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Controllability of fractional stochastic evolution equations with nonlocal conditions and noncompact semigroups

  • Yonghong Ding EMAIL logo and Yongxiang Li
Published/Copyright: July 2, 2020

Abstract

This article deals with the exact controllability for a class of fractional stochastic evolution equations with nonlocal initial conditions in a Hilbert space under the assumption that the semigroup generated by the linear part is noncompact. Our main results are obtained by utilizing stochastic analysis technique, measure of noncompactness and the Mönch fixed point theorem. In the end, an example is presented to illustrate that our theorems guarantee the effectiveness of controllability results in the infinite dimensional spaces.

MSC 2010: 93B05; 60H15; 47J35

1 Introduction

In this article, we shall be concerned with the controllability for the following fractional evolution equations with nonlocal initial conditions of the form:

(1.1) { D t α c x ( t ) + A x ( t ) = f ( t , x ( t ) ) + σ ( t , x ( t ) ) d W ( t ) d t + B u ( t ) , t J = [ 0 ,   b ] , x ( 0 ) + g ( x ) = x 0 ,

where D t α c is the Caputo fractional derivatives of order 1 2 < α < 1 . Let and K be two separable Hilbert spaces and the state x ( ) takes its values in . A : D ( A ) is a closed linear operator, and A is the infinitesimal generator of a C 0 -semigroup T ( t ) ( t 0 ) on . For convenience, we will use the same notation to denote the norms in and K and use ( , ) to denote the inner product of and K without any confusion. We are also employing the same notation for the norm of L ( K , ) , which denotes the space of all bounded linear operators from K to . Suppose that { W ( t ) : t 0 } is a K -valued Brownian motion or Wiener process with a finite trace nuclear covariance operator Q 0 defined on a filtered complete probability space ( Ω , , { t } t 0 , P ) . The control function u ( ) belongs to the space L 2 ( J ,   U ) , a Banach space of admissible control functions, for a separable Hilbert space U , B : U is a bounded linear operator. f ,   σ and g are appropriate functions to be given later. x 0 is an 0 measurable -value random variable.

Fractional evolution equations have gained considerable importance due to their application in various sciences [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17]. On the other hand, controllability for various types of linear and nonlinear dynamical systems have been considered in many publications by using different approaches due to its applications in many fields of science and engineering [1,2,3,4,5,6,7,18,19,20,21,22,23,24,25,26,27,28,29]. It should be emphasized that there are many different notions of controllability for dynamical systems, for example, approximate controllability, exact controllability, null controllability and so on. There have been many studies on the approximate controllability for semilinear evolution systems in abstract spaces (see [1,2,3,4,20,21,30,31] and references therein). Several authors have studied exact controllability for differential control systems (see [5,6,7,22,23,24] and references therein). It should be pointed out that some studies on controllability of abstract control systems contain a similar technical error when the compactness of the semigroup generated by the linear part and the invertibility of the controllability operator are satisfied, and in this case the application of exact controllability results is just restricted to the finite dimensional space and it fails in infinite dimensional space [23].

In recent years, Stochastic differential equations have attracted great interest due to their successful applications to problems in mechanics, electricity, economics, physics and several fields in engineering. For details, see [8,9,32,33,34,35,36,37,38] and references therein. In particular, some researchers investigated controllability of stochastic dynamical control systems in infinite dimensional spaces [25,26,27,28,29]. It is generally known that nonlocal initial conditions can be applied in physics with better effect than the classical Cauchy problem traditional initial condition. However, to the best of our knowledge, the exact controllability of stochastic control systems with nonlocal conditions of the form (1.1) has not yet been studied. Therefore, a natural problem is as follows: how to investigate the exact controllability of stochastic evolution equations involving noncompact semigroups?

Motivated by this consideration, in this article we establish the exact controllability for fractional stochastic evolution equations with nonlocal conditions of the form (1.1) in a Hilbert space under the assumption that the semigroup is noncompact. By using some constructive control functions, we transfer the controllability problem into a fixed-point problem and then apply the measure of noncompactness and the Mönch fixed point theorem to discuss the controllability for problem (1.1). We delete the compactness of semigroup T ( t ) ( t > 0 ) , so our theorems guarantee the effectiveness of controllability results in the infinite dimensional spaces. Furthermore, we give a useful way to discuss stochastic control systems with noncompact semigroups.

We organize the article in the following way. In Section 2, we introduce some useful definitions and preliminary results to be used in this article. In Section 3, we state and prove the exact controllability results for fractional stochastic evolution equations with nonlocal conditions. Finally, in Section 4, an example is provided to illustrate the applications of the obtained results.

2 Preliminaries

In this section, we introduce notations, definitions and preliminary facts, which are used throughout this article.

Let ( Ω , , { t } t 0 , P ) be a filtered complete probability space satisfying the usual condition, which means that the filtration is a right continuous increasing family and 0 contains all P-null sets. Let { e k , k } be a complete orthonormal basis of K . { W ( t ) : t 0 } is a cylindrical K -valued Brownian motion or Wiener process defined on the probability space ( Ω , , { t } t 0 , P ) with a finite trace nuclear covariance operator Q 0 , we denote Tr ( Q ) = k = 1 λ k = λ < , which satisfies that Q e k = λ k e k , k . Let { W k ( t ) , k } be a sequence of one-dimensional standard Wiener processes mutually independent on ( Ω , , { t } t 0 , P ) such that

W ( t ) = k = 1 λ k W k ( t ) e k , t 0 .

Furthermore, we assume that t = σ { W ( s ) , 0 s t } is the σ -algebra generated by W and b = .

