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On the stability of a strongly stabilizing control for degenerate systems in Hilbert spaces

  • Mohamed Hariri EMAIL logo , Zohra Bouteffal , Nor-el-houda Beghersa and Mehdi Benabdallah
Published/Copyright: July 29, 2023
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Abstract

In this article, we explain how a recent Lyapunov theorem on stability plays a role in the study of the strong stabilizability problem in Hilbert spaces. We explore a degenerate controlled system and investigate the properties of a feedback control to stabilize such system in depth. The spectral theory of an appropriate pencil operator is used to generate robustness constraints for a stabilizing control.

MSC 2010: 93D15; 47A13; 34A09

1 Introduction

In the present article, we study the controlled system described by the degenerate differential equation:

(1) L ξ ( t ) = M ξ ( t ) + C u ( t ) , ξ , u , t 0 ξ ( 0 ) = ξ 0 ,

where L , M , and C are bounded operators in Hilbert spaces on the complex number C . The operator L is not necessarily invertible and u is the control.

ξ ( t ) = e λ t ξ 0 ,

we obtain the equation

( λ L M ) ξ 0 = C u ( t ) e λ t ,

where λ L M is the pencil operator related to the linear part of system (1).

Stability and stabilization is one of the important concepts of control theory in mathematics. Our purpose in the present work is to check if the characteristic of feedback control u = ξ , q , q is stabilizing. The literature on controlled systems is more appropriate to study stabilization since the conditions of form are usually too strong for infinite dimensional spaces. Numerous researchers focused on the stability and stabilizability problems, see [1,2] and the references therein.

Many articles dealt with the study of strong stabilizability and steady Riccati equation approach. Moreover, the linear and nonlinear system of delay differential equations (DDEs) with constant time retardation, new approach to qualitative analyses of differential systems with time-varying delays via Lyapunov-Krasovskii have proved some results to the distinguishability of descriptor systems with a regular pencil [36]. Korobov and Sklyar have used analytic semigroups governed by explicit differential equations, with the strong stabilizability of contractive systems in Hilbert spaces [7]. Recently, the approximate controllability of Sobolev-type Hilfer neutral fractional stochastic differential inclusions in Hilbert spaces was examined [8,9]. The stability theory for quasi-linear implicit differential equations was considered in terms exponential solution, while the present work deals with the strongly stabilizing control for degenerate systems, which led to more efficient consequences.

This article is organized as follows: in Section 2, we use spectral theory of operators and an appropriate conformal mapping to generalize Lyapunov’s famous result for the spectrum of the pencil operator λ L M . The stability of the related stationary degenerate systems of the form:

(2) L ξ ( t ) = M ξ ( t ) , t 0 ,

in particular, the linear system with the identity operator L = I and M = T , i.e.,

(3) ξ ( t ) = T ξ ( t ) , t 0 ,

is said to be explicit, where T is a linear bounded operator, with Ker L { 0 } , the degenerate system (1) is said to be implicit [10]. In Section 3, we show that operator λ ˜ n L M ˜ preserves the Riesz basis property of its eigenelements if c q < Δ σ 2 . (Theorem 4.2). This fact, in particular implies (compare Theorem 3.3) that for the strong stability of the semigroup { e ( M + c q ) t } t 0 . The result of Sections 3 and 4 is a development for the case of semigroup { e ( M + c q ) t } t 0 by degenerate differential equation [7]. In Section 5, we give a robustness analysis for a stabilizing control u = ξ , q + p , q , p .

2 Preliminaries

We consider the following assumptions:

  1. The operator λ L M is bounded by the discrete spectrum of simple eigenvalues denoted by { λ k } k = 1 .

  2. Let M be the generator of a C 0 -semigroup { e M t } t 0 on a Hilbert space , and

    1. the set σ ( L , M ) ( i R ) is at most countable,

    2. if adjoint operator M has no pure imaginary eigenvalues, then the semigroup { e M t } t 0 is strongly exponentially stable if and only if it is uniformly bounded.

