Abstract
In this paper, we introduce the notion of state maps from a semihoop H1 to another semihoop H2, which is a generalization of internal states (or state operators) on a semihoop H. Also we give a type of special state maps from a semihoop H1 to H1, which is called internal state maps (or IS-maps). Then we give some examples and basic properties of (internal) state maps on semihoops. Moreover, we discuss the relations between state maps and internal states on other algebras. Then we introduce several kinds of filters by state maps on semihoops, called SM-filters, state filters and dual state filters, respectively, and discuss the relations among them. Furthermore we introduce and study the notion of prime SM-filters on semihoops. Finally, using SM-filter, we characterize two kinds of state semihoops.
1 Introduction
Residuated structures arise in many areas of mathematics, and are particularly common among algebras associated with logical systems. The essential ingredients are a partial order ≤, a binary operation of associative and commutative multiplication ⊙ that respects the partial order, and a binary (left-)residuation operation → characterized by x ⊙ y ≤ z if and only if x ≤ y → z. Semihoops [14] are very important and basic residuated structures in which the community of many-valued logicians got interested in the last years, as they are building blocks for several interesting structures being the algebraic semantics for relevant many-valued logics such as basic fuzzy logic (BL, for short). Apart from their logic interest, semihoops have interesting algebraic properties and include kinds of important classes of algebras: Hoops which were originally introduced by Bosbach [6, 7] under the name of complementary semigroups and Brouwerian semilattices-the models of the conjunction-implication fragment of the intuitionistic propositional calculus. A semihoop is called a hoop if x ⊙ (x → y) = y ⊙ (y → x) and a semihoop does not satisfy the divisibility condition x ∧ y = x ⊙ (x → y). Therefore, semihoops are the most fundamental fuzzy structures. It will play an important role in studying fuzzy logics and the related algebraic structures.
In order to measure the average truth-value of propositions in Lukasiewicz logic, Mundici [24] presented an analogue of probability measure, called a state, as averaging process for formulas in Łukasiewicz logic. States on MV-algebras have been deeply investigated. Consequently, the notion of states has been extended to other logical algebras such as BL-algebras [25], MTL-algebras [20, 21], R0-algebras [22] and residuated lattices [12, 19, 23, 26].
Since MV-algebras with state are not universal algebras, they do not automatically induce an assertional logic. Flaminio and Montagna [15, 16] presented an algebraizable logic using a probabilistic approach, and its equivalent algebraic semantics is precisely the variety of state MV-algebras. We recall that a state MV-algebra is an MV-algebra whose language is extended by adding an operator(also called an internal state), whose properties are inspired by ones of states with the addition property. State MV-algebras generalize, for example, Hajek’s approach [17] to fuzzy logic with modality Pr (interpreted as probably) which has the following semantic interpretation: The probability of an event a is presented as the truth value of Pr(a). On the other hand, if s is a state, then s(a) is interpreted as the average appearance of the many valued event a. Consequently, the notion of internal states has also been extended to other algebraic structures. For example, the concept of a state BL-algebra was introduced by Ciungu et al.[11], as an extension of the concept of a state MV-algebra. Subsequently, the concept of internal states was extended by Dvurečenskij et al.[13] to Rℓ-monoids (not necessarily commutative). More generally, the state residuated lattices were introduced by He and Xin [18].
We observed that the states and internal state on MV-algebras, BL-algebras, BCK-algebras and residuated lattices are maps from an algebra X to [0, 1] and X to X, respectively. From the viewpoint of universal algebras, it is meaningful to study a state map from an algebra X to another algebra Y. In particular, if Y = [0, 1], a state can be seen as a state map from X to [0, 1], and if X = Y, a state operator can also be seen as a state map from X → X. Based on this idea, we can conclude that a state map is not only a generalization of internal states but also preserves the usual properties of states. Therefore, it is meaningful to introduce state map to the more general fuzzy structures semihoops and providing an algebraic foundation for reasoning about probabilities of fuzzy events in a new way. This is the motivation for us to investigate state maps on semihoop.
This paper is structured in five sections. In order to make the paper as self-contained as possible, we recapitulate in Section 2 the definition of semihoops, and review their basic properties that will be used in the remainder of the paper. In Section 3, we introduce the notion of state maps (or simply, S-maps), which is a generalization of states on semihoops. Also, we give a characterization of two kinds of semihooops. In Section 4, we discuss the relations between state maps on semihoops and internal states on other algebras, respectively. In Section 5, we introduce several kinds of filters by state maps on semihoops, called SM-filters, state filters and dual state filters, respectively, and discuss the relations among them. Using SM-filter, we characterize two kinds of state semihoops.
2 Preliminaries
In this section, we summarize some definitions and results about semihoop, which will be used in the following sections of the paper.
Definition 2.1
([14]). An algebra (H, ⊙, →, ∧, 1) of type (2, 2, 2, 0) is called a semihoop if it satisfies the following conditions:
(H, ∧, 1) is a ∧-semilattice with upper bound 1,
(H, ⊙, 1) is a commutative monoid,
(x ⊙ y) → z = x → (y → z), for allx, y, z ∈ H.
In what follows, by H we denote the universe of a semihoop (H, ⊙, →, ∧, 1). For any x ∈ H and a natural number n, we define x0 = 1 and xn = xn−1 ⊙ x for n ≥ 1.
On a semihoop (H, ⊙, →, ∧, 1) we define x ≤ y iff x → y = 1. It is easy to check that ≤ is a partial order relation on H and for all x ∈ H, x ≤ 1. A semihoop H is bounded if there exists an element 0 ∈ H such that 0 ≤ x for all x ∈ H. In a bounded semihoop (H, ⊙, →, ∧, 0, 1), we define the negation ∗ : x∗ = x → 0 for all x ∈ L. If x∗∗ = x, for all x ∈ H, then the bounded semihoop H is said to have the Double Negation Property, or (DNP) for short. We define a relation ⊥ on H by x ⊥ y iff y∗∗ ≤ x∗. If x ⊙ x = x, that is, x2 = x for all x ∈ H, then the semihoop H is said to be idemopent. A semihoop H is called a hoop if x ⊙ (x → y) = y ⊙ (y → x) for all x, y ∈ H. Also, in every hoop H, x ∧ y = x ⊙ (x → y) for all x, y ∈ H, see [14].
Proposition 2.2
([14, 30]). In any semihoop (H, ⊙, →, ∧, 1), the following properties hold: for allx, y, z ∈ H,
x ⊙ y ≤ ziffx ≤ y → z,
x ⊙ y ≤ x ∧ y, x ≤ y → x,
1 → x = x, x → 1 = 1,
x ⊙ (x → y) ≤ y,
Ifx ≤ y, theny → z ≤ x → z, z → x ≤ z → yandx ⊙ z ≤ y ⊙ z,
x ≤ (x → y) → y,
((x → y) → y) → y = x → y,
x → (y → z) = y → (x → z),
x → y ≤ (z → x) → (z → y), x → y ≤ (y → z) → (x → z),
x → (x ∧ y) = x → y,
x ⊙ y = x ⊙ (x → x ⊙ y).
Proposition 2.3
([4, 30]). In a bounded semihoop (H, ⊙, →, ∧, 0, 1), the following properties hold: for allx, y, z ∈ H,
1∗ = 0, 0∗ = 1,
x ≤ x∗∗, wherex∗∗ = (x∗)∗,
x ⊙ x∗ = 0, x∗∗∗ = x∗,
x ≤ yimpliesy∗ ≤ x∗,
x → y ≤ y∗ → x∗,
(x → y∗∗)∗∗ = x → y∗∗,
x∗∗ ⊙ y∗∗ ≤ (x ⊙ y)∗∗,
(x∗∗ ⊙ y)∗ = (x ⊙ y)∗.
Proposition 2.4
([14]). Let (H, ⊙, →, ∧, 1) be a semihoop and for allx, y ∈ H, we definex ⊔ y = ((x → y) → y) ∧ ((y → x) → x). Then the following conditions are equivalent:
⊔ is an associative operation onH,
x ≤ yimpliesx ⊔ z ≤ y ⊔ zfor allx, y, z ∈ H,
x ⊔ (y ∧ z) ≤ (x ⊔ y) ∧ (x ⊔ z) for allx, y, z ∈ H,
⊔ is the join operation onH.
