Recurrence Relations between Symmetric Polynomials of n-th Order

Size: px
Start display at page:

Download "Recurrence Relations between Symmetric Polynomials of n-th Order"

Transcription

1 Applied Mathematical Sciences, Vol. 8, 214, no. 15, HIKARI Ltd, Recurrence Relations between Symmetric Polynomials of n-th Order Yuriy N. Belyayev Syktyvkar University, Syktyvkar-1671, Russia Copyright c 214 Yuriy N. Belyayev. 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. Abstract The method of symmetric polynomials (MSP) was developed for computation analytical functions of matrices, in particular, integer powers of matrix. MSP does not require for its realization finding eigenvalues of the matrix. A new type of recurrence relations for symmetric polynomials of order n is found. Algorithm for the numerical calculation of high powers of the matrix is proposed.this computational procedure is more accurate in comparison with ordinary matrix multiplication. Mathematics Subject Classification: 11C, 34A Keywords: matrix functions, symmetric polynomials, roundoff error 1 Introduction Two groups of method play an important role in the theory of matrix functions and their practical applications. First group of approaches to the calculation of analytical function f(a) of matrix A a ij is based on the similarity transformations of matrices. For example, if a matrix A is normal, it can be represented by the formula A = UΛU 1, where U is a unitary matrix, Λ = λ i δ ij and λi are roots of the characteristic equation of matrix A: λ n p 1 λ n 1 p 2 λ n 2... p n 1 λ p n =. (1) Here p j = ( 1) j 1 σ j, j = 1,..., n, and σ j are sums of all principal minors of j-th order of det A, namely σ 1 = a 11 + a a nn, σ 2 = a ii a ij j>i a ji a jj,...,

2 5196 Yuriy N. Belyayev σ n = det A. After the matrices U, U 1, and eigenvalues λ i, i = 1,..., n, are found, matricies A k = U λ k i δ ij U 1 and hence f(a) = U f(λ i )δ ij U 1 can be calculated. Another category of methods is based on the Cayley-Hamilton theorem: each square matrix A satisfies its characteristic equation (1), in other words, A n = n i=1 p ia n i. It follows that any integer power j of matrix A can be expressed in terms of the first n powers A I, A,..., A n 1 : A j = C jl A l. (2) l= Well known formulas of Lagrange-Sylvester and Vandermonde [1, ] use the representation (2) and express an analytic function f(a) through eigenvalues λ j of the matrix A. To resolve the main problem of the above two groups of methods, - finding the eigenvalues λ j of matrix A, algorithms of Danilevsky, Hessenberg, Krylov, Samuelson and others are applied. Features of the application of these methods are considered in the monograph [2]. In this paper, to calculate an analytic functions of matrices we develop a method of symmetric polynomials (MSP) [3]. This method is based on the representation of A j by means of the coefficients p j of characteristic equation (1), but does not require finding the eigenvalues of the matrix A. This is a major MSP advantage over the methods mentioned above. 2 Basic relations Coefficients p l of the characteristic equation (1) relate with λ j by Viète s formulas: p 1 = 6 j=1 λ j, p 2 = g<j n λ g λ j,..., p n = ( 1) n 1 λ j. In other words, the coefficients p l, l = 1,..., n, are equal, to within a sign, elementary symmetric polynomials with respect to the eigenvalues of matrix. Therefore, any function of the variables p 1,..., p n is also symmetric with respect to λ j. D e f i n i t i o n. Solutions B g (n) B g (p 1,..., p n ) of equations j=1 B g (n) = p 1 B g 1 (n) + p 2 B g 2 (n) p n B g n (n), B g (n) =, g =, 1,..., n 2, B n 1 (n) = 1, are called symmetric polynomials of n-th order. (3)

3 Recurrence relations 5197 Obviously, that (3) allow us to calculate the values of functions B g (n) with indices g n recursively in terms of the previous n symmetric polynomials. For example, B n (n) = p 1 B n 1 (n) = p 1, B n+1 (n) = p 1 B n (n) + p 2 B n 1 (n) = p p 2,... If p n symmetric polynomials B g (n) with g < also exist and can be found recursively by the formula: B g (n) = 1 p n ( Bg+n (n) p 1 B g+n 1 (n)... p n 1 B g+1 (n) ), (4) namely B 1 (n) = B n 1(n) p n = 1 p n, B 2 (n) = p n 1B 1 (n)) p n = p n 1 p 2 n,... R e m a r k. Symmetric polynomials B g (n) with negative indices g for singular matrices (p n = ) are not defined. However, the following combinations of symmetric polynomials with indices g = 1, 2,..., n have meaning: p n B 1 (n) = B n 1 (n) p 1 B n 2 (n)... p n 1 B (n) = 1, 1 p n 1 B 1 (n) + p n B 2 (n) = B n 2 (n) p 1 B n 3 (n)... p n 2 B (n) =,. (5) p 2 B 1 (n) + p 2 B 2 (n) p n B n+1 (n) = B 1 (n) p 1 B (n) =, p 1 B 1 (n) + p 2 B 2 (n) p n B n (n) = B (n) =. These equalities follow directly from the relations (3). It was proved [3]: 1) for any integer j the coordinates C jl of the nonsingular matrix A j in the basis A, A,..., A n 1 are represented by the formulas: C jl = l p n l+g B j 1 g (n), l =,..., n 1; (6) g= 2) if det A =, then (6) determine the coefficients C jl for j. 3 Splitting of index polynomial T h e o r e m. Coordinates (6) of nonsingular matrix A j are the expansion coefficients of the polynomial B j+l (n) as a linear combination of polynomials B l (n), B l+1 (n),..., B l+n 1 (n) for any integers j and l: B j+l (n) = C jh B h+l (n). (7)

