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Approximation of the image of the Lp ball under Hilbert-Schmidt integral operator

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Published/Copyright: April 11, 2023
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Abstract

In this article, an approximation of the image of the closed ball of the space L p ( p > 1 ) centered at the origin with radius r under Hilbert-Schmidt integral operator F ( ) : L p L q , 1 p + 1 q = 1 is considered. An error evaluation for the given approximation is obtained.

MSC 2010: 47G10; 47B38; 65R10; 93C35

1 Introduction

Integral operators arise in various problems of theory and applications and are one of the important tools to investigate different types of problems in mathematics. For example, integral operators are used in integral equations of the Fredholm, Volterra, Urysohn-Hammerstein and other types and play a crucial role in the definition of solution concepts for different types of initial and boundary value problems of differential equations (see, e.g., [13] and references therein). It is necessary to underline that the theory of linear integral equations is considered one of the origins of contemporary functional analysis [46]. In particular, the integral operators are used to describe the behavior of some input–output systems (see, e.g., [79]).

In this article an approximation of the image of the closed ball of the space L p ( p > 1 ) centered at the origin under the Hilbert-Schmidt integral operator is considered. The presented approximation method allows for every ε > 0 to construct a finite ε -net on the image of the closed ball, which consists of the images of a finite number of piecewise-constant functions. An approximation of the image of a given closed ball can be used in infinite-dimensional optimization problems for predetermining the desirable inputs for the input–output system described by Hilbert-Schmidt integral operator. Note that the input functions with integral constraints are usually applied when the input resources of the system are exhausted by consumption, such as energy, fuel, and finance (see, e.g., [1012] and references therein). An error evaluation of the Hausdorff distance between the image of the closed ball and its approximation, which consists of a finite number of functions, is given.

The article is organized as follows. In Section 2, the conditions and auxiliary propositions that are used in the following arguments are formulated. In Section 3, the image of the integral operator is approximated by the set, consisting of a finite number of functions. An error estimation depending on the approximation parameters is given (Theorem 1).

2 Preliminaries

Consider the Hilbert-Schmidt integral operator

(1) F ( x ( ) ) ( ξ ) = Ω K ( ξ , s ) x ( s ) d s for almost all ξ E ,

where x ( s ) R n , K ( ξ , s ) is an m × n dimensional matrix function, ( ξ , s ) E × Ω , E R b and Ω R k are compact sets.

For given p > 1 and r > 0 , we denote

B p ( r ) = { x ( ) L p ( Ω ; R n ) : x ( ) p r } ,

where L p ( Ω ; R n ) is the space of Lebesgue measurable functions x ( ) : Ω R n such that x ( ) p < + , x ( ) p = Ω x ( s ) p d s 1 p , and denotes the Euclidean norm.

It is assumed that the matrix function K ( , ) : E × Ω R m × n is Lebesgue measurable and

E Ω K ( ξ , s ) q d s d ξ < + ,

where 1 q + 1 p = 1 . Denote

(2) p ( r ) = { F ( x ( ) ) ( ) : x ( ) B p ( r ) } .

It is obvious that the set p ( r ) is the image of the set B p ( r ) under Hilbert-Schmidt integral operator (1). Since operator F ( ) is linear and compact one, then the set p ( r ) is a convex and compact subset of the space L q ( E ; R m ) .

Since the set of continuous functions Φ ( , ) : E × Ω R m × n is dense in the space L q ( E × Ω ; R m × n ) (see, e.g., [13], p. 318), then, for every λ > 0 , there exists a continuous function K λ ( , ) : E × Ω R m × n such that

(3) E Ω K ( ξ , s ) K λ ( ξ , s ) q d s d ξ 1 q λ 2 r .

