Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2013, Article ID 973501, 10 pages http://dx.doi.org/10.1155/2013/973501 Research Article A Discrete Dynamical Model of Signed Partitions G. Chiaselotti, G. Marino, P. A. Oliverio, and D. Petrassi Dipartimento di Matematica, UniversitaΜ della Calabria, Via Pietro Bucci, Cubo 30B, 87036 Arcavacata di Rende, Italy Correspondence should be addressed to G. Marino; gmarino@unical.it Received 28 November 2012; Accepted 19 February 2013 Academic Editor: Luigi Muglia Copyright © 2013 G. Chiaselotti et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. We use a discrete dynamical model with three evolution rules in order to analyze the structure of a partially ordered set of signed integer partitions whose main properties are actually not known. This model is related to the study of some extremal combinatorial sum problems. 1. Introduction A dynamical system is by definition a system whose state changes with time π‘. We have a discrete dynamical system when π‘ is an integer or a natural number, and the elements of the system can be obtained in the form π’π‘+1 = πΉ(π’π‘ ), where πΉ is some global function which describes the evolution rule of the system (see [1]). In a series of very recent works, the theory of discrete dynamical systems has been applied in several contexts. In [2], the theory of discrete dynamical systems is applied in order to analyze some models of concurrent computing systems. In [3], a dynamical model of parallel computation on bi-infinite time scale with an approach similar to two-sided symbolic dynamics is constructed. In [4], the authors analyze the orbit structure of parallel discrete dynamical systems over directed dependency graphs, with Boolean functions as global functions. In [5], the authors extend the manner of defining the evolution update of discrete dynamical systems on Boolean functions, without limiting the local functions to being dependent restrictions of a global one. Finally, in [6] is given a complete characterization of the orbit structure of parallel discrete dynamical systems with maxterm and minterm Boolean functions as global functions. In [7], the authors have introduced the poset (π(π, π, π), β) of all the signed integer partitions π ≥ ππ ≥ ⋅ ⋅ ⋅ ≥ π1 ≥ 0 ≥ π1 ≥ ⋅ ⋅ ⋅ ≥ ππ−π ≥ −(π − π), where the positive parts and the negative parts are all distinct between them and the number of nonzero parts is exactly π. In this case, the partial order β is that on the components. The concept of signed integer partition has been introduced in [8] and studied in [9] from an arithmetical point of view. In [7, 10], it is shown that the structure of the lattice π(π, π, π) is strictly related to the study of some combinatorial extremal sum problems. In this paper, we study some particular type of signed partitions (specifically, of the signed partitions of π(π, π, π)) by adopting the interesting point of view of the discrete dynamical models. In particular, we analyze the lattice π(π, π, π) as a discrete dynamical model with three local evolution rules whose dynamics is studied in a sequential mode. The way to study a lattice of classical partitions as a discrete dynamic model having some particular evolution rules is implicit in [11], where Brylawski proposed a dynamical approach to study the lattice πΏ π΅ (π) of all the partitions of the fixed positive integer π with the dominance ordering. In such a context, a configuration of the system is represented by an ordered partition of an integer π, that is, a decreasing sequence π = (π1 , . . . , ππ ) having sum π, whose blocks of the corresponding Young diagram are considered as mobile sand grain, and the movement of a sand grain, respects the following rules. Rule 1 (vertical rule). One grain can move from a column to the next column if the difference of height of these two columns is greater than or equal to 2. Rule 2 (horizontal rule). If a column containing π + 1 grains is followed by a sequence of columns containing π grains and then one column containing π − 1 grains, then one grain of the first column can slip to the last column. In this paper, we prove that the covering relation in the lattice π(π, π, π) is uniquely determined by three evolution rules of our discrete dynamical model. We articulate the proof 2 Journal of Applied Mathematics of this result by contradiction by using only the first-order logic. This method of proof is very laborious; however, its advantage is that it can be easily implemented on a proof assistant checker based on the first-order logic (e.g., Mizar). The paper is articulated as follows. In Section 2, we recall some basic definitions and preliminary results, for example, the definition of π(π, π, π) and some of its properties. In Section 3, we explain how to see the signed partitions of π(π, π, π) as configurations of our discrete dynamical model and we also describe its evolution rules. In Section 4, we assume by contradiction that there is a generic element π€σΈ of π(π, π, π) that covers another generic element π€ ∈ π(π, π, π) but π€σΈ is not generated by π€ with none of our evolution rules. From this assumption we deduce several propositions and conditions that we use in order to prove our principal result, that is, Theorem 4. 