Let L 2 0 = L 2 ( Q 1 / 2 K ,   ) denote the space of all Hilbert-Schmidt operators from Q 1 / 2 K into with the inner product ( ϕ , φ ) = Tr ( ϕ Q φ ) . It also turns out to be a separable Hilbert space. The collection of all b -measurable, square-integrable -valued random variables, denoted L 2 ( Ω , ) , is a Banach space equipped with the norm x L 2 = ( E x ( ω ) 2 ) 1 / 2 , where E denotes the expectation with respect to the measure P. Let C ( J , L 2 ( Ω , ) ) be the Banach space of all continuous mappings from J to L 2 ( Ω , ) satisfying sup t J ( E x ( t ) 2 ) < . We use to denote the space of all t -adapted measurable processes x C ( J , L 2 ( Ω , ) ) endowed with the norm x = ( sup t J E x ( t ) 2 ) 1 / 2 . The theory of stochastic integrals in a Hilbert space can be found in [34,36].

In the rest of the manuscript, we suppose that A generates an equicontinuous C 0 -semigroup T ( t ) ( t 0 ) of uniformly bounded linear operator in . That is, there exists a positive constant M 1 such that T ( t ) M for all t 0 . For any constant r > 0 , let B r = { x : x 2 r } . Evidently, B r is a bounded closed convex set in .

By [29, Proposition 2.8], we have the following result which will be used throughout this article.

Lemma 2.1

If h : J × L ( K ,   ) is continuous and x C ( J , L 2 ( Ω , ) ) , then

E J h ( t ,   x ( t ) ) d W ( t ) 2 Tr ( Q ) J E h ( t ,   x ( t ) ) 2 d t .

Definition 2.1

[10] The Riemann-Liouville fractional integral of order α > 0 of a function y : ( 0 , + ) is given by

I 0 α y ( t ) = 1 Γ ( α ) 0 t ( t s ) α 1 y ( s ) d s ,

provided the right side is pointwise defined on ( 0 , + ) .

Definition 2.2

[10] The Riemann-Liouville fractional derivative of order α > 0 of a function y : [ 0 , + ) is given by

D 0 α y ( t ) = 1 Γ ( n α ) ( d d t ) n 0 t y ( s ) ( t s ) α n + 1 d s ,

where n = [ α ] + 1 , provided that the right side is pointwise defined on ( 0 , + ) .

Definition 2.3

[10] The Caputo fractional derivative of order α > 0 of a function y : [ 0 , + ) is given by

D 0 α c y ( t ) = D 0 α [ y ( t ) k = 0 n 1 t k k ! y ( k ) ( 0 ) ] ,

where n = [ α ] + 1 , provided that the right side is pointwise defined on ( 0 , + ) .

Remark 2.1

  1. In the case y ( t ) C n [ 0 , + ) , then

D 0 α c y ( t ) = 1 Γ ( n α ) 0 t y ( n ) ( s ) ( t s ) α n + 1 d s = I 0 n α y ( n ) ( t ) .

  1. If y ( t ) is an abstract function with values in E, then the integrals which appear in Definitions 2.1, 2.2 and 2.3 are taken in Bochner’s sense.

  1. The Caputo derivative of a constant is equal to zero.

For x , we define two operators T α ( t ) ( t 0 ) and S α ( t ) ( t 0) as follows:

(2.1) T α ( t ) x = 0 ζ α ( θ ) T ( t α θ ) x d θ ,     S α ( t ) x = α 0 θ ζ α ( θ ) T ( t α θ ) x d θ ,

where

ζ α ( θ ) = 1 α θ 1 1 / α ρ α ( θ 1 / α ) , ρ α ( θ ) = 1 π k = 0 ( 1 ) n 1 θ α n 1 Γ ( n α + 1 ) n ! sin ( n π α ) , θ ( 0 , ) .

ζ α ( θ ) is a probability density function defined on ( 0 , + ) , that is,

(2.2) ζ α ( θ ) 0 ,   θ ( 0 , ) , 0 ζ α ( θ ) d θ = 1 , 0 θ ζ α ( θ ) d θ = 1 Γ ( 1 + α ) .

The following properties about the operators T α ( t ) ( t 0 ) and S α ( t ) ( t 0 ) , which can be found in [11,12], will be needed in our argument.

Lemma 2.2

The operators T α ( t ) ( t 0 ) and S α ( t ) ( t 0 ) satisfy the following properties:

  1. For any fixed t 0 , T α ( t ) and S α ( t ) are linear and bounded operators in , i.e., for any x ,

    (2.3) T α ( t ) x M x ,    S α ( t ) x M Γ ( α ) x .

  2. For every x , t T α ( t ) x and t S α ( t ) x are continuous functions from [ 0 , ) into .

  3. The operators T α ( t ) and S α ( t ) are strongly continuous.

  4. If semigroup T ( t ) is an equicontinuous semigroup, T α ( t ) and S α ( t ) are also equicontinuous in for t > 0 .

Now, we recall some properties of the measure of noncompactness, which will be used later.

Let μ ( ) denote the Kuratowski measure of noncompactness of the bounded set. For the details of the definition and properties of the measure of noncompactness [39]. Let X be a Banach space, for any D C ( J , X ) and t J , let D ( t ) = { x ( t ) : x D } X . If D is bounded in C ( J , X ) , then D ( t ) is bounded in X, and μ ( D ( t ) ) μ ( D ) .

The following lemmas are needed in our arguments.

Lemma 2.3

[40] Let X be a Banach space and D C ( J , X ) be bounded and equicontinuous, where J is a finite closed interval in . Then, μ ( D ( t ) ) is continuous on J, and

μ ( D ) = max t J μ ( D ( t ) ) = μ ( D ( J ) ) .

Lemma 2.4

[41] Let D = { u n } C ( J , X ) be a bounded and countable set. Then, μ ( D ( t ) ) is the Lebesgue integral on J, and

μ ( { J u n ( t ) d t | n } ) 2 J μ ( D ( t ) ) d t .

In this article, we adopt the following definition of the mild solution of (1.1) based on [27,36].