Denote

(4) M ( λ ) = max { K λ ( ξ , s ) : ( ξ , s ) E × Ω } ,

(5) ω λ ( Δ ) = max { K λ ( ξ , s 2 ) K λ ( ξ , s 1 ) : ( ξ , s 2 ) E × Ω , ( ξ , s 1 ) E × Ω , s 2 s 1 Δ } ,

where Δ > 0 is a given number. The compactness of the sets E R b and Ω R k and continuity of the function K λ ( , ) : E × Ω R m × n imply that, for each fixed λ > 0 , we have ω λ ( Δ ) 0 as Δ 0 + and ω λ ( Δ 1 ) ω λ ( Δ 2 ) if Δ 1 < Δ 2 .

Let us define a finite Δ -partition of a given set D R n 0 , which will be used in following arguments.

Definition 1

Let Δ > 0 and D R n 0 . A finite family of sets Λ = { D 1 , D 2 , , D l } is called a finite Δ -partition of the set D , if

  1. D i D and D i is Lebesgue measurable for every i = 1 , 2 , , l ;

  2. D i D j = for every i j , where i = 1 , 2 , , l and j = 1 , 2 , , l ;

  3. D = i = 1 l D i ;

  4. diam ( D i ) Δ for every i = 1 , 2 , , l , where diam ( D i ) = sup { x y : x D i , y D i } .

Proposition 1

Let D R n 0 be a compact set. Then, for each Δ > 0 , it has a finite Δ -partition.

3 Approximation

Let γ > 0 and σ > 0 be given numbers, Λ = { Ω 1 , Ω 2 , , Ω N } be a finite Δ -partition of the compact set Ω R k , Λ = { 0 = r 0 , r 1 , , r a = γ } be a uniform partition of the closed interval [ 0 , γ ] , δ = r j + 1 r j , j = 0 , 1 , , a 1 , be a diameter of the partition Λ , P = { x R n : x = 1 } , and P σ = { e 1 , e 2 , , e c } be a finite σ -net on P . Denote

(6) B p γ , Δ , δ , σ ( r ) = x ( ) : Ω R n : x ( s ) = r j i e l i for every s Ω i , where r j i Λ , e l i P σ , i = 1 , 2 , , N , i = 1 N μ ( Ω i ) r j i p r p ,

(7) p γ , Δ , δ , σ ( r ) = { F ( x ( ) ) ( ) : x ( ) B p γ , Δ , δ , σ ( r ) } ,

where μ ( ) means the Lebesgue measure of a set. It is obvious that the set p γ , Δ , δ , σ ( r ) consists of a finite number of functions. We set

(8) c = 2 r p [ μ ( E ) ] 1 q ,

(9) ψ λ ( Δ ) = 2 r [ μ ( Ω ) μ ( E ) ] 1 q ω λ ( Δ ) ,

(10) φ λ ( δ ) = M ( λ ) μ ( Ω ) [ μ ( E ) ] 1 q δ ,

(11) α λ ( γ , σ ) = M ( λ ) μ ( Ω ) [ μ ( E ) ] 1 q γ σ ,

where M ( λ ) is defined by (4).

The Hausdorff distance between the sets U L q ( E ; R m ) and V L q ( E ; R m ) is denoted by h q ( U , V ) .

Theorem 1

For every λ > 0 , γ > 0 , finite Δ -partition of the compact set Ω R k , uniform δ -partition of the closed interval [ 0 , γ ] , and σ > 0 , the inequality

h q ( p ( r ) , p γ , Δ , δ , σ ( r ) ) λ + c M ( λ ) γ p 1 + ψ λ ( Δ ) + φ λ ( δ ) + α λ ( γ , σ )

is satisfied, where the sets p ( r ) and p γ , Δ , δ , σ ( r ) are defined by (2) and (7), respectively.

Proof

Denote

(12) F λ ( x ( ) ) ( ξ ) = Ω K λ ( ξ , s ) x ( s ) d s for every ξ E

and

p λ ( r ) = { F λ ( x ( ) ) ( ) : x ( ) B p ( r ) } ,

where K λ ( , ) is defined in (3). The set p λ ( r ) is the image of the closed ball B p ( r ) under the Hilbert-Schmidt integral operator (12), and the compactness of the operator F λ ( ) implies that the set p λ ( r ) is a compact subset of the space C ( E ; R m ) , where C ( E ; R m ) is the space of continuous functions y ( ) : E R m with norm y ( ) C = max { y ( ξ ) : ξ E } .

