Printer Friendly

Deterministic soliton graphs.

Soliton graphs are studied in the context of a reduction procedure that simplifies the structure of graphs without affecting the deterministic property of the corresponding automata. It is shown that an elementary soliton graph defines a deterministic automaton iff it reduces to a graph not containing even-length cycles. Based on this result, a general characterization is given for deterministic soliton graphs using chestnut graphs, generalized trees, and graphs having a unique perfect matching.

Keywords: soliton automata, matching theory

Povzetek: Clanek obravnava grafe brez lihih ciklov.

1 Introduction

One of the most ambitious goals of research (1) in modern bioelectronics is to develop a molecular computer. The introduction of the concept "soliton automaton" in [5] has been inspired by this research, with the intention to capture the phenomenon called soliton waves [4] through an appropriate graph model.

Soliton graphs and automata have been systematically studied by the authors on the grounds of matching theory in a number of papers. Perhaps the most significant contribution among these is [2], where soliton graphs have been decomposed into elementary components, and these components have been grouped into pairwise disjoint families based on how they can be reached by alternating paths starting from external vertices. This paper can also serve as a source of further references on soliton automata for the interested reader.

Since soliton automata are proposed as switching devices, deterministic automata are in the center of investigations. The results reported in this paper are aimed at providing a complete characterization of deterministic soliton automata. The two major aspects of this characterization are:

1. Describing elementary deterministic soliton graphs.

2. Recognizing that deterministic soliton graphs having an alternating cycle follow a simple hierarchical pattern called a chestnut.

An important tool in the study of both aspects is a reduction procedure, which might be of interest by itself. It allows elementary deterministic soliton graphs to be reduced to generalized trees, and it can also be used to reduce chestnut graphs to really straightforward ones, called baby chestnuts.

2 Soliton graphs and automata

By a graph G = (V(G), E(G)) we mean an undirected graph with multiple edges and loops allowed. A vertex v [member of] V(G) is called external if its degree is one, and internal if the degree of [epsilon] is at least two. An internal vertex is base if it is adjacent to an external one. External edges are those of E(G) that are incident with at least one external vertex, and internal edges are those connecting two internal vertices. Graph G is called open if it has at least one external vertex.

A walk in a graph is an alternating sequence of vertices and edges, which starts and ends with a vertex, and in which each edge is incident with the vertex immediately preceding it and the vertex immediately following it. The length of a walk is the number of occurrences of edges in it. A trail is a walk in which all edges are distinct and a path is a walk in which all vertices are distinct. A cycle is a trail which can be decomposed into a path and an edge connecting the endpoints of the path. If [alpha] = v[e.sub.1] ... [e.sub.n]w is a walk from v to w and [beta] = w[f.sub.1] ... [f.sub.k]z is a walk from v to w then the concatenation of [alpha] and [beta] is the walk [alpha] [parallel] [beta] = v[e.sub.1] ... [e.sub.n]w[f.sub.1] ... [f.sub.k]z from v to z.

A matching M of graph G is a subset of E(G) such that no vertex of G occurs more than once as an endpoint of some edge in M. It is understood by this definition that loops cannot participate in any matching. The endpoints of the edges contained in M are said to be covered by M. A perfect internal matching is a matching that covers all of the internal vertices. An edge e [member of] E(G) is allowed (mandatory) if e is contained in some (respectively, all) perfect internal matching(s) of G. Forbidden edges are those that are not allowed. We shall also use the term constant edge to identify an edge that is either forbidden or mandatory. An open graph having a perfect internal matching is called a soliton graph. A soliton graph G is elementary if its allowed edges form a connected subgraph covering all the external vertices. Observe that if G is elementary, then it cannot contain a mandatory edge, unless G is a mandatory edge by itself with a number of loops incident with one of its endpoints.

Let G be an elementary soliton graph, and define the relation ~ on Int(G) as follows: [v.sub.1] ~ [v.sub.2] if an extra edge e connecting [v.sub.1] with [v.sub.2] becomes forbidden in G + e. It is known, cf. [6, 2], that ~ is an equivalence relation, which determines the so called canonical partition of (the internal vertices of) G. The reader is referred to [6] for more information on canonical equivalence, and on matching theory in general.

Let G be a graph and M be a matching of G. An edge e [member of] E(G) is said to be M-positive (M-negative) if e [member of] M (respectively, e [??] M). An M-alternating path (cycle) in G is a path (respectively, even-length cycle) stepping on M-positive and M-negative edges in an alternating fashion. An M-alternating loop is an odd-length cycle having the same alternating pattern of edges, except that exactly one vertex has two negative edges incident with it. Let us agree that, if the matching M is understood or irrelevant in a particular context, then it will not be explicitly indicated in these terms. An external alternating path is one that has an external endpoint. If both endpoints of the path are external, then it is called a crossing. An alternating path is positive if it is such at its internal endpoints, meaning that the edges incident with those endpoints are positive.