4 5198 Yuriy N. Belyayev If p n =, then the formula (7) holds for j + l and l n. P r o o f of this theorem we will carry out by induction. 1. Verification the relation (7), provided that l n 1. For this it is necessary to calculate the sum n 1 C jhb h+l (n). It should be noted that summand with number h = n 1 l contains B h+l (n) = B n 1 (n) = 1. Using definition (3), we find: C jh B h+l (n) = C j B l (n) C j(n 2 l) B n 2 (n) +C j(n 1 l) B n 1 (n) 1 + C j(n l) B n (n) + C j(n l+1) B n+1 (n) C j(n 1) B n 1+l (n). We express here the coefficients C j(n 1 l),..., C j(n 1) according to formulas (6) and recurrence relations (3): C j(n 1 l) = B j+l (n) p 1 B j+l 1 (n)... p l 1 B j+1 (n) p l B j (n), C j(n l) = B j+l 1 (n) p 1 B j+l 2 (n)... p l 2 B j+1 (n) p l 1 B j (n),. C j(n 2) = B j+1 (n) p 1 B j (n), C j(n 1) = B j (n), As a result of this C jh B h+l (n) = [ B j+l (n) p 1 B j+l 1 (n)... p l 1 B j+1 (n) p l B j (n) ] B n 1 (n) + [ B j+l 1 (n) p 1 B j+l 2 (n)... p l 2 B j+1 (n) p l 1 B j (n) ] B n (n) [ B j+2 (n) p 1 B j+1 (n) p 2 B j (n) ] B n 3+l (n) + [ B j+1 (n) p 1 B j (n) ] B n 2+l (n) + [ B j (n) ] B n 1+l (n). Rearrangement of summands in the last expression gives C jh B h+l (n) = B j+l (n) B n 1 (n) +B j+l 1 (n) ( B n (n) p 1 B n 1 (n) ) 1 + B j+l 2 (n) ( B n+1 (n) p 1 B n (n) p 2 B n 1 (n) ) } {{ } p 3 B n 2 (n)+p 4 B n 3 (n)+...+p nb 1 (n)= B j+1 (n) ( B n 2+l (n) p 1 B n 3+l (n)... p l 2 B n (n) p l 1 B n 1 (n) ) p l B n 2 (n)+...+p nb l 2 (n)= + B j (n) ( B n 1+l (n) p 1 B n 2+l (n)... p l B n 1 (n) ) = B j+l (n), p l+1 B n 2 (n)+...+p nb l 1 (n)=

5 Recurrence relations 5199 was to be shown. 2. Let (7) holds for values l = g, g + 1,..., g + n 1, where g integer. a) If g, then (7) is also true for l = g + n. Indeed, according to the definition (3) B j+g+n (n) = p 1 B j+g+n 1 (n) + p 2 B j+g+n 2 (n) p n B j+g (n). Each of the symmetric polynomials of n-th order in the right-hand side of last expression we represent according to the formula (7) and transform the resulting expression using the recursive formula (3). ( B j+g+n (n) = C jh p1 B h+g+n 1 (n) p n B h+g (n) ) = C jh B h+g+n (n), was to be proved. b) If g (it is assumed that the matrix A is nonsingular, i.e. p n ), then (7) is also true for l = g 1. The proof of this is analogous to the previous one and is based on the relations of the form (4): B j+g 1 (n) = 1 p n ( Bj+g+n 1 (n) p 1 B j+g+n 2 (n)... p n 1 B j+g (n) ) = 1 ( C jh Bh+g+n 1 (n) p 1 B h+g+n 2 (n)... p n 1 B h+g (n) ) p n n 1 = C jh B h+g 1 (n). We again have obtained confirmation of the rule (7). 3. If l = 1, 2,..., n, but j+l, equality (7) holds even for symmetric polynomials B j+l (n) of singular matrices. Let us show this using relations (5). Transforming n 1 C jhb h+l (n) for the case n l 1, we find C j B l (n) + + C j( l 1) B 1 (n) + C j( l) B (n) C j(n 1) B n 1+l (n) = p n B j 1 (n)b l (n) + ( p n 1 B j 1 (n) + p n B j 2 (n) ) B l+1 (n) ( p n+l+2 B j 1 (n) + p n+l+3 B j 2 (n) p n B j+l+1 (n) ) B 2 (n) + ( p n+l+1 B j 1 (n) + p n+l+2 B j 2 (n) p n B j+l (n) ) B 1 (n) = B j 1 (n) ( p n+l+1 B 1 (n) + p n+l+2 B 2 (n) p n 1 B l+1 (n) + p n B l (n) ) B n+l (n) p 1 B n+l 1 (n)... p n+l B (n)= + B j 2 (n) ( p n+l+2 B 1 (n) + p n+l+3 B 2 (n) p n B l+1 (n) ) +... B n+l+1 (n) p 1 B n+l (n)... p n+l+1 B (n)= + B j+l+1 (n) ( p n 1 B 1 (n) + p n B 2 (n) ) +B j+l (n) p n B 1 (n) = B j+l (n), 1

6 52 Yuriy N. Belyayev which completes the proof. 4 Symmetric polynomials of doubled index Formula (7) allows us to compute the symmetric polynomial B k (n) with a large index k = j + l using two sets of polynomials B j n (n),..., B j 1 (n) and B l (n),..., B l+n 1 (n) with smaller indices. In particular, from the formulas (7) it follows that B 2j g (n) = C jh B h+j g (n), g j. (8) Consider in detail these relations by the following example. E x a m p l e. D o u b l i n g o f t h e i n d e x i n t h e s e c o n d o r d e r s y m- m e t r i c p o l y n o m i a l s. According to the formula (6) for the case n = 2 we find C j = p 2 B j 1 (2), C j1 = p 1 B j 1 (2) + p 2 B j 2 (2) = B j (2). and from (8) equations are obtained: B 2j (2) = p 2 B j 1 (2)B j (2) + B j (2)B j+1 (2) = p 2 B j 1 (2)B j (2) + B j (2) ( p 1 B j (2) + p 2 B j 1 (2) ) = p 1 B 2 j (2) + 2p 2 B j 1 (2)B j (2), (9) B 2j 1 (2) = p 2 B 2 j 1(2) + B 2 j (2) (1) = p 2 B 2 j 1(2) + ( p 1 B j 1 (2) + p 2 B j 2 (2) ) 2, (11) B 2j 2 (2) = p 2 B j 1 (2)B j 2 (2) + B j (2)B j 1 (2) = p 2 B j 1 (2)B j 2 (2) + ( p 1 B j 1 (2) + p 2 B j 2 (2) ) B j 1 (2) = p 1 B 2 j 1(2) + 2p 2 B j 1 (2)B j 2 (2). (12) In deriving these equations we used the definition of symmetric polynomials B j (2) (see formulas (3)): B j (2) = p 1 B j 1 (2) + p 2 B j 2 (2). An important feature of these formulas is that they allow to calculate a set polynomials B 2j (2), B 2j 1 (2) directly through a set B j (2), B j 1 (2) (relations (9) and (1)), or set B 2j 1 (2), B 2j 2 (2) through set B j 1 (2), B j 2 (2) (equations (11) and (12)). Recurrence relations (8) for symmetric polynomials of orders n > 2 have the same meaning. Recurrence relations (8) can significantly improve the accuracy of calculation of high powers of matrices, in particular A 2j. Consider this on the example of second-order matrices. We compare two methods of computations

