(ProQuest: ... denotes non-US-ASCII text omitted.)
Academic Editor:Zidong Wang
School of Science, Linyi University, Shuangling Road, Linyi 276005, China
Received 9 April 2014; Accepted 30 April 2014; 18 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
Skew circulant and circulant matrices have important applications in various networks engineering. Joy and Tavsanoglu [1] showed that feedback matrices of ring cellular neural networks, which can be described by the ODE, are block circulants. A special class of the feedback delay network using circulant matrices was proposed [2]. Jing and Jafarkhani [3] proposed distributed differential space-time codes that work for networks with any number of relays using circulant matrices. Exploiting the circulant structure of the channel matrices, Eghbali et al. [4] analysed the realistic near fast fading scenarios with circulant frequency selective channels. Rocchesso [5] presented particular choices of the feedback coefficients, namely, Galois sequences, arranged in a circulant matrix, to produce a maximum echo density in the time response. Sardellitti et al. [6] used an analytical expression for the eigenvalues of a block circulant matrix as a function of the coverage radius. Li et al. [7] gave a low-complexity binary frame-wise network coding encoder design based on circulant matrix. Hirt and Massey [8] introduced discrete time Fourier transform precoding to the proposed multihop relay system involving circulant matrix. When considering a single-input single-output transmission with CFO and omitting the relay index subscript, Wang et al. [9] proved that the intercarrier interference matrix is a circulant matrix. The system model of the OFDM based AF relay networks as well as the strategy of the superimposed training involves circulant matrix [10]. Two-way transmission model considered in [11] ensured the circular convolution between two frequency selective channels.
The skew circulant matrices as preconditioners for linear multistep formulae- (LMF-) based ordinary differential equations (ODEs) codes, Hermitian, and skew-Hermitian Toeplitz systems were considered in [12-15]. Lyness and Sørevik employed a skew circulant matrix to construct s-dimensional lattice rules in [16]. Compared with cyclic convolution algorithm, the skew cyclic convolution algorithm [17] was able to perform filtering procedure in approximately half of computational cost for real signals. In [18] two new normal-form realizations were presented which utilize circulant and skew circulant matrices as their state transition matrices. The well-known second-order coupled form is a special case of the skew circulant form. Li et al. [19] gave the style spectral decomposition of skew circulant matrix firstly and then dealt with the optimal backward perturbation analysis for the linear system with skew circulant coefficient matrix. In [20], a new fast algorithm for optimal design of block digital filters (BDFs) was proposed based on skew circulant matrix.
Besides, some scholars have given various algorithms for the determinants and inverses of nonsingular circulant matrices. Unfortunately, the computational complexity of these algorithms is very amazing huge with the order of matrix increasing. However, some authors gave the explicit determinants and inverses of circulant and skew circulant matrices involving some famous numbers. For example, Yao and Jiang [21] considered the determinants, inverses, norm, and spread of skew circulant type matrices involving any continuous Lucas numbers. Shen et al. considered circulant matrices with Fibonacci and Lucas numbers and presented their explicit determinants and inverses by constructing the transformation matrices [22]. Gao et al. [23] gave explicit determinants and inverses of skew circulant and skew left circulant matrices with Fibonacci and Lucas numbers. Jiang et al. [24, 25] considered the skew circulant and skew left circulant matrices with the k -Fibonacci numbers and the k -Lucas numbers and discussed the invertibility of the these matrices and presented their determinant and the inverse matrix by constructing the transformation matrices, respectively. Jaiswal evaluated some determinants of circulant whose elements are the generalized Fibonacci numbers [26]. Lind presented the determinants of circulant and skew circulant involving Fibonacci numbers [27]. Dazheng [28] gave the determinant of the Fibonacci-Lucas quasi-cyclic matrices.
