All pairs of neurons A,B in the H series were considered for which there
was a synaptic connection both from A to B and from A to B
(A,B are the contralateral homologues of A,B), but where the
adjacency between A and B was different from that between A and
B. Let S1 be the number of synapses from A to B,
S2 can be the number from A to B, a1 be the
adjacency of A and B, and a2 be the adjacency of A and
B. Since each set of four is only counted once we can assume that
a1 > a2. The ai are treated as
independent variables (i.e. they do not depend on the si), and
the si are treated as the outcomes of randome variables
Si, which are possibly dependant on the ai. There
are two hypotheses that will be tested: a proportional relationship between
Si and ai, and independence. More precisely, the
proportional model presumes that synapses are made with a certain
probability per unit of length of contact. In this case Si will
be Poisson distributed with mean (and variance) proportional to
ai. However the constant of proportionality may differ for
different sets of A,B,A,B. The independent model proposes that
the Si have mean S, independent of ai, but again
possibly different for different sets of neurons.
The test statistic that was used is the sum over all chosen sets of T =
(a1s2 a2s1).
If Si is proportional to ai, then T should have mean
value zero. Its variance can be estimated as the sum of the variances of
the contributing terms, which are (a12a2m
+ a22a1m) where m is the Poisson rate,
best estimated by (s1+s2) /
(a1+a2). This simplifies to being the sum over all
the sets of a1a2(s1+s2).
If Si is independent of ai, then T should have mean
M, where M is the sum over all the sets of S.(a1-a2),
where S is the mean number of synapses for each set. The best estimator
for S is (s1+s2)/2. In order to estimate the
variance of the differences from the mean, (M-T), we must propose a
variance for Si. (It cannot be estimated because then we would
lose all our degrees of freedom). It seems reasonable to assume in this
case also that the Si have a Poisson distribution, or in any
case that their variance is approximately the same as their mean, S. Then
the estimated variance of (M-T) is the sum over all sets of
S.(a1+a2)2/2.
To test each hypothesis the difference between T and its expected value
under the hypotheses is divided by the standard error (the square root of
the estimated variance) to give a normalised error, U. Since we are adding
together hundreds of similar terms T should be distributed normally, and so
theoretically U has a t-distribution, since we have estimated the variance
of T. However, because there are hundreds of degrees of freedom (one for
each set), U can be tested as if coming from a standard normal
distribution.
In total there were 391 sets. The value of T was 7103. If we assume the
proportional hypothesis then the standard error is 1324.3 and U is 5.36
which is very significant. We can therefore reject the proportional model.
If we assume the independent model then M is 7655 and the standard error is
1338.0 so U is 0.41, which is not significant. So it is quite possible
according to this test that the number of synapses formed is independent of
adjacency.
The basic method of this algorithm is to start with a random ordered list
and repeatedly use a simple rearrangement principle to reduce the overall
number of upward synapses. The process stops when this number cannot be
improved by a rearrangement of the type under consideration. In general
this will not give a true optimum order, because the rearrangement
principle is not general enough. However, by repeated application of the
algorithm to different starting lists one can get an indication of the
distribution of final results. If, as they were in the case under
consideration here, the results of these repeated optimisations are very
similar, then it is likely that they are near the true minimum. The
algorithm was run many times until the lowest value so far had come up
repeatedly, at which point it was accepted as the optimum.
The actual rearrangement system chosen in this case is to run through the
current list and, for each neuron, determine where in the list it should be
placed. If this is different from the current position then it is moved
there and the neurons in between are shunted one place back in the list to
fill the gap.
This method deals with some notional material (sensory influence) which
flows down through the network of connections, moving through a synapse at
each time step. Each sensory neuron under consideration is given a unit
amount of material at time zero. Then at successive time steps the
material is redistributed, all the material in each neuron being divided
amongst the neurons that it both synapses to and is above in the ordering.
The amount that each postsynaptic cell receives is proportional to the
number of synapses made. If there are no postsynaptic partners then the
material is lost. Clearly material can reunite that has come via different
routes but using the same number of synapses from sensory neurons. The
requirement that only downward synapses are permitted prevents problems
with cycling.
This method makes the assumptions that the influence of a connection is
proportional to the number of synapses it contains, and that influence is
neither lost nor amplified, merely passing through neurons and being
redistributed at each time step. Both these assumptions are
neurobiologically unrealistic, but they are probably the best that can be
done with the information available. By keeping track of the distribution
of material at each time step one can build up a picture of the
distribution of time steps required for influence to reach a specific
neuron (muscle can be treated as the final postsynaptic neuron), and also
of the proportion of influence from the chosen set of sensory neurons that
passes through any particular interneuron, or for instance that reaches
head muscle as opposed to body muscle.
This is a hierarchical clustering algorithm (see e.g. Seber, 1984). The
principle is to identify the two items that are most likely to belong to
the same group and to link them together. Then a new distance, or, in our
case, adjacency, is defined between this pair and each of the remaining
items. One then returns to the first step and looks for the most adjacent
pair in the reduced set of items, which will include a combined
pseudo-item. This process of joining the two closest items continues
recursively until only one item is left. At each stage a measure of the
association of the two items joined together is given by their adjacency,
which in general is a combined adjacency.
Different versions of this process vary in the way that the combined
adjacency of the merged item to the remaining items is determined. I used
a variant of the group average method (Seber, 1984) that was tailored to
this particular problem. I kept data on the circumferential zones of the
nerve ring in which each process ran (e.g. lower left). This was necessary
because it is only possible for two processes to be adjacent to the extent
that they run in the same zone. The adjacency between two groups is then
defined as the ratio of the total adjacency between their constituent
processes to the summed circumferential zone length that they have in
common. By keeping the total constituent adjacencies and the summed zonal
lengths at each stage these "zonal ratios" can be easily combined
when two items are merged. I also prevented the fusion of groups with
comparatively small overlaps, because the data for such cases would be
correspondingly noisy and if they were to belong to a genuine bundle there
would have to be an overlapping intermediate fibre in any case. This zonal
ratio system does, however, permit bundles that are longer than some, or
even all, of the constituent processes, and this is an important feature of
it.