7 Recurrence relations 521 A 2j. First approach consists in by usual j-fold squaring A 2j =(... ((A) 2 ) 2...) 2, and new one (second) is based on the formula A 2j = AB 2 j(2) + Ip 2 B 2 j 1(2), (13) which follows from (2) and (6) for the matrix A of order n = 2. Here symmetric polynomials B 2 j(2) and B 2 j 1(2) can be found by recurrence formulas (9) and (1) respectively. T a b l e. Algorithm for computing a matrix A 2j of the second order No Sequence of computing A, M Calculation of the polynomials p 1, p 2, B 1 (2), B 2 (2) 1 p 1 = a 11 + a 22, p 2 = a 12 a 21 a 11 a 22, B 1 (2) = 1, B 2 (2) = p 1 2, 2 2. Computation of B 2 j(2), B 2 j 1(2) by formulas (9)-(1) β 1 = B2(2), 2 β 2 = p 2 B 1 (2), B 3 (2) = β 1 + β 2 B 1 (2), B 4 (2) = p 1 β 1 + 2β 2 B 2 (2) 2, 4 β 1 = B4(2), 2 β 2 = p 2 B 3 (2), B 7 (2) = β 1 + β 2 B 3 (2), B 8 (2) = p 1 β 1 + 2β 2 B 4 (2) 2, 4... β 1 = B 2 2 (2), β j 1 2 = p 2 B 2 j 1 1(2), 2 2.j-1 B 2 j 1(2)= β 1 + β 2 B 2 j 1 1(2), B 2 j(2)= p 1 β 1 + 2β 2 B 2 j 1(2) 2, 4 Calculation of the matrix A 2j 2j a ik by the formula (13) β 3 = p 2 B 2 j 1 1(2), 2j a 12 = a 12 B 2 j(2), 2j a 21 = a 21 B 2 j(2), j a 11 = a 11 B 2 j(2) + β 3, 2j a 22 = a 22 B 2 j(2) + β 3 2, 2 Computational errors caused by rounding the results depend on the total arithmetic operations number. A time of computations also is defined by number of arithmetic operations especially multiplications. One possible sequences of calculations by formula (13) with numbers of elementary additions A and multiplications M, corresponding to each operation, is shown in the Table. This algorithm requires the fulfillment of A 2 = 2 + 2(j 1) + 2 = 2j + 2 additions and M 2 = 2 + 6(j 1) + 5 = 6j + 1 multiplications. For comparison, the number of additions and multiplications by repeated squaring of the matrix A (first method) are, respectively, A 1 = 4j and M 1 = 8j. Thus, the method of computing the second order matrix A 2j, based on the use of matrix A symmetric polynomials, is more efficient and accurate than

8 522 Yuriy N. Belyayev the method of repeated squaring (even for j = 1!). A similar algorithms for computing matrix A 2j of order n > 2 are based on the formulas (2), (6) and (8). 5 Conclusion The scaling and squaring method for the matrix exponential (see for example [4]) is one of the problems in which the calculations of matrices A 2j are applied. MSP solves this problem as follows. For any n-th order matrix W and scalar z: exp(w z) = [exp (W z/m)] m A m, where integer m is called the scaling parameter, ( ) [ ] l W z 1 l n+n A m l! + B j l g (n) p n l+g, (14) j! l= g= p j, j = 1,..., n, and B l (n) imply respectively the characteristic equation coefficients and n=th order symmetric polynomials for matrix W z/m. An element a jl of the matrix (14) depends from number N: a jl = a jl (N). Approximate equality in (14) is replaced by the exact if N goes to infinity. The relative truncation error ɛ A (N) max (a ik ( ) a ik (N))/a ik ( ) in computation of the matrix (14) satisfies the inequality ξ N+1 ɛ A (N) < (N + n) N i=1 (n + i), provided that ξ = (2n 1)max w ijz < 1. m Choice scaling parameter m allows to control the relative truncation error. If m > n (in particular, m = 2 j, j > n) computation A m by formulas (2), (6) and recurrence relations (3) (or (8)) minimizes roundoff error. References [1] G.A. Korn, T.M. Korn, Mathematical handbook, McGraw-Hill Company, New York, [2] D.K. Faddeev, V.N. Faddeeva, Computational methods of linear algebra, Nauka, Moscow, [3] Yu.N. Belyayev, On the calculation of functions of matrices, Mathematical Notes, 94 (213), S [4] N.J. Higham, The scaling and squaring method for the matrix exponential revisited, SIAM Review, 51-4 (29), Received: July 9, 214 j=n

Solving Homogeneous Systems with Sub-matrices

Solving Homogeneous Systems with Sub-matrices Pure Mathematical Sciences, Vol 7, 218, no 1, 11-18 HIKARI Ltd, wwwm-hikaricom https://doiorg/112988/pms218843 Solving Homogeneous Systems with Sub-matrices Massoud Malek Mathematics, California State

More information

The Improved Arithmetic-Geometric Mean Inequalities for Matrix Norms

The Improved Arithmetic-Geometric Mean Inequalities for Matrix Norms Applied Mathematical Sciences, Vol 7, 03, no 9, 439-446 HIKARI Ltd, wwwm-hikaricom The Improved Arithmetic-Geometric Mean Inequalities for Matrix Norms I Halil Gumus Adıyaman University, Faculty of Arts

More information

Some Formulas for the Principal Matrix pth Root

Some Formulas for the Principal Matrix pth Root Int. J. Contemp. Math. Sciences Vol. 9 014 no. 3 141-15 HIKARI Ltd www.m-hiari.com http://dx.doi.org/10.1988/ijcms.014.4110 Some Formulas for the Principal Matrix pth Root R. Ben Taher Y. El Khatabi and

More information

On Positive Stable Realization for Continuous Linear Singular Systems

On Positive Stable Realization for Continuous Linear Singular Systems Int. Journal of Math. Analysis, Vol. 8, 2014, no. 8, 395-400 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ijma.2014.4246 On Positive Stable Realization for Continuous Linear Singular Systems

More information

of a Two-Operator Product 1

of a Two-Operator Product 1 Applied Mathematical Sciences, Vol. 7, 2013, no. 130, 6465-6474 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ams.2013.39501 Reverse Order Law for {1, 3}-Inverse of a Two-Operator Product 1 XUE

More information

On Some Identities and Generating Functions

On Some Identities and Generating Functions Int. Journal of Math. Analysis, Vol. 7, 2013, no. 38, 1877-1884 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ijma.2013.35131 On Some Identities and Generating Functions for k- Pell Numbers Paula

More information

Explicit Expressions for Free Components of. Sums of the Same Powers

Explicit Expressions for Free Components of. Sums of the Same Powers Applied Mathematical Sciences, Vol., 27, no. 53, 2639-2645 HIKARI Ltd, www.m-hikari.com https://doi.org/.2988/ams.27.79276 Explicit Expressions for Free Components of Sums of the Same Powers Alexander

More information

A Family of Optimal Multipoint Root-Finding Methods Based on the Interpolating Polynomials

