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13th International Conference on Membrane Computing - MTA Sztaki

13th International Conference on Membrane Computing - MTA Sztaki

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One-membrane symport P systems with few extra symbols<br />

– An increment instructi<strong>on</strong> is performed by replacing q by q ′ in two steps with<br />

the help of object p 1 , also bringing an object a i in.<br />

– A decrement instructi<strong>on</strong> is performed by replacing q by q ′ in four steps with<br />

the help of objects p 1 , p 2 , p 3 , also bringing an object a i out. Moreover, rules<br />

6,7 are opti<strong>on</strong>ally applied an arbitrary number of steps. If a i is not present,<br />

then the computati<strong>on</strong> never exits the loop of applying rules 6,7.<br />

– The c<strong>on</strong>flicting counter semantics is implemented by rule 9.<br />

– Once the simulati<strong>on</strong> of M is finished, object q f enters the system. Each<br />

applicati<strong>on</strong> of the group of rules 11,10,12 leads to removal from the skin of<br />

<strong>on</strong>e copy of c and <strong>on</strong>e object from O ′ . Notice that objects from O ′ cannot<br />

reenter the skin without object T . The first applicati<strong>on</strong> of rule 11 actually<br />

happens in the first step of the computati<strong>on</strong>, but the rest of this process<br />

takes place after the simulati<strong>on</strong> of M ′ is finished. The multiplicity of objects<br />

c has been chosen to be |O ′ | − 1 so that objects q f , b stop reentering the skin<br />

exactly when no more objects from O ′ remain there. The computati<strong>on</strong> halts<br />

with the skin c<strong>on</strong>taining the result and objects T , N.<br />

□<br />

Hence, the known bounds can be described as follows.<br />

NOP 1 (sym 2 ) ⊇ SEG 1 ∪ SEG 2 . (1)<br />

NOP 1 (sym 2 ) ⊆ NF IN. (2)<br />

5⋃<br />

NOP 1 (sym 3 ) ⊇ NF IN 1 ∪ (N k F IN k ∪ N k REG k ) ∪ N 6 RE. (3)<br />

k=0<br />

NOP 1 (sym 4 ) ⊇ NF IN 0 ∪ NF IN 1 ∪ N 1 REG 1 ∪ N 2 RE. (4)<br />

NOP 1 (sym ∗ ) ⊆ NF IN ∪ N 1 RE. (5)<br />

3.5 Sequential Mode<br />

Recently, in [4] we obtained the counterpart of these results for sequential systems.<br />

We recall them here.<br />

NOP sequ<br />

1 (sym 2 ) ⊇ SEG 1 ∪ SEG 2 . (6)<br />

NOP sequ<br />

4 Discussi<strong>on</strong><br />

1 (sym 2 ) ⊆ NF IN. (7)<br />

∞⋃<br />

NOP sequ<br />

1 (sym 3 ) ⊇ NF IN 1 ∪ (N k F IN k ∪ N k REG k ). (8)<br />

k=0<br />

NOP sequ<br />

1 (sym ∗ ) = NF IN ∪ N 1 REG. (9)<br />

We have improved the best known lower bounds of the computati<strong>on</strong>al power of<br />

<strong>on</strong>e-membrane P systems with symport <strong>on</strong>ly. Using symport of weight at most 3,<br />

computati<strong>on</strong>al completeness holds with 6 extra objects. With symport of weight<br />

at most 4, 2 extra objects suffice. Since 1 extra object is known to be necessary<br />

to generate infinite sets by any symport-<strong>on</strong>ly P system, a particularly interesting<br />

open questi<strong>on</strong> is whether<br />

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