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The core inverse and constrained matrix approximation problem

  • Hongxing Wang EMAIL logo and Xiaoyan Zhang
Published/Copyright: July 6, 2020

Abstract

In this article, we study the constrained matrix approximation problem in the Frobenius norm by using the core inverse:

| | M x b | | F = min subject to x ( M ) ,

where M n CM . We get the unique solution to the problem, provide two Cramer’s rules for the unique solution and establish two new expressions for the core inverse.

MSC 2010: 15A24; 15A29; 15A57

1 Introduction

Let M , ( M ) and N ( M ) stand for the conjugate transpose, range space and null space of M m × n , respectively. The symbol M ( i b ) denotes a matrix from M by replacing the ith column of M by b n . The symbol e i denotes the ith column of I n in which 1 i n . The Moore-Penrose inverse of M is the unique matrix X n × m satisfying the relations: M X M = M , X M X = X , ( M X ) = M X and ( X M ) = X M and is denoted by X = M [1,2,3].

Let M n × n be singular. The smallest positive integer k for which rk ( M k + 1 ) = rk ( M k ) is called the index of M and is denoted by Ind ( M ) . The index of a non-singular matrix is 0 and the index of a null matrix is 1. Furthermore,

(1.1) n CM = { M | Ind ( M ) 1 , M n × n } .

Let M n × n with Ind ( M ) = k . A matrix X is the Drazin inverse of M if M X M k = M k , X M X = X and M X = X M . We write X = M D for the Drazin inverse of M. In particular, when M n CM , the matrix X is the group inverse of M and is denoted by X = M # [1,2,3].

The core inverse of M n CM is defined as the unique matrix X n × n satisfying the equations: M X M = M , M X 2 = X and ( M X ) = M X and is denoted by X = M [4,5]. It is noteworthy that the core inverse is a “least squares” inverse [6,7]. Moreover, it is proved that M = M # M M [4].

Recently, the relevant conclusions of the core inverse are very rich. In [7,8,9,10], generalizations of core inverse are introduced, for example, the core-EP inverse and the weak group inverse. In [11,12,13,14,15], their algebraic properties and calculating methods are studied. In [16,17], the studying of them is extended to some new fields, for example, ring and operator. Moreover, those inverses are used to study partial orders in [4,5,10,18,19].

Consider the following equation:

(1.2) M x = b .

Let M n × n with Ind ( M ) = k and b ( M k ) . Campbell and Meyer [20] show that x = M D b is the unique solution of (1.2) with respect to x ( M k ) . Wei [21] gets the minimal P-norm solution of (1.2), where P is nonsingular, P 1 M P is the Jordan canonical form of M and x p = P 1 x 2 . Furthermore, let M m × n . Wei [22] considered the unique solution of

W M W x = b subject to x ( ( M W ) k 1 ) ,

where W n × m , k 1 = Ind ( M W ) , k 2 = Ind ( W M ) and b ( ( W M ) k 2 ) . More results of (1.2) under some certain conditions can be found in [3,21,23,24,25,26,27].

It is well known that b ( M ) if and only if (1.2) is solvable. Let b ( M ) and the index of M is 1, then x = M # b is the unique solution with x ( M ) [20]. It follows from M = M # M M that M # b = M b [28]. Furthermore, the unique solution x = M b is given by Cramer’s rule [28, Theorem 3.3].

When b ( M ) , (1.2) is unsolvable, yet, it has least-squares solutions. Motivated by the aforementioned works, it is natural to consider the least-squares solutions of (1.2) under the certain condition x ( M ) , i.e.,

(1.3) M x b F = min subject to x ( M ) ,

where M n CM , rk ( M ) = r < n and b n .

2 Preliminaries

Lemma 2.1

[1] Let M n × n be idempotent. Then, M = P ( M ) , N ( M ) with M N M = n . In contrast, if F G = n , then there exists an idempotent P F , G such that ( P F , G ) = F and N ( P F , G ) = G .

Furthermore, I n P F , G = P G , F .

Lemma 2.2

[3] Let M n × n . Then, Ind ( M ) = k if and only if

(2.1) ( M k ) N ( M k ) = n .

Lemma 2.3

[3] Let M X M = M and X M X = X . Then,

X M = P ( X ) , N ( M ) and M X = P ( M ) , N ( X ) .