A Family of Optimal Multipoint Root-Finding Methods Based on the Interpolating Polynomials Applied Mathematical Sciences, Vol. 8, 2014, no. 35, 1723-1730 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ams.2014.4127 A Family of Optimal Multipoint Root-Finding Methods Based on the Interpolating

More information

Stationary Flows in Acyclic Queuing Networks

Stationary Flows in Acyclic Queuing Networks Applied Mathematical Sciences, Vol. 11, 2017, no. 1, 23-30 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ams.2017.610257 Stationary Flows in Acyclic Queuing Networks G.Sh. Tsitsiashvili Institute

More information

A Note on Multiplicity Weight of Nodes of Two Point Taylor Expansion

A Note on Multiplicity Weight of Nodes of Two Point Taylor Expansion Applied Mathematical Sciences, Vol, 207, no 6, 307-3032 HIKARI Ltd, wwwm-hikaricom https://doiorg/02988/ams2077302 A Note on Multiplicity Weight of Nodes of Two Point Taylor Expansion Koichiro Shimada

More information

On Powers of General Tridiagonal Matrices

On Powers of General Tridiagonal Matrices Applied Mathematical Sciences, Vol. 9, 5, no., 583-59 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.988/ams.5.49 On Powers of General Tridiagonal Matrices Qassem M. Al-Hassan Department of Mathematics

More information

Basins of Attraction for Optimal Third Order Methods for Multiple Roots

Basins of Attraction for Optimal Third Order Methods for Multiple Roots Applied Mathematical Sciences, Vol., 6, no., 58-59 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.988/ams.6.65 Basins of Attraction for Optimal Third Order Methods for Multiple Roots Young Hee Geum Department

More information

Research Article A Generalization of a Class of Matrices: Analytic Inverse and Determinant

Research Article A Generalization of a Class of Matrices: Analytic Inverse and Determinant Advances in Numerical Analysis Volume 2011, Article ID 593548, 6 pages doi:10.1155/2011/593548 Research Article A Generalization of a Class of Matrices: Analytic Inverse and Determinant F. N. Valvi Department

More information

Computing the pth Roots of a Matrix. with Repeated Eigenvalues

Computing the pth Roots of a Matrix. with Repeated Eigenvalues Applied Mathematical Sciences, Vol. 5, 2011, no. 53, 2645-2661 Computing the pth Roots of a Matrix with Repeated Eigenvalues Amir Sadeghi 1, Ahmad Izani Md. Ismail and Azhana Ahmad School of Mathematical

More information

Sums of Tribonacci and Tribonacci-Lucas Numbers

Sums of Tribonacci and Tribonacci-Lucas Numbers International Journal of Mathematical Analysis Vol. 1, 018, no. 1, 19-4 HIKARI Ltd, www.m-hikari.com https://doi.org/10.1988/ijma.018.71153 Sums of Tribonacci Tribonacci-Lucas Numbers Robert Frontczak

More information

Double Total Domination in Circulant Graphs 1

Double Total Domination in Circulant Graphs 1 Applied Mathematical Sciences, Vol. 12, 2018, no. 32, 1623-1633 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ams.2018.811172 Double Total Domination in Circulant Graphs 1 Qin Zhang and Chengye

More information

Linear Systems and Matrices

Linear Systems and Matrices Department of Mathematics The Chinese University of Hong Kong 1 System of m linear equations in n unknowns (linear system) a 11 x 1 + a 12 x 2 + + a 1n x n = b 1 a 21 x 1 + a 22 x 2 + + a 2n x n = b 2.......

More information

On a Certain Representation in the Pairs of Normed Spaces

On a Certain Representation in the Pairs of Normed Spaces Applied Mathematical Sciences, Vol. 12, 2018, no. 3, 115-119 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ams.2018.712362 On a Certain Representation in the Pairs of ormed Spaces Ahiro Hoshida

More information

Factorization of Directed Graph Describing Protein Network

Factorization of Directed Graph Describing Protein Network Applied Mathematical Sciences, Vol. 11, 2017, no. 39, 1925-1931 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ams.2017.76205 Factorization of Directed Graph Describing Protein Network G.Sh. Tsitsiashvili

More information

Cayley-Hamilton Theorem

Cayley-Hamilton Theorem Cayley-Hamilton Theorem Massoud Malek In all that follows, the n n identity matrix is denoted by I n, the n n zero matrix by Z n, and the zero vector by θ n Let A be an n n matrix Although det (λ I n A

More information

Diophantine Equations. Elementary Methods

Diophantine Equations. Elementary Methods International Mathematical Forum, Vol. 12, 2017, no. 9, 429-438 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/imf.2017.7223 Diophantine Equations. Elementary Methods Rafael Jakimczuk División Matemática,

More information

k-pell, k-pell-lucas and Modified k-pell Numbers: Some Identities and Norms of Hankel Matrices

k-pell, k-pell-lucas and Modified k-pell Numbers: Some Identities and Norms of Hankel Matrices International Journal of Mathematical Analysis Vol. 9, 05, no., 3-37 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/0.988/ijma.05.4370 k-pell, k-pell-lucas and Modified k-pell Numbers: Some Identities

More information

A Note on Linearly Independence over the Symmetrized Max-Plus Algebra

A Note on Linearly Independence over the Symmetrized Max-Plus Algebra International Journal of Algebra, Vol. 12, 2018, no. 6, 247-255 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ija.2018.8727 A Note on Linearly Independence over the Symmetrized Max-Plus Algebra

More information

Linear Algebra review Powers of a diagonalizable matrix Spectral decomposition

Linear Algebra review Powers of a diagonalizable matrix Spectral decomposition Linear Algebra review Powers of a diagonalizable matrix Spectral decomposition Prof. Tesler Math 283 Fall 2018 Also see the separate version of this with Matlab and R commands. Prof. Tesler Diagonalizing

More information

The Expansion of the Confluent Hypergeometric Function on the Positive Real Axis

The Expansion of the Confluent Hypergeometric Function on the Positive Real Axis Applied Mathematical Sciences, Vol. 12, 2018, no. 1, 19-26 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ams.2018.712351 The Expansion of the Confluent Hypergeometric Function on the Positive Real

More information

Histogram Arithmetic under Uncertainty of. Probability Density Function

Histogram Arithmetic under Uncertainty of. Probability Density Function Applied Mathematical Sciences, Vol. 9, 015, no. 141, 7043-705 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.1988/ams.015.510644 Histogram Arithmetic under Uncertainty of Probability Density Function

More information

Linear Algebra Primer

Linear Algebra Primer Introduction Linear Algebra Primer Daniel S. Stutts, Ph.D. Original Edition: 2/99 Current Edition: 4//4 This primer was written to provide a brief overview of the main concepts and methods in elementary

More information

MATH 341 MIDTERM 2. (a) [5 pts] Demonstrate that A and B are row equivalent by providing a sequence of row operations leading from A to B.