2. Definitions and Preliminary Results (I2) if π₯, π¦ ∈ π and if π₯ ≤ π¦, then π¦π ≤ π₯π . The map π is called complementation of π and π₯π the complement of π₯. Let us observe that if π is an involution poset, by (πΌ1) it follows that π is bijective and by (πΌ1) and (πΌ2) it holds that if π₯, π¦ ∈ π are such that π₯ < π¦, then π¦π < π₯π . If (π, ≤, π) is an involution poset and if π ⊆ π, we will set ππ = {π§π : π§ ∈ π}. We note that if π is an involution poset, then π is a self-dual poset because from (πΌ1) and (πΌ2) it follows that if π₯, π¦ ∈ π, we have that π₯ ≤ π¦, if and only if π¦π ≤ π₯π , and this is equivalent to say that the complementation is an isomorphism between π and its dual poset π∗ . In [7], it has been shown that (π(π, π), β) is an involution poset and its complementation map π is the following: π (ππ ⋅ ⋅ ⋅ π1 0 ⋅ ⋅ ⋅ 0 | 0 ⋅ ⋅ ⋅ 0 π1 ⋅ ⋅ ⋅ ππ ) σΈ σΈ = ππ−π ⋅ ⋅ ⋅ π1σΈ 0 ⋅ ⋅ ⋅ 0 | 0 ⋅ ⋅ ⋅ 0 π1σΈ ⋅ ⋅ ⋅ ππ−π−π , If (π, ≤) is a poset and π₯, π¦ ∈ π, we write π¦ β π₯ (or π₯ β π¦) if π¦ covers π₯. Now we briefly recall the definition of the lattice π(π, π) that we have introduced in [7] in a more formal context. Let π and π be two nonnegative integers such that π ≤ π. We call (π, π)-string a π-tuplet of integers ππ ⋅ ⋅ ⋅ π1 | π1 ⋅ ⋅ ⋅ ππ−π , (I1) (π₯π )π = π₯, for all π₯ ∈ π; (1) such that (i) π1 , . . . , ππ ∈ {1, . . . , π, 0}; (ii) π1 , . . . , ππ−π ∈ {−1, . . . , −(π − π), 0}; (iii) ππ ≥ ⋅ ⋅ ⋅ ≥ π1 ≥ 0 ≥ π1 ≥ ⋅ ⋅ ⋅ ≥ ππ−π ; (iv) the unique element in (1) which can be repeated is 0. If π€ is a (π, π)-string, we call parts of π€ the integers ππ , . . . , π1 , π1 ⋅ ⋅ ⋅ ππ−π , nonnegative parts of π€ the integers ππ , . . . , π1 , and nonpositive parts of π€ the integers π1 ⋅ ⋅ ⋅ ππ−π . We set π€+ = ππ ⋅ ⋅ ⋅ π1 | and π€− = |π1 ⋅ ⋅ ⋅ ππ−π . In some cases, we do not distinguish between nonnegative and nonpositive parts of π€, and we write more simply π€ = π1 ⋅ ⋅ ⋅ ππ instead of π€ = ππ ⋅ ⋅ ⋅ π1 |π1 ⋅ ⋅ ⋅ ππ−π . We also denote by |π€|> the number of parts of π€ that are strictly positive, with |π€|< the number of parts of π€ that are strictly negative, and we set βπ€β = |π€|> + |π€|< . π(π, π) is the set of all the (π, π)-strings. If π€ = σΈ are two (π, π)ππ ⋅ ⋅ ⋅ π1 |π1 ⋅ ⋅ ⋅ ππ−π and π€σΈ = ππσΈ ⋅ ⋅ ⋅ π1σΈ |π1σΈ ⋅ ⋅ ⋅ ππ−π σΈ σΈ strings, we set π€+ = π€+ if ππ = ππ for all π = π, . . . , 1, π€− = π€−σΈ if ππσΈ = ππ for all π = 1, . . . , π − π, and π€ = π€σΈ if π€+ = π€+σΈ and π€− = π€−σΈ . On π(π, π), we consider the partial order on the components that we denote by β. To simplify the notations, in all the numerical examples the integers on the right of the vertical bar | will be written without minus sign. Since (π(π, π), β) is a finite distributive lattice, it is also graded, with minimal element 0 ⋅ ⋅ ⋅ 0|12 ⋅ ⋅ ⋅ (π − π) and maximal element π(π − 1) ⋅ ⋅ ⋅ 21|0 ⋅ ⋅ ⋅ 0. We recall now the concept of involution poset (see [12, 13] for some recent studies on such class of posets). An involution poset (IP) is a poset (π, ≤, π) with a unary operation π : π₯ ∈ π σ³¨→ π₯π ∈ π, such that (2) σΈ where {π1σΈ , . . . , ππ−π } is the usual complement of {π1 , . . . , ππ } σΈ } is the usual complement of in {1, . . . , π}, and {π1σΈ , . . . , ππ−π−π {π1 , . . . , ππ } in {−1, . . . , −(π − π)} (e.g., in π(7, 4), we have that (4310|001)π = 2000|023). If π is an integer such that 0 ≤ π ≤ π, we set now π(π, π, π) = {π€ ∈ π(π, π) : βπ€β = π}. Its easy to see that (π(π, π, π), β) is a sublattice of (π(π, π), β) and obviously |π(π, π, π)| = ( ππ ). We call signed Young diagrams (briefly SYD) an ordered couple π· = π·1 : π·2 , where π·1 is a Young diagram of an integer partition built with decreasing columns instead with decreasing rows, and π·2 is a Young diagram of an integer partition built with increasing columns. In the sequel, we will call pile a column of a Young diagram and grain a square of a pile. For example, (3) π·= : is determined by the partitions 4331 and 113. If π€ = ππ ⋅ ⋅ ⋅ π1 |π1 ⋅ ⋅ ⋅ ππ−π ∈ π(π, π), we denote by π·(π€) the signed Young diagram π·(π€) = π·+ (π€) : π·− (π€), where π·+ (π€) is the Young diagram of the partition (ππ , . . . , π1 ) and π·− (π€) is the Young diagram of the partition (−π1 , . . . , −ππ−π ). Now, if π· = π·1 : π·2 is a SYD, where (ππ‘ , . . . , π1 ) is the decreasing partition having π·1 as Young diagram and ((−π1 ), . . . , (−ππ )) is the increasing partition having π·2 as Young diagram, we set π(π·) = ππ‘ ⋅ ⋅ ⋅ π1 |(−π1 ) ⋅ ⋅ ⋅ (−ππ ) and we call π(π·) the signed partition of π·. We say that a signed Young diagram π· is a (π, π)-SYD if it results that π(π·) ∈ π(π, π) and we denote with ππ(π, π) the set of all the (π, π)-SYD. It is clear that the map π : π€ σ³¨→ π·(π€) is a bijection between π(π, π) and ππ(π, π), whose inverse function is the map π : π· σ³¨→ π(π·); therefore, in the sequel, we will identify the elements of π(π, π) with the (π, π)SYDs of ππ(π, π). If π΄ and π΅ are two usual Young diagrams, we set π΄ ⊆ π΅ if π΄ is a subdiagram of π΅. If π· = π·1 : π·2 and π·σΈ = π·1σΈ : π·2σΈ are two SYDs, we set π· β π·σΈ ⇐⇒ π·1 ⊆ π·1σΈ , π·2 ⊇ π·2σΈ . (4) Journal of Applied Mathematics 3 Therefore, it is clear that we can identify (π(π, π), β) with (ππ(π, π), β). Now we set ππ(π, π, π) = {π·(π€) : π€ ∈ π(π, π, π)}. Obviously we can identify (ππ(π, π, π), β) with (π(π, π, π), β). If (π») is a statement, in the sequel we denote by ¬(π») the negation of (π»). Rule 3. One grain must be deleted from the πth-minus pile if π€ has a minus cliff at π: β : 3. Description of the Evolution Rules In our dynamic model, the set of all configurations is exactly ππ(π, π, π). Our goal is to define some rules of evolution that starting from the minimum of ππ(π, π, π) allow us to reconstruct the Hasse diagram of ππ(π, π, π) (and therefore to determine the covering relations in π(π, π, π)). Let π€ = ππ ⋅ ⋅ ⋅ π1 |π1 ⋅ ⋅ ⋅ ππ−π ∈ π(π, π, π) and π· = π·(π€) = π·+ (π€) : π·− (π€). If 1 ≤ π ≤ π, we call πth-plus pile of π·, and we denote it by πΆ+ (π, π·), the πth pile of π·+ (π€) that corresponds to part ππ of π€ and, if 1 ≤ π ≤ π − π, we call πth-minus pile of π·, and we denote it by πΆ− (π, π·), the πth pile of π·− (π€) that corresponds to part ππ of π€. We call the pile πΆ+ (π, π·) πππ’π