(ProQuest: ... denotes non-US-ASCII text omitted.)
Zhaolin Jiang 1 and Yanpeng Gong 2 and Yun Gao 2
Academic Editor:Tongxing Li
1, Department of Mathematics, Linyi University, Linyi, Shandong 276000, China
2, Institute of Applied Mathematics, Shandong University of Technology, Zibo, Shandong 255049, China
Received 28 April 2014; Accepted 4 June 2014; 19 June 2014
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.
1. Introduction
Circulant matrices may play a crucial role for solving various differential equations. In [1], Ruiz-Claeyssen and dos Santos Leal introduced factor circulant matrices: matrices with the structure of circulants, but with the entries below the diagonal being multiplied by the same factor. The diagonalization of a circulant matrix and the spectral decomposition are conveniently generalized to block matrices with the structure of factor circulants. Matrix and partial differential equations involving factor circulants are considered. Wu and Zou in [2] discussed the existence and approximation of solutions of asymptotic or periodic boundary value problems of mixed functional differential equations. They focused on ( 5.13 ) in [2] with a circulant matrix, whose principal diagonal entries are zeroes. In [3], some Routh-Hurwitz stability conditions are generalized to the fractional order case. The authors considered the 1-system CML ( 10 ) . They selected a circulant matrix, which reads a tridiagonal matrix. Ahmed and Elgazzar used coupled map lattices (CML) as an alternative approach to include spatial effects in fractional order systems (FOS). Consider the 1-system CML ( 10 ) in [4]. They claimed that the system is stable if all the eigenvalues of the circulant matrix satisfy ( 2 ) in [4]. Trench considered nonautonomous systems of linear differential equations ( 1 ) in [5] with some constraint on the coefficient matrix A ( t ) . One case is that A ( t ) is a variable block circulant matrix. Kloeden et al. adopted the simplest approximation schemes for ( 1 ) in [6] with the Euler method, which reads ( 5 ) in [6]. They exploited that the covariance matrix of the increments can be embedded in a circulant matrix. The total loops can be done by fast Fourier transformation, which leads to a total computational cost of O ( m log ... m ) = O ( n log ... n ) . Guo et al. concerned on generic Dn-Hopf bifurcation to a delayed Hopfield-Cohen-Grossberg model of neural networks ( 5.17 ) in [7], where T denoted an interconnection matrix. They especially assumed T is a symmetric circulant matrix. Lin and Yang discretized the partial integrodifferential equation (PIDE) in pricing options with the preconditioned conjugate gradient (PCG) method, which constructed the circulant preconditioners. By using FFT, the cost for each linear system is O ( n log ... n ) , where n is the size of the system in [8]. Lee et al. investigated a high-order compact (HOC) scheme for the general two-dimensional (2D) linear partial differential equation ( 1.1 ) in [9] with a mixed derivative. Meanwhile, in order to establish the 2D combined compact difference (CCD2) scheme, they rewrote ( 1.1 ) in [9] into ( 2.1 ) in [9]. To write the CCD2 system in a concise style, they employed circulant matrix to obtain the corresponding whole CCD2 linear system ( 2.10 ) in [9], whose entries are circulant block.
Circulant type matrices have important applications in various disciplines including image processing, communications, signal processing, encoding, solving Toeplitz matrix problems, and least squares problems. They have been put on firm basis with the work of Davis [10], Jiang and Zhou [11], and Gray [12].
In [13], the authors pointed out the processes based on the eigenvalue of circulant type matrices with i.i.d. entries. There are discussions about the convergence in probability and in distribution of the spectral norm of circulant type matrices in [14]. The g -circulant matrices play an important role in various applications as well. For details, please refer to [15, 16] and the references therein. Ngondiep et al. showed the singular values of g -circulants in [17]. In [18, 19], the authors gave the limiting spectral distributions of left circulant matrices.