MATH 341 MIDTERM 2. (a) [5 pts] Demonstrate that A and B are row equivalent by providing a sequence of row operations leading from A to B. 11/01/2011 Bormashenko MATH 341 MIDTERM 2 Show your work for all the problems. Good luck! (1) Let A and B be defined as follows: 1 1 2 A =, B = 1 2 3 0 2 ] 2 1 3 4 Name: (a) 5 pts] Demonstrate that A and

More information

Characteristic Polynomial

Characteristic Polynomial Linear Algebra Massoud Malek Characteristic Polynomial Preleminary Results Let A = (a ij ) be an n n matrix If Au = λu, then λ and u are called the eigenvalue and eigenvector of A, respectively The eigenvalues

More information

On Two New Classes of Fibonacci and Lucas Reciprocal Sums with Subscripts in Arithmetic Progression

On Two New Classes of Fibonacci and Lucas Reciprocal Sums with Subscripts in Arithmetic Progression Applied Mathematical Sciences Vol. 207 no. 25 2-29 HIKARI Ltd www.m-hikari.com https://doi.org/0.2988/ams.207.7392 On Two New Classes of Fibonacci Lucas Reciprocal Sums with Subscripts in Arithmetic Progression

More information

Sequences from Heptagonal Pyramid Corners of Integer

Sequences from Heptagonal Pyramid Corners of Integer International Mathematical Forum, Vol 13, 2018, no 4, 193-200 HIKARI Ltd, wwwm-hikaricom https://doiorg/1012988/imf2018815 Sequences from Heptagonal Pyramid Corners of Integer Nurul Hilda Syani Putri,

More information

Some Properties of D-sets of a Group 1

Some Properties of D-sets of a Group 1 International Mathematical Forum, Vol. 9, 2014, no. 21, 1035-1040 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/imf.2014.45104 Some Properties of D-sets of a Group 1 Joris N. Buloron, Cristopher

More information

Linear Algebra. Matrices Operations. Consider, for example, a system of equations such as x + 2y z + 4w = 0, 3x 4y + 2z 6w = 0, x 3y 2z + w = 0.

Linear Algebra. Matrices Operations. Consider, for example, a system of equations such as x + 2y z + 4w = 0, 3x 4y + 2z 6w = 0, x 3y 2z + w = 0. Matrices Operations Linear Algebra Consider, for example, a system of equations such as x + 2y z + 4w = 0, 3x 4y + 2z 6w = 0, x 3y 2z + w = 0 The rectangular array 1 2 1 4 3 4 2 6 1 3 2 1 in which the

More information

Section 9.2: Matrices.. a m1 a m2 a mn

Section 9.2: Matrices.. a m1 a m2 a mn Section 9.2: Matrices Definition: A matrix is a rectangular array of numbers: a 11 a 12 a 1n a 21 a 22 a 2n A =...... a m1 a m2 a mn In general, a ij denotes the (i, j) entry of A. That is, the entry in

More information

Numerical Investigation of the Time Invariant Optimal Control of Singular Systems Using Adomian Decomposition Method

Numerical Investigation of the Time Invariant Optimal Control of Singular Systems Using Adomian Decomposition Method Applied Mathematical Sciences, Vol. 8, 24, no. 2, 6-68 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.2988/ams.24.4863 Numerical Investigation of the Time Invariant Optimal Control of Singular Systems

More information

Generalized eigenvector - Wikipedia, the free encyclopedia

Generalized eigenvector - Wikipedia, the free encyclopedia 1 of 30 18/03/2013 20:00 Generalized eigenvector From Wikipedia, the free encyclopedia In linear algebra, for a matrix A, there may not always exist a full set of linearly independent eigenvectors that

More information

Dynamical Behavior for Optimal Cubic-Order Multiple Solver

Dynamical Behavior for Optimal Cubic-Order Multiple Solver Applied Mathematical Sciences, Vol., 7, no., 5 - HIKARI Ltd, www.m-hikari.com https://doi.org/.988/ams.7.6946 Dynamical Behavior for Optimal Cubic-Order Multiple Solver Young Hee Geum Department of Applied

More information

Morphisms Between the Groups of Semi Magic Squares and Real Numbers

Morphisms Between the Groups of Semi Magic Squares and Real Numbers International Journal of Algebra, Vol. 8, 2014, no. 19, 903-907 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ija.2014.212137 Morphisms Between the Groups of Semi Magic Squares and Real Numbers

More information

Determinants of Partition Matrices

Determinants of Partition Matrices journal of number theory 56, 283297 (1996) article no. 0018 Determinants of Partition Matrices Georg Martin Reinhart Wellesley College Communicated by A. Hildebrand Received February 14, 1994; revised

More information

Basics of Calculus and Algebra

Basics of Calculus and Algebra Monika Department of Economics ISCTE-IUL September 2012 Basics of linear algebra Real valued Functions Differential Calculus Integral Calculus Optimization Introduction I A matrix is a rectangular array

More information

A Class of Multi-Scales Nonlinear Difference Equations

A Class of Multi-Scales Nonlinear Difference Equations Applied Mathematical Sciences, Vol. 12, 2018, no. 19, 911-919 HIKARI Ltd, www.m-hiari.com https://doi.org/10.12988/ams.2018.8799 A Class of Multi-Scales Nonlinear Difference Equations Tahia Zerizer Mathematics

More information

Induced Cycle Decomposition of Graphs

Induced Cycle Decomposition of Graphs Applied Mathematical Sciences, Vol. 9, 2015, no. 84, 4165-4169 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ams.2015.5269 Induced Cycle Decomposition of Graphs Rosalio G. Artes, Jr. Department

More information

Dynamic Model of Space Robot Manipulator

Dynamic Model of Space Robot Manipulator Applied Mathematical Sciences, Vol. 9, 215, no. 94, 465-4659 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.12988/ams.215.56429 Dynamic Model of Space Robot Manipulator Polina Efimova Saint-Petersburg

More information

On the Computation of the Adjoint Ideal of Curves with Ordinary Singularities

On the Computation of the Adjoint Ideal of Curves with Ordinary Singularities Applied Mathematical Sciences Vol. 8, 2014, no. 136, 6805-6812 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ams.2014.49697 On the Computation of the Adjoint Ideal of Curves with Ordinary Singularities

More information

Solving Linear Systems of Equations

Solving Linear Systems of Equations November 6, 2013 Introduction The type of problems that we have to solve are: Solve the system: A x = B, where a 11 a 1N a 12 a 2N A =.. a 1N a NN x = x 1 x 2. x N B = b 1 b 2. b N To find A 1 (inverse