π ππππππ‘ππ ππππ if ππ = 1 and πΆ− (π, π·) ππππ’π π ππππππ‘ππ ππππ if ππ = 1. Let us note that if there exists a plus singleton pile, then it is necessarily unique, analogously for a minus singleton pile. If 1 < π ≤ π, we set Δ+π (π€) = ππ − ππ−1 and we call Δ+π (π€) the plus height difference of π€ in π. If 1 < π ≤ π − π, we set Δ−π (π€) = |ππ | − |ππ−1 | and we call Δ−π (π€) the minus height difference of π€ in π. If 1 < π ≤ π, we say that π€ has a plus cliff at π if Δ+π (π€) ≥ 2. If 1 < π ≤ π − π, we say that π€ has a minus cliff at π if Δ−π (π€) ≥ 2. Remark 1. When we apply the following rules to one element π€ ∈ π(π, π), we impose that there is an “invisible” extra pile in the imaginary place (π + 1) of π·+ (π€) having exactly π + 1 grains. This is only a formal trick for decreas the number of rules necessary for our model; therefore, the (π+1)th pile must be not considered as a part of π€. 3.1. Evolution Rules. Rule 1. If the πth-plus pile has at least one grain and if π€ has a plus cliff at π + 1, then one grain must be added on the πth-plus pile: (5) β : : Rule 2. If there is not a plus singleton pile and there is a minus singleton pile, then the latter must be shifted to the side of the lowest non empty plus pile: (6) : β β : (7) : Remark 2. (i) Under the hypothesis in Rule 3, the πth plus must have at least 2 grains. (ii) In Rule 2, the lowest non empty plus pile can also be the invisible column in the place π + 1. In this case, all the plus piles are empty and a possible minus singleton pile must be shifted in the place π. 4. Main Result In the sequel, we write π€ → π π€σΈ (or π€σΈ = π€ → π ) to denote that π€σΈ is an π-tuplet of integers obtained from π€ applying the Rule π, for π = 1, 2, 3, and that ¬(π€ → π π€σΈ ) if the condition π€ → π π€σΈ is false. We also set ∇ (π€) = {π€σΈ : π€σ³¨→π π€σΈ , π = 1, 2, 3} . (8) Proposition 3. If π€ ∈ π(π, π, π), then ∇(π€) ⊆ {π€σΈ ∈ π(π, π, π) : π€σΈ β π€}. Proof. Let π€ = ππ ⋅ ⋅ ⋅ π1 |π1 ⋅ ⋅ ⋅ ππ−π ∈ π(π, π, π), ππ+1 = π+1 (the invisible pile in the place π+1), and π· = π·(π€). We distinguish the three possible cases related to the previous rules. Case 1. Let us assume that π ≥ π ≥ 1, ππ =ΜΈ 0, and that π€ has a plus cliff at π + 1. If π€σΈ = π€ → 1 , then π€σΈ = ππ ⋅ ⋅ ⋅ ππ+1 (ππ + 1)ππ−1 ⋅ ⋅ ⋅ π1 |π1 ⋅ ⋅ ⋅ ππ−π . It is clear that βπ€σΈ β = π because ππ =ΜΈ 0. Since there is a plus cliff at π + 1, we have ππ+1 − ππ ≥ 2; hence, ππ+1 ≥ ππ + 2 > ππ + 1 > ππ > ππ−1 , and this implies that π€σΈ ∈ π(π, π, π). We must show now that π€σΈ covers π€ in π(π, π, π). Since π€ and π€σΈ differ between them only in the place π for ππ and ππ + 1, respectively, it is clear that there does not exist an element π§ ∈ π(π, π, π) such that π€ β π§ β π€σΈ . Hence, π€σΈ β π€. Case 2. Let us assume that in π·(π€) there is not a plus singleton pile and that there is a minus singleton pile (we say πΆ− (π, π·), for some 1 ≤ π ≤ π − π). Since ππ+1 = π + 1, we can assume that ππ+1 > 0, ππ = 0, for some 1 ≤ π ≤ π. This means that π€ has the following form: π€ = ππ ⋅ ⋅ ⋅ ππ+1 00 ⋅ ⋅ ⋅ 0|0 ⋅ ⋅ ⋅ 0(−1)ππ+1 ⋅ ⋅ ⋅ ππ−π , where ππ+1 > 1 (otherwise π·(π€) has a plus singleton pile). Applying Rule 2 to π€, we obtain π€σΈ = π€ → 2 , where π€σΈ = ππ ⋅ ⋅ ⋅ ππ+1 10 ⋅ ⋅ ⋅ 0|0 ⋅ ⋅ ⋅ 00ππ+1 ⋅ ⋅ ⋅ ππ−π . It is clear then that π€σΈ ∈ π(π, π) and βπ€σΈ β = π since π€σΈ is obtained from π€ with only a shift of the pile-1 to the left in the place π. Let us note that the only elements π§1 , π§2 ∈ π(π, π) such that π€ β π§1 β π€σΈ and π€ β π§2 β π€σΈ are π§1 = ππ ⋅ ⋅ ⋅ ππ+1 10 ⋅ ⋅ ⋅ 0|0 ⋅ ⋅ ⋅ 0(−1)ππ+1 ⋅ ⋅ ⋅ ππ−π and π§2 = ππ ⋅ ⋅ ⋅ ππ+1 00 ⋅ ⋅ ⋅ 0|0 ⋅ ⋅ ⋅ 00ππ+1 ⋅ ⋅ ⋅ ππ−π , but βπ§1 β = π+1 and βπ§2 β = π − 1; hence, π§1 , π§2 are not elements of π(π, π, π). This implies that π€σΈ covers π€ in π(π, π, π). Case 3. If 1 < π ≤ π − π and π€ has a minus cliff at π, we apply Rule 3 to π€ on the pile πΆ− (π, π·) and we obtain π€σΈ = π€ → 3 , 4 Journal of Applied Mathematics where π€σΈ = ππ ⋅ ⋅ ⋅ π1 |π1 ⋅ ⋅ ⋅ ππ−1 (ππ +1)ππ+1 ⋅ ⋅ ⋅ ππ−π . Since π€ has a minus cliff at π, we have −ππ +ππ−1 = |ππ |−|ππ−1 | ≥ 2; therefore, π€σΈ ∈ π(π, π) because 0 ≥ ππ−1 ≥ ππ + 2 > ππ + 1 > ππ > ππ+1 and βπ€σΈ β = π since ππ ≤ −2 implies ππ + 1 < 0. As in Case 1, we note that π€σΈ covers π€ in π(π, π, π) because they differ between them only for a grain in the place π. The main result of this paper is to prove that if π€, π€σΈ ∈ π(π, π, π), then π€σΈ covers π€ in π(π, π, π) if and only if π€ → π π€σΈ for some π ∈ {1, 2, 3}. Obviously this result can be reformulated as follows. (∃π ∈ {1, . . . , π} such that ππ+1 > 0, ππ = 0) AND (Λ+ (π€, π€σΈ ) \ {π} = Λ− (π€, π€σΈ ) \ {π} = 0, ππσΈ = 1, ππσΈ = 0); (3) π€ → 3 π€σΈ is equivalent to Ω3 (π€) =ΜΈ 0 AND (∃π ∈ Ω3 (π€) : (ππσΈ = ππ + 1) AND (Λ+ (π€, π€σΈ ) = Λ− (π€, π€σΈ ) \ {π} = 0)). Negation of Rules 1, 2, and 3. (1) ¬(π€ → 1 π€σΈ ) ⇔ [(1AσΈ ) OR (1B)], where (1B) is (Ω1 (π€) = 0), (1AσΈ ) is [Ω1 (π€) =ΜΈ 0 AND (for all π ∈ Ω1 (π€) (ππσΈ =ΜΈ ππ + 1) OR (Λ+ (π€, π€σΈ ) \ {π} =ΜΈ 0 OR Λ− (π€, π€σΈ ) =ΜΈ 0))]. Theorem 4. If π€ ∈ π(π, π, π), then ∇(π€) = {π€σΈ ∈ π(π, π, π) : π€σΈ β π€}. By Proposition 3, to prove Theorem 4, it suffices to show that {π€σΈ ∈ π(π, π, π) : π€σΈ β π€} ⊆ ∇(π€). To show this inclusion, we proceed by contradiction as follows. We start with the following hypotheses: π€, π€σΈ ∈ π (π, π, π) , π€ = ππ ⋅ ⋅ ⋅ π1 | π1 ⋅ ⋅ ⋅ ππ−π , σΈ , π€σΈ = ππσΈ ⋅ ⋅ ⋅ π1σΈ | π1σΈ ⋅ ⋅ ⋅ ππ−π π€σΈ β π€ (2) ¬(π€ → 2 π€σΈ ) ⇔ [(2AσΈ ) OR (2B) OR (2C) OR (2D)], where (2AσΈ ) is (for all π ∈ {1, . . . , π} ππ =ΜΈ 1) AND (∃π ∈ {1, . . . , π − π} such that ππ = −1) AND (∃π ∈ {1, . . . , π} such that ππ+1 > 0, ππ = 0) AND ((Λ+ (π€, π€σΈ ) \ {π} =ΜΈ 0 OR Λ− (π€, π€σΈ ) \ {π} =ΜΈ 0) OR ππσΈ =ΜΈ 1 OR ππσΈ =ΜΈ 0); (2B) is (∃π ∈ {1, . . . , π} such