Definition 2.5
([14]). A semihoop is called a ⊔-semihoop if it satisfies one of the equivalent conditions of Proposition 2.4.
Proposition 2.6
([30]). In a ⊔-semihoop, the following properties hold: for allx, y, z ∈ H,
x ⊙ (y ⊔ z) = (x ⊙ y) ⊔ (x ⊙ z),
x ⊔ (y ⊙ z) ≥ (x ⊔ y) ⊙ (x ⊔ z),
x ⊔ yn ≥ (x ⊔ y)nandxm ⊔ yn ≥ (x ⊔ y)mn for any natural numbersm, n.
Proof
The proofs are easy, and we hence omit the details. □
Definition 2.7
([1, 2]). Let (H, →, ⊙, 1) be a hoop. His called:
a basic hoop if (x → y) → z ≤ ((y → x) → z) → zfor anyx, y, z ∈ H.
a Wajsberg hoop (x → y) → y = (y → x) → xfor anyx, y ∈ H.
a Gödel hoop ifx ⊙ x = xfor anyx ∈ H.
Proposition 2.8
([3]). Let (H, ⊙, →, 1) be a bounded hoop. Then
bounded basic hoops are definitionally equivalent to BL-algebras.
bounded Wajsberg hoops are definitionally equivalent to MV-algebras.
Let (H, ⊙, →, ∧, 1) be a semihoop. A nonempty set F of H is called a filter of H if it satisfies: (1) x, y ∈ F implies x ⊙ y ∈ F; (2) x ∈ F, y ∈ H and x ≤ y imply y ∈ F. A filter F of H is called a proper filter if F ≠ H. A proper filter F of H is called a maximal filter if it is not contained in any proper filter of H. A nonempty set F of H is a filter of H if and only if 1 ∈ F and if x, x → y ∈ F, then y ∈ F. A proper filter F of a semihoop H is called a prime filter of H, if for any filters F1, F2 of H such that F1 ∩ F2 ⊆ F, then F1 ⊆ F or F2 ⊆ F. For more details about filters in semihoops, see [4].
3 State maps on semihoops
In this section, we introduce the notion of state maps on a semihoop and investigate some related properties of state maps.
Definition 3.1
Let (X, ⊙1, →1, ∧1, 11) and (Y, ⊙2, →2, ∧2, 12) be two semihoops. A mapσ : X → Yis called a state map fromX to Y, which is denoted simply by S-map, if it is satisfies the following conditions:
x ≤1yimpliesσ (x) ≤2σ (y);
σ(x →1y) = σ((x →1y) →1y) →2σ(y);
σ(x ⊙1y) = σ(x) ⊙2σ(x →1 (x ⊙1y));
σ(x) ⊙2σ(y) ∈ σ(X);
σ (x) ∧2σ (y) ∈ σ(X);
σ (x) →2σ (y) ∈ σ(X).
for allx, y ∈ X.
The pair (X, Y, σ) is said to be a S-map semihoop. Moreover, ifX = Yandσ2 = σ, thenσis called an internal state map onX, simply IS-map onX, in this case, (H,σ) is said to be an IS-map semihoop.
Now, we present some examples for S-maps on semihoops.
Example 3.2
LetH1andH2be two semihoops. Then the map 1H1, defined by 1H1(x) = 12for allx ∈ H1, is a S-map fromH1toH2.
Example 3.3
LetHbe a semihoop. One can check thatidHis a S-map onH.
Example 3.4
LetH1 = {01, a1, b1, c1, 11} andH2 = {02, a2, b2, c2, 12}, where 01 ≤ a1 ≤ b1, c1 ≤ 11and 02 ≤ a2 ≤ b2 ≤ c2 ≤ 12. Define operations ⊙iand →ifori = 1, 2 as follows:
Then (H1, →1, ⊙1, ∧1, 11) and (H2, →2, ⊙2, ∧2, 12) are semihoops. Now, we define a mapσ : H1 → H2as follows:
One can check thatσis a S-map fromH1toH2.
Example 3.5
LetH = [0, 1] be the real interval. If forx, y ∈ H, we definex ⊙ y = max{0, x + y−1} andx → y = min{1, 1 − x + y}, then (H, ⊙, →, 0, 1) becomes a hoop, and hence it is a semihoop. Now we defineσ : H1 → Has follows:
whereH1is given in Example 3.4. One can easily check thatσis a S-map fromH1toH.
Next, we present some properties of S-maps on semihoops.
Proposition 3.6
LetHi, i = 1, 2 be semihoops andσbe a S-map fromH1toH2. Then we have: for anyx, y ∈ H1,
σ(11) = 12;
σ(x ⊙1y) ≥ σ(x) ⊙2σ(y);
σ(x →1y) ≤2σ(x) →2σ(y) and ifx ≤1y, thenσ(x →1y) = σ(x) →2σ(y);
σ(H1) is a subalgebra ofH2.
Proof
Applying (SM2), we have σ(11) = σ(01 →1 01) = σ((01 →1 01) →1 01) →2σ(01) = σ(11 →1 01) →2σ(01) = σ(01) →2σ(01) = 12.
From x ⊙1y ≤ x ⊙1y, we get y ≤1x →1 (x ⊙1y) by Proposition 2.2(1). By (SM1), we have σ(y) ≤2σ(x →1( x ⊙1y)). Applying (SM3), we get σ(x ⊙1y) = σ(x) ⊙2σ(x →1 (x ⊙1y)) ≥2σ(x) ⊙2σ(y).
By (SM2), we deduce σ(x →1y) = σ((x →1y) →1y) →2σ(y) ≤2σ(x) →2σ(y) by (5) and (6) of Proposition 2.2. If x ≤1y, then σ(x) ≤2σ(y). This means σ(x) →2σ(y) = 1. Moreover, σ(x →1y) = σ((x →1y) →1y) →2σ(y) = σ(11 →1y) →2σ(y) = σ(y) →2σ(y) = 12. Thus σ(x →1y) = σ(x) →2σ(y).
It follows from (SM4), (SM5), (SM6) and (1). □
Definition 3.7
LetH1andH2be two bounded semihoops. A S-mapσfromH1toH2is called a regular if it satisfiesσ(01) = 02.
Note that the S-map σ given in Example 3.2 is not regular and the S-map σ given in Example 3.4 is regular.
In the following we give some characterizations for a S-map becoming regular.
Theorem 3.8
LetHi, i = 1, 2 be two bounded Wajsberg semihoops andσbe a S-map fromH1toH2. Then the following are equivalent:
σis regular,
σ(x∗1) = (σ(x))∗2for anyx, y ∈ H1,
x ⊥1yimpliesσ(x) ⊥2σ(y) for anyx, y ∈ H1.
Proof
(1) ⇒ (2) By (1) and (SM2), we get σ(x∗1) = σ(x →1 01) = σ((x →1 01) →1 01) →2σ(01) = σ(x) →2 02 = (σ(x))∗2.
(2) ⇒ (3) Suppose that x ⊥1y. Then y∗1∗1 ≤1x∗1, it follows that σ(y∗1∗1) ≤1σ(x∗1). By (2) we have (σ(y))∗2∗2 ≤2 (σ(x))∗. Hence we have σ(x) ⊥2σ(y).
