Bases for Infinite Dimensional Vector Spaces Math 513 Linear Algebra Supplement
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On the Bicoset of a Bivector Space
International J.Math. Combin. Vol.4 (2009), 01-08 On the Bicoset of a Bivector Space Agboola A.A.A.† and Akinola L.S.‡ † Department of Mathematics, University of Agriculture, Abeokuta, Nigeria ‡ Department of Mathematics and computer Science, Fountain University, Osogbo, Nigeria E-mail: [email protected], [email protected] Abstract: The study of bivector spaces was first intiated by Vasantha Kandasamy in [1]. The objective of this paper is to present the concept of bicoset of a bivector space and obtain some of its elementary properties. Key Words: bigroup, bivector space, bicoset, bisum, direct bisum, inner biproduct space, biprojection. AMS(2000): 20Kxx, 20L05. §1. Introduction and Preliminaries The study of bialgebraic structures is a new development in the field of abstract algebra. Some of the bialgebraic structures already developed and studied and now available in several literature include: bigroups, bisemi-groups, biloops, bigroupoids, birings, binear-rings, bisemi- rings, biseminear-rings, bivector spaces and a host of others. Since the concept of bialgebraic structure is pivoted on the union of two non-empty subsets of a given algebraic structure for example a group, the usual problem arising from the union of two substructures of such an algebraic structure which generally do not form any algebraic structure has been resolved. With this new concept, several interesting algebraic properties could be obtained which are not present in the parent algebraic structure. In [1], Vasantha Kandasamy initiated the study of bivector spaces. Further studies on bivector spaces were presented by Vasantha Kandasamy and others in [2], [4] and [5]. In the present work however, we look at the bicoset of a bivector space and obtain some of its elementary properties. -
Introduction to Linear Bialgebra
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by University of New Mexico University of New Mexico UNM Digital Repository Mathematics and Statistics Faculty and Staff Publications Academic Department Resources 2005 INTRODUCTION TO LINEAR BIALGEBRA Florentin Smarandache University of New Mexico, [email protected] W.B. Vasantha Kandasamy K. Ilanthenral Follow this and additional works at: https://digitalrepository.unm.edu/math_fsp Part of the Algebra Commons, Analysis Commons, Discrete Mathematics and Combinatorics Commons, and the Other Mathematics Commons Recommended Citation Smarandache, Florentin; W.B. Vasantha Kandasamy; and K. Ilanthenral. "INTRODUCTION TO LINEAR BIALGEBRA." (2005). https://digitalrepository.unm.edu/math_fsp/232 This Book is brought to you for free and open access by the Academic Department Resources at UNM Digital Repository. It has been accepted for inclusion in Mathematics and Statistics Faculty and Staff Publications by an authorized administrator of UNM Digital Repository. For more information, please contact [email protected], [email protected], [email protected]. INTRODUCTION TO LINEAR BIALGEBRA W. B. Vasantha Kandasamy Department of Mathematics Indian Institute of Technology, Madras Chennai – 600036, India e-mail: [email protected] web: http://mat.iitm.ac.in/~wbv Florentin Smarandache Department of Mathematics University of New Mexico Gallup, NM 87301, USA e-mail: [email protected] K. Ilanthenral Editor, Maths Tiger, Quarterly Journal Flat No.11, Mayura Park, 16, Kazhikundram Main Road, Tharamani, Chennai – 600 113, India e-mail: [email protected] HEXIS Phoenix, Arizona 2005 1 This book can be ordered in a paper bound reprint from: Books on Demand ProQuest Information & Learning (University of Microfilm International) 300 N. -