Recently, there are several papers on the norms of some special matrices. Solak [29] established the lower and upper bounds for the spectral norms of circulant matrices with classical Fibonacci and Lucas numbers entries. Ipek [30] investigated an improved estimation for spectral norms of these matrices. Shen and Cen [31] gave upper and lower bounds for the spectral norms of r -circulant matrices in the form of A = C r ( F 0 , F 1 , ... , F n - 1 ) , B = C r ( L 0 , L 1 , ... , L n - 1 ) , and they also obtained some bounds for the spectral norms of Kronecker and Hadamard products of matrix A and matrix B . Akbulak and Bozkurt [32] found upper and lower bounds for the spectral norms of Toeplitz matrices such that a i j ...1; F i - j and b i j ...1; L i - j . The convergence in probability and in distribution of the spectral norm of scaled Toeplitz, circulant, reverse circulant, symmetric circulant, and a class of k -circulant matrices were discussed in [33].
Beginning with Mirsky [34], several authors [35-37] have obtained bounds for the spread of a matrix.
The Fibonacci sequences are defined by the following recurrence relations [22, 23, 26-32]: [figure omitted; refer to PDF]
The { F n } is given by the formula [figure omitted; refer to PDF] where α and β are the roots of the characteristic equation x 2 - x - 1 = 0 .
The Fibonacci sequences were introduced for the first time by the famous Italian mathematician Leonardo of Pisa (nicknamed Fibonacci). It is well known that the ratio of two consecutive classical Fibonacci numbers converges to the golden mean, or the golden section, ( 1 + 5 ) / 2 , which appears in modern research in many fields from architecture [38, 39] to physics of high energy particles [40]. As is shown in [41, 42], the hyperbolic Fibonacci functions can lead to creation of the Lobachevsky Fibonacci and Minkovsky Fibonacci geometry which are of great importance for theoretical physics. In the 19th century the French mathematician Francois Edouard Anatole Lucas (1842-1891) introduced the so-called Lucas numbers given by the recursive relation L n = L n - 1 + L n - 2 , n ...5; 2 , with the seeds L 0 = 2 and L 1 = 1 . The determinants, inverses, norm, and spread of skew circulant type matrices involving any continuous Lucas numbers are considered in [21].
The purpose of this paper is to obtain the explicit determinants, explicit inverses, norm, and spread of skew circulant type matrices involving any continuous Fibonacci numbers. And we generalize the result [23]. In passing, the norm and spread of skew circulant type matrices have not been research. It is hoped that this paper will help in changing this.
In the following, let r be a nonnegative integer. We adopt the following two conventions 0 0 = 1 and, for any sequence { a n } , ∑ k = i n a k = 0 in case i > n .
Definition 1 (see [21]).
A skew circulant matrix with the first row ( a 1 , a 2 , ... , a n ) is meant to be a square matrix of the form [figure omitted; refer to PDF] denoted by SCirc ( a 1 , a 2 , ... , a n ) .
Definition 2 (see [21]).
A skew left circulant matrix with the first row ( a 1 , a 2 , ... , a n ) is meant to be a square matrix of the form [figure omitted; refer to PDF] denoted by SLCirc ( a 1 , a 2 , ... , a n ) .
Lemma 3 (see [30, 31]).
Let { F n } be Fibonacci numbers; then, [figure omitted; refer to PDF]
2. Determinant and Inverse of Skew Circulant Matrix with the Fibonacci Numbers
In this section, let B r , n = SCirc ( F r + 1 , ... , F r + n ) be a skew circulant matrix. Firstly, we give a determinant explicit formula for the matrix B r , n . Afterwards, we prove that B r , n is an invertible matrix for n ...5; 2 , and then we find the inverse of the matrix B r , n . In the following, let [figure omitted; refer to PDF]
Theorem 4.
Let B r , n = S C i r c ( F r + 1 , ... , F r + n ) be a skew circulant matrix; then, [figure omitted; refer to PDF] where F r + n is the ( r + n ) th Fibonacci number. In particular, when r = 0 , we get the result of [23].
Proof.