(3) ⇒ (1) Since 01∗1∗1 = 1∗1, we get 11 ⊥1 01. By (3) we have σ(11) ⊥2σ(01), and so σ(01)∗2∗2 ≤2σ(11)∗2. From Proposition 3.6(1), σ(01)∗2∗2 ≤2σ(11)∗2 = 12∗2 = 02, and hence σ(01)∗2∗2 = 02. It follows that σ(01)∗2∗2∗2 = 12. By Proposition 2.2(7), σ(01)∗2∗2∗2 = σ(01)∗2 = 12, that is, σ(01) →2 02 = 12. This shows that σ(01) ≤2 02, so σ(01) = 02. □
Proposition 3.9
LetHbe a semihoop andσbe an IS-map onH. Then we have: for anyx, y ∈ H,
σ(1) = 1;
σ(x ⊙ y) ≥ σ(x) ⊙ σ(y);
σ(x → y) ≤ σ(x) → σ(y) and ifx ≤ y, thenσ(x → y) = σ(x) → σ(y);
σ(σ(x) ⊙ σ(y)) = σ(x) ⊙ σ(y);
σ(σ(x) ∧ σ(y)) = σ(x) ∧ σ(y);
σ(σ(x) → σ(y)) = σ(x) → σ(y);
σ(H) = Fix(σ), whereFix(σ) = {x ∈ H ∣ σ(x) = x};
σ(H) is a subalgebra ofH;
Ker(σ) is a filter ofH, whereKer(σ) = {x ∈ H∣σ(x) = 1}.
Proof
It follows from Proposition 3.6(1).
It follows from Proposition 3.6(2).
It follows from Proposition 3.6(3).
From (SM4), we have σ(x) ⊙ σ(y) = σ(z) for some z ∈ H. Hence σ(σ(x) ⊙ σ(y)) = σ2(z) = σ(z) = σ(x) ⊙ σ(y) by the definition of the IS-maps.
It is similar to (4).
It is similar to (1).
Let ∈ σ(H). Then x = σ(z) for some z ∈ H. Hence σ(x) = σ2(z) = σ(z) = x. So x ∈ Fix(σ). Conversely assume x ∈ Fix(σ). Then x = σ(x) ∈ σ(H). This shows that (7) is true.
It follows from (1), (2), (3) and (4).
It is straightforward. □
Next, we consider properties of IS-map to characterize two kinds of semihoops. The following results and the next one are proved in [30], where (SM2) replace by (SM2’)σ(x → y) = σ(x) → σ(x ∧ y). We can show the same results without the identity (SM2’).
Theorem 3.10
LetHbe a semihoop. Then the following are equivalent:
His a hoop;
every IS-mapσonHsatisfiesσ(x) ⊙ σ(x → y) = σ(y) ⊙ σ(y → x) for allx, y ∈ H.
Proof
The proof is similar to that of He et al [30].(Theorem 4.7 ). □
Theorem 3.11
LetHbe a semihoop. Then the following are equivalent:
His idemopent;
every IS-mapσonHsatisfiesσ(x ∧ y) = σ(y) ⊙ σ(y) = σ(x) ⊙ σ(x → y) for allx, y ∈ H.
Proof
The proof is similar to that of He et al [30].(Theorem 4.8 ). □
Here, we give relations between IS-map and Riečan states on semihoops.
Definition 3.12
([30]). LetHbe a bounded semihoop. A Riečan state onHis a founctions : H ⟶ [0, 1] such that the following conditions hold: for allx, y ∈ H,
s(1) = 1,
ifx ⊥ y, thens(x + y) = s(x) + s(y).
Let H be a semihoop, σ be an IS-map on H and s be a Riečan state on H. Then s is called σ-compatible if σ(x) = σ(y) ⇒ s(x) = s(y) for all x, y ∈ H.
We denote by RS[H] and RSσ[H] the set of all Riečan states and σ-compatible Riečan states on H, respectively.
Theorem 3.13
LetHbe a semihoop andσbe an IS-map onH. Then there is a one-to-one correspondence betweenσ-compatible Riečan states onHand Riečan states onσ(H).
Proof
Suppose that s is a Riečan state on σ(H). Define a mapping φ : RS[σ(H)] → RSσ[H] as follows: φ(s)(x) := s(σ(x)) for all x ∈ H. We will prove that φ(s) is a Riečan state on H. Clearly, φ(s)(1) = s(σ(1)) = s(1) = 1. Next, we will show that φ(s)(x + y) = φ(s)(x)+φ(s)(y) when x ⊥ y. In order to do this, we prove that σ(x + y) = σ(x) + σ(y) for x ⊥ y. Now, suppose that x ⊥ y. From Theorem 3.8(3), we have σ(x) ⊥ σ(y). Then σ(x) + σ(y) = (σ(x))∗ → (σ(y))∗∗. Moreover, σ(x + y) = σ(x∗y∗∗) = σ(x∗) → σ(x∗ ∧ y∗∗). Since x ⊥ y, then y∗∗ ≤ x∗. It follows that σ(x + y) = σ(x∗) → σ(y∗∗) = (σ(x))∗ → (σ(y))∗∗ = σ(x) + σ(y). Now, we prove that φ(s)(x + y) = φ(s)(x)+φ(s)(y) when x ⊥ y. Since σ(x + y) = σ(x) + σ(y) for x ⊥ y, we have that φ(s)(x + y) = s(σ(x + y)) = s(σ(x) + σ(y)) = s(σ(x)) + s(σ(y)) = φ(s)(x)+φ(s)(y). Therefore, φ(s) is a Riečan state on H. Moreover, let σ(x) = σ(y) for all x, y ∈ H, then φ(s)(x) = s(σ(x)) = s(σ(y)) = φ(s)(y). Thus, φ(s) is a σ-compatible state on H. Therefore, the mapping φ is well defined.
Assume that s is a σ-compatible Riečan state on H. The mapping ψ : RSσ[H] → RS[σ(H)] is defined by ψ(s)(σ(x)) := s(x) for all x ∈ H. Let σ(x) = σ(y), then s(x) = s(y) for all x, y ∈ H. Now, we show that ψ(s) is a Riečan state on σ(H). Let σ(x) ⊥ σ(y). Then σ(σ(x) + σ(y)) = σ((σ(x))∗ → (σ(y))∗∗) = σ(σ(x∗) → σ(y∗∗)) = σ(x)∗ → σ(y)∗∗ = σ(x) + σ(y). Based on this, we have that ψ(s)(σ(x) + σ(y)) = ψ(s)(σ(σ(x) + σ(y))) = s(σ(x) + σ(y)) = s(σ(x)) + s(σ(y)) = ψ(s)(σ(σ(x))) + ψ(s)(σ(σ(y))) = ψ(s)(σ(x)) + ψ(s)(σ(y)). Moreover, ψ(s)(σ(1)) = s(1) = 1. That means that ψ(s) is a Riečan state on σ(H). Therefore, ψ is a mapping of RSσ[H] into RS[σ(H)].
Let s1, s2 be σ-compatible states on H and ψ(s1) = ψ(s2). Then we have ψ(s1)(σ(x)) = ψ(s2)(σ(x)), which implies s1(x) = s2(x) for all x ∈ H. Thus, s1 = s2. Now, suppose that s is a Riečan state on σ(H), then we have that (ψ(φ(s))(σ(x)) = φ(s)(x) = s(σ(x)). Therefore, ψ is a bijective mapping from RSσ[H] onto RS[σ(H)] and ψ−1 = φ. □
4 Relations between state maps on semihoops and states on other algebras
Definition 4.1
([10]). A Bosbach state on a bounded pseudo-hoop (A, ⊙, →, ⇝, 0, 1) is a functions : A → [0, 1] such that the following conditions hold: for anyx, y ∈ A:
s(x) + s(x → y) = s(y) + s(y → x);
s(x) + s(x ⇝ y) = s(y) + s(y ⇝ x);
s(0) = 0 ands(1) = 1.
Proposition 4.2
([10]). LetAbe a bounded pseudo-hoop andsbe a Bosbach state onA. Then for allx, y ∈ Athe following properties hold:
y ≤ ximpliess(y) ≤ s(x) ands(x → y) = s(x ⇝ y) = 1 − s(x) + s(y);
s(x−) = s(x∼) = 1 − s(x), wherex− = x → 0 andx∼ = x ⇝ 0.
Definition 4.3
A state-morphism map on a bounded hoopAis a functions : A → [0, 1] such that:
m(0) = 0;
m(x → y) = min{1, 1 − m(x) + m(y)}.
Proposition 4.4
Every state-morphism map on a bounded hoopAis a Bosbach state onA.