The Fibonacci and Lucas sequences are defined by the following recurrence relations [20, 21], respectively: [figure omitted; refer to PDF]
For n ...5; 0 , the first few values of the sequences are given by the following equation: [figure omitted; refer to PDF]
Let α , β be the roots of characteristic equation x 2 - x - 1 = 0 ; then the Binet formulas of the sequences { F n } and { L n } have the form [figure omitted; refer to PDF]
Let F n = F n · L n and L n = F n + L n , so we can get two new sequences F n and L n [22]. The two sequences are defined by the following recurrence relations, respectively: [figure omitted; refer to PDF]
For n ...5; 0 , the first few values of the sequences are given by the following equation: [figure omitted; refer to PDF]
The F n is given by the formula F n = ( α 1 n - β 1 n ) / ( α 1 - β 1 ) , where α 1 , β 1 are the roots of x 2 - 3 x + 1 = 0 . L n is given by the formula L n = F n + L n = ( α n - β n ) / ( α - β ) + ( α n + β n ) , where α , β are the roots of x 2 - x - 1 = 0 .
Besides, some scholars have given various algorithms for the determinants and inverses of nonsingular circulant matrices [10, 11]. Unfortunately, the computational complexities of these algorithms are very amazing with the order of matrix increasing. However, some authors gave the explicit determinants and inverse of circulant and skew-circulant involving Fibonacci and Lucas numbers. For example, Dazheng gave the determinant of the Fibonacci-Lucas quasicyclic matrices in [20]. Shen et al. considered circulant matrices with Fibonacci and Lucas numbers and presented their explicit determinants and inverses by constructing the transformation matrices [21]. Jaiswal evaluated some determinants of circulant whose elements are the generalized Fibonacci numbers [23]. Lind presented the determinants of circulant and skew-circulant involving Fibonacci numbers [24]. Bozkurt and Tam gave determinants and inverses of circulant matrices with Jacobsthal and Jacobsthal-Lucas numbers [25].
In [22], the authors gave some determinantal and permanental representations of F n and L n and complex factorization formulas. The purpose of this paper is to obtain the explicit determinants and inverse of circulant type matrices by some perfect properties of F n and L n .
In this paper, we adopt the following two conventions 0 0 = 1 , and for any sequence { a n } , ∑ k = i n a k = 0 in the case i > n .
Definition 1 (see [10, 11]).
In a circulant matrix (or right circulant matrix [26]) [figure omitted; refer to PDF] each row is a cyclic shift of the row above to the right.
Circulant matrix is a special case of a Toeplitz matrix. It is evidently determined by its first row (or column).
Definition 2 (see [11, 26]).
In a left circulant matrix (or reverse circulant matrix [13, 14, 18, 19]) [figure omitted; refer to PDF] each row is a cyclic shift of the row above to the left.
Left circulant matrix is a special Hankel matrix.
Definition 3 (see [14, 27]).
A g -circulant matrix is an n × n complex matrix with the following form: [figure omitted; refer to PDF] where g is a nonnegative integer and each of the subscripts is understood to be reduced modulo n .
The first row of A g , n is ( a 1 , a 2 , ... , a n ) ; its ( j + 1 ) th row is obtained by giving its j th row a right circular shift by g positions (equivalently, g mod n positions). Note that g = 1 or g = n + 1 yields the standard circulant matrix . If g = n - 1 , then we obtain the left circulant matrix .
Lemma 4 (see [21]).
Let A = C i r c ( a 1 , a 2 , ... , a n ) be a circulant matrix; then one has
(i) A is invertible if and only if f ( ω k ) ...0; 0 , ( k = 0,1 , 2 , ... , n - 1 ) , where f ( x ) = ∑ j = 1 n a j x j - 1 and ω = exp ... ( 2 π i / n ) ;
(ii) If A is invertible, then the inverse A - 1 of A is a circulant matrix.
Lemma 5.
Define [figure omitted; refer to PDF] the matrix Δ is an orthogonal cyclic shift matrix (and a left circulant matrix). It holds that L C i r c ( a 1 , a 2 , ... , a n ) = Δ C i r c ( a 1 , a 2 , ... , a n ) .
Lemma 6 (see [27]).
The n × n matrix Q g is unitary if and only if ( n , g ) = 1 , where Q g is a g -circulant matrix with the first row e * = [ 1,0 , ... , 0 ] .
Lemma 7 (see [27]).
A g , n is a g -circulant matrix with the first row [ a 1 , a 2 , ... , a n ] if and only if A g , n = Q g C , where C = C i r c ( a 1 , a 2 , ... , a n ) .