Obviously, det ... B r , 2 = F r + 1 2 + F r + 2 2 satisfies the equation. In case n > 2 , let [figure omitted; refer to PDF] be two n × n matrices; then, we have [figure omitted; refer to PDF] where [figure omitted; refer to PDF] So it holds that [figure omitted; refer to PDF] while taking det ... Γ = det ... Π 1 = ( - 1 ) ( n - 1 ) ( n - 2 ) / 2 , we can get [figure omitted; refer to PDF] This completes the proof.
Theorem 5.
Let B r , n = S C i r c ( F r + 1 , ... , F r + n ) be a skew circulant matrix; then, B r , n is an invertible matrix. Specially, when r = 0 , we get the result of [23].
Proof.
Taking n = 2 in Theorem 4, we have det ... B r , 2 = F r + 1 2 + F r + 2 2 ...0; 0 . Hence B r , 2 is invertible. In case n > 2 , since F r + n = ( α r + n - β r + n ) / ( α - β ) , where α + β = 1 , α β = - 1 , we obtain [figure omitted; refer to PDF] where ω = exp ... ( 2 π i / n ) , η = exp ... ( π i / n ) . If there exists ω l η ( l = 1,2 , ... , n - 1 ) such that f ( ω l η ) = 0 , we obtain F r + 1 + F r + n + 1 + ( F r + F r + n ) ω k η = 0 for 1 - ω l η - ω 2 l η 2 ...0; 0 , and hence it follows that ω l η = - ( F r + 1 + F r + n + 1 ) / ( F r + F r + n ) is a real number. Since [figure omitted; refer to PDF] it yields that sin ( ( 2 l + 1 ) π / n ) = 0 , so we have ω l η = - 1 for 0 < ( 2 l + 1 ) π / n < 2 π . Since x = - 1 is not the root of the equation, [figure omitted; refer to PDF] We obtain f ( ω k η ) ...0; 0 for any ω k η ( k = 1,2 , ... , n - 1 ) , while [figure omitted; refer to PDF] It follows from Lemma 3 in [21] that the conclusion holds.
Lemma 6.
Let the matrix G = [ g i , j ] i , j = 1 n - 2 be of the form [figure omitted; refer to PDF] Then the inverse G - 1 = [ g i , j [variant prime] ] i , j = 1 n - 2 of G is equal to [figure omitted; refer to PDF] In particular, when r = 0 , we get the result of [23].
Proof.
Let c i j = ∑ k = 1 n - 2 g i k g k j [variant prime] .
Then c i , j = 0 , for i < j , c i i = g i i g i i [variant prime] = ( F r + 1 + F r + n + 1 ) · 1 / ( F r + 1 + F r + n + 1 ) = 1 , for i = j , and [figure omitted; refer to PDF] for i ...5; j + 1 .
Hence, we get G G - 1 = I n - 2 , where I n - 2 is an ( n - 2 ) × ( n - 2 ) identity matrix. Similarly, we can verify G - 1 G = I n - 2 . Thus, the proof is completed.
Theorem 7.
Let B r , n = S C i r c ( F r + 1 , ... , F r + n ) be a skew circulant matrix; then, [figure omitted; refer to PDF] where [figure omitted; refer to PDF] In particular, when r = 0 , we get the result of [23].
Proof.
Let [figure omitted; refer to PDF] where [figure omitted; refer to PDF] Then we have [figure omitted; refer to PDF] Γ B r , n Π 1 Π 2 = D 1 [ecedil]5; G , D 1 = diag ... ( F r + 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 B r , n - 1 = Π ( D 1 - 1 [ecedil]5; G - 1 ) Γ .
Since the last row elements of the matrix Π are ( 0,1 , π 23 , π 24 , ... , π 2 ( n - 1 ) , π 2 n ), then the last row elements of the matrix Π ( D 1 - 1 [ecedil]5; G - 1 ) are ( 0 , 1 / f n , U 23 , U 24 , ... , U 2 n ) , where [figure omitted; refer to PDF] Hence it follows from Lemma 6 that letting B r , n - 1 = SCirc ( x 1 , x 2 , ... , x n ) then its last row elements are ( - x 2 , - x 3 , ... , - x n , x 1 ) which are given by the following equations: [figure omitted; refer to PDF] Hence, we obtain [figure omitted; refer to PDF] where [figure omitted; refer to PDF] This completes the proof.