  3. The constant Δ σ = 1 2 min i j λ i λ j > 0 exists.

  4. The space is one dimensional, so we associate C with a vector c ; besides, if { φ n } n = 1 is an orthonormal eigenbasisi ( λ n L M ) φ n = 0 , then c n = c , φ n 0 , n N .

The following notations are used in the sequel:

  1. ( , ) : denotes Hilbert space of all bounded linear operators.

  2. C = { λ C , Re λ < 0 } : open half-plane in C .

  3. σ ( L , M ) : spectrum of pencil operator λ L M , λ C , and L , M ( , ) .

  4. σ p ( L , M ) : point spectrum of pencil operator λ L M , i.e., the set of eigenvalues of λ L M .

  5. H : the subspace of .

  6. The restriction of the operator L , i.e., L H = L 1 .

Definition 2.1

[11] A pencil of matrices λ L M is polynomial matrix whose coefficients are polynomials of degree less than or equal to 1, λ is a variable indeterminate, where L and M are any two matrices of the same order m × n .

Definition 2.2

[11] A pencil of matrices λ L M is called regular if

  1. L and M are square matrices of the same order n , and

  2. The determinant λ L M does not vanish identically.

In all other case ( m n or m = n but λ L M = 0 ), the pencil is called singular.

Definition 2.3

[12,13] The complex number λ C is called a regular value of the pencil λ L M , if the resolvent ( λ L M ) 1 exists and is bounded. The set of all regular values is denoted by ρ ( L , M ) , and its complement σ ( L , M ) = C \ ρ ( L , M ) is called the spectrum of the pencil λ L M . The set of all eigenvalues of the pencil λ L M is denoted by

σ p ( L , M ) = { λ C v 0 : ( λ L M ) v = 0 } ,

where ρ ( L , M ) indicates the pencil resolvent set

ρ ( L , M ) = { λ C : λ is finite and ( λ L M ) 1 is bounded } .

3 Stability of stationary degenerate systems

For the stationary degenerate system (2), we can define the following condition for exponential stability.

Definition 3.1

[12]. If there are two constants K > 0 and α > 0 such that for each solution ξ ( t ) , ( t 0 ) , the system (2) is called exponentially stable

(4) ξ ( t ) K e α t ξ 0 , for any t 0 .

Definition 3.2

[12,14]. If the system (2) satisfies the following qualities:

  1. for any solution ξ ( ) such that ξ ( 0 ) = ξ 0 = 0 then ξ ( t ) = 0 , for all t 0 ,

  2. S M ( t ) is strongly stable semigroup if for all

    ξ , S M ( t ) ξ 0 as t ,

    then it is considered to be well posed.

Theorem 3.3

[1]. The strongly exponentially stable of { e M t } t 0 occurs if and only if there is a norm 1 equivalent to the initial norm of such that M is dissipative in 1 , i.e.,

e M t ξ 1 ξ 1 , ξ , t 0 .

Remark 3.4

[1]. An operator M is said to be dissipative if

( Re M ) ξ , ξ = Re M ξ , ξ 0 .

We call an operator M uniformly dissipative if Re ( M ) 0 .

Theorem 3.5

[12]. If the system (2) is exponentially stable, then all eigenvalues of the pencil λ A B are in the half-plane Re λ α , where α is the constant defined in (4).

Theorem 3.6

Assume that the pencil operator of bounded operators L and M have a spectrum σ ( L , M ) in the left half-plane. Then G 0 is used for any nonnegative uniform operator [1], and there exists an operator W 0 such that.

(5) L W M + M W L = G .

Proof

We suppose that

σ ( L , M ) { λ C : Re λ < 0 } .

Then i is a regular point, and T = i ( i L + M ) ( i L M ) 1 is a bounded operator. By using the conformal mapping method, we obtain

μ = φ ( λ ) = i λ + 1 λ i ,

then

μ I T = i λ + 1 λ i ( i L M ) ( i L M ) 1 i ( i L + M ) ( i L M ) 1 = 2 λ i ( λ L M ) ( i L M ) 1 .