2. Determinant and Inverse of a Circulant Matrix with the Product of the Fibonacci and Lucas Numbers
In this section, let A n = Circ ( F 1 , F 2 , ... , F n ) be a circulant matrix. Firstly, we give the determinant equation of matrix A n . Afterwards, we prove that A n is an invertible matrix for n > 2 , and then we find the inverse of the matrix A n .
Theorem 8.
Let A n = C i r c ( F 1 , F 2 , ... , F n ) be a circulant matrix; then one has [figure omitted; refer to PDF] where F n is the n th F n · L n number.
Proof.
Obviously, det ... A 1 = 1 satisfies (10). In the case n > 1 , let [figure omitted; refer to PDF] We can obtain [figure omitted; refer to PDF] where [figure omitted; refer to PDF] We obtain [figure omitted; refer to PDF] while [figure omitted; refer to PDF] we have [figure omitted; refer to PDF] Thus, the proof is completed.
Theorem 9.
Let A n = C i r c ( F 1 , F 2 , ... , F n ) be a circulant matrix; if n > 2 , then A n is an invertible matrix.
Proof.
When n = 3 , in Theorem 8, we have det ... A 3 = 468 ...0; 0 ; hence A 3 is invertible. In the case n > 3 , since F n = ( α 1 n - β 1 n ) / ( α 1 - β 1 ) , where α 1 + β 1 = 3 , α 1 · β 1 = 1 .We have [figure omitted; refer to PDF]
If there exists ω l ( l = 1,2 , ... , n - 1 ) such that f ( ω l ) = 0 , we obtain 1 - F n + 1 + F n ω l = 0 for 1 - 3 ω l + ω 2 l ...0; 0 ; thus, ω l = ( F n + 1 - 1 ) / F n is a real number. While ω l = exp ... ( 2 l π i / n ) = cos ... ... ( 2 l π / n ) + i sin ... ( 2 l π / n ) , hence, sin ... ( 2 l π / n ) = 0 , so we have ω l = - 1 for 0 < 2 l π / n < 2 π . But x = - 1 is not the root of equation 1 - F n + 1 + F n x = 0 ( n > 3 ) . We obtain f ( ω k ) ...0; 0 for any ω k ( k = 1,2 , ... , n - 1 ) , while f ( 1 ) = ∑ j = 1 n ... F j = F n + 1 - F n - 1 ...0; 0 . By Lemma 4, the proof is completed.
Lemma 10.
Let the matrix G = [ g i , j ] i , j = 1 n - 2 be of the form [figure omitted; refer to PDF] and then the inverse G - 1 = [ g i , j [variant prime] ] i , j = 1 n - 2 of the matrix G is equal to [figure omitted; refer to PDF]
Proof.
Let c i j = ∑ k = 1 n - 2 ... g i k g k j [variant prime] . Obviously, c i , j = 0 for i < j . In the case i = j , we obtain c i i = g i i g i i [variant prime] = ( F 1 - F n + 1 ) · ( 1 / ( F 1 - F n + 1 ) ) = 1 . For i ...5; j + 1 , we obtain [figure omitted; refer to PDF] We verify G G - 1 = I n - 2 , where I n - 2 is the ( n - 2 ) × ( n - 2 ) identity matrix. Similarly, we can verify G - 1 G = I n - 2 . Thus, the proof is completed.
Theorem 11.
Let A n = C i r c ( F 1 , F 2 , ... , F n ) ( n > 2 ) be a circulant matrix; then one has [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
Proof.
Let [figure omitted; refer to PDF] where [figure omitted; refer to PDF] We have [figure omitted; refer to PDF] where D 1 = diag ... ( F 1 , f n ) is a diagonal matrix and D 1 [ecedil]5; G is the direct sum of D 1 and G . If we denote Π = Π 1 Π 2 , then we obtain [figure omitted; refer to PDF]
Since the last row elements of the matrix Π are [figure omitted; refer to PDF]
By Lemma 10, if we let A n - 1 = Circ ( x 1 , x 2 , ... , x n ) , its last row elements are given by the following equations: [figure omitted; refer to PDF] Let C n ( j ) = ∑ i = 1 j ... ( F j + 1 - i ( - F n ) i - 1 / ( F 1 - F n + 1 ) i ) ( j = 1,2 , ... , n - 2 ) ; we have [figure omitted; refer to PDF]
We obtain [figure omitted; refer to PDF]
3. Determinant and Inverse of a Circulant Matrix with the Sum of the Fibonacci and Lucas Numbers
In this section, let B n = Circ ( L 1 , L 2 , ... , L n ) be a circulant matrix. Firstly, we give an explicit determinant formula of matrix B n . Afterwards, we prove that B n is an invertible matrix for any positive integer n , and then we find its inverse.
