Figure 3: A multidimensional network with a triply nested
concatenation.
Expanding the outer IC levels shows an fascinat-
ing feature of the I C notation . Although by con-
struction all graph edges connect lower numbered ver-
tices to higher numbered ones, so the EDSL contains
only positive numbers, a 0 appeared in the final IC
for n = 1, but only as the ending value for the in-
dex:
e
0
j=1
[{1}]. Further examples showed that a 0
or even a negative ending valu e is perf ectly legal for
an indexed concatenation: That subsequence is sim-
ply omitted from th e fully expanded list. Sim ilarly,
e
1
i=1
[{1}] only expands o ut to a single copy of {1}.
(
{1,9, 10},
1
e
i=1
[{1}], {1,11 },
1
e
i=1
[{1}], {1,12 },
1
e
i=1
[{1}], {1,13 },
1
e
i=1
[{1}], {1,14 },
0
e
j=1
[{1}], {},
{1,14,15} ,
2
e
i=1
[{1}], {1,16 },
2
e
i=1
[{1}], {1,17 },
2
e
i=1
[{1}], {1,18 },
2
e
i=1
[{1}], {1,19 },
1
e
j=1
[{1}], {},
{1,19,20} ,
3
e
i=1
[{1}], {1,21 },
3
e
i=1
[{1}], {1,22 },
3
e
i=1
[{1}], {1,23 },
3
e
i=1
[{1}], {1,24 },
2
e
j=1
[{1}], {},.. .
)
(33)
Clearly, once a pattern is d e te cted, it is worth try-
ing to extend it backwards in th e list: it may apply
even where not initially noticed. For reference, the
fully expanded EDSL begins in this way:
{{1, 9,10},{1},{1,11},{1},{1,12},{1},{1,13},
{1}, {1,14},{},{1,1 4,15}, {1},{1},{1,16},
{1}, {1}, {1,17},{1}, {1},{1,18},{1},{ 1},
{1,19},{1},{},{1,1 9,20}, {1},{1},{1},{1,21},
{1}, {1}, {1}, {1,22}, {1},{1},{1},{1,23},
{1}, {1}, {1}, {1,24}, {1},{1}, {},{1,24,25},
{1}, {1}, {1}, {1}, {1, 26},{1}, {1},{1},{1},
{1,27},{1},{1}, {1}, {1},{1, 28},{1},{1},
{1}, {1}, {1,29},{1}, {1},{1}, {},{1,29,30},. ..}
(34)
8 A SELECTION OF NETWORKS
Here is a small co llec tion of different networks we
have successfully compressed, each sh own together
with its c ompressed e dge difference set list (EDSL)
in indexed concatenation form (IC). Many of these in-
clude nested concatenatio ns. All of the networks can
be extend ed by in creasing the end value of the ind ex
variable in the outer indexed concatenation. Replac-
ing the end value by ∞ results in an infinite network,
without adding any complexity to the IC form shown.
Figures 4 and 5 showcase the examples selected,
together with their concatenated EDSLs. Figure 4
consists of examples of networks that c a n extend in-
definitely in one dimension , whether or not a close
view appears one- or two-dimensional. (Cases that
are locally three-dimensional have also been found.)
Figure 5 shows several higher-dimensional networks
along with their EDSLs. Most of these visually ap-
pear to be two-dimensional (expanding in two direc-
tions), and all include at least two levels of indexed
concatenation, one nested inside the other, although
such nesting does not guarantee two-dimensionality,
as can be seen from Figure 4.
One example (Figure 5d) is clearly three-
dimensional (expanding in three directions as the
outer index increases), an d is su mmarized by a three-
level nesting of indexed co ncatenation s. Yet others
we have investigated are too dense to “fit” in three di-
mensions. Figure 5f provides an example of this last
type, which we refer to as growing “exponentially.”
At this point we have no clea r connection between IC
nesting and the “growth dimensionality” of the grap h
represented.
In each of these cases, a complex geometric pat-
tern is captured mathematically by indexed concate-
nation.