* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Transformasi Linear dan Isomorfisma pada Aljabar Max
Matrix multiplication wikipedia , lookup
CayleyβHamilton theorem wikipedia , lookup
Singular-value decomposition wikipedia , lookup
Matrix calculus wikipedia , lookup
Euclidean vector wikipedia , lookup
Eigenvalues and eigenvectors wikipedia , lookup
Exterior algebra wikipedia , lookup
Vector space wikipedia , lookup
Four-vector wikipedia , lookup
Transformasi Linear dan Isomorfisma pada Aljabar Max-Plus (Linear Transformation and Isomorphism in Max-plus Algebra) As in conventional linear algebra we can define the linear dependence and independence of vectors in the max-plus sense. The following can be found in [1], [2], [3] and [4]. Recall that the max-plus algebra is in idempotent semi-ring. In order to define linear dependence, independence and bases we need the definition of a semi-module. A semi-module is essentially a linear space over semi-ring. Semimodules and subsemimodules are analogous to modules and submodules over rings [5]. Definition 1. A set π β βππππ₯ is a commutative idempotent semi-module over βπππ₯ if it closed under β and scalar multiplication; π’ β π£ β π and πΌβ¨π’ β π for all πΌ β βπππ₯ and π’, π£ β π. Definition 2. A finitely generated semi-module π β βππππ₯ is the set of all linear combinations of a finite set {π’1 , π’2 , β¦ , π’π } of vectors in βππππ₯ : π = {β¨ππ=1 πΌπ β¨π’π |πΌ1 , πΌ2 , β¦ , πΌπ β βπππ₯ }. Definition 3. A element π₯ can be written as a finite linear combination of elements of πΉ β π if π₯ = β¨πβπΉ ππ β¨π, for some ππ β βπππ₯ such that ππ β π for all but finitely many π β πΉ. Linear independence and dependence in the max-plus sense are not completely analogous to the conventional definition. There are different interpretations of linear independence and dependence. We will consider the definitions of linear dependence and linear independence due to Gondran and Minoux. Definition 4. A set of set π vectors {π£1 , π£2 , β¦ , π£π } β βππππ₯ is linearly dependent if the set {1, 2, β¦ , π} can be partitioned into disjoint subset πΌ and πΎ such that for π β πΌ βͺ πΎ there exist πΌπ β βπππ₯ not all equal to π and β¨πβπΌ πΌπ β¨π£π = β¨πβπΎ πΌπ β¨π£π . Definition 5. A set of set π vectors {π£1 , π£2 , β¦ , π£π } β βππππ₯ is linearly independent if for all disjoint subset πΌ and πΎ of the set {1, 2, β¦ , π} can be partitioned into disjoint subset πΌ and πΎ such that for π β πΌ βͺ πΎ and all πΌπ β βπππ₯ we have β¨πβπΌ πΌπ β¨π£π β β¨πβπΎ πΌπ β¨π£π unless πΌπ = π for all π β πΌ βͺ πΎ. In other words linearly independent simply means not linearly dependent. Definition 6. A subset πΉ of a semi-module π over βπππ₯ spans π or is a spanning family of βπππ₯ if every element π₯ β π can be written as a finite linear combination of the elements of πΉ. π Definition 7. A family of vectors {π’π }π=1 is a basis of semi-module π if it is a minimal spanning family. A. Linear Transformation Definition 1. If π: π β π is a function from a semi-module π to a semi-module π, then π is called a linear transformation from π to π if the following two properties hold for all vectors π and π in π and for all scalars π: (a) π(πβ¨π’) = πβ¨π(π’) (b) π(π’ β π£) = π(π’) β π(π£) [Homogeneity Property] [Additivity Property] In the special case where π = π, the linear transformation π is called linear operator on the semi-module π. Theorem 1. If π: π β π is a linear transformation, then: π(π) = π. Proof. Let π’ be any vector in π. Since ππ’ = π, it follows from the homogeneity property in Definition 1 that π(π) = π(πβ¨π’) = πβ¨π(π’) = π. Theorem 2. Let π: π β π is a linear transformation, where π is finite dimensional. If π = {π£1 , π£2 , β¦ , π£π } is a basis for π. Then the image of any vector π£ in π can be expressed as π(π£) = (π1 β¨π(π£1 )) β (π2 β¨π(π£2 )) β β¦ β (ππ β¨π(π£π )) Where π1 , π2 , β¦ , ππ are the coefficients required to express π£ as a linear combination of the vectors in π. Proof. Expres π£ = (π1 β¨π£1 ) β (π2 β¨π£2 ) β β¦ β (ππ β¨π£π ) and use the linearity of π. Definition 2. If π: π β π is a linear transformation, then the set of vectors in π that π maps into π is called kernel of π and is denoted by ker(π). The set of all vectors in π that are image under π of at least one vector in π is called the range of π and is denoted by π (π). Theorem 3. If π: π β π is a linear transformation, then: (a) The kernel of π is a subsemi-module of π. (b) The range of π is a subsemi-module of π. Proof (a). We must show that