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13th International Conference on Membrane Computing - MTA Sztaki

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(Tissue) P systems with decaying objects<br />

c<strong>on</strong>sider the c<strong>on</strong>tents, i.e., the number of spikes, of the output neur<strong>on</strong> i 0 in<br />

halting computati<strong>on</strong>s.<br />

We now c<strong>on</strong>sider the ESNP system Π = (m, S, R, i 0 ) as a network of cells<br />

Π ′ = (m, {a} , {a} , S, R ′ , i 0 ) working in the 1-restricted minimally parallel transiti<strong>on</strong><br />

mode, with<br />

R ′ = {( E : ( a k , i ) → (a w1 , l 1 ) . . . (a wn , l n ) ) |<br />

(<br />

i, E/a k → (l 1 , a w1 ) . . . (l n , a wn ) ) ∈ R }<br />

and the partiti<strong>on</strong>ing R ′ i , 1 ≤ i ≤ m, of the rule set R′ according to the set of<br />

neur<strong>on</strong>s, i.e.,<br />

R ′ i = {( E : ( a k , i ) → (a w1 , l 1 ) . . . (a wn , l n ) ) |<br />

(<br />

E :<br />

(<br />

a k , i ) → (a w1 , l 1 ) . . . (a wn , l n ) ) ∈ R ′} .<br />

The 1-restricted minimally parallel transiti<strong>on</strong> mode chooses <strong>on</strong>e rule – if possible<br />

– from every set R i and then applies such a multiset of rules in parallel, which<br />

directly corresp<strong>on</strong>ds to applying <strong>on</strong>e spiking rule in every neur<strong>on</strong> where a rule<br />

can be applied. Hence, it is easy to see that Π ′ and Π generate the same set<br />

from RE {a} if in both systems we take the same cell/neur<strong>on</strong> for extracting the<br />

output. Due to the results valid for ESNP systems, see [1], we obtain<br />

Theorem 2. For all n ≥ 3,<br />

NRE = NO 1 C n (min 1 (n) , H, N) [ESNP] .<br />

In [8] the following results are shown for ESNP systems with decaying objects:<br />

Theorem 3. For all n ≥ 2 and d ≥ 1,<br />

a) NF IN = NO [d]<br />

1 C n (min 1 (n) , H, N) [ESNP] and<br />

b) NREG = NO [d]<br />

1 C n (min 1 (n) , H, E) [ESNP] .<br />

Purely Catalytic P Systems Already in the original papers by Gheorghe<br />

Păun (see [16] and also [6]), membrane systems with catalytic rules were defined,<br />

but computati<strong>on</strong>al completeness was <strong>on</strong>ly shown with using a priority<br />

relati<strong>on</strong> <strong>on</strong> the rules. In [9] it was shown that <strong>on</strong>ly three catalysts are sufficient<br />

in <strong>on</strong>e membrane, using <strong>on</strong>ly catalytic rules with the maximally parallel<br />

transiti<strong>on</strong> mode, in order to generate any recursively enumerable set of natural<br />

numbers. Hence, by showing that P systems with purely catalytic rules working<br />

in the maximally parallel transiti<strong>on</strong> mode can be c<strong>on</strong>sidered as P systems working<br />

with the corresp<strong>on</strong>ding n<strong>on</strong>cooperative rules in the 1-restricted minimally<br />

parallel transiti<strong>on</strong> mode when partiti<strong>on</strong>ing the rule sets for each membrane with<br />

respect to the catalysts, we obtain the ast<strong>on</strong>ishing result that in this case we<br />

get a characterizati<strong>on</strong> of the recursively enumerable sets of natural numbers by<br />

using <strong>on</strong>ly n<strong>on</strong>cooperative rules.<br />

A n<strong>on</strong>cooperative rule is of the form (I : (a, i) → (y 1 , 1) . . . (y n , n)) where a is<br />

a single symbol and I denotes the c<strong>on</strong>diti<strong>on</strong> that is always fulfilled. A catalytic<br />

27

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