Applying (3) and Hölder’s inequality, it is not difficult to show that

(13) h q ( p ( r ) , p λ ( r ) ) λ 2 .

Now we set

B p γ ( r ) = { x ( ) B p ( r ) : x ( s ) γ for almost all s Ω } ,

and let

p λ , γ ( r ) = { F λ ( x ( ) ) ( ) : x ( ) B p γ ( r ) } .

Let y ( ) p λ ( r ) be an arbitrarily chosen function, which is the image of x ( ) B p ( r ) under operator (12). Define the function x ( ) : Ω R n , setting

x ( s ) = x ( s ) if x ( s ) γ , x ( s ) x ( s ) γ if x ( s ) > γ ,

where s Ω . It is not difficult to verify that x ( ) B p γ ( r ) . Let y ( ) p λ , γ ( r ) be the image of x ( ) B p γ ( r ) under operator (12). Denote W = { s Ω : x ( s ) > γ } . From inclusion x ( ) B p ( r ) and Tchebyshev’s inequality (see, [14], p. 82), it follows that

(14) μ ( W ) r p γ p .

Thus, from (8), (14), and Hölder’s inequality, we obtain that

y ( ξ ) y ( ξ ) W K λ ( ξ , s ) x ( s ) x ( s ) d s 2 r M ( λ ) [ μ ( W ) ] 1 q 2 r p M ( λ ) γ p 1

for every ξ E , and consequently,

y ( ) y ( ) q 2 r p M ( λ ) γ p 1 [ μ ( E ) ] 1 q = c M ( λ ) γ p 1 ,

where M ( λ ) is defined by (4). Since y ( ) p λ ( r ) is arbitrarily chosen, we obtain from the last inequality that

(15) p λ ( r ) p λ , γ ( r ) + c M ( λ ) γ p 1 B q ( 1 ) ,

where

(16) B q ( 1 ) = { y ( ) L q ( E ; R m ) : y ( ) q 1 } .

The inclusion p λ , γ ( r ) p λ ( r ) and (15) yield that

(17) h q ( p λ ( r ) , p λ , γ ( r ) ) c M ( λ ) γ p 1 .

For given Δ > 0 and finite Δ -partition Λ = { Ω 1 , Ω 2 , , Ω N } of the compact set Ω R k , we denote

(18) B p γ , Δ ( r ) = { x ( ) B p γ ( r ) : x ( s ) = x i for every s Ω i , i = 1 , 2 , , N }

and

p λ , γ , Δ ( r ) = { F λ ( x ( ) ) ( ) : x ( ) B p γ , Δ ( r ) } .

Choose an arbitrary z ( ) p λ , γ ( r ) , which is the image of v ( ) B p γ ( r ) under operator (12). Define the function v ( ) : Ω R n , setting

(19) v ( s ) = 1 μ ( Ω i ) Ω i v ( τ ) d τ , s Ω i , i = 1 , 2 , , N .

Taking into consideration the inclusion v ( ) B p γ ( r ) and equality (19), we obtain that v ( s ) γ for every s Ω and

Ω i v ( s ) p d s Ω i v ( s ) p d s

for every i = 1 , 2 , , N . Since v ( ) p r , then it follows from last inequality that v ( ) p v ( ) p r . Thus, from (18) and (19), we obtain that v ( ) B p γ , Δ ( r ) .