21. Orthonormal Bases
21. Orthonormal Bases The canonical/standard basis 011 001 001 B C B C B C B0C B1C B0C e1 = B.C ; e2 = B.C ; : : : ; en = B.C B.C B.C B.C @.A @.A @.A 0 0 1 has many useful properties. • Each of the standard basis vectors has unit length: q p T jjeijj = ei ei = ei ei = 1: • The standard basis vectors are orthogonal (in other words, at right angles or perpendicular). T ei ej = ei ej = 0 when i 6= j This is summarized by ( 1 i = j eT e = δ = ; i j ij 0 i 6= j where δij is the Kronecker delta. Notice that the Kronecker delta gives the entries of the identity matrix. Given column vectors v and w, we have seen that the dot product v w is the same as the matrix multiplication vT w. This is the inner product on n T R . We can also form the outer product vw , which gives a square matrix. 1 The outer product on the standard basis vectors is interesting. Set T Π1 = e1e1 011 B C B0C = B.C 1 0 ::: 0 B.C @.A 0 01 0 ::: 01 B C B0 0 ::: 0C = B. .C B. .C @. .A 0 0 ::: 0 . T Πn = enen 001 B C B0C = B.C 0 0 ::: 1 B.C @.A 1 00 0 ::: 01 B C B0 0 ::: 0C = B. .C B. .C @. .A 0 0 ::: 1 In short, Πi is the diagonal square matrix with a 1 in the ith diagonal position and zeros everywhere else. -
Determinants Math 122 Calculus III D Joyce, Fall 2012
Determinants Math 122 Calculus III D Joyce, Fall 2012 What they are. A determinant is a value associated to a square array of numbers, that square array being called a square matrix. For example, here are determinants of a general 2 × 2 matrix and a general 3 × 3 matrix. a b = ad − bc: c d a b c d e f = aei + bfg + cdh − ceg − afh − bdi: g h i The determinant of a matrix A is usually denoted jAj or det (A). You can think of the rows of the determinant as being vectors. For the 3×3 matrix above, the vectors are u = (a; b; c), v = (d; e; f), and w = (g; h; i). Then the determinant is a value associated to n vectors in Rn. There's a general definition for n×n determinants. It's a particular signed sum of products of n entries in the matrix where each product is of one entry in each row and column. The two ways you can choose one entry in each row and column of the 2 × 2 matrix give you the two products ad and bc. There are six ways of chosing one entry in each row and column in a 3 × 3 matrix, and generally, there are n! ways in an n × n matrix. Thus, the determinant of a 4 × 4 matrix is the signed sum of 24, which is 4!, terms. In this general definition, half the terms are taken positively and half negatively. In class, we briefly saw how the signs are determined by permutations. -
28. Exterior Powers
28. Exterior powers 28.1 Desiderata 28.2 Definitions, uniqueness, existence 28.3 Some elementary facts 28.4 Exterior powers Vif of maps 28.5 Exterior powers of free modules 28.6 Determinants revisited 28.7 Minors of matrices 28.8 Uniqueness in the structure theorem 28.9 Cartan's lemma 28.10 Cayley-Hamilton Theorem 28.11 Worked examples While many of the arguments here have analogues for tensor products, it is worthwhile to repeat these arguments with the relevant variations, both for practice, and to be sensitive to the differences. 1. Desiderata Again, we review missing items in our development of linear algebra. We are missing a development of determinants of matrices whose entries may be in commutative rings, rather than fields. We would like an intrinsic definition of determinants of endomorphisms, rather than one that depends upon a choice of coordinates, even if we eventually prove that the determinant is independent of the coordinates. We anticipate that Artin's axiomatization of determinants of matrices should be mirrored in much of what we do here. We want a direct and natural proof of the Cayley-Hamilton theorem. Linear algebra over fields is insufficient, since the introduction of the indeterminate x in the definition of the characteristic polynomial takes us outside the class of vector spaces over fields. We want to give a conceptual proof for the uniqueness part of the structure theorem for finitely-generated modules over principal ideal domains. Multi-linear algebra over fields is surely insufficient for this. 417 418 Exterior powers 2. Definitions, uniqueness, existence Let R be a commutative ring with 1. -