More information

Quadrics Defined by Skew-Symmetric Matrices

Quadrics Defined by Skew-Symmetric Matrices International Journal of Algebra, Vol. 11, 2017, no. 8, 349-356 HIKAI Ltd, www.m-hikari.com https://doi.org/10.12988/ija.2017.7942 Quadrics Defined by Skew-Symmetric Matrices Joydip Saha 1, Indranath Sengupta

More information

Remarks on the Maximum Principle for Parabolic-Type PDEs

Remarks on the Maximum Principle for Parabolic-Type PDEs International Mathematical Forum, Vol. 11, 2016, no. 24, 1185-1190 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/imf.2016.69125 Remarks on the Maximum Principle for Parabolic-Type PDEs Humberto

More information

Research Article The Adjacency Matrix of One Type of Directed Graph and the Jacobsthal Numbers and Their Determinantal Representation

Research Article The Adjacency Matrix of One Type of Directed Graph and the Jacobsthal Numbers and Their Determinantal Representation Applied Mathematics Volume 20, Article ID 423163, 14 pages doi:101155/20/423163 Research Article The Adjacency Matrix of One Type of Directed Graph and the Jacobsthal Numbers and Their Determinantal Representation

More information

On the Characterization Feedback of Positive LTI Continuous Singular Systems of Index 1

On the Characterization Feedback of Positive LTI Continuous Singular Systems of Index 1 Advanced Studies in Theoretical Physics Vol. 8, 2014, no. 27, 1185-1190 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/astp.2014.48245 On the Characterization Feedback of Positive LTI Continuous

More information

a 11 a 12 a 11 a 12 a 13 a 21 a 22 a 23 . a 31 a 32 a 33 a 12 a 21 a 23 a 31 a = = = = 12

a 11 a 12 a 11 a 12 a 13 a 21 a 22 a 23 . a 31 a 32 a 33 a 12 a 21 a 23 a 31 a = = = = 12 24 8 Matrices Determinant of 2 2 matrix Given a 2 2 matrix [ ] a a A = 2 a 2 a 22 the real number a a 22 a 2 a 2 is determinant and denoted by det(a) = a a 2 a 2 a 22 Example 8 Find determinant of 2 2

More information

On the Power of Standard Polynomial to M a,b (E)

On the Power of Standard Polynomial to M a,b (E) International Journal of Algebra, Vol. 10, 2016, no. 4, 171-177 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ija.2016.6214 On the Power of Standard Polynomial to M a,b (E) Fernanda G. de Paula

More information

Direct Product of BF-Algebras

Direct Product of BF-Algebras International Journal of Algebra, Vol. 10, 2016, no. 3, 125-132 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ija.2016.614 Direct Product of BF-Algebras Randy C. Teves and Joemar C. Endam Department

More information

When is the Ring of 2x2 Matrices over a Ring Galois?

When is the Ring of 2x2 Matrices over a Ring Galois? International Journal of Algebra, Vol. 7, 2013, no. 9, 439-444 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ija.2013.3445 When is the Ring of 2x2 Matrices over a Ring Galois? Audrey Nelson Department

More information

MTH 5102 Linear Algebra Practice Final Exam April 26, 2016

MTH 5102 Linear Algebra Practice Final Exam April 26, 2016 Name (Last name, First name): MTH 5 Linear Algebra Practice Final Exam April 6, 6 Exam Instructions: You have hours to complete the exam. There are a total of 9 problems. You must show your work and write

More information

A Short Note on Universality of Some Quadratic Forms

A Short Note on Universality of Some Quadratic Forms International Mathematical Forum, Vol. 8, 2013, no. 12, 591-595 HIKARI Ltd, www.m-hikari.com A Short Note on Universality of Some Quadratic Forms Cherng-tiao Perng Department of Mathematics Norfolk State

More information

Quadratic Optimization over a Polyhedral Set

Quadratic Optimization over a Polyhedral Set International Mathematical Forum, Vol. 9, 2014, no. 13, 621-629 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/imf.2014.4234 Quadratic Optimization over a Polyhedral Set T. Bayartugs, Ch. Battuvshin

More information

Weyl s Theorem and Property (Saw)

Weyl s Theorem and Property (Saw) International Journal of Mathematical Analysis Vol. 12, 2018, no. 9, 433-437 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ijma.2018.8754 Weyl s Theorem and Property (Saw) N. Jayanthi Government

More information

MATH2210 Notebook 2 Spring 2018

MATH2210 Notebook 2 Spring 2018 MATH2210 Notebook 2 Spring 2018 prepared by Professor Jenny Baglivo c Copyright 2009 2018 by Jenny A. Baglivo. All Rights Reserved. 2 MATH2210 Notebook 2 3 2.1 Matrices and Their Operations................................

More information

Second Proof: Every Positive Integer is a Frobenius Number of Three Generators

Second Proof: Every Positive Integer is a Frobenius Number of Three Generators International Mathematical Forum, Vol., 5, no. 5, - 7 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.988/imf.5.54 Second Proof: Ever Positive Integer is a Frobenius Number of Three Generators Firu Kamalov

More information

Fuzzy Sequences in Metric Spaces

Fuzzy Sequences in Metric Spaces Int. Journal of Math. Analysis, Vol. 8, 2014, no. 15, 699-706 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ijma.2014.4262 Fuzzy Sequences in Metric Spaces M. Muthukumari Research scholar, V.O.C.

More information

On a Boundary-Value Problem for Third Order Operator-Differential Equations on a Finite Interval

On a Boundary-Value Problem for Third Order Operator-Differential Equations on a Finite Interval Applied Mathematical Sciences, Vol. 1, 216, no. 11, 543-548 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.12988/ams.216.512743 On a Boundary-Value Problem for Third Order Operator-Differential Equations

More information

MATRICES. a m,1 a m,n A =

MATRICES. a m,1 a m,n A = MATRICES Matrices are rectangular arrays of real or complex numbers With them, we define arithmetic operations that are generalizations of those for real and complex numbers The general form a matrix of

More information

The Greatest Common Divisor of k Positive Integers

The Greatest Common Divisor of k Positive Integers International Mathematical Forum, Vol. 3, 208, no. 5, 25-223 HIKARI Ltd, www.m-hiari.com https://doi.org/0.2988/imf.208.822 The Greatest Common Divisor of Positive Integers Rafael Jaimczu División Matemática,

More information

AN ELEMENTARY PROOF OF THE SPECTRAL RADIUS FORMULA FOR MATRICES

AN ELEMENTARY PROOF OF THE SPECTRAL RADIUS FORMULA FOR MATRICES AN ELEMENTARY PROOF OF THE SPECTRAL RADIUS FORMULA FOR MATRICES JOEL A. TROPP Abstract. We present an elementary proof that the spectral radius of a matrix A may be obtained using the formula ρ(a) lim