ker(π) contains at least one vector and is closed under addition and scalar multiplication. By Theorem 1 the vector πΊ is in ker(π), so the kernel contains at least one vector. Let π£1 and π£2 be vectors in ker(π), and let π be any scalar. Then π(π£1 β π£2 ) = π(π£1 ) β π(π£2 ) = πΊ β πΊ = πΊ so π£1 β π£2 is in ker(π). Also, π(πβ¨π£1 ) = πβ¨π(π£1 ) = πβ¨πΊ = πΊ so ππ’ is in ker(π). (b). We must show that π (π) contains at least one vector and is closed under addition and scalar multiplication. By Theorem 1 the vector πΊ is in π (π), so the range contains at least one vector. Let π€1 and π€2 be vectors in π (π), and let π be any scalar, then there exist vector a and b in π for which π(π) = π€1 β¨π€2 and π(π) = πβ¨π€1 but the fact π€1 and π€2 are vectors in π (π) tells us that there exist vectors π£1 and π£2 in π such that π(π£1 ) = π€1 and π(π£2 ) = π€2 The following computations complete the proof by showing that the vectors π = π£1 β¨π£2 and π = kβ¨π£1 satisfy the equation in π(π) = π(π£1 β π£2 ) = π(π£1 ) β π(π£2 ) = π€1 β¨π€2 π(π) = π(πβ¨π£1 ) = πβ¨π€1 . Theorem 5. If π: π β π is a linear transformation, then: ker(π) = {πΊ}. Proof. By the idempotent property of β¨, so βπππ₯ doesnβt have invers element for β¨. It guarantees that there is no vector π£ β πΊ in π such that π£ β ker(π). Definition 3. Let π: π β π is a linear transformation. If the range of π is finite-dimensional, then its dimension is called the rank of π; and if the kernel of π is finite- dimensional, then its dimension is called the nullity of π. The rank of π is denoted by ππππ(π) and the nullity of π by ππ’ππππ‘π¦(π). Theorem 5. If π: π β π is a linear transformation from an n-dimensional semi-module π to a semi-module π, then: ππππ(π) β¨ ππ’ππππ‘π¦(π) = π. Proof. B. Isomorphism Definition 1. If π: π β π is a linear transformation from an n-dimensional semi-module π to a semi-module π, then π is said to be one-to-one if π maps distinct vectors in π into distinct vectors in π. Definition 2. If π: π β π is a linear transformation from an n-dimensional semi-module π to a semi-module π, then π is said to be onto (or onto π) if every vectors in π is the image of at least one vectors in π. Theorem 1. If π: π β π is a linear transformation and π is one-to-one, then ker(π) = {πΊ}. Proof. Since π is linear, we know that π(π) = π by Theorem 1. Since π is one-toone, there can be no other vectors in π that map into π, so ker(π) = {πΊ}. Theorem 2. If π is a finite-dimensional semi-module, and if π: π β π is a linear operator, then the following statements are equivalent. (a) π is one-to-one (b) ker(π) = {πΊ}. (c) π is onto. Definition 3. If π: π β π is a linear transformation is both one-to-one and onto, then π is said to be an isomorphism, and the semi-module π and π are said to be isomorphic. Theorem 3. Every real π-dimensional semi-module is isomorphic to βππππ₯ . C. Matrices for General Linear Transformation Recall matrices for general linear transformation in conventional sense. Matrices for general transformation in max-plus case is like as in conventional case. Definition 4. π: π β π is a linear transformation. Suppose further that π΅ is a basis for π, that π΅β² is a basis for π. The matrix for π relative to the bases π΅ and π΅β² and will denote by π΄ = [π]π΅β² .π΅ = [[π(π’1 )]π΅β² | [π(π’2 )]π΅β² | β¦ | [π(π’π )]π΅β² ] So, for every vectors π£ in π then π(π£) = π΄π£. Theorem . π: π β π is a linear transformation and suppose π΄ is matrix relative to π. Then the following is equivalent. (a) π is surjective (b) π΄ is invertible (c) π is injective. Theorem . Linear Transformation and Isomorphism in Max-plus Algebra ABSTRACT Max-plus algebra is one of the concepts in algebraic structures. Max-plus algebra βπππ₯ is the set β βͺ {ββ} with max and + as the two binary operations β¨ and β¨, respectively which forms a commutative idempotent semi-field. In this paper we systematically revisit classical algebraic structures used in conventional algebra and we substitute the commutative idempotent semi-field βπππ₯ for the field of scalars. The purpose is to provide the mathematical tools need to study linear transformation and isomorphism in commutative idempotent semi-modules over βπππ₯ . Many researchers have worked on βπππ₯ . Among of them discuss about semi-modules βππππ₯ , vectors, matrices and linear systems of equations. So, we will use their results to define general semi-modules over βπππ₯ , further to identify the properties of linear transformation and isomorphism in βπππ₯ .