Home Almost periodic functions on time scales and their properties
Article Open Access

Almost periodic functions on time scales and their properties

  • Yongkun Li EMAIL logo and Xiaoli Huang
Published/Copyright: December 16, 2024

Abstract

In this article, we first propose a concept of almost periodic functions on arbitrary time scales, which is defined by trigonometric polynomial approximations with respect to supremum norm, and study some basic properties of these kinds of functions. Then, on almost periodic time scales, we introduce the concepts of the mean value and Fourier series of almost periodic functions and give some related results. Finally, we give the definitions of almost periodic functions in the sense of Bohr and in the sense of Bochner on time scales, respectively, and prove the equivalence of the above three definitions on almost periodic time scales.

MSC 2010: 42A10; 42A75; 26E70

1 Introduction

As we all know, the time scale calculus theory can well unify the research of continuous and discrete analysis problems, and this theory has huge potential application value in mathematics itself, economics, physics, population dynamics, neural networks, and many other disciplines [1,2]. Therefore, in the past few decades, this theory has attracted more and more attention.

On the other hand, almost periodic phenomenon is a universal phenomenon in nature. Since Bohr [3] introduced the concept of almost periodic functions in 1920s, the study of the existence of almost periodic solutions of differential equations, difference equations, and dynamic systems has become one of the important research objects in these fields.

In order to unify the research on the existence of almost periodic solutions for continuous time systems and discrete time systems, Li et al. [4,5] in 2011 first introduced the definition of almost periodic functions on almost periodic time scales in the sense of Bohr, and they also showed some basic properties of these kinds of functions. Since then, the existence of almost periodic solutions of dynamic equations, ecological models, and neural network models on time scales has been broadly studied [623]. However, at present, there is no concept of almost periodic functions defined on arbitrary time scales, and there is no Fourier series theory of almost periodic functions on time scales. These are issues worthy of discussion with theoretical and application value.

Inspired by the above discussion, the main purpose of this study is first to propose a concept of almost periodic functions on arbitrary time scales, that is, to define the collection of almost periodic functions as the completion of the set composed of trigonometric polynomials with respect to the supremum norm, and to study some basic properties of these kinds of functions. Then, on almost periodic time scales, we introduce the concepts of mean value and Fourier series of almost periodic functions and give some related results. Finally, we give the definitions of almost periodic functions on time scales in the sense of Bohr and Bochner, respectively, and prove the equivalence of these three definitions on almost periodic time scales.

The rest of the study is organized as follows. In Section 22, we introduce some notations and definitions of time scale calculus. In Section 3, we propose a concept of almost periodic functions on arbitrary time scales defined by the closure of the set of trigonometric polynomials with respect to the supremum norm and investigate some basic properties of these kinds of functions. In Section 4, we propose a concept of Fourier series associated with an almost periodic function on time scales and present some relative results.

2 Preliminaries

In this section, we collect some definitions and lemmas, which will be used later.

A time scale T is an arbitrary non-empty closed subset of the real set R with the topology and ordering inherited from R . The forward and backward jump operators σ , ρ : T T , and the graininess μ : T R + are defined, respectively, by

σ ( t ) = inf { s T : s > t } , ρ ( t ) = sup { s T : s < t } and μ ( t ) = σ ( t ) t .

A point t T is called left-dense if t > inf T and ρ ( t ) = t , left-scattered if ρ ( t ) < t , right-dense if t < sup T and σ ( t ) = t , and right-scattered if σ ( t ) > t . If T has a left-scattered maximum m , then T k = T \ { m } ; otherwise T k = T . If T has a right-scattered minimum m , then T k = T \ { m } ; otherwise T k = T . For the notations [ a , b ] T , [ a , b ) T , and so on, we will denote time scale intervals [ a , b ] T = { t T : a t b } , where a , b T with a < ρ ( b ) .

A function f : T R is rd-continuous, provided it is continuous at right-dense point in T and its left-side limits exist at left-dense points in T . The collection of all rd-continuous functions f : T R will be denoted by C r d ( T ) . If f is continuous at each right-dense point and each left-dense point, then f is said to be continuous on T . The set of continuous functions f : T R will be denoted by C ( T ) .