Lemma 2.4

[3] Let F G = n . Then,

  1. P F , G M = M ( M ) F ;

  2. M P F , G = M N ( M ) G .

Lemma 2.5

[14] Let M n CM with rk ( M ) = r . Then, there exists a unitary matrix V such that

(2.2) M = V T S 0 0 V ,

where T r × r is nonsingular. Furthermore,

(2.3) M = V T 1 0 0 0 V .

3 Main results

3.1 Solution of (1.3)

Theorem 3.1

Let M n CM and b n . Then,

(3.1) x = M b

is the unique solution of ( 1.3 ).

Proof

From x ( M ) , it follows that there exists y n for which x = M y . Then, x is the solution of (1.3) if and only if y is the solution of

(3.2) M 2 y b F = min .

Let the decomposition of M be as in (2.2). Denote

(3.3) V y = y 1 y 2 , V b = b 1 b 2 and M b = V T 1 b 1 0 ,

where y 1 , b 1 and T 1 b 1 rk ( M ) . It follows that

M x b F 2 = T 2 y 1 + T S y 2 b 1 b 2 F 2 = T 2 y 1 + T S y 2 b 1 F 2 + b 2 F 2 .

Since T is invertible, we have min y 1 , y 2 T 2 y 1 + T S y 2 b 1 F 2 = 0 , that is, M 2 y b F = min = b 2 F , in which y 2 n rk ( M ) is arbitrary, and y 1 = T 2 b 1 T 1 S y 2 . It follows that

x = M y = V T S 0 0 V y = V T y 1 + S y 2 0 = V T 1 b 1 0 = M b ,

that is, (3.1) is the unique solution of (1.3).□

3.2 Determinantal formulas

When M n × n is nonsingular, it is well known that the solution of (1.2) is unique and x = M 1 b . Let x = ( x 1 , x 2 , , x n ) T . Then,

(3.4) x i = det ( M ( i b ) ) det ( M ) , i = 1 , 2 , , n ,

is called Cramer’s rule for solving (1.2). In [29], Ben-Israel gets a Cramer’s rule for obtaining the least-norm solution of the consistent linear system (1.2),

x i = det M ( i b ) U V ( i 0 ) 0 det M U V 0 , i = 1 , 2 , , n ,

where U and V are of full column rank, ( U ) = N ( M ) and ( V ) = N ( M ) . In [26], Wang gives a Cramer’s rule for the unique solution x ( M k ) of (1.2), where b ( M k ) and Ind ( M ) = k . In [30], Ji proposes two new condensed Cramer’s rules for the unique solution x ( M k ) of (1.2), where b ( M k ) and Ind ( M ) = k . More details of Cramer’s rules for finding restricted solutions of (1.2) can be found in [1,3,31,32,33,34,35,36]. In Theorems 3.4 and 3.6, we will give two Cramer’s rules for the unique solution of (1.3).

First of all, we give the following two lemmas to prepare for a Cramer’s rule for core inverse in Theorem 3.4.

Lemma 3.2

Let M n CM with rk ( M ) = r , and let L n × ( n r ) with rk ( L ) = n r and ( L ) = N ( M ) . Then,

(3.5) M M + ( I n M M ) L ( L L ) 1 L = I n .

Proof

Let M be as in (2.2), applying Lemma 2.2, we see that

(3.6) ( M ) N ( M ) = n .

Denote M 1 = I n M M and M 2 = L ( L L ) 1 L .

Applying Lemmas 2.1, 2.3 and M M = M # M , we have

(3.7) M M = P ( M ) , N ( M ) ,

(3.8) M 1 = I M M = P N ( M ) , ( M ) .

Since ( L ( L L ) 1 ) L ( L ( L L ) 1 ) = L ( L L ) 1 and L ( L ( L L ) 1 ) L = L , applying Lemma 2.3, we obtain

(3.9) M 2 = P ( L ) , N ( L ) = P N ( M ) , ( M ) .

Since ( L ) = N ( M ) , we obtain M 2 M 1 = M 2 and

(3.10) M 1 M 2 = P N ( M ) , ( M ) .

Therefore, applying Lemma 2.1, (3.7) and (3.10), we gain

M M + M 1 M 2 = P ( M ) , N ( M ) + P N ( M ) , ( M ) = I n ,

i.e., (3.5).□

In [28, Theorems 3.2 and 3.3], let M n C M , b n and b ( M ) , and let M b and M c be of the full column ranks with N ( M ) = ( M b ) and N ( M c ) = ( M ) . Then,

M M b M c 0

is invertible and the unique solution x = M b of (1.2) satisfying

x i = det M i b M b M c i 0 0 / det M M b M c 0 ,

where i = 1 , 2 , , n . In Lemma 3.3 and Theorem 3.4, we give the unique least-squares solution of (1.3) in a similar way.