3. Norm and Spread of Skew Circulant Matrix with the Fibonacci Numbers
Theorem 8.
Let B r , n = S C i r c ( F r + 1 , ... , F r + n ) be a skew circulant matrix; then three kinds of norms of B r , n are given by [figure omitted; refer to PDF]
Proof.
By Definition 8 in [21] and (5), we have [figure omitted; refer to PDF]
According to Definition 8 in [21] and (6), we know [figure omitted; refer to PDF] Thus [figure omitted; refer to PDF]
Theorem 9.
Let [figure omitted; refer to PDF] be an odd-order alternative skew circulant matrix and let n be odd. Then [figure omitted; refer to PDF]
Proof.
By Lemma 3 in [21], we have [figure omitted; refer to PDF] So [figure omitted; refer to PDF] for all j = 0,1 , ... , n - 1 .
Since n is odd, ∑ i = 1 n F r + i is an eigenvalue of B r , n [variant prime] ; that is [figure omitted; refer to PDF] To sum up, we can get [figure omitted; refer to PDF]
Since all skew circulant matrices are normal, by Lemma 9 in [21], (5), and (41), we obtain [figure omitted; refer to PDF] which completes the proof.
Theorem 10.
Let B r , n = S C i r c ( F r + 1 , ... , F r + n ) be a skew circulant matrix; then, the bounds for the spread of B r , n are [figure omitted; refer to PDF]
Proof.
The trace of B r , n is denoted by tr ... B r , n = n F r + 1 . By (18) in [21] and (32), we know [figure omitted; refer to PDF] Since [figure omitted; refer to PDF] furthermore, by (5) and (7), [figure omitted; refer to PDF] By (19) in [21], we have [figure omitted; refer to PDF]
4. Determinant and Inverse of Skew Left Circulant Matrix with the Fibonacci Numbers
In this section, let B r , n [variant prime][variant prime] = SLCirc ( F r + 1 , ... , F r + n ) be a skew left circulant matrix. By using the obtained conclusions in Section 2, we give a determinant explicit formula for the matrix B r , n [variant prime] [variant prime] . Afterwards, we prove that B r , n [variant prime] [variant prime] is an invertible matrix for any positive interger n . The inverse of the matrix B r , n [variant prime] [variant prime] is also presented.
According to Lemma 5 in [21], Lemma 6 in [21], and Theorems 4, 5, and 7, we can obtain the following theorems.
Theorem 11.
Let B r , n [variant prime] [variant prime] = S L C i r c ( F r + 1 , ... , F r + n ) be a skew left circulant matrix; then, [figure omitted; refer to PDF] where F r + n is the ( r + n ) th Fibonacci number.
Theorem 12.
Let B r , n [variant prime] [variant prime] = S L C i r c ( F r + 1 , ... , F r + n ) be a skew left circulant matrix; then, B r , n [variant prime] [variant prime] is an invertible matrix.
Theorem 13.
Let B r , n [variant prime] [variant prime] = S L C i r c ( F r + 1 , ... , F r + n ) be a skew left circulant matrix; then, [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
5. Norm and Spread of Skew Left Circulant Matrix with the Fibonacci Numbers
Theorem 14.
Let B r , n [variant prime] [variant prime] = S L C i r c ( F r + 1 , ... , F r + n ) be a skew left circulant matrix. Then three kinds of norms of B r , n [variant prime] [variant prime] are given by [figure omitted; refer to PDF]
Proof.
Using the method in Theorem 8 similarly, the conclusion is obtained.
Theorem 15.
Let [figure omitted; refer to PDF] be an odd-order alternative skew left circulant matrix; then, [figure omitted; refer to PDF]
Proof.