More information

Double Total Domination on Generalized Petersen Graphs 1

Double Total Domination on Generalized Petersen Graphs 1 Applied Mathematical Sciences, Vol. 11, 2017, no. 19, 905-912 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ams.2017.7114 Double Total Domination on Generalized Petersen Graphs 1 Chengye Zhao 2

More information

Introduction to Matrices

Introduction to Matrices 214 Analysis and Design of Feedback Control Systems Introduction to Matrices Derek Rowell October 2002 Modern system dynamics is based upon a matrix representation of the dynamic equations governing the

More information

k-jacobsthal and k-jacobsthal Lucas Matrix Sequences

k-jacobsthal and k-jacobsthal Lucas Matrix Sequences International Mathematical Forum, Vol 11, 016, no 3, 145-154 HIKARI Ltd, wwwm-hikaricom http://dxdoiorg/101988/imf0165119 k-jacobsthal and k-jacobsthal Lucas Matrix Sequences S Uygun 1 and H Eldogan Department

More information

Refined Inertia of Matrix Patterns

Refined Inertia of Matrix Patterns Electronic Journal of Linear Algebra Volume 32 Volume 32 (2017) Article 24 2017 Refined Inertia of Matrix Patterns Kevin N. Vander Meulen Redeemer University College, kvanderm@redeemer.ca Jonathan Earl

More information

ACI-matrices all of whose completions have the same rank

ACI-matrices all of whose completions have the same rank ACI-matrices all of whose completions have the same rank Zejun Huang, Xingzhi Zhan Department of Mathematics East China Normal University Shanghai 200241, China Abstract We characterize the ACI-matrices

More information

Some Reviews on Ranks of Upper Triangular Block Matrices over a Skew Field

Some Reviews on Ranks of Upper Triangular Block Matrices over a Skew Field International Mathematical Forum, Vol 13, 2018, no 7, 323-335 HIKARI Ltd, wwwm-hikaricom https://doiorg/1012988/imf20188528 Some Reviews on Ranks of Upper Triangular lock Matrices over a Skew Field Netsai

More information

Symmetric Properties for the (h, q)-tangent Polynomials

Symmetric Properties for the (h, q)-tangent Polynomials Adv. Studies Theor. Phys., Vol. 8, 04, no. 6, 59-65 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/0.988/astp.04.43 Symmetric Properties for the h, q-tangent Polynomials C. S. Ryoo Department of Mathematics

More information

Homothetic Exponential Motions with Generalized Quaternions

Homothetic Exponential Motions with Generalized Quaternions Pure Mathematical Sciences, Vol. 3, 204, no. 2, 79-85 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/0.2988/pms.204.424 Homothetic Exponential Motions with Generalized Quaternions Faik Babadağ Kırıkkale

More information

Solution for a non-homogeneous Klein-Gordon Equation with 5th Degree Polynomial Forcing Function

Solution for a non-homogeneous Klein-Gordon Equation with 5th Degree Polynomial Forcing Function Advanced Studies in Theoretical Physics Vol., 207, no. 2, 679-685 HIKARI Ltd, www.m-hikari.com https://doi.org/0.2988/astp.207.7052 Solution for a non-homogeneous Klein-Gordon Equation with 5th Degree

More information

Diagonalizing Hermitian Matrices of Continuous Functions

Diagonalizing Hermitian Matrices of Continuous Functions Int. J. Contemp. Math. Sciences, Vol. 8, 2013, no. 5, 227-234 HIKARI Ltd, www.m-hikari.com Diagonalizing Hermitian Matrices of Continuous Functions Justin Cyr 1, Jason Ekstrand, Nathan Meyers 2, Crystal

More information

Lecture Note 3: Interpolation and Polynomial Approximation. Xiaoqun Zhang Shanghai Jiao Tong University

Lecture Note 3: Interpolation and Polynomial Approximation. Xiaoqun Zhang Shanghai Jiao Tong University Lecture Note 3: Interpolation and Polynomial Approximation Xiaoqun Zhang Shanghai Jiao Tong University Last updated: October 10, 2015 2 Contents 1.1 Introduction................................ 3 1.1.1

More information

Continuum-Wise Expansive and Dominated Splitting

Continuum-Wise Expansive and Dominated Splitting Int. Journal of Math. Analysis, Vol. 7, 2013, no. 23, 1149-1154 HIKARI Ltd, www.m-hikari.com Continuum-Wise Expansive and Dominated Splitting Manseob Lee Department of Mathematics Mokwon University Daejeon,

More information

On Generalized k-fibonacci Sequence by Two-Cross-Two Matrix

On Generalized k-fibonacci Sequence by Two-Cross-Two Matrix Global Journal of Mathematical Analysis, 5 () (07) -5 Global Journal of Mathematical Analysis Website: www.sciencepubco.com/index.php/gjma doi: 0.449/gjma.v5i.6949 Research paper On Generalized k-fibonacci

More information

Foundations of Matrix Analysis

Foundations of Matrix Analysis 1 Foundations of Matrix Analysis In this chapter we recall the basic elements of linear algebra which will be employed in the remainder of the text For most of the proofs as well as for the details, the

More information

On Linear Recursive Sequences with Coefficients in Arithmetic-Geometric Progressions

On Linear Recursive Sequences with Coefficients in Arithmetic-Geometric Progressions Applied Mathematical Sciences, Vol. 9, 015, no. 5, 595-607 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.1988/ams.015.5163 On Linear Recursive Sequences with Coefficients in Arithmetic-Geometric Progressions

More information

On Symmetric Bi-Multipliers of Lattice Implication Algebras

On Symmetric Bi-Multipliers of Lattice Implication Algebras International Mathematical Forum, Vol. 13, 2018, no. 7, 343-350 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/imf.2018.8423 On Symmetric Bi-Multipliers of Lattice Implication Algebras Kyung Ho

More information

A Fixed Point Approach to the Stability of a Quadratic-Additive Type Functional Equation in Non-Archimedean Normed Spaces

A Fixed Point Approach to the Stability of a Quadratic-Additive Type Functional Equation in Non-Archimedean Normed Spaces International Journal of Mathematical Analysis Vol. 9, 015, no. 30, 1477-1487 HIKARI Ltd, www.m-hikari.com http://d.doi.org/10.1988/ijma.015.53100 A Fied Point Approach to the Stability of a Quadratic-Additive

More information

An Abundancy Result for the Two Prime Power Case and Results for an Equations of Goormaghtigh

An Abundancy Result for the Two Prime Power Case and Results for an Equations of Goormaghtigh International Mathematical Forum, Vol. 8, 2013, no. 9, 427-432 HIKARI Ltd, www.m-hikari.com An Abundancy Result for the Two Prime Power Case and Results for an Equations of Goormaghtigh Richard F. Ryan