Proof
Let m be a state-morphism map on A. Then m(1) = m(0−) = m(0 → 0) = min{1, 1 − m(0) + m(0) = 1}. (B3) holds. Consider m(x) + m(x → y) = m(x)+min{1, 1 − m(x) + m(y) = min{1 + m(x), 1 + m(y)} = m(y) + m(y → x). Hence (B1) is true. Since A is a hoop, (B2) is true, too. Combining the above arguments we get that m is a Bosbach state on A. □
Proposition 4.5
Every state-morphism on a bounded hoopAis a state map fromAto the hoopH = ([0, 1], ⊙, →, 0, 1) given in Example 3.5.
Proof
Assume m is a state-morphism map on a bounded hoop A. By Propositions 4.2 and 4.4, (SM1) holds.
Now we check (SM2). Let x, y ∈ A. By definition of 4.3, we have
For (SM3), we have
For (SM4), we have m(x) ⊙ m(y) = max{0, m(x) + m(y) − 1} = 1 − m(y) + m(x) = min{1, 1 − m(y) + m(x)} = m(y → x) and hence m(x) ⊙ m(y) ∈ m(A). This shows that (SM4) holds.
Note that m(x) → m(y) = min{1, 1 − m(x) + m(y)} = m(x → y). It follows that m(x) → m(y) ∈ m(A), that is (SM6).
For (SM5), we have m(x) ∧ m(y) = m(x) ⊙ (m(x) → m(y)). From (SM4) and (SM6), we get that (SM5) holds. □
Definition 4.6
([30]). A state semihoop is a pair (H,σ) whereHis a bounded semihoop andσ : H → His a mapping, called state operator, such that for anyx, y ∈ Hthe following conditions are satisfied:
σ(0) = 0;
x ≤ yimpliesσ(x) ≤ σ(y);
σ(x → y) = σ(x) → σ(x ∧ y);
σ(x ⊙ y) = σ(x) ⊙ σ(x → x ⊙ y);
σ(σ(x) ⊙ σ(y)) = σ(x) ⊙ σ(y);
σ(σ(x) ∧ σ(y)) = σ(x) ∧ σ(y).
Theorem 4.7
LetHbe a bounded semihoop andσ : H → Hbe a mapping onHpreserving → . Then the following conditions are equivalent:
(H,σ) is an IS-map semihoop;
(H,σ) is a state semihoop.
Proof
(1) ⇒ (2) If H is a bounded semihoop and σ : H → H is a mapping on H preserving →. Then σ(x → y) = σ(x → x ∧ y) = σ(x) → σ(x ∧ y). From proposition 3.9 and definition 4.6, we can obtain that (H,σ) a state semihoop.
(2) ⇒ (1) Let (H,σ) be a state semihoop and σ preserving →. We only need to prove that (SM2) holds. Since ((x → y) → y) → y = x → y, so we have σ((x → y) → y) → σ(y) = σ(((x → y) → y) → y) = σ(x → y). Thus σ is an IS-map on H and hence (H,σ) is an IS-map semihoop. □
Inspired by Ciungu’s state BL-algebras [11], He and Xin enlarged the language of residuated lattice by introducing a new operator, an internal state on residuated lattice in [18].
Definition 4.8
([18]). A state residuated lattice is a pair (A, σ) whereAis a residuated lattice andσ: A → Ais a mapping, called state operator, such that for anyx, y ∈ Athe following conditions are satisfied:
σ(0) = 0;
x → y = 1 impliesσ(x) → σ(y) = 1;
σ(x → y) = σ(x) → σ(x ∧ y);
σ(x ⊙ y) = σ(x) ⊙ σ(x → x ⊙ y);
σ(σ(x) ⊙ σ(y)) = σ(x) ⊙ σ(y);
σ(σ(x) → σ(y)) = σ(x) → σ(y);
σ(σ(x) ∨ σ(y)) = σ(x) ∨ σ(y);
σ(σ(x) ∧ σ(y)) = σ(x) ∧ σ(y).
Let (H; ⊙, →, 0, 1) be a bounded ⊔-semihoop. For any x, y ∈ H, we set x ⊔ y = ((x → y) → y) ∧ ((y → x) → x). Then (H, ∧, ⊔, →, ⊙, 0, 1) is a residuated lattice. (see [2, 3])
Theorem 4.9
LetHbe a bounded ⊔-semihoop andσ : H → Hbe a mapping onHpreserving → . Then the following conditions are equivalent:
σis an IS-map onH;
(H,σ) is a state residuated lattice.
Proof
(1) ⇒ (2) If H is a bounded ⊔-semihoop and σ : H → H is a mapping on H preserving →. Then σ(x → y) = σ(x → x ∧ y) = σ(x) → σ(x ∧ y). Moreover, by Proposition 3.9(5),(6), we have σ(σ(x) ⊔ σ(y)) = σ(((σ(x) → σ(y)) → σ(y)) ∧ ((σ(y) → σ(x)) → σ(x))) = σ(x) ⊔ σ(y). Therefore, (H,σ) is a state residuated lattice.
(2) ⇒ (1) Let (H,σ) be a state residuated lattice and σ preserving →. We only need to prove that (SM2) holds. Since ((x → y) → y) → y = x → y, so we have σ((x → y) → y) → σ(y) = σ(((x → y) → y) → y) = σ(x → y). Thus σ is an IS-map on H. □
A state operator σ on a BL-algebra L was introduced in Ciungu et al. (2011) as a mapping σ : L → L satisfying conditions (1) and (3)–(6) in Definition 4.8. We know that BL-algebras are special cases of residuated lattices satisfying the conditions of divisibility and prelinearity. Consequently, a BL-algebra satisfies the property: x ∨ y = ((x → y) → y) ∧ ((y → x) → x) for any x, y ∈ L. Therefore, in the case of BL-algebras, condition (4) implies the validity of (2) and conditions (5) and (6) imply the validity of (7) and (8). Hence the notion of a state residuated lattice essentially generalizes that of a state BL-algebra. Moreover, it has been proved (Ciungu et al. 2011) that a mapping σ : L → L is a state operator on an MV-algebra L (Flaminio and Montagna 2007, 2009) if and only if it is a state operator on L taken as a BL-algebra. From this point of view, the notion of a state residuated lattice also generalizes that of a state MV-algebra. Based on this, we have the following results [18].
Corollary 4.10
LetHbe a bounded basic hoop andσ : H → Hbe a mapping onHpreserving → . Then the following conditions are equivalent:
σis an IS-map onH;
(H,σ) is a state BL-algebra.
Proof
It follows from Proposition 2.8(1) and Theorem 4.9. □
Corollary 4.11
LetHbe a bounded Wajsberg hoop andσ : H → Hbe a mapping onH. Then the following conditions are equivalent:
σis an IS-map onHpreserving → ;
(H,σ) is a state MV-algebra.
Proof
It follows from Proposition 2.8(2) and Theorem 4.9. □
As we know, every hoop H is a BCK-meet semilattice in which a partial order over H can be defined as usual.
Definition 4.12
([5]). A state BCK-meet semilattice is a pair (A, σ) whereAis a BCK-meet semilattices andσ : A → Ais a mapping, called state operator, such that for anyx, y ∈ Athe following conditions are satisfied:
x → y = 1 impliesσ(x) → σ(y) = 1;
σ(x → y) = σ(x → y) → y) → σ(y);
σ(σ(x) → σ(y)) = σ(x) → σ(y);
σ(σ(x) ∧ σ(y)) = σ(x) ∧ σ(y).
Proposition 4.13
LetHbe a hoop andσ : H → Hbe an IS-map onH. Then the {→, ∧} subreduct of (H,σ) is a state BCK-meet semilattice.
Proof
It follows from Definition 3.1 and Definition 4.12. □
Since the class of equality algebra and the class of BCK-∧-semilattice with meet are categorically equivalent, then we have the following result.
Definition 4.14
([27]). A state equality algebra is a pair (A, σ) whereAis an equality algebra andσ : A → Ais a mapping, called state operator, such that for anyx, y ∈ Athe following conditions are satisfied:
x ≤ yimpliesσ(x) ≤ σ(y);
σ(x∼ x ∧ y) = σ(x∼ x ∧ y)∼ y)∼σ(y);
σ(σ(x) → σ(y)) = σ(x) → σ(y);
σ(σ(x) ∧ σ(y)) = σ(x) ∧ σ(y).