Let z ( ) p λ , γ , Δ ( r ) be the image of v ( ) under operator (12). We have

(20) z ( ξ ) z ( ξ ) = i = 1 N Ω i K λ ( ξ , s ) [ v ( s ) v ( s ) ] d s

for every ξ E . Equation (19) yields that

(21) Ω i v ( s ) d s = Ω i v ( s ) d s

for every i = 1 , 2 , , N . Let ξ E and i = 1 , 2 , , N be fixed. Now let us choose an arbitrary s i Ω i . From (21), it follows that

(22) Ω i K λ ( ξ , s ) [ v ( s ) v ( s ) ] d s Ω i K λ ( ξ , s ) K λ ( ξ , s i ) v ( s ) v ( s ) d s .

Since Λ = { Ω 1 , Ω 2 , , Ω N } is a finite Δ -partition of the compact Ω , s i Ω i , then from Definition 1 we obtain that s s i Δ for every s Ω i . Finally, by virtue of (5), we have that

(23) K λ ( ξ , s ) K λ ( ξ , s i ) ω λ ( Δ )

for every s Ω i . Thus, from (22) and (23), it follows that

(24) Ω i K λ ( ξ , s ) [ v ( s ) v ( s ) ] d s ω λ ( Δ ) Ω i v ( s ) v ( s ) d s .

Since v ( ) B p ( r ) and v ( ) B p ( r ) , then (24) yields that

(25) i = 1 N Ω i K λ ( ξ , s ) [ v ( s ) v ( s ) ] d s ω λ ( Δ ) i = 1 N Ω i v ( s ) v ( s ) d s = ω λ ( Δ ) Ω v ( s ) v ( s ) d s 2 r ω λ ( Δ ) [ μ ( Ω ) ] 1 q .

Equations (9), (20), and (25) imply that

z ( ξ ) z ( ξ ) 2 r ω λ ( Δ ) [ μ ( Ω ) ] 1 q

for every ξ E and, consequently,

z ( ) z ( ) q 2 r ω λ ( Δ ) [ μ ( Ω ) μ ( E ) ] 1 q = ψ λ ( Δ ) .

Since z ( ) p λ , γ ( r ) is arbitrarily chosen, the last inequality yields

(26) p λ , γ ( r ) p λ , γ , Δ ( r ) + ψ λ ( Δ ) B q ( 1 ) ,

where B q ( 1 ) is defined by (16).

From inclusion p λ , γ , Δ ( r ) p λ , γ ( r ) and (26), we obtain

(27) h q ( p λ , γ ( r ) , p λ , γ , Δ ( r ) ) ψ λ ( Δ ) .

For given Δ > 0 , δ > 0 , finite Δ -partition Λ = { Ω 1 , Ω 2 , , Ω N } of the compact set Ω R k , and uniform δ -partition Λ = { 0 = r 0 , r 1 , , r a = γ } of the closed interval [ 0 , γ ] , we set

B p γ , Δ , δ ( r ) = { x ( ) B p γ , Δ ( r ) : x ( s ) = x i for every s Ω i , x i Λ for every i = 1 , 2 , , N } ,

p λ , γ , Δ , δ ( r ) = { F λ ( x ( ) ) ( ) : x ( ) B p γ , Δ , δ ( r ) } .

Let y 0 ( ) p λ , γ , Δ ( r ) be an arbitrarily chosen function, which is the image of x 0 ( ) B p γ , Δ ( r ) under operator (12). From inclusion x 0 ( ) B p γ , Δ ( r ) , it follows that

(28) x 0 ( s ) = x i , s Ω i , i = 1 , 2 , , N ,

where

(29) i = 1 N μ ( Ω i ) x i p r p , x i γ for every i = 1 , 2 , , N .

If x i < γ , then there exists r j i Λ such that

(30) x i [ r j i , r j i + 1 ) .

