Membrane systems have been inspired from the structure and the functioning of the living cells. They were introduced and studied by Gh.Paun under the name of P systems [24]; some applications of the membrane systems are presented in [15]. Membrane systems are essentially models of distributed, parallel and nondeterministic systems. Here we motivate and present the mobile membranes. Mobile membranes represent a variant of membrane systems inspired by the biological movements given by endocytosis and exocytosis. They have the expressive power of both P systems and process calculi with mobility such as mobile ambients [11] and brane calculi [10]. Computations with mobile membranes can be defined over specific configurations (like process calculi), while they represent also a rule-based formalism (like P systems).
The model is characterized by two essential features:
The computations are performed in the following way: starting from an initial structure, the system evolves by applying the rules in a nondeterministic and maximally parallel manner. A rule is applicable when all the involved objects and membranes appearing in its left hand side are available. The maximally parallel way of using the rules means that in each step a maximal multiset of rules is applied, namely a multiset of rules such that no further rule can be added to the set. A halting configuration is reached when no rule is applicable. The result is represented by the number of objects associated to a specified membrane.
Mobile membranes represents a formalism which describes the movement of membranes inside a spatial structure by applying rules from a given set of rules
R
{lM}
M,N,...
V*
u,v,...
V
a,b,...
M::=u \mid [ M ]u \mid M\|M
If
M
N
M
N
M → N
R
M
N
R
{\it(Comp1)}
\displaystyleM → M' | |
\displaystyleM\|N → M'\|N |
; {\it(Comp2)}
\displaystyleM → M' \displaystyleN → N' | |
\displaystyleM\|N → M'\|N' |
{\it(Mem)}
\displaystyleM → M' | |
\displaystyle[ M ]u → [ M' ]u |
; {\it (Struc)}
\displaystyleM\equivmemM' M' → N' N'\equivmemN | |
\displaystyleM → N |
When describing a computation of a systems of mobile membranes, an initial configuration
M0
R
{\itobject~evolution}
{\itendocytosis}
{\itexocytosis}
{\itpinocytosis}
{\itphagocytosis}
A specific feature of the mobile membranes is that this new rule-based model is appropriate to prove computability results in terms of Turing machines rather by reduction to the lambda calculus as in the case of process calculi with mobility. In this section are defined four classes of membranes inspired from biological facts, and it is shown that their computational power depends on the initial configuration and on the set of rules used.
The systems of simple mobile membranes (SM) are defined over the set of configurations
l{M}
R
[[a \| M]m \| N]k → [[v \| M]m \| N]k
k,m\inl{N}
a\inV
v\inV*
[a \| M]m → [v \| M]m
m\inl{N}
a\inV
v\inV*
[a \| M1]h \| [M]m → [[b \| M1]h \| M]m
h,m\inl{N}
a,b\inV
[[a \| M1]h \| M]m → [b \| M1]h \| [M]m
h,m\inl{N}
a,b\inV
where
M1
M
N
Turing completeness can be obtained by using nine membranes together with the operations of endocytosis and exocytosis [21]. In [17] it is proven that four mobile membranes are enough to get the power of a Turing machine, while in [4] the number of membranes is decreased to three.
SM(levol,endo,exo)
levol
gevol
levol
gevol
SMn(gevol,endo,exo)
RE
It is proved in [17] that
SM4(gevol,endo,exo)=RE
Theorem.
SM3(levol,endo,exo)=RE
The proof of this result uses a similar technique to that used in [4].
The systems of enhanced mobile membranes are a variant of simple membrane systems proposed in [1] fordescribing some biological mechanisms of the immune system. The operations governing the mobility of the systems of enhanced mobilemembranes are endocytosis (endo), exocytosis (exo), forced endocytosis (fendo), forced exocytosis (fexo).The evolution from aconfiguration to another is made using rules from the set of rules
R
[u \| v \| M]h \| [v' \| N]m → [w' \| [w]h]m
h,m\inl{N};u\inV+,v,v',w,w'\inV*
[v' \| N \| [u \| v \| M]h]m → [w \| M]h \| [w' \| N]m
h,m\inl{N};u\inV+,v,v',w,w'\inV*
[v \| M]h \| [u \| v' \| N]m → [[w \| M]h \| w' \| N]m
h,m\inl{N}
u\inV+,v,v',w,w'\inV*
[u \| v' \| [v \| M]h \| N]m → [w \| M]h \| [w' \| N]m
h,m \inl{N},u\inV+,v,v',w,w'\inV*
\noindent where
M
N
The computational power of the systems of enhanced mobile membranes using these four operations was studied in [20] where it is proved that twelve membranes can provide the computational universality, while in [4] the result is improved by reducing the number of membranes to nine. It is worth to note that unlike the previous results, the rewriting of object by means of context-free rules is not used in any of the results (and their proofs).