According to Lemma 4 in [21], [figure omitted; refer to PDF] for j = 1,2 , ... , ( n - 1 ) / 2 , and [figure omitted; refer to PDF] So [figure omitted; refer to PDF] By (55) and (56), we know [figure omitted; refer to PDF] Since all skew left circulant matrices are symmetrical, by Lemma 9 in [21], (5), and (57), we obtain [figure omitted; refer to PDF]
Theorem 16.
Let B r , n [variant prime] [variant prime] = S L C i r c ( F r + 1 , ... , F r + n ) be skew left circulant matrix, if n is odd, then [figure omitted; refer to PDF] if n is even, then [figure omitted; refer to PDF]
Proof.
Since B r , n [variant prime] [variant prime] is a symmetric matrix, by (20) in [21], [figure omitted; refer to PDF] If n is odd, the trace of B r , n [variant prime] [variant prime] is [figure omitted; refer to PDF] by (5), we know [figure omitted; refer to PDF]
By (18) in [21], (51), and (63), we obtain [figure omitted; refer to PDF] If n is even, the trace of B r , n [variant prime] [variant prime] is [figure omitted; refer to PDF] By (18) in [21], (51), and (65), we can get [figure omitted; refer to PDF] So the result follows.
6. Conclusion
We discuss the invertibility of skew circulant type matrices with any continuous Fibonacci numbers and present the determinant and the inverse matrices by constructing the transformation matrices. The four kinds of norms and bounds for the spread of these matrices are given, respectively. In [20], a new fast algorithm for optimal design of block digital filters (BDFs) was proposed based on skew circulant matrix. The reason why we focus our attentions on skew circulant is to explore the application of skew circulant in the related field in real-time tracking and networks engineering. On the basis of method of [17] and ideas of [43], we will exploit real-time tracking with kernel matrix of skew circulant structure. On the basis of existing application situation [1-11], we will exploit application of network engineering based on skew circulant matrix.
Acknowledgments
The research was supported by the Development Project of Science and Technology of Shandong Province (Grant no. 2012GGX10115) and NSFC (Grant no. 11301251) 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.
[1] M. P. Joy, V. Tavsanoglu, "Circulant matrices and the stability of a class of CNNs," International Journal of Circuit Theory and Applications , vol. 24, no. 1, pp. 7-13, 1996.
[2] D. Rocchesso, J. O. Smith, "Circulant and elliptic feedback delay networks for artificial reverberation," IEEE Transactions on Speech and Audio Processing , vol. 5, no. 1, pp. 51-63, 1997.
[3] Y. Jing, H. Jafarkhani, "Distributed differential space-time coding for wireless relay networks," IEEE Transactions on Communications , vol. 56, no. 7, pp. 1092-1100, 2008.
[4] H. Eghbali, S. Muhaidat, S. A. Hejazi, Y. Ding, "Relay selection strategies for single-carrier frequency-domain equalization multi-relay cooperative networks," IEEE Transactions on Wireless Communications , vol. 12, no. 5, pp. 2034-2045, 2013.
[5] D. Rocchesso, "Maximally diffusive yet efficient feedback delay networks for artificial reverberation," IEEE Signal Processing Letters , vol. 4, no. 9, pp. 252-255, 1997.
[6] S. Sardellitti, S. Barbarossa, A. Swami, "Optimal topology control and power allocation for minimum energy consumption in consensus networks," IEEE Transactions on Signal Processing , vol. 60, no. 1, pp. 383-399, 2012.
[7] J. Li, J. Yuan, R. Malaney, M. Xiao, W. Chen, "Full-diversity binary frame-wise network coding for multiple-source multiple-relay networks over slow-fading channels," IEEE Transactions on Vehicular Technology , vol. 61, no. 3, pp. 1346-1360, 2012.
[8] W. Hirt, J. L. Massey, "Capacity of the discrete-time Gaussian channel with intersymbol interference," IEEE Transactions on Information Theory , vol. 34, no. 3, pp. 380-388, 1988.