Let G be a soliton graph, fixed for the rest of this section, and let M be a perfect internal matching of G. An M-alternating unit is either a crossing or an alternating cycle with respect to M. Switching on an alternating unit amounts to changing the sign of each edge along the unit. It is easy to see that the operation of switching on an M-alternating unit [alpha] creates a new perfect internal matching S(M, [alpha]) for G. Moreover, as it was proved in [1], every perfect internal matching M of G can be transformed into any other perfect internal matching M' by switching on a collection of pairwise disjoint alternating units. Consequently, an edge e of G is constant iff there is no alternating unit passing through e with respect to any perfect internal matching of G. A collection of pairwise disjoint M-alternating units will be called an M-alternating network, and the network transforming one perfect internal matching M into another M' will be denoted by N(M, M'). Clearly, N(M, M') is unique.

Now we generalize the alternating property to trails and walks. An alternating trail is a trail [alpha] stepping on positive and negative edges in such a way that [alpha] is either a path, or it returns to itself only in the last step, traversing a negative edge. The trail [alpha] is a c-trail (l-trail) if it does return to itself, closing up an even-length (respectively, odd-length) cycle. That is, [alpha] = [[alpha].sub.1] [parallel] [[alpha].sub.2], where [[alpha].sub.1] is a path and [[alpha].sub.2] is a cycle. These two components of [alpha] are called the handle and circuit, in notation, h([alpha]) and c([alpha]). The joint vertex on h([alpha]) and c([alpha]) is called the center of [alpha]. An external alternating trail is one starting out from an external vertex, and a soliton trail is a proper external alternating trail, that is, either a c-trail or an 1-trail. See Fig. 1.


The collection of external alternating walks in G with respect to some perfect internal matching M, and the concept of switching on such walks are defined recursively as follows.

(i) The walk [alpha] = [v.sub.0]e[v.sub.1], where e = ([v.sub.0], [v.sub.1]) with [v.sub.0] being external, is an external M-alternating walk, and switching on [alpha] results in the set S(M, [alpha]) = M[DELTA]{e}. (The operation [DELTA] is symmetric difference of sets.)

(ii) If [alpha] = [u.sub.0][e.sub.1] ... [e.sub.n][v.sub.n] is an external M-alternating walk ending at an internal vertex [v.sub.n], and [e.sub.n+1] = ([v.sub.n], [u.sub.n+1]) is such that [e.sub.n+1] [member of] S(M, [alpha]) iff [e.sub.n] [member of] S(M, [alpha]), then [alpha]' = [alpha][e.sub.n+1][u.sub.n+1] is an external M-alternating walk and

S(M, [alpha]') = S(M, [alpha])[DELTA]{[e.sub.n+1]}.

It is required, however, that [e.sub.n+1] [not equal to] [e.sub.n], unless [e.sub.n] [member of] S(M, [alpha]) is a loop.

It is clear by the above definition that S(M, [alpha]) is a perfect internal matching iff the endpoint [v.sub.n] of [alpha] is external, too. In this case we say that [alpha] is a soliton walk.

EXAMPLE Consider the graph G of Fig. 2, and let M = {e, [h.sub.1], [h.sub.2]}. A possible soliton walk from u to v with respect to M is [alpha] = uewg[z.sub.1][h.sub.1][z.sub.2][l.sub.2][z.sub.3][h.sub.2][z.sub.4][l.sub.1] [z.sub.1]gwfv. Switching on [alpha] then results in S(M, [alpha]) = {f, [l.sub.1], [l.sub.2]}.


Graph G gives rise to a soliton automaton [A.sub.G], the states of which are the perfect internal matchings of G. The input alphabet for [A.sub.G] is the set of all (ordered) pairs of external vertices in G, and the state transition function [delta] is defined by

[delta](M, (v, w)) = {S(M, [alpha])| [alpha] is a soliton walk, v to w}.

Graph G is called deterministic if [A.sub.G] is such in the usual sense, that is, if for every state M and input (v, w),

|[delta](M, (v, w))| [less than or equal to] 1.

EXAMPLE (Continued) Observe that the soliton automaton defined by the graph of Fig. 2 is non-deterministic, as [alpha]' = uewfv is also a soliton walk from u to v with respect to state M such that S(M, [alpha]) [not equal to] S(M, [alpha]').

Let [alpha] be a soliton c-trail with respect to M. It is easy to see that the walk

s([alpha]) = h([alpha]) [parallel] c([alpha]) [parallel] h[([alpha]).sup.R]

is a soliton walk, and the effect of switching on s([alpha]) is the same as switching on the cycle c([alpha]) alone. (For any walk [beta], [[beta].sup.R] denotes the reverse of [beta].) If [alpha] is a soliton l-trail, then s([alpha]) is defined as the soliton walk

s([alpha]) = h([alpha]) [parallel] c([alpha]) [parallel] c([alpha]) [parallel] h[([alpha]).sup.R].

Clearly, this walk induces a sell-transition of [A.sub.G], that is, no state change is observed. In the sequel, all perfect internal matchings of G will simply be called states for obvious reasons.

Recall from [5] that an edge e of G is impervious if there is no soliton walk passing through e in any state of G. Edge e is viable if it is not impervious. See Fig. 2, edge h for an example of an impervious edge.