Proposition 4.15
LetHbe a hoop andσ : H → Hbe an IS-map onH. Then the {∼, ∧} subreduction of (H,σ) is a state equality algebra, wherex ∼ y = x → (x ∧ y).
Proof
It follows from Definition 4.14. □
5 State map filters in semihoops
In this section, we introduce state map filters of semihoops.
Definition 5.1
LetH1andH2be semihoops, σ : H1 → H2be a S-map fromH1toH2, Fbe a filter ofH1. Ifσ−1(σ(F)) ⊆ F, we callFto be a SM-filter of (H1, H2, σ).
Example 5.2
Consider the Example 3.4, one can easily check that the SM-filter of (H1, H2, σ) are {a1, b1, c1, 1}, {11} andH1.
Example 5.3
LetH1andH2be semihoops andσbe a S-map fromH1toH2. ThenKer(σ) = {x ∈ H1∣σ(x) = 12} is a SM-filter of (H1, H2, σ).
Proof
Let K = Ker(σ) and x, y ∈ K. Then σ(x) = 12 and σ(y) = 12. By Proposition 3.6(2) we have σ(x ⊙1y) ≥2σ(x) ⊙2σ(y) = 12 ⊙212 = 12. This means x ⊙1y ∈ K. Let x ∈ K and x ≤ y. Then 12 = σ(x) ≤ σ(y) and hence σ(y) = 12. This shows that y ∈ K. It follows that K is a filter of H1. Moreover let x ∈ σ−1σ(K). Then σ(x) ∈ σ(K) = {12} and hence σ(x) = 12. Therefore x ∈ K. This shows that σ−1σ(K) ⊆ K, or K is a SM-filter of (H1, σ). □
Definition 5.4
LetHbe a semihoop andσbe an IS-map onH.
A filterFofHis called state filter of (H,σ) ifx ∈ Fimpliesσ(x) ∈ Ffor allx ∈ H[31],
A filterFofHis called dual state filter of (H, σ) ifσ(x) ∈ Fimpliesx ∈ Ffor allx ∈ H,
A filterFofHis called strong state filter of (H, σ) if it is both a state filter and a dual state filter of (H, σ).
Proposition 5.5
LetHbe a semihoop andσbe an IS-map onH. Then each SM-filter ofHis a state filter onH.
Proof
Let x ∈ F. Then σ(x) ∈ σ (F). Therefore, σ(σ(x)) ∈ σ(F), that is σ(x) ∈ σ−1(σ(F)) ⊆ F. So σ(x) ∈ F. □
However, the converse of Proposition 5.5 is not true in general.
Example 5.6
LetH = {0, a, b, 1} with 0 ≤ a, b ≤ 1. Consider the operation → and ⊙ as follows:
ThenHis semihoop. Now, we defineσfollows: σ0 = a, σa = a, σb = 1, σ 1 = 1. One can easily check thatσis an IS-map onH. It is clear that {a, 1} is a state filter of (H, σ), but it is not a SM-filter of (H, σ).
Proposition 5.7
LetHbe a semihoop, σbe an IS-map onHandF ⊆ H. Then the following are equivalent:
Fis a SM-filter ofH,
Fis a strong state filter onH.
Proof
(1) ⇒ (2) Let F be a SM-filter of (H, σ). By Proposition 5.5 we only need to prove that σ(x) ∈ F implies x ∈ F. Let σ(x) ∈ F. Then σ(x) = σ(σ(x)) ∈ σ(F). Hence there is t ∈ F such that σ(x) = σ(t). It follows from (1) that x ∈ σ−1(σ(t)) ⊆ σ−1(σ(F)) ⊆ F. That is x ∈ F.
(2)⇒ (1) Assume that F is a strong state filter on H. For x ∈ σ−1(σ(F)), we have σ(x) ∈ σ(F). Since F is strong filter of H, we get x ∈ F and hence σ−1(σ(F)) ⊆ F. □
Let H1 and H2 be two semihoops and σ be a S-map from H1 to H2. For any nonempty set X of H1, we denote by 〈X〉σ the SM-filter of (H1, σ) generated by X, that is, 〈X〉σ is the smallest SM-filter of (H1, σ) containing X.
Let H be be a semihoop and σ be an IS-map on H. For any nonempty set X of H, we denote by 〈X〉S (〈X〉DS) the state filter (the dual state filter) of (H, σ) generated by X, that is, 〈X〉S (〈X〉DS) is the smallest state filter (the dual state filter) of (H, σ) containing X.
Denote (X)DS = {x ∈ H ∣ σ(x) ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xm ⊙ σ(xm), xi ∈ X}. In the following we discuss the structures of 〈X〉S, 〈X〉DS and 〈X〉σ.
Theorem 5.8
LetHbe a semihoop, σbe an IS-map onHandX ⊆ H. Then
〈X〉S = {x ∈ H ∣ x ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn), xi ∈ X, m ∈ N},
(X)DSis a dual state filter of (H, σ) containingX, and hence 〈X〉DS ⊆ (X)DS,
〈X〉σ = 〈X〉S ∪ (X)DS.
Proof
The proof is similar to that of He et al [30].(Theorem 4.13).
Let x, y ∈ (X)DS. Then σ(x) ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) for some xi ∈ X, n ∈ N and σ(y) ≥ y1 ⊙ σ(y1) ⊙ ⋯ ⊙ ym ⊙ σ(ym) for some yj ∈ X, m ∈ N. Hence σ(x ⊙ y) ≥ σ(x) ⊙ σ(y) ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) ⊙ y1 ⊙ σ(y1) ⊙ ⋯ ⊙ ym ⊙ σ(ym). So x ⊙ y ∈ (X)DS. Assume x ≤ y and x ∈ (X)DS. Then σ(y) ≥ σ(x) ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) for some xi ∈ X. It follows that y ∈ (X)DS. This shows that (X)DS is a filter of H. Moreover, let σ(x) ∈ (X)DS. Then σ(σ(x)) ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) for some xi ∈ X and hence σ(x) ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) for some xi ∈ X. This shows that x ∈ (X)DS and hence (X)DS is a dual state filter of (H, σ). Clearly X ⊆ (X)DS.
Denote B = 〈X〉S ∪ (X)DS. Let x, y ∈ B. If x, y ∈ 〈X〉S, then x ⊙ y ∈ 〈X〉S ⊆ B by (1). If x, y ∈ (X)DS, then x ⊙ y ∈ (X)DS ⊆ B by (2). Let x ∈ 〈X〉S and y ∈ (X)DS. Then σ(x) ∈ 〈X〉S since 〈X〉S is a state filter of (H, σ) by (1). Hence σ(x) ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) for some xi ∈ X and σ(y) ≥ y1 ⊙ σ(y1) ⊙ ⋯ ⊙ ym ⊙ σ(ym) for some yj ∈ X and hence σ(x ⊙ y) ≥ σ(x) ⊙ σ(y) ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) ⊙ y1 ⊙ σ(y1) ⊙ ⋯ ⊙ ym ⊙ σ(ym) for some xi,yj ∈ X. It follows that x ⊙ y ∈ (X)DS ⊆ B. Combining the above arguments we get that B is closed on ⊙. It is easy to check that if x ∈ B and x ≤ y then y ∈ B. Clearly X ⊆ B. Now we prove that B is a state filter. Let x ∈ B. If x ∈ 〈X〉S, then σ(x) ∈ 〈X〉S since 〈X〉S is a state filter. If x ∈ (X)DS, then σ(x) ∈ 〈X〉S ⊆ B. So B is a state filter. Moreover we prove that B is a dual state filter. Let σ(x) ∈ B. If σ(x) ∈ 〈X〉S, then x ∈ (X)DS ⊆ B. Let σ(x) ∈ (X)DS. Then x ∈ (X)DS since (X)DS is a dual state filter by (2). This shows that B a dual state filter. By Proposition 5.7, B a SM-filter. Let F be a SM-filter of (H, σ) containing X and x ∈ B. If x ∈ 〈X〉S, then x ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) for xi ∈ X. Since X ⊆ F and F is a SM-filter of (H, σ), we have x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) ∈ F. So x ∈ F. If x ∈ (X)DS, then σ(x) ∈ 〈X〉S by (1). If σ(x) ≥ x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) for xi ∈ X. Since F is a SM-filter of (H, σ) containing X, then x1 ⊙ σ(x1) ⊙ ⋯ ⊙ xn ⊙ σ(xn) ∈ F and hence σ(x) ∈ F. Note that F is also a dual state filter, we have x ∈ F. Combining the above arguments we get B ⊆ F. It follows that B = 〈X〉σ. □
Proposition 5.9
LetHbe a semihoop, σbe an IS-map andFbe state filters of (H, σ) anda ∉ F. Then
〈a〉σ = {x ∈ H ∣ x ≥ (a ⊙ σ(a))n, n ≥ 1} ∪ {x ∈ H ∣ σ(x) ≥ (a ⊙ σ(a))n, n ≥ 1},
〈F, {a}〉σ = {x ∈ H ∣ x ≥ f ⊙ (a ⊙ σ(a))n, f ∈ F, n ≥ 1} ∪ {x ∈ H ∣ σ(x) ≥ f ⊙ (a ⊙ σ(a))n, f ∈ F, n ≥ 1},
ifa ≤ b, then 〈b〉σ ⊆ 〈a〉σ,
〈a ⊙ a〉σ = 〈a〉σ,
〈σ(a)〉σ = 〈a〉σ,
〈a ⊙ σ(a)〉σ = 〈a〉σ,
ifHis a ⊔-semihoop, then 〈a〉σ ∩ 〈b〉σ = 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ.