The operator μ I T is invertible. As a result, σ ( T ) = σ ( I , T ) = φ σ ( L , M ) is the spectrum of T . Hence, σ ( T ) is contained in the unit disk. We have the following as a consequence of the general Lyapunov theorem [1]. For each operator H 0 , there is an operator W 0 such that:

Re ( W T ) = W T + T W 2 = 1 2 [ i W ( i L + M ) ( i L M ) 1 i ( i L M ) 1 ( i L + M ) W ] = i 2 ( i L M ) 1 [ ( i L M ) W ( i L + M ) ( i L + M ) W ( i L M ) ] ( i L M ) 1 = ( i L M ) 1 ( L W M + M W L ) ( i L M ) 1 = H .

It is the same as

L W M + M W L = G ,

where G = ( i L + M ) H ( i L M ) 0 . In fact,

G = G and G ξ , ξ a ξ 2 , a > 0 .

Therefore, the equality is proved.□

Theorem 3.7

Assume that i is a regular point for the bounded pencil operator λ L M , there is an operator W 0 such that

(6) L W M + M W L 0 .

Then the pencil operator λ L M spectrum σ ( L , M ) is in the left half-plane.

Proof

If i ρ ( L , M ) the operator

T = i ( i L + M ) ( i L M ) 1

is bounded, and the equality becomes

( i L + M ) R e ( W T ) ( i L M ) = L W M + M W L 0 .

Therefore,

Re ( W T ) 0 .

By using the general Lyapunov theorem [1], the spectrum σ ( T ) will be in the unit disk, then we conclude that

σ ( L , M ) = φ 1 ( σ ( T ) ) { λ C : Re λ < 0 } ,

where λ = φ 1 ( μ ) = i μ + 1 μ + i .

Consequently, Theorem 3.7 is proved.□

Theorem 3.8

[12] If (5) is satisfied for the couple of positive uniform operators ( W , G ) , then λ = i is not an eigenvalue for the pencil λ L M .

Remark 3.9

The necessary and sufficient conditions of stability for stationary degenerate systems can be obtained by using Theorems 3.63.8. We obtain the following crucial result in finite dimensional spaces using the elementary divisors of the pencil of matrices [11].

Corollary 3.10

[12] The following assertions are equivalents in finite dimensional spaces:

  1. the system (2) is exponentially stable;

  2. σ ( L , M ) = σ p ( L , M ) { λ C : Re λ < 0 } ;

  3. there is nonnegative definite matrix W 0 that has the property

L W M + M W L 0 .

Example 3.11

Considering the system (2) in the finite-dimensional spaces.

L = 1 0 0 0 , M = 1 1 0 1 , λ L M = λ + 1 1 0 1 .

So,

det ( λ L M ) = λ + 1 0 ,

it is a regular pencil.

  • Finite elementary dividers (FED)

    D 2 ( λ ) = λ + 1 , D 1 ( λ ) = 1 , D 0 ( λ ) = 1 .

  • Invariant polynomials are given by

    i 1 ( λ ) = D 2 ( λ ) D 1 ( λ ) = λ + 1 , i 2 ( λ ) = D 1 ( λ ) D 0 ( λ ) = 1 .

Then, there is only one FED, so according to Weierstrass’s theorem [11], we obtain

λ L M λ + 1 0 0 1 .

Since

σ ( L ; M ) = σ p ( L ; M ) = { 1 } { λ C : Re λ < 0 } ,

then the system (2) is exponentially stable.

4 Basis and spectral properties of pencil operator λ ˜ n L M ˜

We need to introduce the set:

H c : i , k = 1 c , Φ k c , Φ i < ; c , Φ j 0 , j = 1 , 2 , .

Remark 4.1

If a vector c such that c , Φ k 1 k 2 , then c H .

In this section, we are interested to study the system of one dimensional feedback control in Hilbert space given by

(7) L ξ ( t ) = M ξ ( t ) + c u ( t ) , c , ξ ( 0 ) = ξ 0 , t 0 .

Theorem 4.2

Let c q < Δ σ 2 , where Δ σ = 1 2 min i j λ i λ j > 0 . Then the eigenvectors Φ n of the pencil operator λ ˜ n L M ˜ , where M ˜ = M + c q construct a Riesz basis .