We are going to give a simpler characterization of impervious edges in terms of alternating paths, rather than walks. To this end, we need the following lemma.

Lemma 2.1. If [alpha] is an external M-alternating walk from v to u, then there exists an M-alternating network [GAMMA] and an external M-alternating trail [beta] from v to u such that

1. [GAMMA] consists of cycles only, and it is disjoint from [beta];

2. S(M, [alpha]) = S(S(M, [GAMMA]), [beta]).

Proof. Easy induction on the length of [alpha], left to the reader.

An internal vertex v [member of] V(G) is called accessible with respect to state M if there exists a positive external M-alternating path leading to v. It is easy to see, cf. [2], that vertex v is accessible with respect to some state M iff v is accessible with respect to all states of G.

Proposition 2.2. For every edge e [member of] E(G), e is impervious iff both endpoints of e are inaccessible.

Proof. If either endpoint of e is accessible, then e is clearly viable. Assume therefore that both endpoints [u.sub.1] and [u.sub.2] of e are inaccessible, and let [alpha] be an arbitrary external M-alternating walk from v [member of] Ext(G) to either [u.sub.1] or [u.sub.2], say [u.sub.1]. By Lemma 2.1, there exists a suitable external M-alternating trail [beta] from v to [u.sub.1]. Each internal edge lying on [beta] has an accessible endpoint, so that e is not among them. Moreover, the edge of h([beta]) incident with [u.sub.1] must be positive with respect to S(M, [alpha]), otherwise h([beta]) would be a positive external alternating path with respect to state S(M, [GAMMA]). (Recall that h([beta]) is the handle of [beta], and take h([beta]) = [beta] if [beta] is just a path.) But then e must be negative with respect to S(M, [beta]), or else h([beta])e[u.sub.2] would he a positive external alternating path leading to [u.sub.2] (with respect to S(M, [GAMMA]), or even M, since [GAMMA] is disjoint from [beta]). We conclude that the walk [alpha] cannot continue on e, because it must take the two positive edges incident with [u.sub.1] before and after hitting that vertex. Thus, every time an external alternating walk reaches either endpoint of e, it will miss e as a possible continuation. In other words, e is impervious.

3 Elementary decomposition of soliton graphs

Again, let us fix a soliton graph G for the entire section. In general, the subgraph of G determined by its allowed edges has several connected components, which are called the elementary components of G. Notice that an elementary component can be as small as a single external vertex of G. Such elementary components are called degenerate, and they are the only exception from the general rule that each elementary component is an elementary graph. A mandatory elementary component is a single mandatory edge e [member of] E(G), which might have a loop around one or both of its endpoints.

The structure of elementary components in a soliton graph G has been analysed in [2]. To summarize the main results of this analysis, we first need to review some of the key concepts introduced in that paper. Elementary components are classified as external or internal, depending on whether or not they contain an external vertex. An elementary component of G is viable if it does not contain impervious allowed edges. A viable internal elementary component C is one-way if all external alternating paths (with respect to any state M) enter C in vertices belonging to the same canonical class of C. This unique class, as well as the vertices belonging to this class, are called principal. Furthermore, every external elementary component is considered a priori one-way (with no principal canonical class, of course). A viable elementary component is two-way if it is not one-way. An impervious elementary component is one that is not viable.

EXAMPLE The graph of Fig. 3 has five elementary components, among which [C.sub.1] and D are external, while [C.sub.2], [C.sub.3] and [C.sub.4] are internal. Component [C.sub.3] is one-way with the canonical class {u, v} being principal, while [C.sub.2] is two-way and [C.sub.4] is impervious.


Let C be an elementary component of G, and M be a state. An M-alternating C-ear is a negative M-alternating path or loop having its two endpoints, but no other vertices, in C. The endpoints of the ear will necessarily be in the same canonical class of C. We say that elementary component C' is two-way accessible from component C with respect to any (or all) state(s) M, in notation C[rho]C', if C' is covered by an M-alternating C-ear. It is required, though, that if C is one-way and internal, then the endpoints of this ear not be in the principal canonical class of C. As it was shown in [2], the two-way accessible relationship is matching invariant. A family of elementary components in G is a block of the partition induced by the smallest equivalence relation containing [rho]. A family F is called external if it contains an external elementary component, otherwise F is internal. A degenerate family is one that consists of a single degenerate external elementary component. Family F is viable if every elementary component in F is such, and F is impervious if it is not viable. As it turns out easily, the elementary components of an impervious family are all impervious. Soliton graph G is viable if all of its families are such.

EXAMPLE (CONTINUED) Our example graph in Fig. 3 has four families: [F.sub.1] = {[C.sub.1], [C.sub.2]}, [F.sub.2] = {D}, [F.sub.3] = {[C.sub.3]}, [F.sub.4] = {[C.sub.4]}. Family [F.sub.1] is external, [F.sub.2] is degenerate, and [F.sub.3] is internal. These families are all viable, whereas family [F.sub.4] is impervious.

The first group of results obtained in [2] on the structure of elementary components of G can now be stated as follows.