The interplay between these four operations is quite powerful, and the computational power of a Turing machine is obtained using twelve membranes without using the context-free evolution of objects [20].
The family of all sets generated inside a given membrane by enhanced mobile membranes of degree at most
n
\alpha\subseteq\{exo,endo,fendo,fexo\}
EMn(\alpha)
Theorem.
EM3(endo,exo)=EM3(fendo,fexo)
Theorem.
EM12(endo,exo,fendo,fexo)=RE
When proving the result of the previous theorem the authors have not used an optimal construction of a membrane system. In what follows it is proven that using the same types of rules (endo, exo, fendo, fexo) a membrane system can be constructed using only nine membranes instead of twelve membranes. If this is an optimal construction remains an open problem.
Theorem.
EM9(endo,exo,fendo,fexo)=RE
The proof is similar to that presented in [4].
Following the approach presented in [3], "systems of mutual mobile membranes" representing a variant of systems of simple mobile membranes in which the endocytosis and the exocytosis work whenever the involved membranes "agree" on the movement are defined; this agreement is described by using dual objects
a
\overline{a}
R
[u \| v \| M]h \| [\overline{u} \| v' \| N]m → [ [w \| M]h \| w' \| N]m
h,m\in l{N},u,\overline{u}\inV+,v,v',w,w'\inV*
[\overline{u} \| v' \| N \| [u \| v \| M]h]m → [w \| M]h \| [w' \| N]m
h,m\in l{N},u,\overline{u}\inV+,v,v',w,w'\inV*
where
M
N
It is enough to consider the biologically inspired operations of mutual endocytosis and mutual exocytosis and three membranes to get the full computational power of a Turing machine [6]. Three also represents the minimum number of membranes in order to discuss properly about the movement provided by endocytosis and exocytosis: working with configurations corresponding to a system of two membranes moving inside a skin membrane.
The family of all sets generated inside a given membrane by mutual mobile membranes of degree
n
MMn(mendo,mexo)
Theorem.
MM3(mendo,mexo)=RE
In systems of simple mobile membranes with local evolution rules and mobility rules it is known that systems of degree three have the same power as a Turing machine, while in systems of enhanced mobile membranes using only mobility rules the degree of systems having the same power as a Turing machine increases to nine. In each mobility rule from systems of simple and enhanced mobile membranes, in the left hand side of the rules only one object appears in the proofs. By using multisets instead of objects and synchronization by objects and co-objects, it is proved that it is enough to consider only systems of three mutual mobile membranes together with the operations of mutual endocytosis and mutual exocytosis to get the full computational power of a Turing machine.
The proof is done in a similar manner with the proof for the computational universality of the systems of enhanced mobilemembranes [20].
Membrane systems [24] and brane calculus [10] start from the same observations; however, they are built having in mind different goals: membrane systems investigate formally the computational nature and power of various features of membranes, while the brane calculus is capable to give a faithful and intuitive representation of the biological reality. In [12] the initiators of these two formalisms describe the goals they had in mind: "While membrane computing is a branch of natural computing which tries to abstract computing models, in the Turing sense, from the structure and the functioning of the cell, making use especially of automata, language, and complexity theoretic tools, brane calculi pay more attention to the fidelity to the biological reality, have as a primary target systems biology, and use especially the framework of process~algebra."