Coordinatization
MATH 355 Supplemental Notes Coordinatization Coordinatization In R3, we have the standard basis i, j and k. When we write a vector in coordinate form, say 3 v 2 , (1) “ »´ fi 5 — ffi – fl it is understood as v 3i 2j 5k. “ ´ ` The numbers 3, 2 and 5 are the coordinates of v relative to the standard basis ⇠ i, j, k . It has p´ q “p q always been understood that a coordinate representation such as that in (1) is with respect to the ordered basis ⇠. A little thought reveals that it need not be so. One could have chosen the same basis elements in a di↵erent order, as in the basis ⇠ i, k, j . We employ notation indicating the 1 “p q coordinates are with respect to the di↵erent basis ⇠1: 3 v 5 , to mean that v 3i 5k 2j, r s⇠1 “ » fi “ ` ´ 2 —´ ffi – fl reflecting the order in which the basis elements fall in ⇠1. Of course, one could employ similar notation even when the coordinates are expressed in terms of the standard basis, writing v for r s⇠ (1), but whenever we have coordinatization with respect to the standard basis of Rn in mind, we will consider the wrapper to be optional. r¨s⇠ Of course, there are many non-standard bases of Rn. In fact, any linearly independent collection of n vectors in Rn provides a basis. Say we take 1 1 1 4 ´ ´ » 0fi » 1fi » 1fi » 1fi u , u u u ´ . 1 “ 2 “ 3 “ 4 “ — 3ffi — 1ffi — 0ffi — 2ffi — ffi —´ ffi — ffi — ffi — 0ffi — 4ffi — 2ffi — 1ffi — ffi — ffi — ffi —´ ffi – fl – fl – fl – fl As per the discussion above, these vectors are being expressed relative to the standard basis of R4. -
Review a Basis of a Vector Space 1
Review • Vectors v1 , , v p are linearly dependent if x1 v1 + x2 v2 + + x pv p = 0, and not all the coefficients are zero. • The columns of A are linearly independent each column of A contains a pivot. 1 1 − 1 • Are the vectors 1 , 2 , 1 independent? 1 3 3 1 1 − 1 1 1 − 1 1 1 − 1 1 2 1 0 1 2 0 1 2 1 3 3 0 2 4 0 0 0 So: no, they are dependent! (Coeff’s x3 = 1 , x2 = − 2, x1 = 3) • Any set of 11 vectors in R10 is linearly dependent. A basis of a vector space Definition 1. A set of vectors { v1 , , v p } in V is a basis of V if • V = span{ v1 , , v p} , and • the vectors v1 , , v p are linearly independent. In other words, { v1 , , vp } in V is a basis of V if and only if every vector w in V can be uniquely expressed as w = c1 v1 + + cpvp. 1 0 0 Example 2. Let e = 0 , e = 1 , e = 0 . 1 2 3 0 0 1 3 Show that { e 1 , e 2 , e 3} is a basis of R . It is called the standard basis. Solution. 3 • Clearly, span{ e 1 , e 2 , e 3} = R . • { e 1 , e 2 , e 3} are independent, because 1 0 0 0 1 0 0 0 1 has a pivot in each column. Definition 3. V is said to have dimension p if it has a basis consisting of p vectors. Armin Straub 1 [email protected] This definition makes sense because if V has a basis of p vectors, then every basis of V has p vectors. -
MATH 304 Linear Algebra Lecture 14: Basis and Coordinates. Change of Basis