Theorem 3.1. Each viable family of G contains a unique one-way elementary component, called the root of the family. Each vertex in every member of the family, except for the principal vertices of the root, is accessible. The principal vertices themselves are inaccessible, but all other vertices are only accessible through them.

A family F is called near-external if each forbidden viable edge incident with any principal vertex of its root is external. For two distinct viable families [F.sub.1] and [F.sub.2], [F.sub.2] is said to follow [F.sub.1], in notation [F.sub.1] [right arrow] [F.sub.2], if there exists an edge in G connecting any non-principal vertex in [F.sub.1] with a principal vertex of the root of [F.sub.2]. The reflexive and transitive closure of [right arrow] is denoted by [??]. The second group of results in [2] characterizes the edge connections between members inside one viable family, and those between two different families.

Theorem 3.2. The following four statements hold for the families of G.

1. An edge e inside a viable family F is impervious iff both endpoints of e are in the principal canonical class of the root. Every forbidden edge e connecting two different elementary components in F is part of an ear to some member C [member of] F.

2. For every edge e connecting a viable family [F.sub.1] to any other family (viable or not) [F.sub.2], at least one endpoint of e is principal in [F.sub.1] or [F.sub.2]. If the endpoint of e in [F.sub.1] is not principal, then [F.sub.2] is viable and it follows [F.sub.1].

3 The relation [??] is a partial order between viable families, by which the external families are minimal elements.

4 If F and [??] are families such that F [??] [??], then each non-principal vertex u of [??] is accessible from F, meaning that for every state M there exists a positive M-alternating path to u either from a suitable external vertex of F, if F is external, or from an arbitrary principal vertex of F, if F is internal. The path [alpha] runs entirely in the families between F and [??] according to [??].

For convenience, the inverse of the partial order [??] will be referred to as [[less than of equal to].sub.G. Theorems 3.1 and 3.2 are fundamental regarding the structural decomposition of soliton graphs, and they will be applied liberally throughout the forthcoming sections (especially in Section 4). There will be no explicit reference made, however, to these theorems whenever they apply.

4 Chestnuts

Chestnuts have been introduced in [5] as a group of deterministic soliton graphs having a very simple and easily recognizable structure.

Definition 1. A connected graph G is called a chestnut if it has a representation in the form G = [gamma] + [[alpha].sub.1] + ... + [[alpha].sub.k] with k [greater than or equal to] 1, where [gamma] is a cycle of even length and each [[alpha].sub.i] (i [member of] [k]) is a tree subject to the following conditions:

(i) V([[alpha].sub.i]) [intersection] V([[alpha].sub.j]) = [empty set] for 1 [less than or equal to] i [not equal to] j [less than or equal to] k;

(ii) V([[alpha].sub.i]) [intersection] V([gamma]) consists of a unique vertex-denoted by [v.sub.i]--for each i [member of] [k];

(iii) [v.sub.i] and [v.sub.j] are at even distance on [gamma] for any distinct i, j [member of] [k];

(iv) any vertex [w.sub.i] [member of] V([[alpha].sub.i]) with d([w.sub.i]) > 2 is at even distance from [v.sub.i] in [[alpha].sub.i] for each i [member of] [k].

See Fig. 4 for an example chestnut.


Our first observation regarding chestnuts is that they are bipartite graphs. Let us call a vertex of a chestnut G outer if its distance from any of the [v.sub.i]'s is even, and inner if this distance is odd. Then the inner and outer vertices indeed define a bipartition of G. Moreover, the degree of each inner vertex is at most 2. It is easy to come up with a perfect internal matching for G: just mark the cycle [gamma] in an alternating fashion, then the continuation is uniquely determined by the structure of the trees [[alpha].sub.i]. Thus, G has exactly two states. It is also easy to see that the inner internal vertices are accessible, while the outer ones are inaccessible. Thus, the cycle [gamma] forms an internal elementary component with its outer vertices constituting the principal canonical class of this component. Moreover, [gamma] forms a stand-alone internal family in G. The rest of G's families are all single mandatory edges along the trees [[alpha].sub.i], or they are degenerate ones consisting of a single inner external vertex. Their rank in the partial order [[less than or equal to].sub.G] is consistent with their position in the respective trees [[alpha].sub.i], following a decreasing order from the leafs to the root. The family {[gamma]} is the minimum element of [[less than or equal to].sub.G], and G has no impervious edges.

By the description above, every chestnut G is a deterministic soliton graph. Moreover, G is strongly deterministic [5] in the sense that, for each pair ([v.sub.1], [v.sub.2]) of external vertices, there exists at most one soliton walk from [v.sub.1] to [v.sub.2] in each state of G. We are going to show that for every connected soliton graph G having no impervious edges, but possessing a non-mandatory internal elementary component, G is deterministic iff G is a chestnut.

Lemma 4.1. Let [alpha] be an external M-alternating path of a soliton graph G leading to a principal vertex v in some internal family F. Then [alpha] can be extended to a soliton trail, the center of which lies in a family H [[less than or equal to].sub.G] F.