that ππ = 1); (2C) is (for all π ∈ {1, . . . , π − π} ππ =ΜΈ − 1); (2D) is (for all π ∈ {1, . . . , π} ππ+1 = 0 OR ππ > 0). (9) and we also assume that ¬ (π€σ³¨→π π€σΈ ) for each π = 1, 2, 3. (10) Then the proof of Theorem 4 will consist into show that the hypotheses (9) and the conditions (10) always lead to contradictory cases, so that it must be necessarily verified the inclusion {π€σΈ ∈ π(π, π, π) : π€σΈ β π€} ⊆ ∇(π€). We will articulate the proof of Theorem 4 in several cases. Each possible case will be placed in the form of a proposition and we will obtain a contradiction in all cases, showing, hence, the thesis of the theorem. Before proceeding, let us note that in some cases we also use the alternative notations π€ = π1 ⋅ ⋅ ⋅ ππ and π€σΈ = π1σΈ ⋅ ⋅ ⋅ ππσΈ . We set now Ω1 (π€) = {π ∈ {1, . . . , π} : ππ > 0, ππ+1 − ππ ≥ 2} , Formalization of Rules 1, 2, and 3. The description of Rules 1, 2, and 3 in terms of parts of π€ and π€σΈ is the following: (1) π€ → 1 π€σΈ is equivalent to Ω1 (π€) =ΜΈ 0 AND (∃π ∈ Ω1 (π€) : (ππσΈ = ππ + 1) AND (Λ+ (π€, π€σΈ ) \ {π} = Λ− (π€, π€σΈ ) = 0)); (for all π ∈ {1, . . . , π} ππ =ΜΈ 1) AND (∃π ∈ {1, . . . , π − π} such that ππ = −1) AND we set (1.1b) : π€ = 00 ⋅ ⋅ ⋅ 0 | π1 ⋅ ⋅ ⋅ ππ−π , (1.2b) : π€ = π (π − 1) ⋅ ⋅ ⋅ (π + 1) π ⋅ ⋅ ⋅ 0 | π1 ⋅ ⋅ ⋅ ππ−π (12) (13) Proposition 5. Consider (1B) ⇒ ((1.1b) OR (1.2b)). (11) Λ− (π€, π€σΈ ) = {π ∈ {1, . . . , π − π} : ππσΈ > ππ } . (2) π€ → 2 π€σΈ is equivalent to (3B) is (Ω3 (π€) = 0); (3AσΈ ) is [Ω3 (π€) =ΜΈ 0 AND (for all π ∈ Ω3 (π€) (ππσΈ =ΜΈ ππ + 1) OR (Λ+ (π€, π€σΈ ) =ΜΈ 0 OR Λ− (π€, π€σΈ ) \ {π} =ΜΈ 0))]. for some π ∈ {1, . . . , π} . Ω3 (π€) = {π ∈ {2, . . . , π − π} : ππ−1 − ππ ≥ 2} , Λ+ (π€, π€σΈ ) = {β ∈ {1, . . . , π} : πβσΈ > πβ } , (3) ¬(π€ → 3 π€σΈ ) ⇔ [(3AσΈ ) OR (3B)], where Proof. The condition Ω1 (π€) = 0 means that for all π ∈ {1, . . . , π}, ππ = 0 or 0 ≤ ππ+1 − ππ ≤ 1 (i.e., ππ+1 − ππ = 0 or ππ+1 − ππ = 1). We have then the following possibilities: (j) ππ = 0; (jj) ππ+1 − ππ = 0 (and therefore ππ+1 = ππ = 0 since π€ ∈ π(π, π)); (jjj) ππ+1 = ππ + 1. If ππ = 0 for all π ∈ {1, . . . , π} then (12) holds. Let us assume therefore that π ∈ {1, . . . , π} is the smallest index such that ππ > 0; hence, ππ > ππ−1 > ⋅ ⋅ ⋅ > ππ+1 > ππ > 0 and ππ−1 = ⋅ ⋅ ⋅ = π1 = 0. This means that for all indexes π ∈ {π, π−1, . . . , π+ 1, π} holds necessarily (jjj). In particular, for π = π we have π + 1 = ππ+1 = ππ + 1; hence, ππ = π. Now, if π = π − 1, π = ππ = ππ−1 +1, that is, ππ−1 = π−1. Iterating (13) follows. Journal of Applied Mathematics 5 (iii) (2C) AND (3.2b) ⇒ absurd, We set (2.1d) : π€ = π (π − 1) ⋅ ⋅ ⋅ 2 1 | π1 ⋅ ⋅ ⋅ ππ−π . (14) (iv) (1.1b) AND (3.1b) ⇒ absurd, (v) (1.2b) AND (3.1b) ⇒ absurd. Proposition 6. Consider (2D) ⇔ (2.1d). Proof. By (2D), if we take π = π, we have ππ+1 = 0 or ππ > 0; therefore, it is necessarily ππ > 0 because by hypothesis, ππ+1 = π + 1 > 0. Thus, still by (2D), for π = π − 1, we have π(π−1)+1 = ππ = 0 or ππ−1 > 0; therefore, it must be ππ−1 > 0. By iterating, we can deduce that ππ > 0, ππ−1 > 0,. . ., π1 > 0; hence, π1 = 1, π2 = 2,. . ., ππ = π because π€ is an element of π(π, π), that is, exactly (14). On the other side, if π€ = π(π−1) ⋅ ⋅ ⋅ 2 1|π1 ⋅ ⋅ ⋅ ππ−π , then it is immediate to note that (2D) is verified. Proof. (i), (ii), and (iii) are obvious. (iv) By (12) and (15), it follows that π€ = 0 ⋅ ⋅ ⋅ 0|0 ⋅ ⋅ ⋅ 0, absurd. (v) By Proposition 8, we have π€−σΈ = π€− . Then, since π€ β π€σΈ , βπ€σΈ β = βπ€β and π€−σΈ = π€− , by (13) we deduce that π€+σΈ = π€+ . Hence, the absurd π€σΈ = π€. Proposition 10. Consider (1.2b) AND (2B) ⇒ (2.1d). We set (3.1b) : π€ = ππ ⋅ ⋅ ⋅ π1 | 00 ⋅ ⋅ ⋅ 0, (3.2b) : π€ = ππ ⋅ ⋅ ⋅ π1 | 00 ⋅ ⋅ ⋅ 0 (−1) (−2) ⋅ ⋅ ⋅ (−π) for some π ∈ {1, . . . , π − π} . (15) (16) Proposition 7. Consider (3B) ⇒ ((3.1b) OR (3.2b)). Proof. The condition Ω3 (π€) = 0 means that for all π ∈ {2, . . . , π−π}, 0 ≤ ππ−1 −ππ ≤ 1 (i.e., ππ−1 −ππ = 0 or ππ−1 −ππ = 1). We have then the following possibilities: (i) ππ−1 − ππ = 0 (and therefore ππ−1 = ππ = 0 since π€ ∈ π(π, π)); (ii) ππ−1 = ππ + 1. If (i) holds for all π ∈ {2, . . . , π − π}, then (15) holds. We can assume therefore that π ∈ {2, . . . , π − π} is the smallest index such that (ii) holds. Let us observe then that if in a place π ∈ {2, . . . , π − π}, (ii) holds; then also in the places π + 1, . . . , π − π, (ii) holds. In fact, if ππ = ππ−1 − 1 and by absurd ππ = ππ+1 = 0, then ππ−1 = 1 which is a contradiction because 0 ≥ ππ−1 . Therefore, if (ii) holds in π, then it also holds in π + 1, and therefore, by iteration, it holds for π+1, π+2, . . . , π−π. Now we assume at first that π = 2. In this case, (ii) holds for all indexes in {2, . . . , π − π}; therefore, π1 = 0 or π1 = −1 and π2 = π1 − 1, π3 = π2 −1 ⋅ ⋅ ⋅. If π1 = 0, then π€ = ππ ⋅ ⋅ ⋅ π1 |0(−1)(−2) ⋅ ⋅ ⋅ (−(π− π)+1) and if π1 = −1, then π€ = ππ ⋅ ⋅ ⋅ π1 |(−1)(−2) ⋅ ⋅ ⋅ (−(π−π)); thus in both cases (ii) holds. Let now π ≥ 3. Then ππ−1 = ππ−2 = 0 (because in the place π − 1 (i) holds) and hence 0 = ππ−1 = ππ−2 = ⋅ ⋅ ⋅ = π2 = π1 . Moreover, since (i) holds in the places π, π+1, . . . , π−π, we have ππ = ππ−1 −1 = 0−1 = −1; therefore, ππ+1 = ππ − 1 = −2, . . ., ππ−π = ππ−π−1 − 1 = −(π − π − π) − 1 = −π, where π = π − π − π + 1. This completes the proof. Proposition 8. Consider (3.1b) ⇒ (π€− = π€−σΈ =| 00 ⋅ ⋅ ⋅ 0). Proof. Since π€ β π€σΈ , it must be 0 ≥ ππσΈ ≥ ππ , where ππ = 0 for all π ∈ {1, . . . , π − π} because (15) implies π€ = ππ ⋅ ⋅ ⋅ π1 |00 ⋅ ⋅ ⋅ 0. Therefore, ππ = ππσΈ = 0 for all π ∈ {1, . . . , π − π}; that is, π€σΈ = ππσΈ ⋅ ⋅ ⋅ π1σΈ | 00 ⋅ ⋅ ⋅ 0. Proposition 9. Consider (i) (1.1b) AND (2B) ⇒ absurd, (ii) (1.1b) AND (2.1d) ⇒ absurd, Proof. By (2B), it follows that in (13) it must be π = 1; therefore, π€ = π(π − 1) ⋅ ⋅ ⋅ 2 1|π1 ⋅ ⋅ ⋅ ππ−π . Proposition 11. Consider (2.1d) AND (3.2b) ⇒ absurd. Proof. By (14), it is immediate to observe that π€+σΈ = π€+ because π€ β π€σΈ . Then by (16), since π€+σΈ = π€+ , βπ€−σΈ β = βπ€− β and π€ β π€σΈ , it must also be π€−σΈ = |00 ⋅ ⋅ ⋅ 0(−1)(−2) ⋅ ⋅ ⋅ (−π). Hence, we obtain π€ = π€σΈ , absurd. Proposition 12. Consider (2AσΈ ) ⇒ absurd. Proof. We set (F) [(for all π ∈ {1, . . . , π} ππ =ΜΈ 1) AND (∃π ∈ {1, . . . , π − π} such that ππ = −1) AND (∃π ∈ {1, . . . , π} such that ππ+1 > 0, ππ = 0)]; (G) (Λ+ (π€, π€σΈ ) \ {π} =ΜΈ 0 OR Λ− (π€, π€σΈ ) \ {π} =ΜΈ 0); (H) (ππσΈ =ΜΈ 1 OR ππσΈ =ΜΈ 0). Then (2AσΈ ) is equivalent to ((F) AND (G)) OR ((F) AND (H)). We show at first that ((F) AND (H)) leads to a contradiction. Next we show that ((F) AND (G) AND ¬(H)) also leads to an absurd. This will prove the thesis; ((F) AND (H)) ⇒ absurd. By (F), it follows that π€ satisfies the hypothesis of Rule 2; therefore, by Proposition 3 we can take an element π§ ∈ π(π, π, π) such that π§ = π€ → 2 . As in the proof of the Case 2 in Proposition 3, it results that π€ and π§ must have the following form: π€ = ππ ⋅ ⋅ ⋅ ππ+1 00 ⋅ ⋅ ⋅ 0 | 0 ⋅ ⋅ ⋅ 0 (−1) ππ+1 ⋅ ⋅ ⋅ ππ−π , (17) π§ = ππ ⋅ ⋅ ⋅ ππ+1 10 ⋅ ⋅ ⋅ 0 | 0 ⋅ ⋅ ⋅ 00ππ+1 ⋅ ⋅ ⋅ ππ−π , (18) where ππ+1 > 1 and ππ+1 < −1. We distinguish now several cases. (I) ππσΈ =ΜΈ 0. Then ππσΈ ≤ −1, and also ππσΈ ≥ ππ = −1 because π€ β π€σΈ ; hence ππσΈ = −1. We note now that σΈ ππσΈ > 0, . . . , ππ+1 >0 (19) 6 Journal of Applied Mathematics σΈ because ππσΈ ≥ ππ > 0, . . . , ππ+1 ≥ ππ+1 > 0. Moreover, since σΈ ππ = −1, it follows that σΈ σΈ −1 = ππσΈ > ππ+1 > ⋅ ⋅ ⋅ > ππ−π (20) because π€σΈ ∈ π(π, π). Now, since π€ ∈ π(π, π, π), from the form of π€ it results that π = (π − π) + (π − π − π + 1). Moreover, since also π€σΈ ∈ π(π, π, π), we have βπ€σΈ β = π = (π − π) + (π − π − π + 1). Therefore, since in (19), there are exactly π − π inequalities and in (20) there are exactly π − π − π + 1 inequalities; it follows that σΈ σΈ σΈ 00 ⋅ ⋅ ⋅ 0 | 0 ⋅ ⋅ ⋅ 0 (−1) ππ+1 ⋅ ⋅ ⋅ ππ−π . π€σΈ = ππσΈ ⋅ ⋅ ⋅ ππ+1 (21) (II) ππσΈ = 0. Since π€ β π€σΈ , by (17) we have two possible cases: π€σΈ has the form (21) or σΈ σΈ σΈ π€σΈ = ππσΈ ⋅ ⋅ ⋅ ππ+1 00 ⋅ ⋅ ⋅ 0 | 0 ⋅ ⋅ ⋅ 00 ππ+1 ⋅ ⋅ ⋅ ππ−π (22) σΈ σΈ ≥ ππ+1 > 1 and 0 ≥ ππ+1 . If (22) holds, then βπ€σΈ β ≤ with ππ+1 (π − π) + (π − π − π) = π − 1, which is absurd because π€σΈ ∈ π(π, π, π); hence it must hold necessarily (21). (III) ππσΈ > 1. Since π€ β π€σΈ and π = βπ€β = βπ€σΈ β, by (17) it follows that σΈ σΈ σΈ π€σΈ = ππσΈ ⋅ ⋅ ⋅ ππ+1 ππσΈ 0 ⋅ ⋅ ⋅ 0 | 0 ⋅ ⋅ ⋅ 00 ππ+1 ⋅ ⋅ ⋅ ππ−π . (23) Then from the hypothesis ππσΈ ≥ 2 and by (18), we have π€ β π§ β π€σΈ , which is a contradiction. Hence the unique possibility is that π€σΈ has the form (21). Since π€σΈ β π€, we have ππσΈ ≥ ππ for π = π, . . . , π + 2, π + 1 and ππσΈ ≥ ππ for π = π + 1, π + 2, . . . , π − π. Moreover, at least one inequality of the type ππσΈ > ππ or the type ππσΈ > ππ must hold. We distinguish now the several cases. (Δ1) We assume that a unique inequality of the type ππσΈ > ππ holds for some π = π, . . . , π + 2, π + 1. Therefore, we have ππσΈ = ππ for all π =ΜΈ π and ππσΈ = ππ for all π = π + 1, π + 2, . . . , π − π. σΈ Then, since ππ+1 = ππ+1 > ππσΈ > ππ > 0 (let us note that the previous inequalities also hold if π = π because ππ+1 = π + 1 = σΈ ), we have that ππ+1 − ππ ≥ 2 and ππ > 0. Hence π€ satisfies ππ+1 the hypotheses of Rule 1 in the place π and so π€ → 1 π’, where π’ = ππ ⋅ ⋅ ⋅ ππ+1 (ππ + 1) ππ−1 ⋅ ⋅ ⋅ ππ+1 0 ⋅ ⋅ ⋅ 0 | V = ππ ⋅ ⋅ ⋅ ππ+1 (ππ + 1) ππ−1 ⋅ ⋅ ⋅ ππ+1 0 ⋅ ⋅ ⋅ 0 | 0 ⋅ ⋅ ⋅ 0 (−1) ππ+1 ⋅ ⋅ ⋅ ππ−π . (25) Since ππσΈ > ππ is the first strict inequality by left, we have σΈ σΈ = ππ+1 (also if π = π); hence ππ+1 = ππ+1 > ππσΈ ≥ ππ+1 ππ +1 > ππ > ππ−1 because ππ > 0; this implies that V ∈ π(π, π); therefore V ∈ π(π, π, π) because βVβ = βπ€β = π. Moreover, it is clear that π€ β V. Let us observe now that V β π€σΈ ; in fact, by hypothesis, π€σΈ must have at least another place π =ΜΈ π where ππσΈ > ππ or ππσΈ > ππ and V differs by π€ only in the place π. This shows that π€ β V β π€σΈ , with V ∈ π(π, π, π), which is absurd because π€σΈ β π€. (Δ4) If at least two strict inequalities among the ππσΈ ≥ ππ and ππσΈ ≥ ππ hold and the first (by left) of such strict inequalities is ππσΈ > ππ for some π ∈ {π + 1, π + 2, . . . , π − π}, then we deduce a contradiction in the same way as in the previous case. This concludes the proof that ((F) AND (H)) ⇒ absurd. To complete the proof we show now that ((F) AND (G) AND ¬(H)) ⇒ absurd. Since (H) is false, we have ππσΈ = 1 and ππσΈ = 0; thereσΈ fore, π€ has the form (17) and π€σΈ = ππσΈ ⋅ ⋅ ⋅ ππ+1 10 ⋅ ⋅ ⋅ 0|0 ⋅ ⋅ ⋅ σΈ σΈ ⋅ ⋅ ⋅ ππ−π . We take π§ ∈ π(π, π, π) as in (18), so that π€ 00ππ+1 and π§ differ between them only in the places π,π and π€ β π§. σΈ σΈ σΈ 10 ⋅ ⋅ ⋅ 0|0 ⋅ ⋅ ⋅ 00ππ+1 ⋅ ⋅ ⋅ ππ−π , Moreover, since π€σΈ = ππσΈ ⋅ ⋅ ⋅ ππ+1 σΈ by (G), (18), and (17) it follows that π§ β π€ . Therefore, we obtain π€ β π§ β π€σΈ that is in contrast with the hypothesis π€σΈ β π€. We set now (1A) : Ω1 (π€) =ΜΈ 0, ∀π ∈ Ω1 (π€) ππσΈ =ΜΈ ππ + 1, (26) (3A) : Ω3 (π€) =ΜΈ 0, ∀π ∈ Ω1 (π€) ππσΈ =ΜΈ ππ + 1. (27) Proposition 13. Consider 0 ⋅ ⋅ ⋅ 0 (−1) ππ+1 ⋅ ⋅ ⋅ ππ−π σΈ σΈ σΈ (= ππσΈ ⋅ ⋅ ⋅ ππ+1 (ππ + 1) ππ−1 ⋅ ⋅ ⋅ ππ+1 0⋅⋅⋅0 | as in the proof of the previous case by using Rule 3 instead of Rule 1. (Δ3) We assume now that at least two strict inequalities among the ππσΈ ≥ ππ and ππσΈ ≥ ππ hold, and let us also assume that the first (by left) of such strict inequalities is ππσΈ > ππ for some π ∈ {π, . . . , π + 1}. We consider then the following (π, π)string: (24) σΈ σΈ ⋅ ⋅ ⋅ ππ−π ), 0 ⋅ ⋅ ⋅ 0 (−1) ππ+1 with π’ ∈ π(π, π, π). Now, if ππσΈ = ππ + 1, it results that π€σΈ = π’; therefore, π€ → 1 π€σΈ , which is a contradiction