Proof

Let us consider the spectral equation for the eigenvectors Φ n :

( λ ˜ n L M ˜ ) Φ n = 0 ,

or

( M + c q λ ˜ n L ) Φ n = 0 ,

and apply the pencil resolvent ( λ n L M ) 1 of the operator λ L M . We obtain

Φ n = θ n ( λ n L M ) 1 c ,

where θ n = Φ n , q and λ n is eigenvalue of pencil operator λ L M .

We obtain

( λ n L M ) 1 c , q = 1 ,

with the property λ n λ ˜ j > Δ σ , for all n j , the resolvent

( λ n L M ) 1 c = n = 1 c n φ n λ n λ ˜ j ,

we have

c , φ n φ n , q λ n λ ˜ j = 1 n j c n , φ n φ n , q λ n λ ˜ j .

In the sequel, we need the following theorem.

Theorem 4.3

Let { λ ˜ n } n = 1 any set of complex numbers such that:

  1. λ n λ ˜ n < Δ σ , n N ,

  2. n = 1 λ n λ ˜ n 2 c n 2 < Δ σ c 2 ,

where Δ σ , c n c , φ n , and λ n are as in Theorem 4.2. Then there exists a unique control u ( ξ ) = q ξ such that the spectrum σ ( L , M ˜ ) of the pencil operator λ ˜ n L M ˜ is { λ ˜ n } n = 1 the corresponding eigenvectors ( λ ˜ n L M ˜ ) Φ n = 0 .

5 Strong stability of stationary degenerate systems

We provide a detailed analysis and precise description of the norms that guarantee the dissipativity of the operator M ˜ .

Definition 5.1

The controlled degenerate system (7) is said to be exponentially stabilizable by means of a direct feedback u ( t ) = q ξ ( t ) , q if the corresponding system

(8) L ξ ( t ) = ( M + c q ) ξ ( t ) = M ˜ ξ ( t ) , ξ ( 0 ) = ξ 0 , t 0 ,

is strongly exponentially stable.

Theorem 5.2

Let system (8) is strongly exponentially stable and c q < Δ σ 2 . Then there exists a Hilbert norm W = W , 1 2 with positive definite W such that the operator M ˜ is dissipative then:

  1. the system (8) is well posed,[2]

  2. for any solution ξ ( t ) of the system (8), one has

    d d t ξ ( t ) W 2 = d d t W ξ ( t ) , ξ ( t ) = G 0 ξ ( t ) , ξ ( t ) ,

    where G 0 is self-adjoint nonnegative compact operator G 0 = i = 1 N ζ i ω i ω i , { ω i } i = 1 is orthonormal basis of eigenvectors corresponding to eigenvalues ζ i 0 ; i > 1 , such that:

    1. i = 1 N ζ i < ,

    2. there exist α 1 , α 2 > 0 such that for any normed eigenelement Φ n of pencil operator λ ˜ n L M ˜ and ( λ ˜ n L M ˜ ) Φ n = 0 ; n 1 , the following estimate holds

      α 1 i = 1 N ζ i ω i , Φ i 2 Re λ ˜ i α 2 , i = 1 , , N ,

  3. the operator W is given by

    W = 0 i = 1 N ζ i e L 1 1 M ˜ t ω i ω i e L 1 1 M ˜ t d t , t 0 .

Corollary 5.3

If c q < Δ σ 2 , then the following assertions are equivalents

  1. the system (8) is strongly exponentially stable;

  2. all the eigenvalues λ ˜ n of pencil operator λ ˜ n L M ˜ have a negative real part Re λ ˜ n < 0 , i.e.,

    σ ( L , M ˜ ) = σ p ( L , M ˜ ) = { λ ˜ n C , n 1 : Re λ ˜ n < 0 } ;

  3. operator L 1 1 M ˜ is uniformly W-dissipative in some Hilbert norm and has not pure imaginary eigenvalues;

  4. there exists a nonnegative matrix W 0

    Q 1 L W M ˜ + M ˜ W L = G 0 0 .

6 Robustness of a stabilizing control for degenerate systems

In this section, we deal with system (7) with a feedback control is as follows:

u ( ξ ) = q ξ + p ξ = ξ , q + p ,

it takes the form

(9) L ξ ( t ) = ( M + c q + c p ) ξ ( t ) = ( M ˜ + c p ) ξ ( t ) , c , q , p , t 0 .

