.

The function itself has arguments srclocs and dstlocs, which are Lists of Tuples, each Tuple containing the x, y, and z co-ordinates of the neuron at that index in the List.

Because the error feedback within SpineCreator is very limited, I usually develop my connectionFunc externally, using matplotlib to look at the connection patterns. Here’s an example, called gabor.py:

#
# 1) Define the connectionFunc - the code that will be pasted into the
# python script settings window in SpineCreator.
#

#PARNAME=sigma_g  #LOC=1,1
#PARNAME=gain_g   #LOC=1,2
#PARNAME=lambda_s #LOC=2,1
#PARNAME=gain_s   #LOC=2,2
#PARNAME=dir_s    #LOC=3,1
#PARNAME=wco      #LOC=3,2
#PARNAME=roi      #LOC=4,1
#HASWEIGHT

# This implements a Gabor connection; a 2-D Gaussian multiplied by a
# 1-D sine. Arguments are:
#
# sigma_g - sigma of the gaussian
# gain_g - a gain for the gaussian
# lambda_s - wavelength of sine
# gain_s - gain of sine
# dir_s - direction of (1-D) sine in degrees
def connectionFunc(srclocs,dstlocs,sigma_g,gain_g,lambda_s,gain_s,dir_s,wco,roi):

    import math

    twopi = 6.283185307;

    i = 0 # i is 'src iterator'
    j = 0 # j is 'dst iterator'
    out = [] # To return result

    for srcloc in srclocs:
        j = 0
        for dstloc in dstlocs:

            # Avoid many tanh, sin, cos, pow and exp computations for well-separated neurons:
            xdist = srcloc[0] - dstloc[0]
            ydist = srcloc[1] - dstloc[1]
            # Ignore zdist
            if abs(xdist) > roi or abs(ydist) > roi:
                j = j + 1
                continue

            zdist = srcloc[2] - dstloc[2]
            dist = math.sqrt(math.pow(xdist,2) + math.pow(ydist,2) + math.pow(zdist,2))

            # Direction from source to dest
            ##print ('dstloc[1]: ', dstloc[1], ' srcloc[1]:', srcloc[1])
            ##print ('dstloc[0]: ', dstloc[0], ' srcloc[0]:', srcloc[0])
            top = dstloc[1]-srcloc[1]
            bot = dstloc[0]-srcloc[0]
            ##print ('top:',top,'bot:',bot)
            dir_d = math.atan2(top, bot);
            ##print ('dir_d: ', dir_d, 'dir_s:', dir_s)

            # Find the projection of the source->dest direction onto the sine wave direction. Call this distance dprime.
            dprime = dist*math.cos(dir_d + twopi - ((dir_s*twopi)/360));
            ##print ('dprime: ', dprime, ' dist: ', dist)

            # Use dprime to figure out what the sine weight is.
            sine_weight = gain_s*math.sin(dprime*twopi/lambda_s);
            ##print ('sine_weight:', sine_weight)

            gauss_weight = gain_g*math.exp(-0.5*math.pow(dist/sigma_g,2))
            ##print ('gauss_weight:', gauss_weight)

            combined_weight = sine_weight * gauss_weight;
            ##print ('combined_weight:', combined_weight)

            if abs(combined_weight) > wco:
                #sys.stdout.write('gauss>0.0001: i={0} gauss={1}'.format( i, gauss))
                conn = (i,j,0,combined_weight)
                out.append(conn)

            j = j + 1
        i = i + 1
    #sys.stdout.write('out length: %d' % len(out))
    return out

#
# 2) Compute weights for the map
#

# Set up some parameters
rowlen = 50
sigma_g = 2
gain_g = 1
lambda_s = 10
gain_s = 1
dir_s = 45
wco = 0.001
roi = 8; # 'Region of interest' For index n, consider distances +-roi for weights, outside this region, don't add a weight.

# Containers for source/destination locations
srclocs = []
# Make srclocs - this makes rowlen x rowlen grids:
for i in range(0, rowlen):
    for j in range(0, rowlen):
        srcloc=[j,i,0] # [x,y,z] locations
        srclocs.append(srcloc)

# Call the connectionFunc to generate result
result = connectionFunc (srclocs, srclocs, sigma_g, gain_g, lambda_s, gain_s, dir_s, wco, roi)
print "Done computing"


#
# 3) Show weight results for one particular source neuron projecting
# out to destination neurons.
#

import math

# The source neuron index to look at the connection pattern
src_index = 1275

# Extract xs, ys and weights for source-to-destination connection into
# these lists:
xs = []
ys = []
ws = []

for res in result:
    if (res[0] == src_index):
        # In my example, the position x and y come from the
        # destination index, which is found in res[1]. res[2] contains
        # the delay (unused here). res[3] contains the weight.
        xs.append(res[1]%rowlen)
        ys.append(math.floor(res[1]/rowlen))
        ws.append(res[3])
        #print ('Appended ', res[1]%rowlen, math.floor(res[1]/rowlen), res[3])

# Now do a scatter plot of the weights
import matplotlib.pyplot as plt
from mpl_toolkits.mplot3d import Axes3D
fig = plt.figure()
ax = fig.add_subplot(111, projection='3d')
ax.scatter(xs,ys,ws)
plt.show()

Once this works, I copy and paste connectionFunc into SpineCreator for use in my model.