with the hypothesis ¬(π€ → 1 π€σΈ ). Otherwise, if ππ + 1 < ππσΈ , then we have π€ β π’ β π€σΈ , which is absurd because π€σΈ β π€. (Δ2) If a unique inequality of the type ππσΈ > ππ holds for some π = π + 1, π + 2, . . . , π − π, we deduce a contradiction (i) (1AσΈ ) ⇔ (1A), (ii) (3AσΈ ) ⇔ (3A). Proof. (i) The implication ⇐ is obvious. We assume now that (1AσΈ ) holds and there exists π ∈ Ω1 (π€) such that ππσΈ = ππ + 1 and also that Λ+ (π€, π€σΈ )\{π} =ΜΈ 0 (i.e., there exists β =ΜΈ π such that πβσΈ > πβ ) or Λ− (π€, π€σΈ ) =ΜΈ 0 (i.e., there exists π such that ππσΈ > ππ ). Since π ∈ Ω1 (π€), we can apply Rule 1 to π€ and we can take π§ = π€ → 1 . By Proposition 3, we know that π§ ∈ π(π, π, π) and π§ β π€. Moreover, since πβσΈ > πβ (β =ΜΈ π) or ππσΈ > ππ , we also have π§ β π€σΈ ; therefore, π€ β π§ β π€σΈ , which is in contrast with the hypothesis π€σΈ β π€. Hence this proves that the condition Journal of Applied Mathematics 7 ππσΈ =ΜΈ ππ + 1 must be verified for all π ∈ Ω1 (π€), which is exactly (26). (ii) The proof is similar to (i) applying Rule 3 to π€ instead of Rule 1. We set (1a) : Ω1 (π€) =ΜΈ 0, ∀π ∈ Ω1 (π€) ππσΈ = ππ , (28) (3a) : Ω3 (π€) =ΜΈ 0, ∀π ∈ Ω3 (π€) ππσΈ = ππ . (29) Proposition 14. Consider Lemma 17. Assume that (3a) holds. If π ∈ {2, 3, . . . , π − π − 1}, σΈ = ππ+1 . ππσΈ = ππ < 0, then ππ+1 (i) (1A) ⇒ (1a), (ii) (3A) ⇒ (3a). Proof. (i) By (1A), we have Ω1 (π€) =ΜΈ 0, and by the definition of Ω1 (π€) this is equivalent to say that π€ satisfies the hypotheses of Rule 1 for some π ∈ {1, . . . , π}. Therefore, by Proposition 3, there exists an element π§π ∈ π(π, π, π) such that π€ → 1 π§π , where π§π = ππ ⋅ ⋅ ⋅ ππ+1 (ππ + 1)ππ−1 ⋅ ⋅ ⋅ π1 |π1 ⋅ ⋅ ⋅ ππ−π and obviously π€ β π§π . Since ππσΈ =ΜΈ ππ + 1, we distinguish two cases. (a) ππσΈ > ππ + 1. In this case π€ β π§π β π€σΈ , that is in contrast with the hypothesis π€σΈ β π€. (b) ππσΈ < ππ + 1. In this case ππσΈ ≤ ππ ; hence ππσΈ = ππ because ππσΈ ≥ ππ from the hypothesis π€σΈ β π€. (ii) The proof of this case is similar to (i). Lemma 15. Assume that (1a) holds. If π ∈ {2, 3, . . . , π, π + 1}, σΈ = ππ−1 . ππσΈ = ππ , and ππ−1 > 0, then ππ−1 Proof. If π−1 ∈ Ω1 (π€), then the thesis holds by the definition of (1a) in (28). We assume now that π − 1 ∉ Ω1 (π€). Then ππ−1 = 0 or 0 ≤ π(π−1)+1 − ππ−1 = ππ − ππ−1 ≤ 1, and since ππ−1 > 0, we necessarily have 0 ≤ ππ − ππ−1 ≤ 1. Now, if ππ − ππ−1 = 0, we have ππ = ππ−1 = 0 since π€ ∈ π(π, π), which is in contradiction with ππ−1 > 0. Hence, it must be σΈ ππ − ππ−1 = 1; that is, ππ = ππ−1 + 1. Moreover, ππσΈ > ππ−1 σΈ σΈ because ππ−1 ≥ ππ−1 > 0 and π€ ∈ π(π, π). Therefore, since σΈ , which implies ππσΈ = ππ , we have ππ−1 + 1 = ππ = ππσΈ > ππ−1 σΈ σΈ ππ−1 + 1 > ππ−1 ≥ ππ−1 because π€ β π€ . By subtracting ππ−1 from each term of the previous inequalities, we obtain 1 > σΈ σΈ − ππ−1 ≥ 0; therefore, it must be ππ−1 = ππ−1 . ππ−1 We set (1.1a) : ∃π ∈ {π, . . . , 2} such that ππ > 0, π€ = ππ ππ−1 ⋅ ⋅ ⋅ ππ+1 ππ 0 ⋅ ⋅ ⋅ 0 | π1 ⋅ ⋅ ⋅ ππ−π , σΈ π€ = π€ ∈ π(π, π), it must be π1 = 0 or π1 = 1. If π1 = 1, then π2 = 2, . . . , ππ = π, which is in contrast with ππ+1 − ππ ≥ 2. Hence π1 = 0 and therefore there exists π ∈ 2, . . . , π such that ππ > 0 and ππ−1 = ⋅ ⋅ ⋅ = π1 = 0. We take π = π + 1; that is, π − 1 = π. Since ππσΈ = ππ = π + 1 and ππ−1 = ππ ≥ ππ > 0, by Lemma 15 it σΈ = ππ−1 ; that is, ππσΈ = ππ . Let now π = π. If π = π, follows that ππ−1 then we have the thesis otherwise π = π > π; that is, π − 1 ≥ π; therefore ππ−1 ≥ ππ > 0 because π€ ∈ π(π, π). Then since ππσΈ = σΈ = ππσΈ = ππ = ππ , we can apply Lemma 15 and we deduce ππ−1 σΈ ππ−1 ; that is, ππ−1 = ππ−1 . By iteration the thesis follows. σΈ ππ ππ−1 ⋅ ⋅ ⋅ ππ+1 ππ ππ−1 ⋅ ⋅ ⋅ π1σΈ | π1σΈ (30) σΈ ⋅ ⋅ ⋅ ππ−π . Proposition 16. Consider (1a) ⇒ (1.1a). Proof. By (28), there exists at least one element π ∈ Ω1 (π€). In this place we have ππ > 0 and moreover ππ+1 − ππ ≥ 2. Since Proof. If π + 1 ∈ Ω3 (π€), then the thesis holds by definition of (3a) in (29). We assume now that π + 1 ∉ Ω3 (π€). Now, if ππ − ππ+1 = 0, we have ππ = ππ+1 = 0 since π€ ∈ π(π, π), which is in contradiction with the hypothesis ππ < 0. Hence it must be ππ − ππ+1 = 1; that is, 0 > ππ = ππ+1 + 1; therefore 0 > ππ+1 + 1 = σΈ ππ = ππσΈ > ππ+1 ≥ ππ+1 since π€σΈ ∈ π(π, π) and π€ β π€σΈ . The σΈ last inequalities provide ππ+1 + 1 > ππ+1 ≥ ππ+1 . By subtracting ππ+1 from each term of the previous inequalities, we obtain σΈ σΈ 1 > ππ+1 − ππ+1 ≥ 0; therefore it must be ππ+1 = ππ+1 . Proposition 18. If (3a) holds, then π€ has the following form: π€ = ππ ⋅ ⋅ ⋅ π1 |0 ⋅ ⋅ ⋅ 0 ππ ππ+1 ⋅ ⋅ ⋅ ππ−π , with ππ < 0 and π ≥ 2. Moreover, if ππ ≤ −2, we also have π€−σΈ = π€− . Proof. By (3a) in (29), we know that Ω3 (π€) =ΜΈ 0. Moreover, if π ∈ Ω3 (π€), then π ≥ 2 and ππ < 0 because ππ−1 − ππ ≥ 2. Therefore, we can take the minimum π ∈ 2, . . . , π − π such that ππ < 0; hence ππ−1 = ⋅ ⋅ ⋅ = π1 = 0 and this means that π€ = ππ ⋅ ⋅ ⋅ π1 |0 ⋅ ⋅ ⋅ 0ππ ππ+1 ⋅ ⋅ ⋅ ππ−π . Assume now that ππ ≤ −2. Since ππ−1 = 0, we have ππ−1 − ππ ≤ 2; therefore π ∈ Ω3 (π€). By (3a), follows then that ππσΈ = ππ < 0. Now, if π = π − π, the thesis is true, otherwise, if π ∈ {2, . . . , π − π − 1}, by Lemma 17 we σΈ = ππ+1 < 0. Again, if π + 1 = π − π, the thesis is true; have ππ+1 otherwise, if π + 1 ∈ {2, . . . , π − π − 1}, by Lemma 17 we have σΈ = ππ+2 < 0. Proceeding repeatedly in this way we obtain ππ+2 σΈ σΈ = ππ+1 , . . . , ππ−π = ππ−π . Finally, since π1 = ⋅ ⋅ ⋅ = ππσΈ = ππ , ππ+1 σΈ σΈ = 0. This ππ−1 = 0 and π€ β π€ , we also have π1σΈ = ⋅ ⋅ ⋅ = ππ−1 σΈ proves that π€− = π€− . Proposition 19. Consider ((2C) AND (3a)) ⇒ π€−σΈ = π€− . Proof. (2C) implies that π€ has the form π€ = ππ ⋅ ⋅ ⋅ π1 |0 ⋅ ⋅ ⋅ 0 ππ ππ+1 ⋅ ⋅ ⋅ ππ−π , with ππ ≤ −2. Since (3a) holds, by Proposition 18, the thesis follows. Proposition 20. Consider ((1.1a) AND (2C) AND (3a)) ⇒ absurd. Proof. By Proposition 19, we have that π€−σΈ = π€− . Moreover, by (1.1a) in (30), we also have π€+σΈ = π€+ because βπ€σΈ β = βπ€β = π and π€−σΈ = π€− ; therefore, π€ = π€σΈ . This is absurd because π€σΈ β π€ by hypothesis. 