Proof. Every possible continuation [beta] of [alpha] as an M-alternating path can only leave the family F by entering another family [??] [<.sub.G] F. It is therefore inevitable that, when [beta] finally returns to itself, this will happen in a family H [[less than or equal to].sub.G] F. The path [beta] must eventually return to itself, since G is finite.

Lemma 4.2. Let [beta] be a soliton c-trail of a deterministic soliton graph G starting from v [member of] Ext(G) with respect to state M. Then, starting from v, there exists no soliton trail with respect to M that is different from [beta].

Proof. Assume, by contradiction, that an unwanted [delta] [not equal to] [beta] exists. Clearly, c([delta]) = c([beta]), otherwise the soliton walks s([beta]) and s([beta]) would define two different transitions of [A.sub.G] in state M on input (v, v). Therefore we have h([beta]) [not equal to] h([delta]). Starting from v, let z be the first vertex on both h([beta]) and h([beta]) where these paths split into two different directions (or just use a pair of parallel edges to reach the same vertex). Thus, [beta] = [gamma] [parallel] [beta]' and [delta] = [gamma] [parallel] [delta]', where [gamma] is a suitable path from v to z, and [beta]', [delta]' are M-alternating c-trails starting out from z on different edges. Clearly, the last edge of [gamma] incident with z is positive, and the first edges of [beta]' and [delta]' incident with z are negative. Therefore the walk

[chi] = [gamma] [parallel] [beta]' [parallel] h[([beta]').sup.R] [parallel] [delta]' [parallel] h[([delta]').sup.R] [parallel] [[gamma].sup.R]

is a soliton walk from v to v, which defines a self-transition of [A.sub.G]. This transition, however, is different from the one defined by the walks s([beta]) and s([gamma]); a contradiction.

Theorem 4.3. Let G be a deterministic soliton graph with no impervious edges, and assume that G has a non-mandatory elementary component C lying in an internal family F. Then C consists of a single even-length cycle, F = {C} and F is a minimal element with respect to to the partial order [[less than or equal to].sub.G].

Proof. Let M be an arbitrary state of G, and [alpha] be a negative external M-alternating path from some v [member of] Ext(G) to a principal vertex z of the root R of F. Furthermore, let [gamma] be an M-alternating cycle in C. Since C is accessible through z, we can fix a soliton c-trail [beta] with respect to M such that [beta] starts out from v and c([beta]) = [gamma]. We can assume, without loss of generality, that R = C. For, we need to rule out the only possible scenario that is incompatible with this assumption, namely when R is a single mandatory edge e = (z, w). Since in this case there are two-way members of the family F (e.g. C), there exists an M-alternating R-ear (loop) [member of] around w. The loop [member of] gives rise to a soliton l-trail [delta] = [alpha]e[member of], which, by Lemma 4.2, cannot co-exist with [beta].

Now let us assume that R = C has an allowed edge different from the ones along [gamma]. Clearly, C then has another M-alternating cycle [gamma]' [not equal to] [gamma]. As above, it is possible to extend [alpha] to a soliton c-trail [beta]' with respect to M such that c([beta]') = [gamma]'. Again, this contradicts Lemma 4.2, knowing that [beta] [not equal to] [beta]'.

We have seen so far that R = C, and C is spanned by [gamma]. Moreover, the principal and non-principal vertices determine the two classes of C's canonical partition. No two principal vertices can be connected in C by an edge, since such an edge would be impervious in G. Suppose that there exists an edge e connecting two non-principal vertices [u.sub.1] and [u.sub.2] of [gamma]. The edge e divides [gamma] into two M-alternating loops [[chi].sub.1] and [[chi].sub.2] originating from [u.sub.1] and [u.sub.2], respectively.

Also notice that vertex z on [gamma] lies outside one of [[chi].sub.1] and [[chi].sub.2]. Consequently, [alpha] can again be extended to a soliton l-trail [delta] such that c([delta]) = [[chi].sub.1] or c([delta]) = [[chi].sub.2]. (Remember that z and [u.sub.1(2)] are in different canonical classes.) A contradiction with Lemma 4.2 is reached, showing that C = [gamma].

remains to be seen that F = {C}, and F is minimal with respect to [[less than or equal to].sub.G]. Any M-alternating C-ear [member of] originating from two different non-principal vertices [u.sub.1] and [u.sub.2] is equivalent to an edge connecting [u.sub.1] directly with [u.sub.2], and so need not be considered separately. On the other hand, if the ear [member of] was an M-alternating loop, then [alpha] could again be trivially extended to a soliton l-trail [delta] with c([delta]) = [member of], which is impossible. Now assume that there exists a family [??] [<.sub.G] F, and continue [alpha] to obtain a negative external M-alternating path [alpha]' leading to a principal vertex of the root of [??]. By Lemma 4.1, [alpha]' can further be extended to a soliton trail [delta] having its center in a family H [less than or equal to] [??]. The trail [delta] is therefore different from [beta], which contradicts Lemma 4.2. The proof is now complete.