Define new function v 0 ( ) : Ω R n , setting

(31) v 0 ( s ) = x i x i r j i if 0 < x i < γ , x i if x i = 0 or x i = γ ,

where s Ω i , i = 1 , 2 , , N , and r j i Λ is defined by (30). It is not difficult to observe that v 0 ( s ) x 0 ( s ) for every s Ω . Moreover, from equations (28)–(31) it follows that v 0 ( ) B p γ , Δ , δ ( r ) and

(32) x 0 ( s ) v 0 ( s ) δ

for every s Ω . Now, let z 0 ( ) p λ , γ , Δ , δ ( r ) be the image of v 0 ( ) B p γ , Δ , δ ( r ) under operator (12). Thus, (4) and (32) imply that

z 0 ( ξ ) y 0 ( ξ ) M ( λ ) μ ( Ω ) δ

for every ξ E . From the last inequality and (10), we conclude that

(33) z 0 ( ) y 0 ( ) q M ( λ ) μ ( Ω ) [ μ ( E ) ] 1 q δ = φ λ ( δ ) .

Since y 0 ( ) p λ , γ , Δ ( r ) is arbitrarily chosen and z 0 ( ) p λ , γ , Δ , δ ( r ) , the inequality (33) yields that

(34) p λ , γ , Δ ( r ) p λ , γ , Δ , δ ( r ) + φ λ ( δ ) B q ( 1 ) .

The inclusion p λ , γ , Δ , δ ( r ) p λ , γ , Δ ( r ) and (34) imply that

(35) h q ( p λ , γ , Δ ( r ) , p λ , γ , Δ , δ ( r ) ) φ λ ( δ ) .

Let us set

p λ , γ , Δ , δ , σ ( r ) = { F λ ( x ( ) ) ( ) : x ( ) B p γ , Δ , δ , σ ( r ) } ,

where the set B p γ , Δ , δ , σ ( r ) is defined by (6).

Choose an arbitrary w ( ) p λ , γ , Δ , δ ( r ) , which is the image of u ( ) B p γ , Δ , δ ( r ) under operator (12). From inclusion u ( ) B p γ , Δ , δ ( r ) , it follows that there exist r j i Λ , g i P ( i = 1 , 2 , , N ) such that

(36) u ( s ) = r j i g i , s Ω i , i = 1 , 2 , , N ,

where

(37) i = 1 N μ ( Ω i ) r j i p r p .

Since g i P for every i = 1 , 2 , , N , P σ is a finite σ -net on P , then, for each g i P , there exists e l i P σ such that

(38) g i e l i σ .

Define function u ( ) : Ω R n , setting

(39) u ( s ) = r j i e l i , s Ω i , i = 1 , 2 , , N .

From equations (36)–(39) it follows that u ( ) B p γ , Δ , δ , σ ( r ) and

(40) u ( s ) u ( s ) r j i g i e l i γ σ

for every s Ω . Now let w ( ) p λ , γ , Δ , δ , σ ( r ) be the image of u ( ) B p γ , Δ , δ , σ ( r ) under operator (12). Then, (40) yields

w ( ξ ) w ( ξ ) M ( λ ) μ ( Ω ) γ σ

for every ξ E and hence

(41) w ( ) w 0 ( ) q M ( λ ) μ ( Ω ) [ μ ( E ) ] 1 q γ σ = α λ ( γ , σ ) ,

where M ( λ ) is defined by (4) and α λ ( γ , σ ) is defined by (11). Thus, for arbitrary chosen w ( ) p λ , γ , Δ , δ ( r ) , there exists w ( ) p λ , γ , Δ , δ , σ ( r ) such that the inequality (41) is satisfied. This means that

p λ , γ , Δ , δ ( r ) p λ , γ , Δ , δ , σ ( r ) + α λ ( γ , σ ) B q ( 1 ) .

The last inclusion and inclusion p λ , γ , Δ , δ , σ ( r ) p λ , γ , Δ , δ ( r ) imply that

(42) h q ( p λ , γ , Δ , δ , σ ( r ) , p λ , γ , Δ , δ ( r ) ) α λ ( γ , σ ) .

Analogous to (13), it is not difficult to show that

(43) h q ( p λ , γ , Δ , δ , σ ( r ) , p γ , Δ , δ , σ ( r ) ) λ 2 ,

where the set p γ , Δ , δ , σ ( r ) is defined by (7).