More information

Advanced Studies in Theoretical Physics Vol. 8, 2014, no. 22, HIKARI Ltd,

Advanced Studies in Theoretical Physics Vol. 8, 2014, no. 22, HIKARI Ltd, Advanced Studies in Theoretical Physics Vol. 8, 204, no. 22, 977-982 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/0.2988/astp.204.499 Some Identities of Symmetry for the Higher-order Carlitz Bernoulli

More information

Boundary Value Problem for Second Order Ordinary Linear Differential Equations with Variable Coefficients

Boundary Value Problem for Second Order Ordinary Linear Differential Equations with Variable Coefficients International Journal of Mathematical Analysis Vol. 9, 2015, no. 3, 111-116 HIKARI Ltd, www.m-hikari.com http://d.doi.org/10.12988/ijma.2015.411353 Boundary Value Problem for Second Order Ordinary Linear

More information

A Note of the Strong Convergence of the Mann Iteration for Demicontractive Mappings

A Note of the Strong Convergence of the Mann Iteration for Demicontractive Mappings Applied Mathematical Sciences, Vol. 10, 2016, no. 6, 255-261 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ams.2016.511700 A Note of the Strong Convergence of the Mann Iteration for Demicontractive

More information

Networks of Queues Models with Several. Classes of Customers and Exponential. Service Times

Networks of Queues Models with Several. Classes of Customers and Exponential. Service Times Applied Mathematical Sciences, Vol. 9, 2015, no. 76, 3789-3796 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ams.2015.53287 Networks of Queues Models with Several Classes of Customers and Exponential

More information

Quasi-Bigraduations of Modules, Slow Analytic Independence

Quasi-Bigraduations of Modules, Slow Analytic Independence International Mathematical Forum, Vol 13, 2018, no 12, 547-563 HIKRI Ltd, wwwm-hikaricom https://doiorg/1012988/imf201881060 Quasi-Bigraduations of Modules, Slow nalytic Independence Youssouf M Diagana

More information

ON ORTHOGONAL REDUCTION TO HESSENBERG FORM WITH SMALL BANDWIDTH

ON ORTHOGONAL REDUCTION TO HESSENBERG FORM WITH SMALL BANDWIDTH ON ORTHOGONAL REDUCTION TO HESSENBERG FORM WITH SMALL BANDWIDTH V. FABER, J. LIESEN, AND P. TICHÝ Abstract. Numerous algorithms in numerical linear algebra are based on the reduction of a given matrix

More information

Some Properties of a Semi Dynamical System. Generated by von Forester-Losata Type. Partial Equations

Some Properties of a Semi Dynamical System. Generated by von Forester-Losata Type. Partial Equations Int. Journal of Math. Analysis, Vol. 7, 2013, no. 38, 1863-1868 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ijma.2013.3481 Some Properties of a Semi Dynamical System Generated by von Forester-Losata

More information

Inverses of regular Hessenberg matrices

Inverses of regular Hessenberg matrices Proceedings of the 10th International Conference on Computational and Mathematical Methods in Science and Engineering, CMMSE 2010 27 30 June 2010. Inverses of regular Hessenberg matrices J. Abderramán

More information

On a Principal Ideal Domain that is not a Euclidean Domain

On a Principal Ideal Domain that is not a Euclidean Domain International Mathematical Forum, Vol. 8, 013, no. 9, 1405-141 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.1988/imf.013.37144 On a Principal Ideal Domain that is not a Euclidean Domain Conan Wong

More information

A Practical Method for Decomposition of the Essential Matrix

A Practical Method for Decomposition of the Essential Matrix Applied Mathematical Sciences, Vol. 8, 2014, no. 176, 8755-8770 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ams.2014.410877 A Practical Method for Decomposition of the Essential Matrix Georgi

More information

A Note on the Carlitz s Type Twisted q-tangent. Numbers and Polynomials

A Note on the Carlitz s Type Twisted q-tangent. Numbers and Polynomials Applied Mathematical Sciences, Vol. 12, 2018, no. 15, 731-738 HIKARI Ltd www.m-hikari.com https://doi.org/10.12988/ams.2018.8585 A Note on the Carlitz s Type Twisted q-tangent Numbers and Polynomials Cheon

More information

MATH 5640: Functions of Diagonalizable Matrices

MATH 5640: Functions of Diagonalizable Matrices MATH 5640: Functions of Diagonalizable Matrices Hung Phan, UMass Lowell November 27, 208 Spectral theorem for diagonalizable matrices Definition Let V = X Y Every v V is uniquely decomposed as u = x +

More information

s-generalized Fibonacci Numbers: Some Identities, a Generating Function and Pythagorean Triples

s-generalized Fibonacci Numbers: Some Identities, a Generating Function and Pythagorean Triples International Journal of Mathematical Analysis Vol. 8, 2014, no. 36, 1757-1766 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/ijma.2014.47203 s-generalized Fibonacci Numbers: Some Identities,

More information

Formula for Lucas Like Sequence of Fourth Step and Fifth Step

Formula for Lucas Like Sequence of Fourth Step and Fifth Step International Mathematical Forum, Vol. 12, 2017, no., 10-110 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/imf.2017.612169 Formula for Lucas Like Sequence of Fourth Step and Fifth Step Rena Parindeni

More information

Chapter 3 Transformations

Chapter 3 Transformations Chapter 3 Transformations An Introduction to Optimization Spring, 2014 Wei-Ta Chu 1 Linear Transformations A function is called a linear transformation if 1. for every and 2. for every If we fix the bases

More information

The Second Solution of the Hermite Equation and the Monomiality Formalism

The Second Solution of the Hermite Equation and the Monomiality Formalism Pure Mathematical Sciences, Vol. 2, 2013, no. 4, 147-152 HIKARI Ltd, www.m-hikari.com The Second Solution of the Hermite Equation and the Monomiality Formalism G. Dattoli Gruppo Fisica Teorica e Matematica

More information

Mathematical Methods for Engineers and Scientists 1

Mathematical Methods for Engineers and Scientists 1 K.T. Tang Mathematical Methods for Engineers and Scientists 1 Complex Analysis, Determinants and Matrices With 49 Figures and 2 Tables fyj Springer Part I Complex Analysis 1 Complex Numbers 3 1.1 Our Number

More information

Linear Algebra 1. M.T.Nair Department of Mathematics, IIT Madras. and in that case x is called an eigenvector of T corresponding to the eigenvalue λ.

Linear Algebra 1. M.T.Nair Department of Mathematics, IIT Madras. and in that case x is called an eigenvector of T corresponding to the eigenvalue λ. Linear Algebra 1 M.T.Nair Department of Mathematics, IIT Madras 1 Eigenvalues and Eigenvectors 1.1 Definition and Examples Definition 1.1. Let V be a vector space (over a field F) and T : V V be a linear

More information