Theorem 4.4. Let G be a connected deterministic soliton graph having no impervious edges. If G has a non-mandatory internal elementary component, then G is a chestnut.

Proof. Induction on the number of non-degenerate elementary components of G. Assume that a non-mandatory internal elementary component C exists in G. If C is the only non-degenerate elementary component in G, then C is an internal family by itself, and the statement of the theorem follows directly from Theorem 4.3. Now let G have more than one non-degenerate elementary component, and suppose that the statement is true for all appropriate soliton graphs having fewer non-degenerate elementary components than G. Let F denote the family of C. By Theorem 4.3, if F is internal, then F = {C} and F is minimal with respect to [[less than or equal to].sub.G]. Let [??] be a non-degenerate family such that F [[less than or equal to].sub.G] [??], and [??] is either external or near-external. Clearly, if F is external, then [??] = F. Otherwise [??] can be found by stepping upwards in the partial order [[less than or equal to].sub.G] starting from family F, which is a minimal element by Theorem 4.3. Notice that this search must reject F itself, as F being near-external would imply that its sole member C is the only non-degenerate elementary component in G. Thus, in this case, [??] [not equal to] F.

Let R be the root of [??]. We are going to prove that

1. R is mandatory,

2. [??] = {R}, and

3. there is exactly one forbidden edge incident with R's unique non-principal (or non-external) vertex.

Fix a state M for G, and choose an M-alternating cycle [gamma] in C. Since C is accessible from [??], [gamma] can be extended to a soliton c-trail [beta] from v [member of] Ext(G), where v is either in R, or it is adjacent to a principal vertex in R.

Proof of Statement 1. Assume, by contradiction, that R is non-mandatory, and distinguish the following two cases.

Case 1: R is external. Let u be the vertex in R where the path h([beta]) finally leaves this elementary component. By [1], there exists a crossing [delta] in R from v to another external vertex z via u with respect to some state [[bar.M].sub.R] of R. Modify M, so that its restriction to R is replaced by [[bar.M].sub.R], and let M' denote the resulting state. Clearly, the straight crossing [delta] between v and z in either direction is a possible transition of [A.sub.G] in state M'. On the other hand, this crossing can also make a detour to include [gamma] through the appropriate section of [beta] that starts at u. Notice, however, that this detour is only available from one direction, depending on whether the M'-positive edge incident with u on [delta] points toward v or z. Nevertheless, the co-existence of these two different transitions violates the deterministic property.

Case 2: R is internal. Trivially, there exists a soliton c-trail [delta] with respect to M starting from v such that c([delta]) runs entirely in R; a contradiction with Lemma 4.2.

Proof of Statement 2. As in the proof of Theorem 4.3, the existence of an R-ear as an M-alternating loop would immediately contradict Lemma 4.2.

Proof of Statement 3. Assume that there is more than one forbidden edge going out from the non-principal (or non-external) vertex of [??] to different internal families of G. By Lemma 4.1, each of these edges can be made part of a suitable soliton trail in G with respect to M, starting from vertex v. Since [beta] is also such a trail, a contradiction with Lemma 4.2 is inevitable.

Now we are ready to synthesize statements 1, 2, 3, and finish the proof of Theorem 4.4. It has turned out that the case F = [??] is not possible. Detach the mandatory family [??] from G, keeping the unique forbidden edge specified in statement 3 as an external edge in the remainder graph G'. Notice that, if R is internal, then its principal vertex can only be adjacent to external vertices, or else G would have impervious edges. Observe that G' is also deterministic, connected, has no impervious edges, and still has the non-mandatory internal elementary component C in it. Apply the induction hypothesis to establish G' as a chestnut. Finally, conclude that G is also a chestnut by sticking back the mandatory family [??] onto G'. The proof is complete.

5 Reducing soliton graphs

A redex r in graph G consists of two adjacent edges e = (u, z) and f = (z, v) such that u [not equal to] v are both internal and the degree of z is 2. The vertex z is called the center of r, while u and v (e and f) are the two focal vertices (respectively, focal edges) of r.

Let r be a redex in G. Contracting r in G means creating a new graph [G.sub.r] from G by deleting the center of r and merging the two focal vertices of r into one vertex s. Now suppose that G is a soliton graph. For a state M of G, let [M.sub.r] denote the restriction of M to edges in [G.sub.r]. Clearly, [M.sub.r] is a state of [G.sub.r]. Notice that the state M can be reconstructed from [M.sub.r] in a unique way. In other words, the connection M [right arrow] [M.sub.r] is a one-to-one correspondence between the states of G and those of [G.sub.r].

For any walk [alpha] in G, let [trace.sub.r]([alpha]) denote the restriction of [alpha] to edges in [G.sub.r]. It is easy to see that if [alpha] is a soliton walk in G with respect to M, then so is [trace.sub.r]([alpha]) in [G.sub.r] with respect to [M.sub.r]. Moreover, the soliton walk [alpha] can again be uniquely recovered from [trace.sub.r]([alpha]). Consequently, the connection [alpha][right arrow] [trace.sub.r]([alpha]) is also a one-to-one correspondence between soliton walks in G and soliton walks in [G.sub.r]. Furthermore, M' = S(M, [alpha]) holds in G iff [(M').sub.r] = S([M.sub.r], [trace.sub.r]([alpha])) holds in [G.sub.r]. We thus have proved the following statement.