Lemma 3.3

Let M and L be as in Lemma 3.2. Then,

(3.11) G = M L L 0

is invertible and

(3.12) G 1 = M ( I n M M ) L ( L L ) 1 ( L L ) 1 L 0 .

Proof

Since ( L ) = N ( M ) and M = M # M M , we have M L = M # M M L = 0 and ( L L ) 1 L M = 0 . Furthermore, applying (3.5), we have

M ( I n M M ) L ( L L ) 1 ( L L ) 1 L 0 M L L 0 = M M + ( I n M M ) L ( L L ) 1 L M L ( L L ) 1 L M ( L L ) 1 L L = I 2 n r ,

that is, G is invertible and G 1 is of the form (3.12).□

Based on Lemmas 3.2 and 3.3, we get a Cramer’s rule for the unique solution of (1.3).

Theorem 3.4

Let M and b be as in Lemma 3.2, and let L be as in Lemma 3.2. Then, (1.3) has the unique solution x = ( x 1 , x 2 , , x n ) T satisfying

(3.13) x i = det M ( i b ) L L ( i 0 ) 0 / det M L L 0 ,

where i = 1 , 2 , , n .

Proof

Since G is invertible, applying Lemma 3.3, we get the unique solution x ˆ = G 1 b ˆ of G x ˆ = b ˆ , in which x ˆ = [ x y ] and b ˆ = b 0 . It follows from (3.12) that

x y = M ( I n M M ) L ( L L ) 1 ( L L ) 1 L 0 b 0 = M b ( L L ) 1 L b .

Applying (3.4) we obtain (3.13).□

In the following theorem, we give a characterization of the core inverse and prepare for a Cramer’s rule for the core inverse in Theorem 3.6.

Theorem 3.5

Let M and L be as in Lemma 3.2. Then,

(3.14) M = ( M M M + L L ) 1 M M .

Proof

Since ( L ) = N ( M ) , M n CM and ( M ) = N ( M ) , we obtain

( L L ) ( L L ) = P N ( M ) , ( M ) , ( M M M ) ( M M M ) = P ( M ) , N ( M )

and

( M M M + L L ) ( ( M M M ) + ( L L ) ( M M M ) M M M ( L L ) ) = ( M M M ) ( M M M ) + ( L L ) ( L L ) = P ( M ) , N ( M ) + P N ( M ) , ( M ) = I n .

Therefore, M M M + L L is invertible.

Since ( L L ) M M = 0 and ( M M M ) M M = M , we have

( M M M + L L ) 1 M M = ( M M M ) M M + ( L L ) M M = M .

It follows that we get (3.14).□

Theorem 3.6

Let M and L be as in Lemma 3.2. Then, (1.3) has the unique solution x = ( x 1 , x 2 , , x n ) T satisfying

(3.15) x j = det ( M M M + L L ) ( j M M b ) det ( M M M + L L ) ,

where j = 1 , 2 , , n .

Proof

Applying Theorems 3.5 to 3.1, we have

x = ( M M M + L L ) 1 M M b ,

that is,

( M M M + L L ) x = M M b .

It follows from (3.4) that we get (3.15).□

In [30], Ji obtains the condensed determinantal expressions of M and M D . By using Theorem 3.5, we get a condensed determinantal expression of M .

Theorem 3.7

Let M and L be defined as in (3.11). Then, the core inverse M is given by:

(3.16) M i , j = det ( M M M + L L ) ( i ( M M ) e j ) det ( M M M + L L ) ,

where 1 i , j n .

Proof

Since M M M + L L is invertible, we consider

( M M M + L L ) x = ( M M ) e j

and get the solution

e i T x = det ( M M M + L L ) ( i ( M M ) e j ) det ( M M M + L L ) ,

in which i , j = 1 , , n .

It follows from (3.14) and M i , j = e i T M e j that we get (3.16).□

3.3 Examples

In the following examples, we show that our results are effective.