Theorem 12.
Let B n = C i r c ( L 1 , L 2 , ... , L n ) be a circulant matrix; then one has [figure omitted; refer to PDF] where L n is the n th F n + L n number.
Proof.
Obviously, B 1 = 2 satisfies (31), when n > 1 . Let [figure omitted; refer to PDF] Then [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
We can obtain [figure omitted; refer to PDF] while [figure omitted; refer to PDF] We have [figure omitted; refer to PDF]
Theorem 13.
Let B n = C i r c ( L 1 , L 2 , ... , L n ) be a circulant matrix; then B n is invertible for any positive integer n .
Proof.
Since L n = ( α n - β n ) / ( α - β ) + α n + β n , where α + β = 1 , α · β = - 1 . We have [figure omitted; refer to PDF]
If there exist ω l ( l = 1,2 , ... , n - 1 ) such that f ( ω l ) = 0 , we obtain 2 - L n + 1 - ( L n - 2 ) ω l = 0 for 1 - ω l - ω 2 l ...0; 0 ; ω l = ( 2 - L n + 1 ) / ( L n - 2 ) is a real number, while ω l = exp ... ( 2 l π i / n ) = cos ... ... ( 2 l π / n ) + i sin ( 2 l π / n ) .
Hence, sin ( 2 l π / n ) = 0 , so we have ω l = - 1 for 0 < 2 l π / n < 2 π . But x = - 1 is not the root of the equation 2 - L n + 1 - ( L n - 2 ) x = 0 for any positive integer n . We obtain f ( ω k ) ...0; 0 for any ω k ( k = 1,2 , ... , n - 1 ) , while f ( 1 ) = ∑ j = 1 n L j = L n + 1 + L n - 4 ...0; 0 . By Lemma 4, the proof is completed.
Lemma 14.
Let matrix H = [ h i j ] i , j = 1 n - 2 be of the form [figure omitted; refer to PDF] and then inverse H - 1 = [ h i , j [variant prime] ] i , j = 1 n - 2 of the matrix H is equal to [figure omitted; refer to PDF]
Proof.
Let r i j = ∑ k = 1 n - 2 h i k h k j [variant prime] . Obviously, r i j = 0 for i < j . In the case i = j , we obtain [figure omitted; refer to PDF] For i ...5; j + 1 , we obtain [figure omitted; refer to PDF] We verify H H - 1 = I n - 2 , where I n - 2 is the ( n - 2 ) × ( n - 2 ) identity matrix. Similarly, we can verify H - 1 H = I n - 2 . Thus, the proof is completed.
Theorem 15.
Let B n = C i r c ( L 1 , L 2 , ... , L n ) be a circulant matrix; then one has [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
Proof.
Let [figure omitted; refer to PDF] where [figure omitted; refer to PDF] We have [figure omitted; refer to PDF] where D 2 = diag ... ( L 1 , l n ) is a diagonal matrix and D 2 [ecedil]5; H is the direct sum of D 2 and H . If we denote Ω = Ω 1 Ω 2 , then we obtain [figure omitted; refer to PDF] Since the last row elements of the matrix Ω are [figure omitted; refer to PDF]
By Lemma 14, if we let B n - 1 = Circ ( y 1 , y 2 , ... , y n ) , then its last row elements are given by the following equations: [figure omitted; refer to PDF] Let D n ( j ) = ∑ i = 1 j ... ( ( 2 L j + 2 - i - L j + 3 - i ) ( L n - 2 ) i - 1 / ( L 1 - L n + 1 ) i ) ( j = 1,2 , ... , n - 2 ) ; we have [figure omitted; refer to PDF]
We obtain [figure omitted; refer to PDF]
4. Determinant and Inverse of a Left Circulant Matrix with F n and L n Numbers
In this section, let A n [variant prime] = LCirc ( F 1 , F 2 , ... , F n ) and B n [variant prime] = LCirc ( L 1 , L 2 , ... , L n ) be left circulant matrices. By using the obtained conclusions, we give a determinant formula for the matrix A n [variant prime] and B n [variant prime] . Afterwards, we prove that A n [variant prime] is an invertible matrix for n > 2 and B n [variant prime] is an invertible matrix for any positive integer n . The inverses of the matrices A n [variant prime] and B n [variant prime] are also presented.