[9] H. Wang, X.-G. Xia, Q. Yin, "Distributed space-frequency codes for cooperative communication systems with multiple carrier frequency offsets," IEEE Transactions on Wireless Communications , vol. 8, no. 2, pp. 1045-1055, 2009.
[10] F. Gao, B. Jiang, X. Gao, X.-D. Zhang, "Superimposed training based channel estimation for OFDM modulated amplify-and-forward relay networks," IEEE Transactions on Communications , vol. 59, no. 7, pp. 2029-2039, 2011.
[11] G. Wang, F. Gao, Y.-C. Wu, C. Tellambura, "Joint CFO and channel estimation for OFDM-based two-way relay networks," IEEE Transactions on Wireless Communications , vol. 10, no. 2, pp. 456-465, 2011.
[12] D. Bertaccini, M. K. Ng, "Skew-circulant preconditioners for systems of LMF-based ODE codes," Numerical Analysis and Its Applications , vol. 1988, of Lecture Notes in Computer Science, pp. 93-101, 2001.
[13] R. H. Chan, X.-Q. Jin, "Circulant and skew-circulant preconditioners for skew-Hermitian type Toeplitz systems," BIT , vol. 31, no. 4, pp. 632-646, 1991.
[14] R. H. Chan, M.-K. Ng, "Toeplitz preconditioners for Hermitian Toeplitz systems," Linear Algebra and Its Applications , vol. 190, pp. 181-208, 1993.
[15] T. Huckle, "Circulant and skewcirculant matrices for solving Toeplitz matrix problems," SIAM Journal on Matrix Analysis and Applications , vol. 13, no. 3, pp. 767-777, 1992.
[16] J. N. Lyness, T. Sørevik, "Four-dimensional lattice rules generated by skew-circulant matrices," Mathematics of Computation , vol. 73, no. 245, pp. 279-295, 2004.
[17] M. J. Narasimha, "Linear convolution using skew-cyclic convolutions," IEEE Signal Processing Letters , vol. 14, no. 3, pp. 173-176, 2007.
[18] V. C. Liu, P. P. Vaidyanathan, "Circulant and skew-circulant matrices as new normal-form realization of IIR digital filters," IEEE Transactions on Circuits and Systems , vol. 35, no. 6, pp. 625-635, 1988.
[19] J. Li, Z. Jiang, N. Shen, J. Zhou, "On optimal backward perturbation analysis for the linear system with skew circulant coefficient matrix," Computational and Mathematical Methods in Medicine , vol. 2013, 2013.
[20] D. Q. Fu, Z. L. Jiang, Y. F. Cui, S. T. Jhang, "A new fast algorithm for optimal design of block digital filters by skew-cyclic convolution," IET Signal Processing , 2014.
[21] J.-J. Yao, Z.-L. Jiang, "The determinants, inverses, norm, and spread of skew circulant type matrices involving any continuous lucas numbers," Journal of Applied Mathematics , vol. 2014, 2014.
[22] S.-Q. Shen, J.-M. Cen, Y. Hao, "On the determinants and inverses of circulant matrices with Fibonacci and Lucas numbers," Applied Mathematics and Computation , vol. 217, no. 23, pp. 9790-9797, 2011.
[23] Y. Gao, Z. Jiang, Y. Gong, "On the determinants and inverses of skew circulant and skew left circulant matrices with Fibonacci and Lucas numbers," WSEAS Transactions on Mathematics , vol. 12, no. 4, pp. 472-481, 2013.
[24] X.-Y. Jiang, Y. Gao, Z.-L. Jiang, "Determinants and inverses of skew and skew left circulant matrices involving the k -Fibonacci numbers in communications-I," Far East Journal of Mathematical Sciences , vol. 76, no. 1, pp. 123-137, 2013.
[25] X.-Y. Jiang, Y. Gao, Z.-L. Jiang, "Determinants and inverses of skew and skew left circulant matrices involving the k -Lucas numbers in communications-II," Far East Journal of Mathematical Sciences , vol. 78, no. 1, pp. 1-17, 2013.