Proposition 5.1. The soliton automata [A.sub.G] and [A.sub.[G.sub.r]] are isomorphic.

Notice, furthermore, that if an alternating unit goes through both focal vertices of r, then it must do so along the center of r. As a consequence we have:

Proposition 5.2. The function [trace.sub.r] establishes a one-to-one correspondence between the alternating units of G and those of [G.sub.r].

It follows from the previous two propositions that every edge e of [G.sub.r] is allowed in [G.sub.r] iff e is allowed in G. As to the two focal edges of r, they can either be allowed or not in G, even when [G.sub.r]. is elementary. This issue is addressed by Proposition 5.3 below.

Proposition 5.3. Let r be a redex in soliton graph G, and assume that [G.sub.r]. is elementary. Then G is elemental, iff both focal edges of r are allowed in G, or, equivalently, each focal vertex of r has at least one allowed edge of [G.sub.r] incident with it.

Proof. It is sufficient to note that either focal edge of r is forbidden in G iff the other focal edge is mandatory. Moreover, an arbitrary internal edge e of G is mandatory iff all edges adjacent to e are forbidden.

Another natural simplifying operation on graphs is the removal of a loop from around a vertex v if, after the removal, v still remains internal. Such loops will be called secondary. Let [G.sub.v] denote the graph obtained from G by removing a secondary loop e at vertex v. Clearly, if G is a soliton graph, then so is [G.sub.v], and the states of [G.sub.v] are exactly the same as those of G. The automata [A.sub.G] and [A.sub.[G.sub.v]], however, need not be isomorphic. This follows from the fact that any external alternating walk reaching v on a positive edge can turn back in G after having made the loop e twice, while this may not be possible for the same walk without the presence of e. Nevertheless, it is still true that for every elementary soliton graph G, G is deterministic iff [G.sub.v] is such.

There are loops, however, the removal of which preserves isomorphism of soliton automata. These loops are exactly the ones around the inaccessible vertices of G. Each such loop is impervious, so that its removal does not affect the automaton behavior of G.

6 General characterization of deterministic soliton graphs

Graph G is said to be reduced if it is free from redexes and secondary loops. A generalized tree is a connected graph not containing any even-length cycles. By this definition, the odd-length cycles possibly present in a generalized tree must be pairwise edge-disjoint, which explains the terminology.

The proof of the following statement is left to the reader as a simple exercise.

Lemma 6.1. Let [alpha] be an alternating cycle with respect to state M of an elementary soliton graph G. Then G has an M-alternating cycle [alpha]' and a crossing [beta] that intersects [alpha]'.

Proposition 6.2. If G is nondeterministic, then G has an alternating cycle with respect to some state M. Conversely, if G is elementary and has an alternating cycle with respect to some state AI, then G is nondeterministic.

Proof. Assume that G is nondeterministic. Then there exists a state M and soliton walks [alpha], [beta] connecting the same pair of external vertices in such a way that S(M, [alpha]) [not equal to] S(M, [beta]). Consider the network N(S(M, [alpha]), S(M, [beta])). This network is not empty, and it consists of alternating cycles only.

Now let G be elementary, having an M-alternating cycle [alpha]. By Lemma 6.1 we can assume that G also has a crossing [beta] with respect to the same state M that intersects [alpha]. Consider the network N(S(M, [beta]), S(M, [alpha])). This network will contain a crossing [beta]' different from [beta], yet connecting the same two external vertices [v.sub.1], [v.sub.2]. Thus, for the state M' = S(M, [beta]), [A.sub.G] has two different transitions on input ([v.sub.1], [v.sub.2]) resulting in states S(M', [beta]') and S(M', [beta]) = M, respectively.

The key step to our results in this section is Theorem 6.3 below. The proof of this theorem is rather complex, therefore we do not present it here. The interested reader is referred to [3] for a complete proof.

Theorem 6.3. Let G be a reduced elementary soliton graph, If G contains an even-length cycle, then it also has an alternating cycle with respect to some state of G.

For an arbitrary graph G, contract all redexes and remove all secondary loops in an iterative manner to obtain a reduced graph r(G). Observe that this reduction procedure has the so called Church-Rosser property, that is, if G admits two different one-step reductions to graphs [G.sub.1] and [G.sub.2], then either [G.sub.1] is isomorphic to [G.sub.2], or [G.sub.1] and [G.sub.1] can further be reduced to a common graph [G.sub.1,2]. In this context, one reduction step means contracting a redex or removing a single secondary loop. As an immediate consequence of the Church-Rosser property, the graph r(G) above is unique up to graph isomorphism. In a similar fashion, the process of contracting all redexes and removing all impervious secondary loops is called i-reduction, and the graph obtained from G after i-reduction is denoted by [r.sub.i] (G)

Theorem 6.4. For any graph G, if r(G) is a generalized tree, then G is a deterministic soliton graph. Conversely, if G is a deterministic elementary soliton graph, then r(G) is a generalized tree.