MATH 304 Linear Algebra Lecture 14: Basis and coordinates. Change of basis. Linear transformations. Basis and dimension Definition. Let V be a vector space. A linearly independent spanning set for V is called a basis. Theorem Any vector space V has a basis. If V has a finite basis, then all bases for V are finite and have the same number of elements (called the dimension of V ). Example. Vectors e1 = (1, 0, 0,..., 0, 0), e2 = (0, 1, 0,..., 0, 0),. , en = (0, 0, 0,..., 0, 1) form a basis for Rn (called standard) since (x1, x2,..., xn) = x1e1 + x2e2 + ··· + xnen. Basis and coordinates If {v1, v2,..., vn} is a basis for a vector space V , then any vector v ∈ V has a unique representation v = x1v1 + x2v2 + ··· + xnvn, where xi ∈ R. The coefficients x1, x2,..., xn are called the coordinates of v with respect to the ordered basis v1, v2,..., vn. The mapping vector v 7→ its coordinates (x1, x2,..., xn) is a one-to-one correspondence between V and Rn. This correspondence respects linear operations in V and in Rn. Examples. • Coordinates of a vector n v = (x1, x2,..., xn) ∈ R relative to the standard basis e1 = (1, 0,..., 0, 0), e2 = (0, 1,..., 0, 0),. , en = (0, 0,..., 0, 1) are (x1, x2,..., xn). a b • Coordinates of a matrix ∈ M2,2(R) c d 1 0 0 0 0 1 relative to the basis , , , 0 0 1 0 0 0 0 0 are (a, c, b, d). 0 1 • Coordinates of a polynomial n−1 p(x) = a0 + a1x + ··· + an−1x ∈Pn relative to 2 n−1 the basis 1, x, x ,..., x are (a0, a1,..., an−1). -
Inner Product Spaces
CHAPTER 6 Woman teaching geometry, from a fourteenth-century edition of Euclid’s geometry book. Inner Product Spaces In making the definition of a vector space, we generalized the linear structure (addition and scalar multiplication) of R2 and R3. We ignored other important features, such as the notions of length and angle. These ideas are embedded in the concept we now investigate, inner products. Our standing assumptions are as follows: 6.1 Notation F, V F denotes R or C. V denotes a vector space over F. LEARNING OBJECTIVES FOR THIS CHAPTER Cauchy–Schwarz Inequality Gram–Schmidt Procedure linear functionals on inner product spaces calculating minimum distance to a subspace Linear Algebra Done Right, third edition, by Sheldon Axler 164 CHAPTER 6 Inner Product Spaces 6.A Inner Products and Norms Inner Products To motivate the concept of inner prod- 2 3 x1 , x 2 uct, think of vectors in R and R as x arrows with initial point at the origin. x R2 R3 H L The length of a vector in or is called the norm of x, denoted x . 2 k k Thus for x .x1; x2/ R , we have The length of this vector x is p D2 2 2 x x1 x2 . p 2 2 x1 x2 . k k D C 3 C Similarly, if x .x1; x2; x3/ R , p 2D 2 2 2 then x x1 x2 x3 . k k D C C Even though we cannot draw pictures in higher dimensions, the gener- n n alization to R is obvious: we define the norm of x .x1; : : : ; xn/ R D 2 by p 2 2 x x1 xn : k k D C C The norm is not linear on Rn. -
Orthonormal Bases
Math 108B Professor: Padraic Bartlett Lecture 3: Orthonormal Bases Week 3 UCSB 2014 In our last class, we introduced the concept of \changing bases," and talked about writ- ing vectors and linear transformations in other bases. In the homework and in class, we saw that in several situations this idea of \changing basis" could make a linear transformation much easier to work with; in several cases, we saw that linear transformations under a certain basis would become diagonal, which made tasks like raising them to large powers far easier than these problems would be in the standard basis. But how do we find these \nice" bases? What does it mean for a basis to be\nice?" In this set of lectures, we will study one potential answer to this question: the concept of an orthonormal basis. 1 Orthogonality To start, we should define the notion of orthogonality. First, recall/remember the defini- tion of the dot product: n Definition. Take two vectors (x1; : : : xn); (y1; : : : yn) 2 R . Their dot product is simply the sum x1y1 + x2y2 + : : : xnyn: Many of you have seen an alternate, geometric definition of the dot product: n Definition. Take two vectors (x1; : : : xn); (y1; : : : yn) 2 R . Their dot product is the product jj~xjj · jj~yjj cos(θ); where θ is the angle between ~x and ~y, and jj~xjj denotes the length of the vector ~x, i.e. the distance from (x1; : : : xn) to (0;::: 0). These two definitions are equivalent: 3 Theorem. Let ~x = (x1; x2; x3); ~y = (y1; y2; y3) be a pair of vectors in R . -