[26] D. V. Jaiswal, "On determinants involving generalized Fibonacci numbers," The Fibonacci Quarterly , vol. 7, pp. 319-330, 1969.
[27] D. A. Lind, "A Fibonacci circulant," The Fibonacci Quarterly , vol. 8, no. 5, pp. 449-455, 1970.
[28] L. Dazheng, "Fibonacci-Lucas quasi-cyclic matrices," The Fibonacci Quarterly , vol. 40, no. 3, pp. 280-286, 2002.
[29] S. Solak, "On the norms of circulant matrices with the Fibonacci and Lucas numbers," Applied Mathematics and Computation , vol. 160, no. 1, pp. 125-132, 2005.
[30] A. Ipek, "On the spectral norms of circulant matrices with classical Fibonacci and Lucas numbers entries," Applied Mathematics and Computation , vol. 217, no. 12, pp. 6011-6012, 2011.
[31] S. Shen, J. Cen, "On the bounds for the norms of r -circulant matrices with the Fibonacci and Lucas numbers," Applied Mathematics and Computation , vol. 216, no. 10, pp. 2891-2897, 2010.
[32] M. Akbulak, D. Bozkurt, "On the norms of Toeplitz matrices involving Fibonacci and Lucas numbers," Hacettepe Journal of Mathematics and Statistics , vol. 37, no. 2, pp. 89-95, 2008.
[33] A. Bose, R. S. Hazra, K. Saha, "Spectral norm of circulant-type matrices," Journal of Theoretical Probability , vol. 24, no. 2, pp. 479-516, 2011.
[34] L. Mirsky, "The spread of a matrix," Mathematika , vol. 3, pp. 127-130, 1956.
[35] R. Sharma, R. Kumar, "Remark on upper bounds for the spread of a matrix," Linear Algebra and Its Applications , vol. 438, no. 11, pp. 4359-4362, 2013.
[36] J. Wu, P. Zhang, W. Liao, "Upper bounds for the spread of a matrix," Linear Algebra and Its Applications , vol. 437, no. 11, pp. 2813-2822, 2012.
[37] C. R. Johnson, R. Kumar, H. Wolkowicz, "Lower bounds for the spread of a matrix," Linear Algebra and Its Applications , vol. 29, pp. 161-173, 1985.
[38] V. W. de Spinadel, K. Williams, "The metallic means and design," Nexus II: Architecture and Mathematics , vol. 5, pp. 143-157, Edizioni dell'Erba, 1998.
[39] V. W. de Spinadel, "The metallic means family and forbidden symmetries," International Mathematical Journal , vol. 2, no. 3, pp. 279-288, 2002.
[40] M. S. El Naschie, "Modular groups in Cantorian E∞ high-energy physics," Chaos, Solitons & Fractals , vol. 16, no. 2, pp. 353-366, 2003.
[41] S. Falcón, Á. Plaza, "The k -Fibonacci hyperbolic functions," Chaos, Solitons & Fractals , vol. 38, no. 2, pp. 409-420, 2008.
[42] A. P. Stakhov, I. S. Tkachenko, "Hyperbolic trigonometry of Fibonacci," Reports of the National Academy of Sciences of Ukraine , vol. 208, no. 7, pp. 9-14, 1993.
[43] J. F. Henriques, R. Caseiro, P. Martins, J. Batista, "Exploiting the circulant structure of tracking-by-detection with kernels," in Proceedings of the European Conference on Computer Vision (ECCV '12), pp. 1-14, 2012.
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Abstract
Circulant and skew circulant matrices have become an important tool in networks engineering. In this paper, we consider skew circulant type matrices with any continuous Fibonacci numbers. We discuss the invertibility of the skew circulant type matrices and present explicit determinants and inverse matrices of them by constructing the transformation matrices. Furthermore, the maximum column sum matrix norm, the spectral norm, the Euclidean (or Frobenius) norm, and the maximum row sum matrix norm and bounds for the spread of these matrices are given, respectively.
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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