Definition 2.4

For any given u L 2 ( J ,   U ) , a stochastic process x is said to be a mild solution of (1.1) on J if x satisfies

  1. x ( t ) is measurable and adapted to t ;

  2. x ( t ) satisfies the following integral equation:

x ( t ) = T α ( t ) ( x 0 g ( x ) ) + 0 t ( t s ) α 1 S α ( t s ) [ f ( s ,   x ( s ) ) + B u ( s ) ] d s + 0 t ( t s ) α 1 S α ( t s ) σ ( s ,   x ( s ) ) d W ( s ) .

Let x ( b ; u ) be the state value of system (1.1) at terminal time b corresponding to control u. The set ( b ) = { x ( b ; u ) :   u L 2 ( J ,   U ) } is called the reachable set of (1.1) at the terminal time b.

Definition 2.5

[28] (Exact controllability) The fractional stochastic control system (1.1) is called exact controllable on the interval J if ( b ) = L 2 ( Ω , ) .

To prove the controllability result, the following hypotheses are necessary throughout the article: (H1) The linear operator Φ : L 2 ( J ,   U ) defined by

Φ u = 0 b ( b s ) α 1 S α ( b s ) B u ( s ) d s

satisfies:

  1. Φ has an inverse operator Φ 1 which takes values in L 2 ( J ,   U ) \ ker Φ , and there exist two constants L B and L Φ such that B L B , Φ 1 L Φ ;

  2. There exist a constant q 0 ( 0 ,   q ) and a function k Φ L 1 / q 0 ( J ,   + ) such that

μ ( Φ 1 ( D ) ( t ) ) k Φ ( t ) μ ( D )

for any countable subset D .

(H2) The function f : J × satisfies:

  1. For any t J , f ( t ,   ) is continuous, and f ( ,   x ) is strongly measurable for all x ;

  2. For some r > 0 , there exists a function ξ f L 1 ( J ,   + ) such that

    sup x 2 r E f ( t ,   x ) 2 ξ f ( t ) , t J ,

    where ξ f ( t ) satisfies

    lim inf r + ξ f L 1 r Λ 1 < ;

  3. For any bounded and countable set D , there exist a constant q 1 ( 0 ,   α ) and a function k f L 1 / q 1 ( J ,   + ) such that

μ ( f ( t ,   D ) ) k f ( t ) μ ( D ) , t J .

(H3) The function σ : J × L 2 0 satisfies the following conditions:

  1. For t J , σ ( t ,   ) is continuous, and σ ( ,   x ) is strongly measurable for all x ;

  2. For some r > 0 , there exist a constant q 2 ( 0 ,  2 α 1 ) and a function ξ σ L 1 / q 2 ( J ,   + ) such that

    sup x 2 r E σ ( t ,   x ) L 2 0 2 ξ σ ( t ) , t J ,

    where ξ σ ( t ) satisfies

    lim inf r + ξ σ L 1 / q 2 r Λ 2 < ;

  3. For any bounded and countable set D , there exist a constant q 3 ( 0 , 2 α 1 2 ) and a function k σ L 1 / q 3 ( J ,   + ) such that

μ ( σ ( t D ) ) k σ ( t ) μ ( D ),     t J .

(H4) g : is continuous and there exists a constant K > 0 such that for any r > 0

E g ( x ) g ( y ) 2 K x y 2 , x , y B r .

For any x 1 L 2 ( Ω , ) , we introduce a control u ( t ) u ( t ; x ) by

u ( t ; x ) = Φ 1 [ x 1 T α ( b ) ( x 0 g ( x ) ) 0 b ( b s ) α 1 S α ( b s ) f ( s ,   x ( s ) ) d s 0 b ( b s ) α 1 S α ( b s ) σ ( s ,   x ( s ) ) d W ( s ) ] ( t ) .

Next, we estimate some properties of control u ( t ) defined above.

Lemma 2.5

Suppose that assumptions (H1)–(H4) are satisfied, then for any x B r , the following conclusions hold:

  1. E u ( t ; x ) 2 L u ;

  2. u ( t ; x ) is continuous in B r ,

where

L u = L Φ 2 ( 4 E x 1 2 + 12 M 2 E x 0 2 + 12 M 2 r + 12 M 2 E g ( θ ) 2 + 4 c 0 ξ f L 1 + 4 T r ( Q ) c 2 ξ σ L 1 / q 2 ) , c 0 = M 2 Γ 2 ( α ) b 2 α 1 2 α 1 , c 2 = M 2 Γ 2 ( α ) ( 1 q 2 2 α 1 q 2 ) 1 q 2 b 2 α 1 q 2 .

Proof

For t J and x B r , by the Hölder inequality, conditions (H1)(i), (H2)(i)(ii), (H3)(i)(ii), (H4), (2.3) and Lemma 2.1, we get that

E u ( t ; x ) 2 L Φ 2 ( 4 E x 1 2 + 4 M 2 E x 0 g ( x ) 2 + 4 E 0 b ( b s ) α 1 S α ( b s ) f ( s ,   x ( s ) ) d s 2 + 4 E 0 b ( b s ) α 1 S α ( b s ) σ ( s ,   x ( s ) ) d W ( s ) 2 ) L Φ 2 ( 4 E x 1 2 + 12 M 2 E x 0 2 + 12 M 2 x 2 + 12 M 2 E g ( θ ) 2 + 4 M 2 Γ 2 ( α ) b 2 α 1 2 α 1 0 b ξ f ( s ) d s + 4 Tr ( Q ) M 2 Γ 2 ( α ) 0 b ( b s ) 2 α 2 E σ ( s ,   x ( s ) ) L 2 0 2 d s ) L Φ 2 ( 4 E x 1 2 + 12 M 2 E x 0 2 + 12 M 2 r + 12 M 2 E g ( θ ) 2 + 4 M 2 Γ 2 ( α ) b 2 α 1 2 α 1 ξ f L 1 + 4 Tr ( Q ) M 2 Γ 2 ( α ) ( 1 q 2 2 α 1 q 2 ) 1 q 2 b 2 α 1 q 2 ξ σ L 1 / q 2 ) = L u .

Next, we prove (ii). Let x n x in B r , then we have

f ( t ,   x n ( t ) ) f ( t ,   x ( t ) ) , σ ( t ,   x n ( t ) ) σ ( t ,   x ( t ) ) , ( n ) .

Moreover, for all t J , using the Hölder inequality and Lebesgue dominated convergence theorem, we can get

(2.4) E 0 t ( t s ) α 1 S α ( t s ) [ f ( s ,   x n ( s ) ) f ( s ,   x ( s ) ) ] d s 2 M 2 Γ 2 ( α ) 0 t ( t s ) 2 α 2 d s 0 t E f ( s ,   x n ( s ) ) f ( s ,   x ( s ) ) 2 d s M 2 Γ 2 ( α ) b 2 α 1 2 α 1 0 t E f ( s ,   x n ( s ) ) f ( s ,   x ( s ) ) 2 d s 0 ( n ) .

On the other hand, from Lemma 2.1, the Hölder inequality and Lebesgue dominated convergence theorem, we obtain

(2.5) E 0 t ( t s ) α 1 S α ( t s ) [ σ ( s ,   x n ( s ) ) σ ( s ,   x ( s ) ) ] d W ( s ) 2 4 Tr ( Q ) M 2 Γ 2 ( α ) 0 t ( t s ) 2 α 2 E σ ( s ,   x n ( s ) ) σ ( s ,   x ( s ) ) 2 d s 0 ( n ) .

According to the inequality obtained above, we obtain the following relation:

E u ( t ; x n ) u ( t ; x ) 2 3 L Φ 2 M 2 E g ( x n ) g ( x ) 2 + 3 L Φ 2 E 0 b ( b s ) α 1 S α ( b s ) [ f ( s ,   x n ( s ) ) f ( s ,   x ( s ) ) ] d s 2 + 3 L Φ 2 E 0 b ( b s ) α 1 S α ( b s ) [ σ ( s ,   x n ( s ) ) σ ( s ,   x ( s ) ) ] d W ( s ) 2 0 ( n ) .

Therefore, u ( t ; x ) is continuous in B r . This completes the proof of Lemma 2.5.□

At the end of this section, we present the Mönch fixed point theorem, which plays a key role in our proof of controllability for system (1.1).

Lemma 2.6

[42] Let Ω be a closed convex subset of a Banach space X and θ Ω . Assume that P :   Ω Ω is a continuous map, which satisfies Mönch’s condition, i.e., for D Ω is countable and D c o ¯ ( { θ } P ( D ) ) D is compact. Then, P has at least one fixed point in X.

3 Main results

In this section, we shall discuss the exact controllability of the fractional stochastic dynamical control system (1.1) by using the measure of noncompactness and Mönch fixed point theorem.

Theorem 3.1

Assume that A generates an equicontinuous C 0 -semigroup T ( t ) ( t 0 ) of uniformly bounded operators in Hilbert space . If assumptions (H1)–(H4) are satisfied, then fractional stochastic control systems with nonlocal conditions ( 1.1 ) are exact controllability on J provided that

(3.1) 9 M 2 + 6 c 0 Λ 1 + 72 c 0 b M 2 L Φ 2 L B 2 + 24 c 0 2 b L Φ 2 L B 2 Λ 1 + 24 c 0 c 2 b Tr ( Q ) L Φ 2 L B 2 Λ 2 + 3 c 2 Tr ( Q ) Λ 2 < 1

and

(3.2) ρ ( M ¯ + L B M ¯ b α q 0 ξ Φ L 1 / q 0 ( 1 q 0 α q 0 ) 1 q 0 ) < 1 ,

where

M ¯ = M K 1 / 2 + 2 M b 1 q 1 k f L 1 / q 1 Γ ( α ) ( 1 q 1 α q 1 ) 1 q 1 + M k σ L 1 / q 3 ( 2 T r ( Q ) b 2 α 1 2 q 3 ) 1 / 2 Γ ( α ) ( 1 2 q 3 2 α 1 2 q 3 ) 1 2 q 3 / 2 .

Proof

To begin with, we define an operator F :   as follows:

(3.3) ( F x ) ( t ) = T α ( t ) ( x 0 g ( x ) ) + 0 t ( t s ) α 1 S α ( t s ) [ f ( s ,   x ( s ) ) + B u ( s ;   x ) ] d s + 0 t ( t s ) α 1 S α ( t s ) σ ( s ,   x ( s ) ) d W ( s ) .

It is easy to see that the mild solution of control system (1.1) is equivalent to the fixed point of the operator F defined by (3.3). Next, we complete the proof by four steps.

Step 1. We show that there exists a positive constant r such that F ( B r ) B r . If this is not true, then for any r > 0 , there would exist x r B r and t r J such that E ( F x r ) ( t r ) 2 > r . From Lemma 2.5, we obtain

r < E ( F x r ) ( t r ) 2 3 E T α ( t r ) ( x 0 g ( x r ) ) 2 + 3 E 0 t r ( t r s ) α 1 S α ( t r s ) [ f ( s ,   x r ( s ) ) + B u ( s ;   x r ) ] d s 2 + 3 E 0 t r ( t r s ) α 1 S α ( t r s ) σ ( s ,   x r ( s ) ) d W ( s ) 2 9 M 2 E x 0 2 + 9 M 2 x r 2 + 9 M 2 E g ( θ ) 2 + 3 M 2 Γ 2 ( α ) b 2 α 1 2 α 1 × 0 t r E f ( s ,   x r ( s ) ) + B u ( s ;   x r ) 2 d s + 3 Tr ( Q ) M 2 Γ 2 ( α ) 0 t r ( t r s ) 2 α 2 E σ ( s ,   x r ( s ) ) L 2 0 2 d s 9 M 2 E x 0 2 + 9 M 2 r + 9 M 2 E g ( θ ) 2 + 3 c 0 ( 2 ξ f L 1 + 2 b L B 2 L u ) + 3 c 2 T r ( Q ) ξ σ L 1 / q 1 .