Example 3.1

Let M = 1 2 2 0 0 0 0 0 0 , L = 0 0 1 0 0 1 and b = 1 1 1 . It is easy to check that ( L ) = N ( M ) . By applying Lemma 3.3, we have M = 1 0 0 0 0 0 0 0 0 . Then, ( I n M M ) L ( L L ) 1 = 2 2 1 0 0 1 , ( L L ) 1 L = 0 1 0 0 0 1 , G = 1 2 2 0 0 0 0 0 1 0 0 0 0 0 1 0 1 0 0 0 0 0 1 0 0 , det ( G ) = 1 and G 1 = 1 0 0 2 2 0 0 0 1 0 0 0 0 0 1 0 1 0 0 0 0 0 1 0 0 .

By applying Theorem 3.1, we get the solution of (1.3) is x = M b = 1 0 0 .

For det 1 0 0 2 2 1 0 0 1 0 1 0 0 0 1 0 1 0 0 0 0 0 1 0 0 = 1 and det 1 1 2 0 0 0 1 0 1 0 0 1 0 0 1 0 0 0 0 0 0 0 1 0 0 = det 1 2 1 0 0 0 0 1 1 0 0 0 1 0 1 0 1 0 0 0 0 0 0 0 0 = 0 , by applying Theorem 3.4, we get x 1 = 1 1 , x 2 = 0 1 and x 3 = 0 1 . Therefore, the solution of (1.3) is x = 1 0 0 .

For det ( M M M + L L ) = det 9 18 18 0 1 0 0 0 1 = 9 , M M b = 9 0 0 ,

det ( M M M + L L ) ( 1 M M b ) = det 9 18 18 0 1 0 0 0 1 = 9 ,

det ( M M M + L L ) ( 2 M M b ) = 0 , det ( M M M + L L ) ( 3 M M b ) = 0 , and by applying Theorem 3.6, we get x 1 = 9 9 , x 2 = 0 9 and x 3 = 0 9 . Therefore, the solution of (1.3) is x = 1 0 0 .

Example 3.2

Let

M = 1 / 4 1 / 8 1 / 8 1 / 4 1 / 8 1 / 8 1 / 4 0 1 / 4 .

Then,

M # = 1 3 2 1 3 2 1 5 6 , M # = 4 / 3 4 / 3 0 8 / 3 8 / 3 4 4 / 3 4 / 3 4 , M = 2 2 2 2 2 2 2 2 6

and

L = 1 1 0

with rk ( L ) = n r and ( L ) = N ( M ) . It is easy to check that

M M M + L L = 137 / 128 125 / 128 3 / 64 119 / 128 131 / 128 3 / 64 5 / 64 3 / 128 7 / 128 .

By applying Theorem 3.5, we get

( M M M + L L ) 1 M M = 2 2 2 2 2 2 2 2 6 = M .

For

det ( M M M + L L ) = 3 / 4096 , det ( M M M + L L ) ( 1 ( M M ) e 1 ) = 3 / 2048 , det ( M M M + L L ) ( 1 ( M M ) e 2 ) = 3 / 2048 , det ( M M M + L L ) ( 1 ( M M ) e 3 ) = 3 / 2048 , det ( M M M + L L ) ( 2 ( M M ) e 1 ) = 3 / 2048 , det ( M M M + L L ) ( 2 ( M M ) e 2 ) = 3 / 2048 , det ( M M M + L L ) ( 2 ( M M ) e 3 ) = 3 / 2048 , det ( M M M + L L ) ( 3 ( M M ) e 1 ) = 3 / 2048 , det ( M M M + L L ) ( 3 ( M M ) e 2 ) = 3 / 2048 , det ( M M M + L L ) ( 3 ( M M ) e 3 ) = 9 / 2048 ,

by applying Theorem 3.7, we get

M 11 = 2 , M 12 = 2 , M 13 = 2 , M 21 = 2 , M 22 = 2 , M 23 = 2 , M 31 = 2 , M 32 = 2 , M 33 = 6 ,

that is,

M = 2 2 2 2 2 2 2 2 6 .

Acknowledgments

Hongxing Wang was supported partially by the Guangxi Natural Science Foundation (grant number 2018GXNSFAA138181), the Special Fund for Science and Technological Bases and Talents of Guangxi (grant number GUIKE AD19245148), the Xiangsihu Young Scholars Innovative Research Team of Guangxi University for Nationalities (grant number 2019RSCXSHQN03) and the Special Fund for Bagui Scholars of Guangxi (grant number 2016A17). Xiaoyan Zhang was supported partially by the National Natural Science Foundation of China (grant number 11361009) and High Level Innovation Teams and Distinguished Scholars in Guangxi Universities (grant number GUIJIAOREN201642HAO).