Proof
The proofs of (1)–(4) are obvious.
(5) Let x ∈ 〈σ(a)〉σ. Then x ≥ (σ(a) ⊙ σ2(a))n = (σ(a))2n ≥ (a ⊙ σ(a))2n or σ(x) ≥ (a ⊙ σ(a))2n and hence x ∈ 〈a〉σ. Conversely, let x ∈ 〈a〉σ. Then x ≥ (a ⊙ σ(a))n or σ(x) ≥ (a ⊙ σ(a))n. Hence σ(x) ≥ (σ(a) ⊙ σ2(a))n. It follows that σ(x) ∈ 〈σ(a)〉σ. Since 〈σ(a)〉σ is a dual state filter we have x ∈ 〈σ(a)〉σ.
(6) Since a ⊙ σ(a) ≤ a we have 〈a〉σ ⊆ 〈a ⊙ σ(a)〉σ by (3). Conversely, by use of (3), (4) and (5) we have 〈a ⊙ σ(a)〉σ = 〈σ(a ⊙ σ(a))〉σ ⊆ 〈σ(a) ⊙ σ2(a)〉σ = 〈σ(a) ⊙ σ(a)〉σ = 〈 σ(a)〉σ = 〈a〉σ.
(7) Suppose that H is a ⊔-semihoop. From a ⊙ σ(a) ≤ (a ⊙ σ(a)) ⊔ (b ⊙ σ(b)), we have that 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ ⊆ 〈a ⊙ σ(a)〉σ = 〈a〉σ. Similarly, we can prove 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ ⊆ 〈b〉σ. Thus, 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ ⊆ 〈a〉σ ∩ 〈b〉σ. Conversely, let x ∈ 〈a〉σ ∩ 〈b〉σ. Then there exist n, m, s, t ≥ 1, such that x ≥ (a ⊙ σ(a))n or σ(x) ≥ (a ⊙ σ(a))n, and x ≥ (b ⊙ σ(b))n or σ(x) ≥ (b ⊙ σ(b))n. To complete the proof, we divide four cases as following:
Let x ≥ (a ⊙ σ(a))n and x ≥ (b ⊙ σ(b))n. Then x ≥ (a ⊙ σ(a))n ⊔ (b ⊙ σ(b))n ≥ ((a ⊙ σ(a)) ⊔ (b ⊙ σ(b)))ns ≥ (((a ⊙ σ(a)) ⊔ (b ⊙ σ(b))) ⊙ σ((a ⊙ σ(a)) ⊔ (b ⊙ σ(b))))ns by Proposition 2.6(3). We deduce that x ∈ 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ.
Let σ(x) ≥ (a ⊙ σ(a))n and σ(x) ≥ (b ⊙ σ(b))n. Similarly to (a) we can get σ(x) ∈ 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ. Since 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ is a dual state filter we have x ∈ 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ.
Let x ≥ (a ⊙ σ(a))n and σ(x) ≥ (b ⊙ σ(b))n. Then σ(x) ≥ (σ(a) ⊙ σ(a))n ≥ (a ⊙ σ(a))2n and σ(x) ≥ (b ⊙ σ(b))n. Thus σ(x) ≥ (a ⊙ σ(a))2n ⊔ (b ⊙ σ(b))n ≥ ((a ⊙ σ(a)) ⊔ (b ⊙ σ(b)))2nt ≥ (((a ⊙ σ(a)) ⊔ (b ⊙ σ(b))) ⊙ σ((a ⊙ σ(a)) ⊔ (b ⊙ σ(b))))2nt. It follows that σ(x) ∈ 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ. Since 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ is a dual state filter we have x ∈ 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ.
Let σ(x) ≥ (a ⊙ σ(a))n and x ≥ (b ⊙ σ(b))n. Similarly to the case (c) we can get x ∈ 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ.
Combining the above arguments we can prove 〈a〉σ ∩ 〈b〉σ ⊆ 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ. Therefore 〈a〉σ ∩ 〈b〉σ = 〈(a ⊙ σ(a)) ⊔ (b ⊙ σ(b))〉σ. □
Definition 5.10
LetH1andH2be two semihoops andσbe a S-map fromH1toH2. A proper SM-filterFof (H1, H2, σ) is called a prime SM-filter of (H1, H2, σ), if for all SM-filtersF1, F2of (H1, σ) such thatF1 ∩ F2 ⊆ F, thenF1 ⊆ ForF2 ⊆ F.
Let H1 and H2 be two semihoops and σ be a S-map from H1 to H2. We denote by PSMF[H] the set of all prime SM-filters of (H1, σ).
Example 5.11
Consider the Example 3.4, one can check thatF = {a1, b1, c1, 11} is a prime SM-filter of (H1, σ).
Theorem 5.12
LetHbe a ⊔-semihoop, σbe an IS-map andFbe a proper SM-filter of (H, σ). Then the following are equivalent:
Fis a prime SM-filter of (H, σ),
if ((x ⊙ σ(x)) ⊔ (y ⊙ σ(y))) ⊙ σ((x ⊙ σ(x)) ⊔ (y ⊙ σ(y))) ∈ Ffor somex, y ∈ H, thenx ∈ Fory ∈ F.
Proof
(1) ⇒ (2) Let ((x ⊙ σ(x)) ⊔ (y ⊙ σ(y))) ⊙ σ((x ⊙ σ(x)) ⊔ (y ⊙ σ(y))) ∈ F for some x, y ∈ H. Then 〈x〉σ ∩ 〈y〉σ = 〈(x ⊙ σ(x)) ⊔ (y ⊙ σ(y))〉σ ⊆ F. Since F is a prime SM-filter of (H, σ), then 〈x〉σ ⊆ F or 〈y〉σ ⊆ F. Therefore, x ∈ F or y ∈ F.
(2) ⇒ (1) Suppose that F1, F2 ∈ SMF[L] such that F1 ∩ F2 ⊆ F and F1 ⊈ F and F2 ⊈ F. Then there exist x ∈ F1 and y ∈ F2 such that x, y ∉ F. Since F1, F2 are SM-filter of (H, σ), then x ⊙ σ(x) ∈ F1 and y ⊙ σ(y) ∈ F2. From x ⊙ σ(x), y ⊙ σ(y) ≤ (x ⊙ σ(x)) ⊔ (y ⊙ σ(y)), we obtain (x ⊙ σ(x)) ⊔ (y ⊙ σ(y)) ∈ F1 ∩ F2 ⊆ F and hence ((x ⊙ σ(x)) ⊔ (y ⊙ σ(y))) ⊙ σ((x ⊙ σ(x)) ⊔ (y ⊙ σ(y))) ∈ F1 ∩ F2 ⊆ F. By (2), we get that x ∈ F or y ∈ F, which is a contradiction. Therefore, F is a prime SM-filter of (H, σ). □
Definition 5.13
LetH1andH2be two semihoops andσbe a S-map fromH1toH2. A proper SM-filter of (H1, H2, σ) is called a maximal SM-filter if it not strictly contained in any proper SM-filter of (H1, H2, σ).