Dividing both sides by r and taking the lower limit as r + , we obtain

9 M 2 + 6 c 0 Λ 1 + 72 c 0 b M 2 L Φ 2 L B 2 + 24 c 0 2 b L Φ 2 L B 2 Λ 1 + 24 c 0 c 2 b Tr ( Q ) L Φ 2 L B 2 Λ 2 + 3 c 2 Tr ( Q ) Λ 2 1 ,

which contradicts (3.1). Hence, for some positive integer r > 0 , F ( B r ) B r .

Step 2. we prove that F : B r B r is a continuous operator. Let x n ,   x B r and x n x ( n ) , then for any t J , we have

E ( F x n ) ( t ) ( F x ) ( t ) 2 4 E T α ( t ) ( g ( x n ) g ( x ) ) 2 + 4 E 0 b ( b s ) α 1 S α ( t s ) [ f ( s ,   x n ( s ) ) f ( s ,   x ( s ) ) ] d s 2 + 4 E 0 b ( b s ) α 1 S α ( b s ) [ σ ( s ,   x n ( s ) ) σ ( s ,   x ( s ) ) ] d W ( s ) 2 + 4 E 0 b ( b s ) α 1 S α ( t s ) B [ u ( s ,   x n ) u ( s ,   x ) ] d s 2 .

For t J , (2.4), (2.5) and the Lebesgue dominated convergence theorem then give

E ( F x n ) ( t ) ( F x ) ( t ) 2 0 ( n ) , t J .

Therefore, ( F x n ) ( t ) ( F x ) ( t ) 0 ( n ) , which means that F is continuous in B r .

Step 3. We prove that F ( B r ) is an equicontinuous family of functions on [ 0 , b ] . For any x B r and 0 t 1 < t 2 b , we get that

E ( F x ) ( t 2 ) ( F x ) ( t 1 ) 2 = 7 E ( T α ( t 2 ) T α ( t 1 ) ) ( x 0 g ( x ) ) 2 + 7 E t 1 t 2 ( t 2 s ) α 1 S α ( t 2 s ) [ f ( s ,   x ( s ) ) + B u ( s , x ) ] d s 2 + 7 E 0 t 1 [ ( t 2 s ) α 1 ( t 1 s ) α 1 ] S α ( t 2 s ) [ f ( s ,   x ( s ) ) + B u ( s , x ) ] 2 + 7 E 0 t 1 ( t 1 s ) α 1 [ S α ( t 2 s ) S α ( t 1 s ) ] [ f ( s ,   x ( s ) ) + B u ( s , x ) ] 2 + 7 E t 1 t 2 ( t 2 s ) α 1 S α ( t 2 s ) σ ( s ,   x ( s ) ) d W ( s ) 2 + 7 E 0 t 1 [ ( t 2 s ) α 1 ( t 1 s ) α 1 ] S α ( t 2 s ) σ ( s ,   x ( s ) ) d W ( s ) 2 + 7 E 0 t 1 ( t 1 s ) α 1 [ S α ( t 2 s ) S α ( t 1 s ) ] σ ( s ,   x ( s ) ) d W ( s ) 2 = I 1 + I 2 + I 3 + I 4 + I 5 + I 6 + I 7 .

In order to prove that E ( F x ) ( t 2 ) ( F x ) ( t 1 ) 2 0 ( t 2 t 1 0 ) , we only need to check I i 0 independently of x B r when t 2 t 1 0 for i = 1 , 2 , , 7 .

Applying Lemma 2.2, it is easy to see that I 1 0 as t 2 t 1 0 . For I 2 and I 5, from (H2)(ii), (H3)(ii), Lemmas 2.1 and 2.5, we obtain the estimate

I 2 = 7 E t 1 t 2 ( t 2 s ) α 1 S α ( t 2 s ) [ f ( s ,   x ( s ) ) + B u ( s , x ) ] d s 2 7 M 2 Γ 2 ( α ) t 1 t 2 ( t 2 s ) 2 α 2 d s t 1 t 2 E f ( s ,   x ( s ) ) + B u ( s , x ) 2 d s 7 M 2 ( 2 ξ f L 1 + 2 L B 2 L u b ) Γ 2 ( α ) ( t 2 t 1 ) 2 α 1 2 α 1 ( t 2 t 1 0 ) ,

I 5 = 7 E t 1 t 2 ( t 2 s ) α 1 S α ( t 2 s ) σ ( s ,   x ( s ) ) d W ( s ) 2 7 Tr ( Q ) M 2 Γ 2 ( α ) t 1 t 2 ( t 2 s ) 2 α 2 E σ ( s ,   x ( s ) ) 2 d s 7 Tr ( Q ) M 2 ξ σ L 1 / q 1 Γ 2 ( α ) ( 1 q 1 2 α 1 q 1 ) 1 q 1 ( t 2 t 1 ) 2 α 1 q 1 ( t 2 t 1 0 ) .

Similarly, for I 3 and I 6 , we get

I 3 = 7 E 0 t 1 [ ( t 2 s ) α 1 ( t 1 s ) α 1 ] S α ( t 2 s ) [ f ( s ,   x ( s ) ) + B u ( s , x ) ] 2 7 M 2 Γ 2 ( α ) 0 t 1 [ ( t 2 s ) α 1 ( t 1 s ) α 1 ] 2 d s 0 t 1 E f ( s ,   x ( s ) ) + B u ( s , x ) 2 d s 7 M 2 ( 2 ξ f L 1 + 2 L B 2 L u b ) Γ 2 ( α ) 0 t 1 [ ( t 2 s ) α 1 ( t 1 s ) α 1 ] 2 d s ( t 2 t 1 0 ) ,

I 6 = 7 E 0 t 1 [ ( t 2 s ) α 1 ( t 1 s ) α 1 ] S α ( t 2 s ) σ ( s ,   x ( s ) ) 2 7 Tr ( Q ) M 2 Γ 2 ( α ) 0 t 1 [ ( t 2 s ) α 1 ( t 1 s ) α 1 ] 2 E σ ( s ,   x ( s ) ) 2 d s 7 Tr ( Q ) M 2 ξ σ L 1 / q 2 Γ 2 ( α ) ( 0 t 1 [ ( t 2 s ) α 1 ( t 1 s ) α 1 ] 2 / 1 q 2 d s ) 1 q 2 ( t 2 t 1 0 ) .