  1. Conflict of interest: The authors report no potential conflict of interest.

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Received: 2019-08-30
Revised: 2020-03-07
Accepted: 2020-04-28
Published Online: 2020-07-06

© 2020 Hongxing Wang and Xiaoyan Zhang, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  39. Analysis of F-contractions in function weighted metric spaces with an application
  40. On finite dual Cayley graphs
  41. Left and right inverse eigenpairs problem with a submatrix constraint for the generalized centrosymmetric matrix
  42. Controllability of fractional stochastic evolution equations with nonlocal conditions and noncompact semigroups
  43. Levinson-type inequalities via new Green functions and Montgomery identity
  44. The core inverse and constrained matrix approximation problem
  45. A pair of equations in unlike powers of primes and powers of 2
  46. Miscellaneous equalities for idempotent matrices with applications
  47. B-maximal commutators, commutators of B-singular integral operators and B-Riesz potentials on B-Morrey spaces
  48. Rate of convergence of uniform transport processes to a Brownian sheet
  49. Curves in the Lorentz-Minkowski plane with curvature depending on their position
  50. Sequential change-point detection in a multinomial logistic regression model
  51. Tiny zero-sum sequences over some special groups
  52. A boundedness result for Marcinkiewicz integral operator
  53. On a functional equation that has the quadratic-multiplicative property
  54. The spectrum generated by s-numbers and pre-quasi normed Orlicz-Cesáro mean sequence spaces
  55. Positive coincidence points for a class of nonlinear operators and their applications to matrix equations
  56. Asymptotic relations for the products of elements of some positive sequences
  57. Jordan {g,h}-derivations on triangular algebras
  58. A systolic inequality with remainder in the real projective plane
  59. A new characterization of L2(p2)
  60. Nonlinear boundary value problems for mixed-type fractional equations and Ulam-Hyers stability
  61. Asymptotic normality and mean consistency of LS estimators in the errors-in-variables model with dependent errors
  62. Some non-commuting solutions of the Yang-Baxter-like matrix equation
  63. General (p,q)-mixed projection bodies
  64. An extension of the method of brackets. Part 2
  65. A new approach in the context of ordered incomplete partial b-metric spaces
  66. Sharper existence and uniqueness results for solutions to fourth-order boundary value problems and elastic beam analysis
  67. Remark on subgroup intersection graph of finite abelian groups
  68. Detectable sensation of a stochastic smoking model
  69. Almost Kenmotsu 3-h-manifolds with transversely Killing-type Ricci operators
  70. Some inequalities for star duality of the radial Blaschke-Minkowski homomorphisms
  71. Results on nonlocal stochastic integro-differential equations driven by a fractional Brownian motion
  72. On surrounding quasi-contractions on non-triangular metric spaces
  73. SEMT valuation and strength of subdivided star of K 1,4
  74. Weak solutions and optimal controls of stochastic fractional reaction-diffusion systems
  75. Gradient estimates for a weighted nonlinear parabolic equation and applications
  76. On the equivalence of three-dimensional differential systems
  77. Free nonunitary Rota-Baxter family algebras and typed leaf-spaced decorated planar rooted forests
  78. The prime and maximal spectra and the reticulation of residuated lattices with applications to De Morgan residuated lattices
  79. Explicit determinantal formula for a class of banded matrices
  80. Dynamics of a diffusive delayed competition and cooperation system
  81. Error term of the mean value theorem for binary Egyptian fractions
  82. The integral part of a nonlinear form with a square, a cube and a biquadrate
  83. Meromorphic solutions of certain nonlinear difference equations
  84. Characterizations for the potential operators on Carleson curves in local generalized Morrey spaces
  85. Some integral curves with a new frame
  86. Meromorphic exact solutions of the (2 + 1)-dimensional generalized Calogero-Bogoyavlenskii-Schiff equation
  87. Towards a homological generalization of the direct summand theorem
  88. A standard form in (some) free fields: How to construct minimal linear representations
  89. On the determination of the number of positive and negative polynomial zeros and their isolation
  90. Perturbation of the one-dimensional time-independent Schrödinger equation with a rectangular potential barrier
  91. Simply connected topological spaces of weighted composition operators
  92. Generalized derivatives and optimization problems for n-dimensional fuzzy-number-valued functions
  93. A study of uniformities on the space of uniformly continuous mappings