Pl¨Ucker Basis Vectors
Pluck¨ er Basis Vectors Roy Featherstone Department of Information Engineering The Australian National University Canberra, ACT 0200, Australia Email: [email protected] Abstract— 6-D vectors are routinely expressed in Pluck¨ er Pluck¨ er coordinate vector and the 6-D vector it represents; it coordinates; yet there is almost no mention in the literature of explains the relationship between a 6-D vector and the two the basis vectors that give rise to these coordinates. This paper 3-D vectors that define it; and it shows how to differentiate identifies the Pluck¨ er basis vectors, and uses them to explain the following: the relationship between a 6-D vector and its Pluck¨ er a 6-D vector in a moving Pluck¨ er coordinate system, using coordinates, the relationship between a 6-D vector and the pair of acceleration as an example. For the sake of a concrete expo- 3-D vectors used to define it, and the correct way to differentiate sition, this paper uses the notation and terminology of spatial a 6-D vector in a moving coordinate system. vectors; but the results apply generally to any 6-D vector that is expressed using Pluck¨ er coordinates. I. INTRODUCTION The rest of this paper is organized as follows. First, the 6-D vectors are used to describe the motions of rigid bodies Pluck¨ er basis vectors are described. Then the topic of dual and the forces acting upon them. They are therefore useful for coordinate systems is discussed. This is relevant to those 6-D describing the kinematics and dynamics of rigid-body systems vector formalisms in which force vectors are deemed to occupy in general, and robot mechanisms in particular. -
Linear Transformations and Determinants Matrix Multiplication As a Linear Transformation
Linear transformations and determinants Math 40, Introduction to Linear Algebra Monday, February 13, 2012 Matrix multiplication as a linear transformation Primary example of a = matrix linear transformation ⇒ multiplication Given an m n matrix A, × define T (x)=Ax for x Rn. ∈ Then T is a linear transformation. Astounding! Matrix multiplication defines a linear transformation. This new perspective gives a dynamic view of a matrix (it transforms vectors into other vectors) and is a key to building math models to physical systems that evolve over time (so-called dynamical systems). A linear transformation as matrix multiplication Theorem. Every linear transformation T : Rn Rm can be → represented by an m n matrix A so that x Rn, × ∀ ∈ T (x)=Ax. More astounding! Question Given T, how do we find A? Consider standard basis vectors for Rn: Transformation T is 1 0 0 0 completely determined by its . e1 = . ,...,en = . action on basis vectors. 0 0 0 1 Compute T (e1),T(e2),...,T(en). Standard matrix of a linear transformation Question Given T, how do we find A? Consider standard basis vectors for Rn: Transformation T is 1 0 0 0 completely determined by its . e1 = . ,...,en = . action on basis vectors. 0 0 0 1 Compute T (e1),T(e2),...,T(en). Then || | is called the T (e ) T (e ) T (e ) 1 2 ··· n standard matrix for T. || | denoted [T ] Standard matrix for an example Example x 3 2 x T : R R and T y = → y z 1 0 0 1 0 0 T 0 = T 1 = T 0 = 0 1 0 0 0 1 100 2 A = What is T 5 ? 010 − 12 2 2 100 2 A 5 = 5 = ⇒ − 010− 5 12 12 − Composition T : Rn Rm is a linear transformation with standard matrix A Suppose → S : Rm Rp is a linear transformation with standard matrix B.