Considering an arbitrary finite or infinite orthonormal system { ω i } i = 1 N and { ς i } i = 1 N ; ς i 0 . We define a self-adjoint compact operator by

G 1 = i = 1 N ς i ω i ω i 0 .

We examine the Lyapunov equation

(10) L W ( M ˜ + c p ) ξ + ( M ˜ + c p ) W L ξ = G 1 ξ ,

and it has unique operator solution W 0

(11) W ξ = 0 e L 1 1 ( M ˜ + c p ) t G 1 e L 1 1 ( M ˜ + c p ) t ξ d t , t 0 .

using (11) and fact that the family { ω i } i = 1 N is a basis in for more details see [1]. The operator W 0 satisfies the condition of Theorem 3.7:

Re ( W L 1 1 ( M ˜ + c p ) ) 0 .

Theorem 6.1

Suppose that

  1. the system (8) is strongly exponentially stable and c q < Δ σ 2 ;

  2. for any vector p for which there exist a finite or infinite orthonormal system { ω i } i = 1 N H , and { ζ i } i = 1 N H , ζ i 0 such that

    p , W , c { ω i } i = 1 N , L 1 = L H

    and the condition

    λ + ξ + , ω i < ζ i ξ + , i = 1 , 2 , , N .

Then the system (7) is exponentially stabilizable.

Proof

The norm 1 satisfies ξ ( t ) 1 ξ ( 0 ) 1 , t 0 for all solutions of (9) and the compact nonnegative operator G 1 , constructed by { ω i } i = 1 N , { ς i } i = 1 N and the operator G 0 (Theorem 5.2). This yields for the eigenelements Φ n of pencil operator λ ˜ n L M ˜ :

Q 1 Φ n , Φ n = G 0 Φ n , Φ n = [ L W M ˜ + M ˜ W L ] Φ n , Φ n = [ L W λ ˜ n L ] Φ n + [ λ ˜ n L W L ] Φ n , Φ n = 2 Re λ ˜ n W Φ n , Φ n = i = 1 N ς i ω i , Φ n 2 , n 1 .

The existence of such constants α 1 , α 2 > 0 with α 1 2 W Φ n , Φ n α 2 2 , and since Re λ ˜ n = Re λ ˜ n (see property ii of Theorem 5.2), by Corollary 5.3, equation (10) is equivalent to

( L W M ˜ + M ˜ W L + L W c p + p c W L ) ξ = G 1 ξ ,

or

( Q 1 + Q 2 ) ξ = G 1 ξ 0 .

We denote by λ ± and ξ ± the eigenvalues and eigenvectors of the two-dimensional self-adjoint operator

Q 2 ( L W c p + p c W L ) 0

given by

λ ± = L 1 W c , p ± W L 1 c . p , λ + > 0 , λ < 0 , L 1 = L H

with λ + ε λ ˜ n , we obtain

λ ˜ n min { λ 1 , λ 2 , λ } , ε [ 0 , 1 ] ,

then, for all ξ , we have

ξ ± = L 1 W c p ± p W L 1 c , lim t S M ˜ + c p ( t ) ξ + , ξ = 0 .

The eigenvalues λ 1 < 0 and λ 2 < 0 of the self-adjoint nonpositive operator Q 2 L 1 W c p p c W L 1 given by

  1. if W , c 0 , then

    λ 1 , 2 = c 2 W 2 2 ± c 2 W 2 2 2 + 4 W , c ;

  2. if W , c = 0 , then

    λ 1 = 2 c 2 and λ 2 = W 2 .

It is easy to notice that the condition λ + ξ + , ω i < ζ i ξ + , i 1 is sufficient for the from

(12) d d t ξ ( t ) 1 2 = ( Q 1 + Q 2 ) ξ , ξ .

It is used to prove that M ˜ + c p has no imaginary eigenvalues. Assume that exists λ ˜ n i R such that

( M ˜ + c p ) ξ ˆ = λ ˜ n L ξ ˆ .