8 Journal of Applied Mathematics Proposition 21. Consider ((1.1b) AND (2C) AND (3a)) ⇒ absurd. Proof. By (1.1b) in (12), we know that π€ = 0 ⋅ ⋅ ⋅ 0|π1 ⋅ ⋅ ⋅ ππ−π , and this implies βπ€+ β = 0 and βπ€− β = π. Moreover, by Proposition 19, π€−σΈ = π€− ; therefore it follows that βπ€−σΈ β = π; hence βπ€+σΈ β = 0 since π€σΈ ∈ π(π, π, π). This shows that π€ = π€σΈ and this is absurd because π€ β π€σΈ . Proposition 22. Consider ((1.1a) AND (2B)) ⇒ π€+σΈ = π€+ . Proof. By (1.1a) in (30) and (2B), it follows that π€ = ππ ⋅ ⋅ ⋅ σΈ ⋅ ⋅ ⋅ π1σΈ |π1 ⋅ ⋅ ⋅ ππ−π . ππ+1 10 ⋅ ⋅ ⋅ 0|π1 ⋅ ⋅ ⋅ ππ−π and π€σΈ = ππ ⋅ ⋅ ⋅ ππ+1 1ππ−1 Now, since π€σΈ ∈ π(π, π) and ππ = ππσΈ = 1, we have that 1 = ππσΈ > σΈ σΈ ππ−1 ≥ ⋅ ⋅ ⋅ ≥ π1σΈ ≥ 0; that is, ππ−1 = ⋅ ⋅ ⋅ = π1σΈ = 0. Therefore σΈ π€+ = π€+ . Proposition 23. Consider ((1.1a) AND (2B) AND (3.1b)) ⇒ absurd. Proof. By Proposition 22 π€+σΈ = π€+ and by Proposition 8 π€ = π€−σΈ ; hence π€ = π€σΈ and this is a contradiction. Proposition 24. Consider ((1.1a) AND (3.1b)) ⇒ absurd. Proof. By Proposition 8, π€ = π€−σΈ = |00 ⋅ ⋅ ⋅ 0; hence βπ€+σΈ β = βπ€+ β = π because π€, π€σΈ ∈ π(π, π, π). Moreover, by (1.1a) in (30), it follows that π€+σΈ = π€+ = ππ ⋅ ⋅ ⋅ ππ+1 ππ 0 ⋅ ⋅ ⋅ 0. (31) Proof. By Proposition 22, π€+σΈ = π€+ . Then by (3.2b) in (16), since π€+σΈ = π€+ , βπ€−σΈ β = βπ€− β, and π€ β π€σΈ , it must also be π€−σΈ =| 00 ⋅ ⋅ ⋅ 0 (−1) (−2) ⋅ ⋅ ⋅ (−π) . Hence we obtain π€ = π€σΈ , absurd. Proposition 27. Consider ((1.2b) AND (2C) AND (3a)) ⇒ absurd. Proof. By Proposition 19, π€−σΈ = π€− . Then, since π€ β π€σΈ , βπ€σΈ β = βπ€β, and π€−σΈ = π€− , by (1.2b) in (13) we deduce that π€+σΈ = π€+ . Hence the absurd π€σΈ = π€. Proposition 28. Consider ((2.1d) AND (3a)) ⇒ absurd. Proof. Since π€ β π€σΈ by (2.1d) in (14), it follows that π€+σΈ = π€+ . Then, since (3a) in (29) holds, the same proof of Proposition 25 leads to the absurd π€ = π€σΈ . We complete now the proof of our main result; that is, we provide three syntactic trees where each possible path from the roots to the leaves leads to a contradiction. In the following we draw each tree and next we also write all the implication chains for each path from the roots to the leafs. We recall at first some useful implications and equivalences already proved in the previous section: (Θ1A) (1AσΈ ) ⇔ [by Proposition 13 (i)] (1A) ⇒ [by Proposition 14] (1a) ⇒ [by Proposition 16] (1.1a) Therefore, π€ = π€σΈ , which is absurd. (Θ2A) (2AσΈ ) ⇒ [by Proposition 12] absurd Proposition 25. Consider ((1.1a) AND (2B) AND (3a)) ⇒ absurd. (Θ2D) (2D) ⇔ [by Proposition 6] (2.1d) Proof. By Proposition 18, we have π€ = ππ ⋅ ⋅ ⋅ π1 |0 ⋅ ⋅ ⋅ 0ππ ππ+1 ⋅ ⋅ ⋅ ππ−π with ππ < 0 and π ≥ 2. By Proposition 22, π€+σΈ = π€+ . Now, if ππ ≤ −2, by Proposition 18 we have π€−σΈ = π€− and therefore π€σΈ = π€, which is absurd. So we can assume that ππ = −1. Since π€+σΈ = π€+ , βπ€σΈ β = βπ€β = π and π€ β π€σΈ , it follows that ππσΈ cannot be 0; otherwise, it is βπ€σΈ β < π. This implies that it must be ππσΈ = −1. We distinguish now two cases. (Θ3A) (3AσΈ ) ⇔ [by Proposition 13 (ii)] (3A) ⇒ [by Proposition 14] (3a) ⇒ [see statement of Proposition 18] Proposition 18. The first tree that we consider is that having the condition (1AσΈ ) as root (we denote such tree with TREE(1AσΈ )). TREE (1AσΈ ): 1Aσ³° ππσΈ Case 1. If π ∈ {2, . . . , π−π−1}, since ππ = = −1, by Lemma 17 σΈ (with π = π) we obtain ππ+1 = ππ+1 < 0. Now, if π + 1 = π − π, σΈ then π€− = π€− , and as before this provides a contradiction. If π + 1 < π − π, we can still apply Lemma 17 (with π = π + 1) and σΈ < 0. Proceeding in this way in all therefore have ππ+2 = ππ+2 cases we always obtain π€− = π€−σΈ and hence is absurd. Case 2. If π = π − π, then π€ = ππ ⋅ ⋅ ⋅ π1 | 0 ⋅ ⋅ ⋅ 0(−1), and since βπ€σΈ β = βπ€β = π, π€ β π€σΈ , and π€+σΈ = π€+ , it must also be π€σΈ = ππ ⋅ ⋅ ⋅ π1 |0 ⋅ ⋅ ⋅ 0(−1); that is, π€ = π€σΈ , absurd. Proposition 26. Consider ((1.1a) AND (2B) AND (3.2b)) ⇒ absurd. (32) 2Aσ³° Absurd 3Aσ³° 2B 2C 3Aσ³° 3B 3.1b 3.2b 2D 3Aσ³° 3B 3.1b 3.2b 3B 3.1b 3.2b (33) We observe now that by virtue of Proposition 5 when we start from the condition (1B), we must consider two subtrees, the first with root (1.1b) (which we denote by TREE(1.1b)) that is Journal of Applied Mathematics 9 (1AσΈ ) AND (2D) AND (3.1b) ⇒ absurd by Θ1A and Proposition 24 TREE (1.1b): 1.1b 2Aσ³° 2B σ³° Absurd 3A 2C 3Aσ³° 3B 3.1b 3.2b (1AσΈ ) AND (2D) AND (3.2b) ⇒ absurd by Θ2D and Proposition 11 2D 3Aσ³° 3B 3.1b 3.2b 3B 3.1b 3.2b (1.1b) AND (2B) AND (3AσΈ ) ⇒ absurd by Proposition 9 (i) (34) (1.1b) AND (2B) AND (3.1b) ⇒ absurd by Proposition 9 (i) and the second (which we denote by TREE(1.2b)) that is TREE (1.2b): (1.1b) AND (2B) AND (3.2b) ⇒ absurd by Proposition 9 (i) (1.1b) AND (2C) AND (3AσΈ ) ⇒ absurd by Θ3A and by Proposition 21 1.2b 2Aσ³° 2B σ³° Absurd 3A 2C 3Aσ³° 3B 3.1b 3.2b (1.1b) AND (2C) AND (3.1b) ⇒ absurd by Proposition 9 (iv) 2D 3Aσ³° 3B 3.1b 3.2b 3B 3.1b (1.1b) AND (2C) AND (3.2b) ⇒ absurd by Proposition 9 (iii) 3.2b (35) (1.1b) AND (2D) AND (3.1b) ⇒ absurd by Θ2D and by Proposition 9 (ii) Let us note that the ramification 3B (36) 3.1b (1.1b) AND (2D) AND (3AσΈ ) ⇒ absurd by Θ2D and by Proposition 9 (ii) (1.1b) AND (2D) AND (3.2b) ⇒ absurd by Θ2D and by Proposition 9 (ii) 3.2b in each of the previous trees follows by Proposition 7. We have then exactly 27 possible paths from the roots to the leafs in all the previous trees (we exclude the paths that lead to (2AσΈ ) because we already