Proof. Clearly, G is a soliton graph iff r(G) is such. By Proposition 5.2, if r(G) is a generalized tree, then G does not contain alternating cycles with respect to any of its states. Proposition 6.2 then implies that G is deterministic. Conversely, if G is a deterministic elementary soliton graph, then so is r(G), containing no alternating cycles with respect to any of its states. (See again Propositions 5.2 and 6.2.) Thus, by Theorem 6.3, r(G) is a generalized tree.

Corollary 6.5. An elementary soliton graph is deterministic iff it reduces to a generalized tree.

Definition 2. A baby chestnut is a chestnut [gamma] + [[alpha].sub.1] + ... + [[alpha].sub.k] such that [gamma] is a pair of parallel edges and each tree [a.sub.i] (1 [less than or equal to] i [less than or equal to] k) consists of one edge or two adjacent edges.

Theorem 6.6. let G be a viable connected soliton graph possessing a non-mandatory internal elementary component. Then G is deterministic iff [r.sub.i] (G) is a baby chestnut.

Proof. 'Only if' By Theorem 4.4, G is a chestnut augmented by some impervious edges connecting the outer internal vertices with each other. Since each internal inner vertex, different from the base ones, is the center of a redex, we can eliminate all of these vertices using reduction, except of course the last inner vertex in [gamma], which will no longer identify a redex. After removing the secondary impervious loops generated during redex elimination, [r.sub.i](G) becomes a baby chestnut.

'If' Blowing up [gamma] by inverse redex elimination, or stretching the trees [[alpha].sub.i] in this manner preserves the property of being a chestnut, and any impervious loops added during this procedure may only stretch into impervious edges. Thus, the graph resulting from a baby chestnut after any number of blow-ups and stretches is still a chestnut with some additional impervious edges.

Now we are ready to state the main result of this paper.

Theorem 6.7. Let G be a connected viable soliton graph. Then G is deterministic iff it satisfies one of the following two conditions.

1. G i-reduces to a baby chestnut.

2. Each external component of G reduces to a generalized tree, and the subgraph of G determined by its internal components has a unique perfect matching.

Proof. Immediate by Theorems 4.4, 6.6, and Corollary 6.5.

7 Conclusion

We have presented a detailed analysis of deterministic soliton graphs. First we proved that every connected deterministic soliton graph having no impervious edges, but possessing a non-mandatory internal elementary component is a chestnut. Then we introduced a simple reduction procedure on graphs, and showed that an elementary soliton graph is deterministic iff it reduces to a generalized tree. Using i-reduction, we could provide a yet simpler description of chestnut graphs, and gave a characterization of deterministic soliton graphs in general.

(1) Partially supported by Natural Science and Engineering Research Council of Canada, Discovery Grant #170493-03


[1] M. Bartha, E. Gombas, On graphs with perfect internal matchings, Acta Cybernetica 12 (1995), 111-124.

[2] M. Bartha, M. Kresz, Structuring the elementary components of graphs having a perfect internal matching, Theoretical Computer Science 299 (2003), 179-210.

[3] M. Bartha, M. Kresz, Deterministic soliton automata defined by elementary graphs, in Kalmar Workshop on Logic and Computer Science, Technical Report, University of Szeged, 2003, pp. 69-79.

[4] F. L. Carter, A. Schultz, D. Duckworth, Soliton switching and its implications for molecular electronics, in Molecular Electronic Devices II (F. L. Carter Ed.), Marcel Dekker Inc., New york, 1987, pp. 149-182.

[5] J. Dassow, H. Jurgensen, Soliton automata, J. Comput. System Sci. 40 (1990), 154-181.

[6] L. Lovasz, M. D. Plummer, Matching Theory, North Holland, Amsterdam, 1986.

Miklos Bartha

Department of Computer Science

Memorial University of Newfoundland

St. John's, NL, Canada


Miklos Kresz

Department of Computer Science

Juhasz Gyula Teacher Training College

University of Szeged, Hungary


Received: March 23, 2005
COPYRIGHT 2006 Slovenian Society Informatika
No portion of this article can be reproduced without the express written permission from the copyright holder.
Copyright 2006 Gale, Cengage Learning. All rights reserved.

Article Details
Printer friendly Cite/link Email Feedback
Author:Bartha, Miklos; Kresz, Miklos
Geographic Code:4EXHU
Date:Oct 1, 2006
Previous Article:Jozef Stefan Institute.
Next Article:Expected case for projecting points.

Related Articles
Solitons under the sea.
Topological solitons.
Discrete and continuous nonlinear Schrodinger systems.
The Direct Method in Soliton Theory.
Topological solitons.
Dissipationless waves for information transfer in neurobiology--some implications.
A Java library of graph algorithms and optimization.
On the propagation of localized perturbations in media with microstructure/lokaliseeritud hairituste levist mikrostruktuurses keskkonnas.

Terms of use | Privacy policy | Copyright © 2021 Farlex, Inc. | Feedback | For webmasters |