  94. The strong nil-cleanness of semigroup rings
  95. On an equivalence between regular ordered Γ-semigroups and regular ordered semigroups
  96. Evolution of the first eigenvalue of the Laplace operator and the p-Laplace operator under a forced mean curvature flow
  97. Noetherian properties in composite generalized power series rings
  98. Inequalities for the generalized trigonometric and hyperbolic functions
  99. Blow-up analyses in nonlocal reaction diffusion equations with time-dependent coefficients under Neumann boundary conditions
  100. A new characterization of a proper type B semigroup
  101. Constructions of pseudorandom binary lattices using cyclotomic classes in finite fields
  102. Estimates of entropy numbers in probabilistic setting
  103. Ramsey numbers of partial order graphs (comparability graphs) and implications in ring theory
  104. S-shaped connected component of positive solutions for second-order discrete Neumann boundary value problems
  105. The logarithmic mean of two convex functionals
  106. A modified Tikhonov regularization method based on Hermite expansion for solving the Cauchy problem of the Laplace equation
  107. Approximation properties of tensor norms and operator ideals for Banach spaces
  108. A multi-power and multi-splitting inner-outer iteration for PageRank computation
  109. The edge-regular complete maps
  110. Ramanujan’s function k(τ)=r(τ)r2(2τ) and its modularity
  111. Finite groups with some weakly pronormal subgroups
  112. A new refinement of Jensen’s inequality with applications in information theory
  113. Skew-symmetric and essentially unitary operators via Berezin symbols
  114. The limit Riemann solutions to nonisentropic Chaplygin Euler equations
  115. On singularities of real algebraic sets and applications to kinematics
  116. Results on analytic functions defined by Laplace-Stieltjes transforms with perfect ϕ-type
  117. New (p, q)-estimates for different types of integral inequalities via (α, m)-convex mappings
  118. Boundary value problems of Hilfer-type fractional integro-differential equations and inclusions with nonlocal integro-multipoint boundary conditions
  119. Boundary layer analysis for a 2-D Keller-Segel model
  120. On some extensions of Gauss’ work and applications
  121. A study on strongly convex hyper S-subposets in hyper S-posets
  122. On the Gevrey ultradifferentiability of weak solutions of an abstract evolution equation with a scalar type spectral operator on the real axis
  123. Special Issue on Graph Theory (GWGT 2019), Part II
  124. On applications of bipartite graph associated with algebraic structures
  125. Further new results on strong resolving partitions for graphs
  126. The second out-neighborhood for local tournaments
  127. On the N-spectrum of oriented graphs
  128. The H-force sets of the graphs satisfying the condition of Ore’s theorem
  129. Bipartite graphs with close domination and k-domination numbers
  130. On the sandpile model of modified wheels II
  131. Connected even factors in k-tree
  132. On triangular matroids induced by n3-configurations
  133. The domination number of round digraphs
  134. Special Issue on Variational/Hemivariational Inequalities
  135. A new blow-up criterion for the Nabc family of Camassa-Holm type equation with both dissipation and dispersion
  136. On the finite approximate controllability for Hilfer fractional evolution systems with nonlocal conditions
  137. On the well-posedness of differential quasi-variational-hemivariational inequalities
  138. An efficient approach for the numerical solution of fifth-order KdV equations
  139. Generalized fractional integral inequalities of Hermite-Hadamard-type for a convex function
  140. Karush-Kuhn-Tucker optimality conditions for a class of robust optimization problems with an interval-valued objective function
  141. An equivalent quasinorm for the Lipschitz space of noncommutative martingales
  142. Optimal control of a viscous generalized θ-type dispersive equation with weak dissipation
  143. Special Issue on Problems, Methods and Applications of Nonlinear analysis
  144. Generalized Picone inequalities and their applications to (p,q)-Laplace equations
  145. Positive solutions for parametric (p(z),q(z))-equations
  146. Revisiting the sub- and super-solution method for the classical radial solutions of the mean curvature equation
  147. (p,Q) systems with critical singular exponential nonlinearities in the Heisenberg group
  148. Quasilinear Dirichlet problems with competing operators and convection
  149. Hyers-Ulam-Rassias stability of (m, n)-Jordan derivations
  150. Special Issue on Evolution Equations, Theory and Applications
  151. Instantaneous blow-up of solutions to the Cauchy problem for the fractional Khokhlov-Zabolotskaya equation
  152. Three classes of decomposable distributions
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