It is easy to deduce from (12) that ( Q 1 + Q 2 ) ξ ˆ , ξ ˆ = 0 . If p , W , c { ω i } i = 1 N , then ξ ˆ is orthogonal to { ω i } i = 1 N . Hence, ξ ˆ , p = 0 implies that M ˜ ξ ˆ = λ ˜ n L ξ ˆ , which contradicts the exponential stability of M ˜ since λ ˜ n is a pure imaginary eigenvalue. Consequently, Theorem 6.1 is proved.□

Example 6.2

Considering system (1) in the infinite-dimensional Hilbert spaces.

Let us denote by S n the set

S n = λ C , c H , Re λ < 0 : 5 3 c , φ n q , φ n λ λ n 5 c , φ n q , φ n .

It can be shown that system (8) is strongly exponentially stable if and only if

( λ n L M ) 1 c , q = 1 .

We study system (8) with the feedback control u ( ξ ) = ξ , q + p , q , p . Let

L ( γ n ) = ( λ ˜ n γ n ) L 1 ( γ n ) = δ n if L 1 = L H for n N , M ˜ ( ϖ n ) = ( λ ˜ n ϖ n ) , C u ( c n ) u = c ξ , q + p and u = ξ , q + p ,

where λ ˜ n 0 ; c = ( c n ) H , c n 0 for n N , and n = 1 1 λ ˜ n c n 2 < + , with c n 0 for n N , that system (7) is approximately controllable for any feedback law, on the other hand, the system

L ξ = M ξ + c ξ , q + p , ξ ( 0 ) ,

is not exponentially stable, and

δ n = λ ˜ n ϖ n + c n p , n N ,

or

ϖ n = 1 λ ˜ n δ n 1 λ ˜ n c n p , n N .

Finally, ( ϖ n ) is the solution only for some ( δ n ) , such that

n = 1 1 λ ˜ n δ n 2 < + .

7 Conclusion

This article has discussed the stability of a new class for control systems defined by the degenerate differential equation in Hilbert spaces, and this was the major focus of this work. By using the spectral theory of pencil operator λ L M , we have established some requirements for the stability of Lyapunov results, and an example was presented to illustrate the main results. Furthermore, the subjects that will be considered in the future are as follows: non local degenerate fractional integro-differential inclusions with Brownian motion, approximate boundary strong stabilizability, and controllability.

Acknowledgements

The authors would like to thank the referees for their suggestions that helped improve the original manuscript in its present form.

  1. Conflict of interest: The authors state no conflict of interest.

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Received: 2022-05-28
Revised: 2023-04-20
Accepted: 2023-04-30
Published Online: 2023-07-29

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

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  27. Global optimum solutions for a system of (k, ψ)-Hilfer fractional differential equations: Best proximity point approach
  28. The study of solutions for several systems of PDDEs with two complex variables
  29. Regularity criteria via horizontal component of velocity for the Boussinesq equations in anisotropic Lorentz spaces
  30. Generalized Stević-Sharma operators from the minimal Möbius invariant space into Bloch-type spaces
  31. On initial value problem for elliptic equation on the plane under Caputo derivative
  32. A dimension expanded preconditioning technique for block two-by-two linear equations
  33. Asymptotic behavior of Fréchet functional equation and some characterizations of inner product spaces
  34. Small perturbations of critical nonlocal equations with variable exponents
  35. Dynamical property of hyperspace on uniform space
  36. Some notes on graded weakly 1-absorbing primary ideals
  37. On the problem of detecting source points acting on a fluid
  38. Integral transforms involving a generalized k-Bessel function
  39. Ruled real hypersurfaces in the complex hyperbolic quadric
  40. On the monotonic properties and oscillatory behavior of solutions of neutral differential equations
  41. Approximate multi-variable bi-Jensen-type mappings
  42. Mixed-type SP-iteration for asymptotically nonexpansive mappings in hyperbolic spaces
  43. On the equation fn + (f″)m ≡ 1
  44. Results on the modified degenerate Laplace-type integral associated with applications involving fractional kinetic equations
  45. Characterizations of entire solutions for the system of Fermat-type binomial and trinomial shift equations in ℂn#
  46. Commentary
  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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