In [2] are defined systems of mutual membranes with objects on surface, following the idea of adding objects on membrane and using the biologically inspired rules pino/exo/phago coming from [12,14,18,19]. Objects and co-objects are used in phago and exo rules in order to illustrate the fact that both involved membranes agree on the movement.The evolution from a configuration to another is made using rules from the set of rules
R
[M]v \| a \| u → [[~]u \| x \| M]v \| y
a\inV,u,v,x,y\inV*, ux,vy\inV+
[[M]a \| u \| N]\overline{a \| v} → M \| [N]u \| v \| x
,\overline{a}\inV,u,v,x\inV*,uvx\inV+
[M1]a \| u \| [N]\overline{a \| b \| v} → [[[M1]u \| x]b \| N]v \| y
a,\overline{a},b\inV,u,v,x,y\inV*,ux,vy\inV+
\noindent where
M1
M
N
The computational power of systems of mutual membranes with objects on surface controlled by pairs of rules is investigated:pino/exo or phago/exo, proving that they are universal even using a small number of membranes. These cases were already investigated in [19]; however better results are provided by improving the number of membranes. A summary of the results (existing and new ones) is given in what follows:
Operations |
|
|
|
| |
---|---|---|---|---|---|
Pino, exo | 8 | 4,3 | Yes | Theorem 6.1 [19] | |
Pino, exo | 3 | 5,4 | Yes | Here | |
Phago, exo | 9 | 5,2 | Yes | Theorem 6.2 [19] | |
Phago, exo | 9 | 4,3 | Yes | Theorem 6.2 [19] | |
Phago, exo | 4 | 6,3 | Yes | Here |
The multiplicity vector of the multiset from all membranes is considered as a result of the computation. Thus, the result of a halting computation consists of all the vectors describing the multiplicity of objects from all the membranes; a non-halting computation provides no output. The number of objects from the right-hand side of a rule is called its weight. The family of all sets generated by systems of mutual membranes with objects on surface using at any moment during a halting computationat most
n
r1,r2\in\{pino,exo,phago\}
r,s
MMOSn(r1(r),r2(s)
*
It is proven in [19] that systems of eight membranes with objects on surface and using pino and exo operations of weight four and three are universal. The number of membranes can be reduced from eight to three. However, in order to do this is increased the weight of the pino and exo operations with one, namely from four and three to five and four. This means that in order to construct a universal system of mobile membranes with objects on surface by using pino and exo operations, one needs to decide either he wants to minimize the number of membranes, or the weights of the operations.
Theorem.
MMOSm(pino(r),exo(s))=RE
m\geq3,r\geq5,s\geq4
It is proven in [19] that systems of nine membranes with objects on surface and using phago and exo operations of weight four and three (or five and two) are universal. The number of membranes can be reduced from nine to four, but in order to do this the weight of the phago and exo operations are increased from four and three (or five and two) to six and three. When constructing a Turing complete system of mobile membranes with objects on surface by using phago and exo operations, the same problem appears as when using pino and exo operations: namely, to choose either minimizing the number of membranes, or the weights of the operations.
Theorem.
MMOSm(phago(r),exo(s))=RE
m\geq4,r\geq6,s\geq3
In what follows it is shown that mobile membranes have at least the expressive power of mobile ambients and brane calculi by encoding mobile ambients and brane calculi in certain systems of mobile membranes.
The mobile membranes and the mobile ambients [11] have similar structures and common concepts. Both have a hierarchical structure representing locations, intend to describe mobility, and are used in describing various biological phenomena [10,15]. The mobile ambients are suitable to represent the movement of ambients through ambients and the communication which takes place inside the boundaries of ambients. Membrane systems are suitable to represent the evolution of objects and movement of objects and membranes through membranes. A comparing between these new models (mobile ambients and mobile membranes) is provided, and an encoding the ambients into membranes. This embedding is essentially presented in [5].
Safe ambients represent a variant of mobile ambients in which any movement of an ambient takes place only if both participants agree. The mobility is provided by the consumption of certain pairs of capabilities. The safe ambients differ from mobile ambients by the addition of co-actions: if in mobile ambients a movement is initiated only by the moving ambient and the target ambient has no control over it, in safe ambients both participants must agree by using a matching between action and co-action. A short description of pure safe ambients (SA) is given below; more information can be found in [22,23]. Given an infinite set of names
{lN}
m,n,...
{lA}
A,A',B,B',...
C,C',...