Furthermore, for I 4 and I 7 , if t 1 = 0 ,  0 < t 2 < b , it is easy to see I 4 = I 7 = 0 , so for t 1 > 0 and 0 < ε < t 1 small enough, we obtain the following inequalities:

I 4 = 7 E 0 t 1 ( t 1 s ) α 1 [ S α ( t 2 s ) S α ( t 1 s ) ] [ f ( s ,   x ( s ) ) + B u ( s , x ) ] d s 2 14 E 0 t 1 ε ( t 1 s ) α 1 [ S α ( t 2 s ) S α ( t 1 s ) ] [ f ( s ,   x ( s ) ) + B u ( s , x ) ] d s 2 + 14 E t 1 ε t 1 ( t 1 s ) α 1 [ S α ( t 2 s ) S α ( t 1 s ) ] [ f ( s ,   x ( s ) ) + B u ( s , x ) ] d s 2 14 sup s [ 0 , t 1 ε ] S α ( t 2 s ) S α ( t 1 s ) 2 ( 2 ξ f L 1 + 2 L B 2 L u b ) t 1 2 α 1 ε 2 α 1 2 α 1 + 14 ( 2 M Γ ( α ) ) 2 ( 2 ξ f L 1 + 2 L B 2 L u b ) ε 2 α 1 2 α 1 ( t 2 t 1 0 and ε 0 ) ,

I 7 = 7 E 0 t 1 ( t 1 s ) α 1 [ S α ( t 2 s ) S α ( t 1 s ) ] σ ( s ,   x ( s ) ) d W ( s ) 2 14 E 0 t 1 ε ( t 1 s ) α 1 [ S α ( t 2 s ) S α ( t 1 s ) ] σ ( s ,   x ( s ) ) d s 2 + 14 E t 1 ε t 1 ( t 1 s ) α 1 [ S α ( t 2 s ) S α ( t 1 s ) ] σ ( s ,   x ( s ) ) d s 2 14 Tr ( Q ) ( 1 q 2 ) 2 α 1 q 2 sup s [ 0 , t 1 ε ] S α ( t 2 s ) S α ( t 1 s ) 2 ξ σ 1 / L q 2 ( t 1 2 α 1 q 2 1 q 2 ε 2 α 1 q 2 1 q 2 ) 1 q 2 + 14 Tr ( Q ) ( 2 M Γ ( α ) ) 2 ξ σ 1 / L q 2 ( 1 q 1 2 α 1 q 2 ) 2 α 1 q 2 ε 2 α 1 q 2 ( t 2 t 1 0 and ε 0 ) .

Above all, we have I i 0 as t 2 t 1 0 and ε 0 , which means F ( B r ) is equicontinuous.

Step 4. We will prove that F satisfies Mönch’s condition. Let F = F 1 + F 2 , where

F 1 ( x ) ( t ) = T α ( t ) ( x 0 g ( x ) ) ,

F 2 ( x ) ( t ) = 0 t ( t s ) α 1 S α ( t s ) [ f ( s ,   x ( s ) ) + B u ( s ;   x ) ] d s + 0 t ( t s ) α 1 S α ( t s ) σ ( s ,   x ( s ) ) d W ( s ) .

Suppose that D B r be countable and D c o ¯ ( { 0 } F ( D ) ) , for any t J ,   x , y D , by (H1), we get

E F 1 ( x ) ( t ) F 1 ( y ) ( t ) 2 = E T α ( t ) ( g ( x ) g ( y ) ) 2 M 2 K x y 2 .

Moreover, we obtain

F 1 ( x ) ( t ) F 1 ( y ) ( t ) M K 1 / 2 x y .

From the definition of the measure of noncompactness, it follows that

(3.4) μ ( F 1 ( D ) ) M K 1 / 2 μ ( D ) .

Applying Lemma (2.1), we obtain the estimate

0 t ( t s ) α 1 S α ( t s ) [ σ ( s ,   x ( s ) ) σ ( s ,   y ( s ) ) ] d W ( s ) ( 0 t ( t s ) α 1 S α ( t s ) [ σ ( s ,   x ( s ) ) σ ( s ,   y ( s ) ) ] d W ( s ) 2 ) 1 / 2 M Γ ( α ) ( Tr ( Q ) 0 t ( t s ) 2 α 2 σ ( s ,   x ( s ) ) σ ( s ,   y ( s ) ) 2 d s ) 1 / 2 .

So,

(3.5) μ ( 0 t ( t s ) α 1 σ ( s ,   D ( s ) ) d W ( s ) ) M Γ ( α ) ( 2 Tr ( Q ) 0 t ( t s ) 2 α 2 [ μ ( σ ( s ,   D ( s ) ) ) ] 2 d s ) 1 / 2 .