Finally, the proof of the theorem follows from the inequalities (13), (17), (27), (35), (42), and (43).□

From Theorem 1, it follows the validity of the following corollary.

Corollary 1

For every ε > 0 , there exist λ ( ε ) > 0 , γ ( ε ) = γ ( ε , λ ( ε ) ) > 0 , Δ ( ε ) = Δ ( ε , λ ( ε ) ) > 0 , δ ( ε ) = δ ( ε , λ ( ε ) ) > 0 , and σ ( ε ) = σ ( ε , λ ( ε ) , γ ( ε ) ) > 0 such that, for every finite Δ -partition of the compact set Ω R k , uniform δ -partition of the closed interval [ 0 , γ ( ε ) ] , and σ > 0 , the inequality

h q ( p ( r ) , p γ ( ε ) , Δ , δ , σ ( r ) ) ε

is satisfied for each Δ ( 0 , Δ ( ε ) ] , δ ( 0 , δ ( ε ) ] , and σ ( 0 , σ ( ε ) ] .

Proof

Let us choose λ ( ε ) = ε 5 , and fix it, and let

γ ( ε ) = γ ( ε , λ ( ε ) ) = 5 c M ( λ ( ε ) ) ε 1 p 1 .

By virtue of (5) and (9), we have that ψ λ ( Δ ) 0 as Δ 0 + . Define Δ ( ε ) = Δ ( ε , λ ( ε ) ) > 0 such that the inequality

ψ λ ( ε ) ( Δ ) ε 5

is satisfied for every Δ ( 0 , Δ ( ε ) ] .

Furthermore, we denote

δ ( ε ) = δ ( ε , λ ( ε ) ) = ε 5 M ( λ ( ε ) ) μ ( Ω ) [ μ ( E ) ] 1 q ,

σ ( ε ) = σ ( ε , λ ( ε ) , γ ( ε ) ) = ε 5 M ( λ ( ε ) ) μ ( Ω ) [ μ ( E ) ] 1 q γ ( ε ) .

Now the proof of the corollary follows from Theorem 1.□

4 Conclusion

In this article, an approximation of the image of the closed ball B p ( r ) = { x ( ) L p ( Ω ; R m ) : x ( ) p r } under the Hilbert-Schmidt integral operator is presented. The closed ball B p ( r ) L p ( Ω ; R m ) is replaced by the set, which consists of a finite number of piecewise constant functions, and it is proved that the images of these functions form an approximation of the image of the ball B p ( r ) . An error evaluation for the Hausdorff distance between the image of the closed ball and its approximation, which consists of a finite number of functions, is given. The obtained result can be used to construct a set of outputs of the input–output system with integrally constrained inputs, which will allow the design of system outputs with prescribed properties.

  1. Funding information: This research received no external funding.

  2. Conflict of interest: The author declares that he has no conflict of interest.

  3. Data availability statement: Not applicable.

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Received: 2022-08-20
Accepted: 2023-03-09
Published Online: 2023-04-11