C::=in n \mid \overline{in} n \mid out n \mid \overline{out} n \mid open n \mid \overline{open} n
A::=0 \mid A \mid B \mid C.A \mid n[ A ]
Process
0
C.A
C
A
n[ A ]
n
A
A\midB
A
B
(\nun)A
n
A
\equivamb
(l{A},\mid,0)
The operational semantics of pure ambient safe calculus are defined in terms of a reduction relation
⇒ amb
Axioms:
(In) n[ in m.A\midA' ]\midm[ \overline{in} m.B\midB' ] ⇒ ambm[ n[ A\midA' ]\midB\midB' ]
(Out) m[ n[ out m.A\midA' ]\mid\overline{out} m.B\midB' ] ⇒ ambn[ A\midA' ]\midm[ B\midB' ]
(Open) open n.A \mid n[ \overline{open} n.B\midB' ] ⇒ ambA \mid B \mid B'
Rules:
(Comp1) | \displaystyleA ⇒ amb A' | ; (Comp2) |
\displaystyleA \mid B ⇒ ambA' \mid B |
\displaystyleA ⇒ ambA' \displaystyleB ⇒ ambB' | |
\displaystyleA \mid B ⇒ ambA' \mid B' |
(Amb) | \displaystyleA ⇒ ambA' | ; (Struc) |
\displaystylen[ A ] ⇒ ambn[ A' ] |
\displaystyleA\equivA', A' ⇒ ambB', B'\equivB | |
\displaystyleA ⇒ ambB |
* | |
⇒ | |
amb |
⇒ amb
A translation from the set
l{A}
l{M}
Definition. A translation
l{T}:l{A} → l{M}
l{T}(A)=dlock~l{T}1(A)
l{T}1: l{A} → l{M}
l{T}1(A)=
\begin{cases}cap~n \| [~]cap~n&ifA=cap~n\\ cap~n \| [ l{T}1(A1) ]cap~n&ifA=cap~n.A1\\ [ l{T}1(A1) ]n&ifA=n[ A1 ]\\ [~]n&ifA=n[~]\\ l{T}1(A1) \| l{T}1(A2)&ifA=A1\midA2\\ λ&ifA=0 \end{cases}
An object
dlock
Proposition. Structurally congruent ambients are translated into structurally congruent membrane systems; moreover, structurally congruent translated membrane systems correspond to structurally congruent ambients:
A\equivambB
l{T}(A)\equivmeml{T}(B)
Considering two membrane systems
M
N
dlock
M ⇒ memN
r1,\ldots,ri
M
N
Proposition. If
A
B
M
A ⇒ ambB
M=l{T}(A)
M
M ⇒ memN
N=l{T}(B)
Proposition. Let
M
N
dlock
A
M=l{T}(A)
M
M ⇒ memN
B
*B | |
A ⇒ | |
amb |
N=l{T}(B)
Theorem. (Operational correspondence)
A ⇒ ambB
l{T}(A) ⇒ meml{T}(B)
l{T}(A) ⇒ memM
B
A ⇒ ambB
M=l{T}(B)
A fragment of brane calculus called PEP, and mutual mobile membranes with objects on surface as a variant of systems with mobile membranes are considered. The mobile membranes with objects on surface is inspired by a model of membrane system introduced in [12] having objects attached to membranes. A simulation of the PEP fragment of brane calculus by using mutualmembranes with objects on surface is presented. This approach is related to some other papers trying to show the relationship between membrane systems and brane calculus [8,9,14,18,19].
As it is expressed in [24], "at the first sight the role of objects placed on membranes is different in membrane and brane systems: in membrane computing the focus is on the evolution of objects themselves, while in brane calculi the objects ("proteins") mainly control the evolution of membranes". By defining an encoding of the PEP fragment of brane calculus into mutual membranes with objects on surface, it is shown that the difference between the two models is not significant. Another difference regarding the semantics of the two formalisms is expressed in [8]: "whereas brane calculi are usually equipped with an interleaving, sequential semantics (each computational step consists of the execution of a single instruction), the usual semantics in membrane computing is based on maximal parallelism (a computational step is composed of a maximal set of independent interactions)".
Brane calculus [10] deals with membranes representing the sites of activity; thus a computation happens on the membrane surface. The operations of the two basic brane calculi, pino, exo, phago (PEP) and mate, drip, bud (MBD) are directly inspired by biologic processes such as endocytosis, exocytosis and mitosis. The latter operations can be simulated using the formers one [10].