From the above inequalities (3.4), (3.5) and using assumptions (H1)(ii), (H2)(iii), (H3)(iii) and Lemma 2.4, we have

μ ( u ( t , D ) ) k Φ ( t ) μ ( x 1 T α ( b ) ( x 0 g ( x ) ) 0 b ( b s ) α 1 S α ( t s ) f ( s ,   D ( s ) ) d s 0 b ( b s ) α 1 S α ( b s ) σ ( s ,   D ( s ) ) d W ( s ) ) k Φ ( t ) ( μ ( T α ( b ) ( x 0 g ( x ) ) ) + μ ( 0 b ( b s ) α 1 S α ( t s ) f ( s ,   D ( s ) ) d s ) + μ ( 0 b ( b s ) α 1 S α ( b s ) σ ( s ,   D ( s ) ) d W ( s ) ) ) k Φ ( t ) ( M K 1 / 2 μ ( D ) + 2 M Γ ( α ) 0 b ( b s ) α 1 μ ( f ( s ,   D ( s ) ) ) d s + M Γ ( α ) ( 2 Tr ( Q ) 0 b ( t s ) 2 α 2 [ μ ( σ ( s ,   D ( s ) ) ) ] 2 d s ) 1 / 2 ) k Φ ( t ) ( M K 1 / 2 + 2 M b α q 1 k f L 1 q 1 Γ ( α ) ( 1 q 1 α q 1 ) 1 q 1 + M k σ L 1 / q 3 ( 2 Tr ( Q ) b 2 α 1 2 q 3 ) 1 / 2 Γ ( α ) ( 1 2 q 3 2 α 1 2 q 3 ) 1 2 q 3 / 2 ) μ ( D ) = k Φ ( t ) M ¯ μ ( D ) .

Now we estimate the measure of noncompactness of F ( D ) . For t J , we have

μ ( ( F D ) ( t ) ) = μ ( ( F 1 D ) ( t ) ) + μ ( ( F 2 D ) ( t ) ) μ ( F 1 D ) + μ ( 0 t ( t s ) α 1 S α ( t s ) [ f ( s ,   D ( s ) ) + B u ( s , D ) ] d s + 0 t ( t s ) α 1 S α ( t s ) σ ( s ,   D ( s ) ) d W ( s ) ) M K 1 2 μ ( D ) + 2 M Γ ( α ) 0 t ( t s ) α 1 μ ( f ( s ,   D ( s ) ) + B u ( s , D ) ) ) d s + M Γ ( α ) ( 2 Tr ( Q ) 0 t ( t s ) 2 α 2 [ μ ( σ ( s ,   D ( s ) ) ) ] 2 d s ) 1 / 2 M K 1 / 2 μ ( D ) + 2 M Γ ( α ) ( b α q 1 k f L 1 / q 1 ( 1 q 1 α q 1 ) 1 q 1    + L B M ¯ b α q 0 ξ Φ L 1 / q 0 ( 1 q 0 α q 0 ) 1 q 0 ) μ ( D ) + ( M k σ L 1 / q 3 ( 2 Tr ( Q ) b 2 α 1 2 q 3 ) 1 / 2 Γ ( α ) ( 1 2 q 3 2 α 1 2 q 3 ) 1 2 q 3 2 ) μ ( D ) = ( M ¯ + L B M ¯ b α q 0 ξ Φ L 1 / q 0 ( 1 q 0 α q 0 ) 1 q 0 ) μ ( D ) = ρ μ ( D ) .

It follows from Lemma 2.3 that

μ ( F ( D ) ) = max t J μ ( ( F D ) ( t ) ) ρ μ ( D ) .

Hence, we get

μ ( D ) μ ( c o ¯ ( { 0 } F ( D ) ) ) μ ( F D ) ρ μ ( D ) .

From assumption (3.2), we know that ρ < 1 , which means μ ( D ) = 0 , that is, D is relatively compact. By Lemma 2.6, F has at least one fixed point x B r , which is a mild solution of the fractional stochastic control system (1.1) and it satisfies x ( b ) = x 1 for any x 1 L 2 ( Ω , ) . Therefore, the fractional stochastic control system (1.1) is exact controllable on J.

This completes the proof of Theorem 3.1.□

Remark 3.2

Impulsive effects exist in many evolution processes, so it is necessary to study impulsive stochastic evolution equations. Upon making some appropriate assumptions, by applying the ideas and techniques as in this article, one can obtain the exact controllability results for a class of fractional impulsive stochastic evolution equations with nonlocal conditions.

4 Application

Example 4.1

Consider the following fractional stochastic control system of the form:

(4.1) { 2 3 t 2 3 x ( z , t ) x ( z , t ) z = x ( z , t ) e t ( 1 + x 2 ( z , t ) ) + e 2 t x ( z , t ) 1 + e t d W ( t ) d t + u ( z , t ) ,   t J ,   z ( 0 , 1 ) , x ( 0 , t ) = x ( 1 , t ) , t J , x ( 0 ) = k = 1 m ( 1 ) k c k x ( z , k ) , z ( 0 , 1 ) ,

where c k , and k = 1 m | c k | 1 . W ( t ) is a standard one-dimensional Brownian motion defined on the filtered probability space ( Ω , , { t } t 0 , P ) . To write the above system (4.1) into the abstract form of (1.1), let = E = U = L 2 [ 0 ,  1 ] with the norm , define the operator A : D ( A ) X by

A v = v , v D ( A ) , D ( A ) = { v ,   v X ,   v ( 0 ) = v ( 1 ) = 0 } .

We know that A generates an equicontinuous semigroup T ( t ) ( t 0 ) in . For any v , T ( t ) v ( s ) = v ( t + s ) . Then, T ( t ) is not a compact semigroup and T ( t ) 1 .

For any t J , let x ( t ) ( z ) = x ( z , t ) , f ( t , x ( t ) ) ( z ) = x ( z , t ) e t ( 1 + x 2 ( z , t ) ) , σ ( t , x ( t ) ) ( z ) = e 2 t x ( z , t ) 1 + e t , B u ( t ) ( z ) = u ( z , t ) and g ( x ) = k = 1 m ( 1 ) k c k x ( z , k ) . Then, problem (4.1) can be rewritten into the abstract form of (1.1). From the definitions of nonlinear terms f and σ , for any r > 0 and x ( t ) , when x ( t ) 2 r , t > 0 , we can easily verify that assumptions (H2)(ii) and (H3)(ii) hold with ξ f ( t ) = r e 2 t ,   ξ σ ( t ) = r e 4 t and Λ 1 = Λ 2 = 1 . Moreover, (H2)(iii) and (H3)(iii) hold with k f ( t ) = k σ ( t ) = 1 e 2 t . (H4) holds with K = k = 1 m | c k | 2 .