Example 5.14
LetH1andH2be two semihoops andσbe a S-map fromH1toH2in Example 3.4. One can easily check thatF = {a1, b1, c1, 11} is a maximal SM-filter of (H1, H2, σ).
Proposition 5.15
LetHbe a bounded ⊔-semihoop, σbe an IS-map andFbe a proper SM-filter of (H, σ). Then the following are equivalent:
Fis a maximal SM-filter of (H, σ),
for anya ∉ F, there is an integern ≥ 1 such that (σ(a)n)∗ ∈ F.
Proof
(1) ⇒ (2) Suppose that F is a maximal SM-filter of (H, σ), and let a ∉ F. Then 〈F,a〉σ = H, which implies 0 ∈ 〈F, a〉σ. Then there is f ∈ F and an integer n ≥ 1 such that 0 = f ⊙ (a ⊙ σ(a))n. So we have 0 = σ(0) ≥ σ(f) ⊙ σ(a)2n. Therefore, σ(f) ≥ (σ(a)2n)∗. Thus, (σ(a)2n)∗ ∈ F.
(2) ⇒ (1) Let a satisfy the condition. Since (σ(a)n)∗ ⊙ (a ⊙ σ(a))n ≤ (σ(a)n)∗ ⊙ (σ(a))n = 0 and (σ(a)n)∗ ∈ F, we obtain 0 ∈ 〈F,a〉σ, that is, 〈F, a〉σ = H. Therefore, F is a maximal SM-filter of (H, σ). □
Proposition 5.16
LetH1andH2be two bounded semihoops andσbe a S-map fromH1toH2.
IfF2is filter ofσ(H1), thenσ−1(F2) is a SM-filter of (H1, H2, σ).
Ifσis an IS-map onHandFis a maximal filter ofσH, thenσ−1(F) is a maximal SM-filter ofH.
Proof
Suppose that F2 is a filter of σ(H1). If x, y ∈ σ−1(F2), then σ(x),σ(y) ∈ F2. It follows that σ(x) ⊙ σ(y) ∈ F2. Since σ(x ⊙ y) ≥ σ(x) ⊙ σ(y) and σ(x ⊙ y) ∈ σ(H1), we have σ(x ⊙ y) ∈ F2, that is, x ⊙ y ∈ σ−1(F2). Let x, y ∈ H1 such that x ∈ σ−1(F2) and x ≤ y. Then σ(x) ≤ σ(y). Since σ(x) ∈ F and σ(y) ∈ σ(H1), we can obtain that σ(y) ∈ F2, that is, y ∈ σ−1(F2). Thus, σ−1(F2) is a filter of H1. Note that σ(σ−1(x) = x for any x ∈ H1. Hence σ−1(σ(σ−1(F)) = σ−1(F). Thus σ−1(F2) is a SM-filter of H1.
Now, suppose that F is a maximal filter of σ(H). Let a ∉ σ−1(F), thus σ(a) ∉ F. By the maximality of F, there is an integer n ≥ 1 such that (σ(a)n)∗ ∈ F ⊆ σ(H). Since σ ((σ(a)n)∗) = (σ(a)n)∗ ∈ F, we have (σ(a)n)∗ ∈ σ−1(F). Therefore, σ−1(F) is a maximal SM-filter of H. □
Proposition 5.17
LetHbe a bounded semihoop andσbe an IS-map onHpreserving ⊙.
IfFis a SM-filter of (H, σ), thenσ(F) is a SM-filter of (σ(H),σ).
IfFis a maximal SM-filter of (H, σ), thenσ(F) is a maximal SM-filter of (σ(H),σ).
Proof
Let σ(x),σ(y) ∈ σ(F), then x, y ∈ σ−1σ(F) ⊆ F. Since F is a filter, thus x ⊙ y ∈ F and hence σ(x) ⊙ σ(y) = σ(x ⊙ y) ∈ σ(F). Let σ(x), σ(y) ∈ σ(H) such that σ(x) ∈ σ(F) and σ(x) ≤ σ(y). Since σ(x) ∈ σ(F) we have x ∈ σ−1σ(F) ⊆ F. So x ∈ F. By Proposition 5.7 we have σ(x) ∈ F. Since σ(x) ≤ σ(y) we get σ(y) ∈ F. Using Proposition 5.7 again we obtain y ∈ F, and so σ(y) ∈ σ(F). Thus, σ(F) is a filter of σ(H). Now let x ∈ σ(F). Then x = σ(t) for some t ∈ F and hence σ(x) = σ2(t) = σ(t) = x ∈ σ(F). It follows that σ(F) is a state filter of (H, σ). Let x ∈ σ(H) and σ(x) ∈ σ(F). Then x = σ(t) for some t ∈ H. Hence x = σ(t) = σ2(t) = σ(σ(t)) = σ(x) ∈ σ(F). This means that σ(F) is a dual state filter of (σ(H),σ). Therefore σ(H) is a strong state filter of (σ(H),σ). By Proposition 5.7 we have that σ(F) is a SM-filter of (σ(H),σ).
Now, let F be maximal and σ(a) ∉ σ(F). Then a ∉ F, and there is an integer n ≥ 1 such that (σ(a)n)∗ ∈ F and hence σ ((σ(a)n)∗) = (σ(a)n)∗ ∈ σ(F). Since σ(σ(a)n) ≥ (σσ(a))n = (σ(a))n, we have (σ(a)n)∗ ≥ σ ((σ(a)n)∗). Hence (σ(a)n)∗ ∈ σ(F). Therefore, σ(F) is a maximal SM-filter of (σ(H),σ). □
Corollary 5.18
LetHbe a bounded semihoop andσbe an IS-map onH.
IfFis a (maximal) filter ofσ(H), thenσ−1(F) is a strong state (maximal)filter of (H, σ).
Ifσis preserving ⊙ andFis a strong state (maximal) filter of (H, σ), thenσ(F) is a strong state (maximal) filter of (σ(H),σ).
Proof
It follows from Proposition 5.7 and 5.16.
It follows from Proposition 5.7 and 5.17. □
Now, we introduce two kinds of semihoops and give some characterizations of them.
Definition 5.19
LetHbe a semihoop andσ : H → Hbe an IS-map onH. If (H, σ) has exactly one maximal SM-filter, we call (H, σ) to be state local.
Theorem 5.20
LetHbe a semihoop andσbe an IS-map onH. Then the following are equivalent:
(H, σ) is state local;
σ(H) is local.
Proof
(1) ⇒ (2) Let F be the only maximal SM-filter of (H, σ). We prove that σ(F) is the only maximal filter of σ(H). First, σ(F) is a proper filter of σ(H). In fact, if σ(F) = σ(H), then 0 ∈ σ(F), which implies 0 ∈ F, a contradiction. Now, let G be a filter of σ(H), G ≠ σ(H) and let x ∈ G. It follows from Corollary 5.18(1) that σ−1(G) is a SM-filter of (H, σ). Thus σ−1(G) is a proper SM-filter of (H, σ). Moreover, if σ−1(G) = H, then 0 ∈ σ−1(G), so 0 ∈ G, a contradiction. It follows that σ−1(G) ⊆ F. if x = σ(x) ∈ G, then x ∈ σ−1(G), it follows that x ∈ F. But x = σ(x), so x ∈ σ(H). Thus G ⊆ σ(F). Hence σ(G) is the only maximal filter of σ(H). Therefore, σ(H) is local.