Systems | P,Q | ::= | P\circQ \mid \sigma(~) \mid \sigma(P) | nests of membranes | |
---|---|---|---|---|---|
Branes | \sigma,\tau | ::= | O \mid \sigma\mid\tau \mid a.\sigma | combinations of actions | |
Actions | a,b | ::= | n\searrow \mid \overline{n}\searrow(\sigma) \mid n\nwarrow \mid \overline{n}\nwarrow \mid pino(\sigma) | phago \searrow \nwarrow |
Membranes are formed of patches, where a patch
s
s=s1 \mid s2
s
a
s1s=a.s1
n
l{P}
a.0
a
0(P)
(P)
0(~)
(~)
The structural congruence relation is a way of rearranging the system such that the interacting parts come together, as illustratedin what follows:
P\circQ\equivbQ\circP |
| \sigma \mid \tau\equivb\tau \mid \sigma | |
---|---|---|---|
P\circ(Q\circR)\equivb(P\circQ)\circR |
| \sigma \mid (\tau \mid \rho)\equivb(\sigma \mid \tau) \mid \rho | |
|
| \sigma \mid 0\equivb\sigma | |
|
|
| |
P\equivbQimpliesP\circR\equivbQ\circR |
| \sigma \equivb\tauimplies\sigma \mid \rho\equivb\tau \mid \rho | |
P\equivbQand\sigma\equivb\tauimplies\sigma(P) \equivb\tau(Q) |
| \sigma\equivb\tauimpliesa.\sigma \equivba.\tau |
In what follows the reduction rules of the calculus are presented:
pino(\rho).\sigma\mid\sigma0(P) → b\sigma\mid\sigma0(\rho(~)\circP) |
| (Pino) | ||||||
---|---|---|---|---|---|---|---|---|
\overline{n}\nwarrow
.\sigma\mid\sigma0(P)\circ Q) → bP\circ\sigma\mid\sigma0\mid\tau\mid\tau0(Q) |
| (Exo) | ||||||
n\searrow.\sigma\mid\sigma0(P)\circ \overline{n}\searrow(\rho).\tau\mid\tau0(Q) → b\tau\mid\tau0(\rho(\sigma\mid\sigma0(P))\circQ) |
| (Phago) | ||||||
P → bQimpliesP\circR → bQ\circR |
| (Par) | ||||||
P → bQimplies\sigma(P) → b\sigma(Q) |
| (Brane) | ||||||
P\equivbP'andP' → bQ'andQ'\equivbQimpliesP → bQ |
| (Struct) |
The action
pino(\rho)
pino
\sigma
pino
n\nwarrow
\overline{n}\nwarrow
P
n\searrow
\overline{n}\searrow(\rho)
Q
P
Q
P
\rho
A translation from the set
l{P}
l{M}
Definition A translation
l{T}:l{P} → l{M}
l{T}(P)=
\begin{cases} [~]l{S(\sigma)}&ifP=\sigma(~)\\ [l{T}(R)]l{S(\sigma)}&ifP=\sigma(R)\\ l{T}(Q) \| l{T}(R)&ifP=Q\midR\\ \end{cases}
where
l{S}:l{P} → V*
l{S}(\sigma)=
\begin{cases} \sigma&if\sigma=n\searrowor\sigma=n\nwarrowor\sigma=\overline{n}\nwarrow\\ \overline{n}\searrow \| S(\rho)&if\sigma=\overline{n}\searrow(\rho)\\ pino \| S(\rho)&if\sigma=pino(\rho)\\ l{S}(a) \| l{S}(\rho)&if\sigma=a.\rho\\ l{S}(\tau) \| l{S}(\rho)&if\sigma=\tau\mid\rho\\ λ&if\sigma=0 \end{cases}
The rules of the systems of mutual membranes with objects on surface (MMOS) are presented in what follows.
Pino |
|
→ [ [~]S(\rho)
| |||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Exo |
|
.\tau\mid\tau0)} → M \ | \;[N]_ | ||||||||||
Phago |
| [M1]
\ | \;[N]_ \rightarrow M_1_]_\;\|\;N]_ |
where
M1
M
N
The next result claims that two PEP systems which are structurally equivalent are translated into systems of mutual membranes with objects on surface which are structurally equivalent.
Proposition. If
P
M=l{T}(P)
N
M\equivmN
N=l{T}(Q)
P\equivbQ
Proposition. If
P
M=l{T}(P)
Q
N=l{T}(Q)
M\equivmN
Remark. In the last proposition it is possible that
P\not\equivbQ
P=n\searrow.n\nwarrow(~)
M=l{T}=[~] | |
n\searrow \| n\nwarrow |
\equivm
[~] | |
n\nwarrow \| n\searrow |
=N
Q=n\nwarrow.n\searrow(~)
Q=n\nwarrow\midn\searrow(~)
N=l{T}(Q)
P\not\equivbQ
Proposition. If
P
M=l{T}(P)
N
M → N
N=l{T}(Q)
P → bQ
Proposition. If
P
M=l{T}(P)
Q
N=l{T}(Q)
M → N
The following remark is a consequence of the fact that a formalism using an interleaving semantic is translated into a formalism working in parallel.
Remark. The last proposition allows
P\not → bQ
P=\overline{n}\nwarrow.\overline{n}\nwarrow(n\nwarrow.n\searrow(~))
M=((~) | |
n\nwarrow \| n\searrow |
\nwarrow \| \overline{n} | |
) | |
\overline{n |
\nwarrow}
M →
\nwarrow} | |
[~] | |
n\searrow \| \overline{n |
Q=n\searrow.\overline{n}\nwarrow(~)
N=l{T}(Q)
P\not → bQ
These results are presented together with their proofs in [2].