For z ( 0 , 1 ) , the linear operator Φ is given by

( Φ u ) ( z ) = 0 b ( b s ) 1 3 S 2 3 ( b s ) ω u ( z , s ) d s ,

where

S 2 3 ( s ) β ( s ) = 2 3 0 θ ζ 2 3 ( θ ) β ( t 2 3 θ + s ) d θ .

Suppose that Φ satisfies assumption (H1), then applying Theorem 3.1, we get that stochastic control system (4.1) is exact controllable on J provided that (3.1) and (3.2) hold.

Example 4.2

Consider the following fractional stochastic control system of the form:

(4.2) { α t α x ( z , t ) x ( z , t ) z = t x ( z , t ) 2 ( 1 + | x ( z , t ) | ) + x ( z , t ) + e t x ( z , t ) d W ( t ) d t + u ( z , t ) ,   t J ,   z ( 0 , 1 ) , x ( 0 , t ) = x ( 1 , t ) , t J , x ( 0 ) = 0 b t x ( z , t ) d t , z ( 0 , 1 ) ,

where 0 < α < 1 , c k and k = 1 m | c k | 1 . W ( t ) is a standard one-dimensional Brownian motion defined on the filtered probability space ( Ω , , { t } t 0 , P ) .

Let = E = U = L 2 [ 0 ,  1 ] with the norm . Define the operator A : D ( A ) X by

A v = v , v D ( A ) , D ( A ) = { v ,   v X ,   v ( 0 ) = v ( 1 ) = 0 } .

Then, A generates an equicontinuous semigroup T ( t ) ( t 0 ) in , and T ( t ) is not a compact semigroup.

For any t J , let x ( t ) ( z ) = x ( z , t ) , and

f ( t , x ( t ) ) ( z ) = t x ( z , t ) 2 ( 1 + | x ( z , t ) | ) + x ( z , t ) , σ ( t , x ( t ) ) ( z ) = e t x ( z , t ) , B u ( t ) ( z ) = u ( z , t ) ,   g ( x ) = 0 b t x ( z , t ) d t .

Then, problem (4.2) can be rewritten into the abstract form of (1.1). For any r > 0 and x ( t ) 2 r , we have

f ( t ,   x ) 2 = 0 1 | t x ( z , t ) 2 ( 1 + | x ( z , t ) | ) + x ( z , t ) | 2 d z ( t 2 2 + 2 ) 0 1 | x ( z , t ) | 2 d z ( t 2 2 + 2 ) r .

Therefore,

sup x 2 r E f ( t ,   x ) 2 ( t 2 2 + 2 ) r , t J .

In addition,

σ ( t ,   x ) 2 = 0 1 | e t x ( z , t ) | 2 d z e 2 t 0 1 | x ( z , t ) | 2 d z e 2 t r .

So assumptions (H2)(ii) and (H3)(ii) hold with ξ f ( t ) = ( t 2 2 + 2 ) r ,   ξ σ ( t ) = e 2 t r and Λ 1 = Λ 2 = 1 . Moreover, for any x 1 ( t ) ,   x 2 ( t )

f ( t ,   x 2 ( t ) ) f ( t ,   x 1 ( t ) ) 2 = 0 1 | t x 2 ( z , t ) 2 ( 1 + | x 2 ( z , t ) | ) + x 2 ( z , t ) t x 1 ( z , t ) 2 ( 1 + | x 1 ( z , t ) | ) + x 1 ( z , t ) | 2 d z ( t 2 2 + 2 ) 0 1 | x 2 ( z , t ) x 1 ( z , t ) | 2 d z ( t 2 2 + 2 ) x 2 ( t ) x 1 ( t ) 2 ,

σ ( t ,   x 2 ( t ) ) σ ( t ,   x 1 ( t ) ) 2 = 0 1 | e t x 2 ( z , t ) e t x 1 ( z , t ) | 2 d z e 2 t x 2 ( t ) x 1 ( t ) 2 .

Hence, (H2)(iii) and (H3)(iii) hold with k f ( t ) = ( t 2 2 + 2 ) 1 / 2 , k σ ( t ) = e t . For any x , y B r ,

g ( x ) g ( y ) 2 = 0 1 | 0 b t x ( z , t ) t y ( z , t ) d t | 2 d z b 3 3 0 1 0 b | x 2 ( z , t ) x 1 ( z , t ) | 2 d t d z b 4 3 sup x 2 ( t ) x 1 ( t ) 2 ,

which means

E g ( x ) g ( y ) 2 K x y 2 ,

where K = b 4 3 .

Suppose that Φ satisfies assumption (H1), then applying Theorem 3.1, we get that stochastic control system (4.2) is exact controllable on J provided that (3.1) and (3.2) hold.

5 Conclusion

In this article, the exact controllability for a class of fractional stochastic evolution equations with nonlocal initial conditions in a Hilbert space is studied. We delete the compactness of semigroup T ( t ) ( t > 0 ) , so our theorems guarantee the effectiveness of controllability results in the infinite dimensional spaces. Moreover, the regularity of mild solution for fractional stochastic evolution equations with nonlocal initial conditions will be the topic of our future work.



Acknowledgments

This research was supported by the National Natural Science Foundation of China (grant numbers 11661071, 11261053 and 11361055).

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Received: 2019-09-11
Revised: 2020-03-13
Accepted: 2020-05-15
Published Online: 2020-07-02

© 2020 Yonghong Ding and Yongxiang Li, published by De Gruyter

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

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  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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