(2) ⇒ (1) Suppose that G is the only maximal filter of σ(H). By Corollary 5.18(1), we have that σ−1(G) is a maximal SM-filter of (H, σ). We will prove that σ−1(G) is the only maximal SM-filter of (H, σ). Let G be a SM-filter of (H, σ), F ≠ L. Then σ(F) is a proper filter of σ(H), so σ(F) ⊆ G. Let x ∈ F then σ(x) ∈ σ(F) ⊆ G. Thus, x ∈ σ−1(G). It follows that F ⊆ σ−1(G). Therefore, (H, σ) is state local. □
Definition 5.21
LetHa be semihoop andσ : H → Hbe an IS-map onH. If (H, σ) has two SM-filters {1} andH, we call (H, σ) to be simple.
Theorem 5.22
LetHa be semihoop andσ : H → Hbe an IS-map onHsuch thatσpreserving ⊙ . Then the following are equivalent:
(H, σ) is simple;
σ(H) is simple andKer(σ) = {1}.
Proof
(1) ⇒ (2) Let F be a filter of σ(H) and F ≠ {1}. It follows from Corollary 5.18(1) that σ−1F is a SM-fiter of (H, σ). Since (H, σ) is state simple, we have that σ−1(F) = {1} or σ−1(F) = H. Notice that F ⊆ σ−1F (if x ∈ F, then σx = x, that is, x ∈ σ−1F, we obtain that σ−1F ≠ {1}. Thus, σ−1F = H. Then 0 ∈ σ−1F, that is, 0 = σ 0 ∈ F. So we obtain that F = σH. Therefore, σH is simple.
By Example 5.3 we have Ker(σ) is a SM-filter of (H, σ) and Ker(σ) ≠ H. It follows that Ker(σ) = {1}.
(2) ⇒ (1) Let F be a SM-filter of (H, σ) and F ≠ {1}. By Corollary 5.18(2), we obtain that σF is a filter of σH. Since σH is simple, we obtain that σF = {1} or σF = σx. Since Ker(σ) = {1}, we have F ≠ {1}. Thus, σF = σx. Then 0 ∈ σF, that is, 0 ∈ F. It follows that F = H. Therefore (H, σ) is state simple. □
6 Conclusion
We observed that the states and state operators on MV-algebras, BL-algebras and BCK-algebras, are maps from an algebra X to [0, 1] and X to X, respectively. From the viewpoint of universal algebras, it is meaningful to study a state map from an algebra X to anther algebra Y. Indeed, if Y = [0, 1], a state can be seen as a state map from X to [0, 1], and if X = Y, a state operator can also be seen as a state map from X → X. Based on this idea, we introduce a notion of state maps on semihoops by extending the codomain of a state (or internal state) to a more general algebraic structure, that is, from a semihoop H1 to an arbitrary semihoop H2. We give a type of special state map from a semihoop H to H, called internal state map (or IS-map), which is a generalization of internal states (or state operators) on some types of semihoops. We try to give a unified model of states and internal states on some important logic algebras. By the arguments in the paper we can see that state maps on an semihoops are generalization of internal states on BL-algebras, MV-algebras, equality algebras and BCK-algebras. In the next work, it is worthy to portray some types of logic algebras and corresponding logics by use of state maps.
Acknowledgement
This research is partially supported by a grant of National Natural Science Foundation of China (11571281, 61602359), China Postdoctoral Science Foundation (2015M582618), China 111 Project (B16037).
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- On the boundedness of square function generated by the Bessel differential operator in weighted Lebesque Lp,α spaces
- On the different kinds of separability of the space of Borel functions
- Curves in the Lorentz-Minkowski plane: elasticae, catenaries and grim-reapers
- Functional analysis method for the M/G/1 queueing model with single working vacation
- Existence of asymptotically periodic solutions for semilinear evolution equations with nonlocal initial conditions
- The existence of solutions to certain type of nonlinear difference-differential equations
- Domination in 4-regular Knödel graphs
- Stepanov-like pseudo almost periodic functions on time scales and applications to dynamic equations with delay
- Algebras of right ample semigroups
- Random attractors for stochastic retarded reaction-diffusion equations with multiplicative white noise on unbounded domains
- Nontrivial periodic solutions to delay difference equations via Morse theory
- A note on the three-way generalization of the Jordan canonical form
- On some varieties of ai-semirings satisfying xp+1 ≈ x
- Abstract-valued Orlicz spaces of range-varying type
- On the recursive properties of one kind hybrid power mean involving two-term exponential sums and Gauss sums
- Arithmetic of generalized Dedekind sums and their modularity
- Multipreconditioned GMRES for simulating stochastic automata networks
- Regularization and error estimates for an inverse heat problem under the conformable derivative
- Transitivity of the εm-relation on (m-idempotent) hyperrings
- Learning Bayesian networks based on bi-velocity discrete particle swarm optimization with mutation operator
- Simultaneous prediction in the generalized linear model
- Two asymptotic expansions for gamma function developed by Windschitl’s formula
- State maps on semihoops
- 𝓜𝓝-convergence and lim-inf𝓜-convergence in partially ordered sets
- Stability and convergence of a local discontinuous Galerkin finite element method for the general Lax equation
- New topology in residuated lattices
- Optimality and duality in set-valued optimization utilizing limit sets
- An improved Schwarz Lemma at the boundary
- Initial layer problem of the Boussinesq system for Rayleigh-Bénard convection with infinite Prandtl number limit
- Toeplitz matrices whose elements are coefficients of Bazilevič functions
- Epi-mild normality
- Nonlinear elastic beam problems with the parameter near resonance
- Orlicz difference bodies
- The Picard group of Brauer-Severi varieties
- Galoisian and qualitative approaches to linear Polyanin-Zaitsev vector fields
- Weak group inverse
- Infinite growth of solutions of second order complex differential equation
- Semi-Hurewicz-Type properties in ditopological texture spaces
- Chaos and bifurcation in the controlled chaotic system
- Translatability and translatable semigroups
- Sharp bounds for partition dimension of generalized Möbius ladders
- Uniqueness theorems for L-functions in the extended Selberg class
- An effective algorithm for globally solving quadratic programs using parametric linearization technique
- Bounds of Strong EMT Strength for certain Subdivision of Star and Bistar
- On categorical aspects of S -quantales
- On the algebraicity of coefficients of half-integral weight mock modular forms
- Dunkl analogue of Szász-mirakjan operators of blending type
- Majorization, “useful” Csiszár divergence and “useful” Zipf-Mandelbrot law
- Global stability of a distributed delayed viral model with general incidence rate
- Analyzing a generalized pest-natural enemy model with nonlinear impulsive control
- Boundary value problems of a discrete generalized beam equation via variational methods
- Common fixed point theorem of six self-mappings in Menger spaces using (CLRST) property
- Periodic and subharmonic solutions for a 2nth-order p-Laplacian difference equation containing both advances and retardations
- Spectrum of free-form Sudoku graphs
- Regularity of fuzzy convergence spaces
- The well-posedness of solution to a compressible non-Newtonian fluid with self-gravitational potential
- On further refinements for Young inequalities
- Pretty good state transfer on 1-sum of star graphs
- On a conjecture about generalized Q-recurrence
- Univariate approximating schemes and their non-tensor product generalization
- Multi-term fractional differential equations with nonlocal boundary conditions
- Homoclinic and heteroclinic solutions to a hepatitis C evolution model
- Regularity of one-sided multilinear fractional maximal functions
- Galois connections between sets of paths and closure operators in simple graphs
- KGSA: A Gravitational Search Algorithm for Multimodal Optimization based on K-Means Niching Technique and a Novel Elitism Strategy
- θ-type Calderón-Zygmund Operators and Commutators in Variable Exponents Herz space
- An integral that counts the zeros of a function
- On rough sets induced by fuzzy relations approach in semigroups
- Computational uncertainty quantification for random non-autonomous second order linear differential equations via adapted gPC: a comparative case study with random Fröbenius method and Monte Carlo simulation
- The fourth order strongly noncanonical operators
- Topical Issue on Cyber-security Mathematics
- Review of Cryptographic Schemes applied to Remote Electronic Voting systems: remaining challenges and the upcoming post-quantum paradigm
- Linearity in decimation-based generators: an improved cryptanalysis on the shrinking generator
- On dynamic network security: A random decentering algorithm on graphs