© 2023 the author(s), published by De Gruyter

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  47. On I. Meghea and C. S. Stamin review article “Remarks on some variants of minimal point theorem and Ekeland variational principle with applications,” Demonstratio Mathematica 2022; 55: 354–379
  48. Special Issue on Fixed Point Theory and Applications to Various Differential/Integral Equations - Part II
  49. On Cauchy problem for pseudo-parabolic equation with Caputo-Fabrizio operator
  50. Fixed-point results for convex orbital operators
  51. Asymptotic stability of equilibria for difference equations via fixed points of enriched Prešić operators
  52. Asymptotic behavior of resolvents of equilibrium problems on complete geodesic spaces
  53. A system of additive functional equations in complex Banach algebras
  54. New inertial forward–backward algorithm for convex minimization with applications
  55. Uniqueness of solutions for a ψ-Hilfer fractional integral boundary value problem with the p-Laplacian operator
  56. Analysis of Cauchy problem with fractal-fractional differential operators
  57. Common best proximity points for a pair of mappings with certain dominating property
  58. Investigation of hybrid fractional q-integro-difference equations supplemented with nonlocal q-integral boundary conditions
  59. The structure of fuzzy fractals generated by an orbital fuzzy iterated function system
  60. On the structure of self-affine Jordan arcs in ℝ2
  61. Solvability for a system of Hadamard-type hybrid fractional differential inclusions
  62. Three solutions for discrete anisotropic Kirchhoff-type problems
  63. On split generalized equilibrium problem with multiple output sets and common fixed points problem
  64. Special Issue on Computational and Numerical Methods for Special Functions - Part II
  65. Sandwich-type results regarding Riemann-Liouville fractional integral of q-hypergeometric function
  66. Certain aspects of Nörlund -statistical convergence of sequences in neutrosophic normed spaces
  67. On completeness of weak eigenfunctions for multi-interval Sturm-Liouville equations with boundary-interface conditions
  68. Some identities on generalized harmonic numbers and generalized harmonic functions
  69. Study of degenerate derangement polynomials by λ-umbral calculus
  70. Normal ordering associated with λ-Stirling numbers in λ-shift algebra
  71. Analytical and numerical analysis of damped harmonic oscillator model with nonlocal operators
  72. Compositions of positive integers with 2s and 3s
  73. Kinematic-geometry of a line trajectory and the invariants of the axodes
  74. Hahn Laplace transform and its applications
  75. Discrete complementary exponential and sine integral functions
  76. Special Issue on Recent Methods in Approximation Theory - Part II
  77. On the order of approximation by modified summation-integral-type operators based on two parameters
  78. Bernstein-type operators on elliptic domain and their interpolation properties
  79. A class of strongly convergent subgradient extragradient methods for solving quasimonotone variational inequalities
  80. Special Issue on Recent Advances in Fractional Calculus and Nonlinear Fractional Evaluation Equations - Part II
  81. Application of fractional quantum calculus on coupled hybrid differential systems within the sequential Caputo fractional q-derivatives
  82. On some conformable boundary value problems in the setting of a new generalized conformable fractional derivative
  83. A certain class of fractional difference equations with damping: Oscillatory properties
  84. Weighted Hermite-Hadamard inequalities for r-times differentiable preinvex functions for k-fractional integrals
  85. Special Issue on Recent Advances for Computational and Mathematical Methods in Scientific Problems - Part II
  86. The behavior of hidden bifurcation in 2D scroll via saturated function series controlled by a coefficient harmonic linearization method
  87. Phase portraits of two classes of quadratic differential systems exhibiting as solutions two cubic algebraic curves
  88. Petri net analysis of a queueing inventory system with orbital search by the server
  89. Asymptotic stability of an epidemiological fractional reaction-diffusion model
  90. On the stability of a strongly stabilizing control for degenerate systems in Hilbert spaces
  91. Special Issue on Application of Fractional Calculus: Mathematical Modeling and Control - Part I
  92. New conticrete inequalities of the Hermite-Hadamard-Jensen-Mercer type in terms of generalized conformable fractional operators via majorization
  93. Pell-Lucas polynomials for numerical treatment of the nonlinear fractional-order Duffing equation
  94. Impacts of Brownian motion and fractional derivative on the solutions of the stochastic fractional Davey-Stewartson equations
  95. Some results on fractional Hahn difference boundary value problems
  96. Properties of a subclass of analytic functions defined by Riemann-Liouville fractional integral applied to convolution product of multiplier transformation and Ruscheweyh derivative
  97. Special Issue on Development of Fuzzy Sets and Their Extensions - Part I
  98. The cross-border e-commerce platform selection based on the probabilistic dual hesitant fuzzy generalized dice similarity measures
  99. Comparison of fuzzy and crisp decision matrices: An evaluation on PROBID and sPROBID multi-criteria decision-making methods
  100. Rejection and symmetric difference of bipolar picture fuzzy graph
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