According to Lemma 5 and Theorems 8, 9, and 11, we can obtain the following theorems.
Theorem 16.
Let A n [variant prime] = L C i r c ( F 1 , F 2 , ... , F n ) be a left circulant matrix; then one has [figure omitted; refer to PDF] where F n is the n th F n · L n number.
Theorem 17.
Let A n [variant prime] = L C i r c ( F 1 , F 2 , ... , F n ) be a left circulant matrix; if n > 2 , then A n [variant prime] is an invertible matrix.
Theorem 18.
Let A n [variant prime] = L C i r c ( F 1 , F 2 , ... , F n ) ( n > 2 ) be a left circulant matrix; then one has [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
By Lemma 5 and Theorems 12, 13, and 15, the following conclusions can be attained.
Theorem 19.
Let B n [variant prime] = L C i r c ( L 1 , L 2 , ... , L n ) be a left circulant matrix; then one has [figure omitted; refer to PDF] where L n is the n th F n + L n number.
Theorem 20.
Let B n [variant prime] = L C i r c ( L 1 , L 2 , ... , L n ) be a left circulant matrix; then B n [variant prime] is invertible for any positive integer n .
Theorem 21.
Let B n [variant prime] = L C i r c ( L 1 , L 2 , ... , L n ) be a left circulant matrix; then one can obtain [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
5. Determinant and Inverse of g -Circulant Matrix with F n and L n Numbers
In this section, let A g , n = g - Circ ( F 1 , F 2 , ... , F n ) and B g , n = g - Circ ( L 1 , L 2 , ... , L n ) be g -circulant matrices. By using the obtained conclusions, we give a determinant formula for the matrices A g , n and B g , n . Afterwards, we prove that A g , n is an invertible matrix for n > 2 and B g , n is an invertible matrix if ( n , g ) = 1 . The inverse of the matrices A g , n and B g , n are also presented.
From Lemmas 6 and 7 and Theorems 8, 9, and 11, we deduce the following results.
Theorem 22.
Let A g , n = g - C i r c ( F 1 , F 2 , ... , F n ) be a g -circulant matrix; then one has [figure omitted; refer to PDF] where F n is the n th F n · L n number.
Theorem 23.
Let A g , n = g - C i r c ( F 1 , F 2 , ... , F n ) be a g -circulant matrix and ( g , n ) = 1 ; if n > 2 , then A g , n is an invertible matrix.
Theorem 24.
Let A g , n = g - C i r c ( F 1 , F 2 , ... , F n ) ( n > 2 ) be a g -circulant matrix and ( g , n ) = 1 ; then [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
Taking Lemmas 6 and 7 and Theorems 12, 13, and 15 into account, one has the following theorems.
Theorem 25.
Let B g , n = g - C i r c ( L 1 , L 2 , ... , L n ) be a g -circulant matrix; then one has [figure omitted; refer to PDF] where L n is the n F n + L n number.
Theorem 26.
Let B g , n = g - C i r c ( L 1 , L 2 , ... , L n ) be a g -circulant matrix and ( g , n ) = 1 ; then B g , n is invertible for any positive integer n .
Theorem 27.
Let B g , n = g - C i r c ( L 1 , L 2 , ... , L n ) be a g -circulant matrix and ( g , n ) = 1 ; then [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
Acknowledgments
The research was supported by the Development Project of Science & Technology of Shandong Province (Grant no. 2012GGX10115) and NSFC (Grant no. 11301252) and the AMEP of Linyi University, China.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
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Abstract
Circulant type matrices have become an important tool in solving differential equations. In this paper, we consider circulant type matrices, including the circulant and left circulant and g -circulant matrices with the sum and product of Fibonacci and Lucas numbers. Firstly, we discuss the invertibility of the circulant matrix and present the determinant and the inverse matrix by constructing the transformation matrices. Furthermore, the invertibility of the left circulant and g -circulant matrices is also discussed. We obtain the determinants and the inverse matrices of the left circulant and g -circulant matrices by utilizing the relation between left circulant, and g -circulant matrices and circulant matrix, respectively.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer