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2.1
Multiple Attractor Cellular Automata
The state transition graph of an MACA consists of a number of cyclic and
non-cyclic states. The set of non-cyclic states of an MACA forms inverted
trees rooted at the cyclic states. The cycles are referred to as attractors . Fig.1
depicts the state transition diagram of a 5-cell MACA with four attractors
{ 00000,00011,00110,00101 } having self loop. In rest of the paper, by an attrac-
tor we will refer to a cycle of length 1. The states of a tree rooted at the cyclic
state α forms the α-basin .
With reference to the state transition diagram of a CA , the depth d of the
CA is the number of edges between a non-reachable state and the attractor. The
depth d of the 5-cell MACA of Fig.1 is 3.
01000
01010
10100
10110
01001
01011
10101
10111
3
11100
11110
11111
11101
2
00010
00001
1
(0)
000 00
(3)
000 11
0
10010
10000
01110
01100
01101
01111
10011
10001
3
11000
11010
11001
11011
2
11000
11000
T =
01100
00101
00001
00100
00111
1
(6)
001 10
(5)
001 01
0
Fig. 1. State transition diagram of a 5-cell MACA
The detailed characterization of MACA is available in [1]. A few fundamen-
tal results for an n -cell MACA having k number of attractors is next outlined.
Result I: The characteristic polynomial of the MACA is x n−m (1 + x ) m ,
where m = log 2 ( k ).
Result II: The characteristic polynomial noted above can be also written
in elementary divisor form as
(1 + x )(1 + x ) ··m times
x d 1 x d 2 ··x d p
where d 1 ≥ d 2 ·· ≥ d p and
d 1 + d 2 ···· + d p = n − m .
Result III: The minimal polynomial of an MACA is x d 1 (1 + x ), where
depth = d 1 .
Definition 1 An m-bit field of an n-bit pattern set is said to be pseudo-
exhaustive if all possible 2 m patterns appear in the set.
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