know that they lead to a contradiction by Θ2A). In the following we write all these 27 paths and, for each, the related proposition that leads to a contradiction together with some implication among the Θ1A, Θ2D, and Θ3A. In the sequel, the node (3B) is omitted for brevity because it is only an intermediate node and in the paths that involve (3B) we use only the leafs (3.1b) and (3.2b) to deduce the related contradictions: (1.2b) AND (2B) AND (3AσΈ ) ⇒ (1.2b) AND (2D) AND (3AσΈ ) (that we examine below) by Θ2D and by Proposition 10 (1.2b) AND (2B) AND (3.1b) ⇒ (1.2b) AND (2D) AND (3.1b) (that we examine below) by Θ2D and by Proposition 10 (1.2b) AND (2B) AND (3.2b) ⇒ (1.2b) AND (2D) AND (3.2b) (that we examine below) by Θ2D and by Proposition 10 (1.2b) AND (2C) AND (3AσΈ ) ⇒ absurd by Θ3A and by Proposition 27 (1AσΈ ) AND (2B) AND (3AσΈ ) ⇒ absurd by Θ1A, Θ3A, and Proposition 25 (1.2b) AND (2C) AND (3.1b) ⇒ absurd by Proposition 9 (v) (1AσΈ ) AND (2B) AND (3.1b) ⇒ absurd by Θ1A and Proposition 23 (1.2b) AND (2C) AND (3.2b) ⇒ absurd by Proposition 9 (iii) (1AσΈ ) AND (2B) AND (3.2b) ⇒ absurd by Θ1A and Proposition 26 (1.2b) AND (2D) AND (3AσΈ ) ⇒ absurd by Θ2D, Θ3A, and Proposition 28 (1AσΈ ) AND (2C) AND (3AσΈ ) ⇒ absurd by Θ1A, Θ3A, and Proposition 20 (1.2b) AND (2D) AND (3.1b) ⇒ absurd by Proposition 9 (v) (1AσΈ ) AND (2C) AND (3.1b) ⇒ absurd by Θ1A and Proposition 24 (1.2b) AND (2D) AND (3.2b) ⇒ absurd by Θ2D and by Proposition 11 (1AσΈ ) AND (2C) AND (3.2b) ⇒ absurd by Θ1A and Proposition 9 (iii) (1AσΈ ) AND (2D) AND (3AσΈ ) ⇒ absurd by Θ2D, Θ3A, and Proposition 28 This concludes the proof of Theorem 4. Below we draw the Hasse diagram of the lattice π(5, 3, 2) by using the evolution Rules 1, 2, and 3 starting with the minimum element of this lattice, which is 00|123. We label a generic edge of the 10 Journal of Applied Mathematics next diagram with the symbol π π if it leads to a production that uses the Rule π, for π ∈ {1, 2, 3}: π 3 : : : π 3 π 1 : π 1 : π 1 π 2 π 3 : (37) π 3 : π 2 π 3 π 3 : π 2 : : References [1] D. K. Arrowsmith and C. M. Place, An Introduction to Dynamical Systems, Cambridge University Press, Cambridge, UK, 1990. [2] J. L. G. Guirao, F. L. Pelayo, and J. C. Valverde, “Modeling the dynamics of concurrent computing systems,” Computers & Mathematics with Applications, vol. 61, no. 5, pp. 1402–1406, 2011. [3] W. ForysΜ, J. L. G. Guirao, and P. Oprocha, “A dynamical model of parallel computation on bi-infinite time-scale,” Journal of Computational and Applied Mathematics, vol. 235, no. 7, pp. 1826–1832, 2011. [4] J. A. Aledo, S. MartΔ±Μnez, and J. C. Valverde, “Parallel dynamical systems over directed dependency graphs,” Applied Mathematics and Computation, vol. 219, no. 3, pp. 1114–1119, 2012. [5] J. A. Aledo, S. Martinez, and J. C. Valverde, “Parallel discrete dynamical systems on independent local functions,” Journal of Computational and Applied Mathematics, vol. 237, no. 1, pp. 335– 339, 2013. [6] J. A. Aledo, S. MartΔ±Μnez, F. L. Pelayo, and J. C. Valverde, “Parallel discrete dynamical systems on maxterm and minterm Boolean functions,” Mathematical and Computer Modelling, vol. 55, no. 3-4, pp. 666–671, 2012. [7] C. Bisi and G. Chiaselotti, “A class of lattices and boolean functions related to the Manickam-MikloΜs-Singhi conjecture,” Advances in Geometry, vol. 13, no. 1, pp. 1–27, 2013. [8] G. E. Andrews, “Euler’s ‘De Partitio numerorum’,” Bulletin of American Mathematical Society, vol. 44, no. 4, pp. 561–573, 2007. [9] W. J. Keith, “A bijective toolkit for signed partitions,” Annals of Combinatorics, vol. 15, no. 1, pp. 95–117, 2011. [10] G. Chiaselotti, G. Marino, and C. Nardi, “A minimum problem for finite sets of real numbers with nonnegative sum,” Journal of Applied Mathematics, vol. 2012, Article ID 847958, 15 pages, 2012. [11] T. Brylawski, “The lattice of integer partitions,” Discrete Mathematics, vol. 6, pp. 201–219, 1973. [12] K. J. Al-Agha and R. J. Greechie, “The involutory dimension of involution posets,” Order, vol. 18, no. 4, pp. 323–337, 2002. [13] K. Brenneman, R. Haas, and A. G. Helminck, “Implementing an algorithm for the twisted involution poset for Weyl groups,” in Proceedings of the 37th Southeastern International Conference on Combinatorics, Graph Theory and Computing, vol. 182, pp. 137–144, 2006. Advances in Operations Research Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Advances in Decision Sciences Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Mathematical Problems in Engineering Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Algebra Hindawi Publishing Corporation http://www.hindawi.com Probability and Statistics Volume 2014 The Scientific World Journal Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Differential Equations Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Volume 2014 Submit your manuscripts at http://www.hindawi.com International Journal of Advances in Combinatorics Hindawi Publishing Corporation http://www.hindawi.com Mathematical Physics Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Complex Analysis Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Mathematics and Mathematical Sciences Journal of Hindawi Publishing Corporation http://www.hindawi.com Stochastic Analysis Abstract and Applied Analysis Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com International Journal of Mathematics Volume 2014 Volume 2014 Discrete Dynamics in Nature and Society Volume 2014 Volume 2014 Journal of Journal of Discrete Mathematics Journal of Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Applied Mathematics Journal of Function Spaces Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Optimization Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014