Definition 2.1

Let f : T R be a function and t T k . If for every ε > 0 , there exist a δ δ ( ε , t ) > 0 and a number f Δ ( t ) such that

f ( σ ( t ) ) f ( s ) f Δ ( t ) ( σ ( t ) s ) ε σ ( t ) s

for all s U ( t , δ ) ( t δ , t + δ ) T , then we call f Δ ( t ) the delta derivative of f at t .

If f is continuous, then f is right-dense continuous, and if f is delta differentiable at t , then f is continuous at t .

Let f : T R be right-dense continuous. If F Δ ( t ) = f ( t ) , then we define the delta integral by a t f ( s ) Δ s = F ( t ) F ( a ) .

A function p : T R is called regressive if 1 + μ ( t ) p ( t ) 0 for all t T k . The set of all regressive and right-dense continuous functions p : T R will be denoted by = ( T , R ) . We define the set + = { p : 1 + μ ( t ) p ( t ) > 0 , t T } .

Lemma 2.1

[2] If a , b , c T , α R , and f , g C r d ( T ) , then

  1. a b ( f + g ) ( t ) Δ t = a b f ( t ) Δ t + a b g ( t ) Δ t ,

  2. a b α f ( t ) Δ t = α a b f ( t ) Δ t ,

  3. a b f ( t ) Δ t = b a f ( t ) Δ t ,

  4. a b f ( t ) Δ t = a c f ( t ) Δ t + c d f ( t ) Δ t ,

  5. a b f ( σ ( t ) ) g Δ ( t ) Δ t = ( f g ) ( b ) ( f g ) ( a ) a b f Δ ( t ) g ( t ) Δ t ,

  6. a b f ( t ) g Δ ( t ) Δ t = ( f g ) ( b ) ( f g ) ( a ) a b f Δ ( t ) g ( σ ( t ) ) Δ t .

Lemma 2.2

[2] If f , g are delta differentiable on T k , then

  1. ( v 1 f + v 2 g ) Δ = v 1 f Δ + v 2 g Δ , for any constants v 1 , v 2 ;

  2. ( f g ) Δ ( t ) = f Δ ( t ) g ( t ) + f ( σ ( t ) ) g Δ ( t ) = f ( t ) g Δ ( t ) + f Δ ( t ) g ( σ ( t ) ) .

Lemma 2.3

[2] If f is continuous on [ a , b ] and delta differentiable in [ a , b ) , then there exist ξ 1 , ξ 2 [ a , b ) such that

f Δ ( ξ 1 ) ( b a ) f ( b ) f ( a ) f Δ ( ξ 2 ) ( b a ) .

Lemma 2.4

[2] Let f be a function defined on [ a , b ) and c T with a < c < b . If f is Δ -integrable from a to c and c to b, respectively, then f is Δ -integrable on [ a , b ) and

a b f ( t ) Δ t = a c f ( t ) Δ t + c d f ( t ) Δ t .

Throughout this study, X denotes a Banach space with the norm X . Let T be a given time scale, and T is a complete metric space with the metric d defined by

d ( t , t 0 ) = t t 0 for t , t 0 T .

For a given δ > 0 , the δ -neighborhood U ( t 0 , δ ) of a given point t 0 T is the set of all points t T such that d ( t 0 , t ) < δ .

Definition 2.2

[4] Function f : D X is called continuous at t 0 D T if and only if (iff) for any ε > 0 , there exists a δ > 0 such that for any s U ( t 0 , δ ) ( t 0 δ , t 0 + δ ) T ,

f ( s ) f ( t 0 ) X < ε .

The f is called continuous on D , provided that it is continuous for every t D .

Definition 2.3

[4] Function f : D X is called uniformly continuous on D T iff for any ε > 0 , there exists δ ( ε ) such that for any t 1 , t 2 D with t 1 t 2 < δ ( ε ) , it is implied that

f ( t 1 ) f ( t 2 ) X < ε .

3 Almost periodic functions on arbitrary time scales

In this section, we first introduce a new definition of almost periodic functions on arbitrary time scales, then we discuss some properties of these kinds of functions.

Let C ( T , X ) denote the space of all continuous functions from T to X and B C ( T , X ) denote the space of all bounded continuous functions from T to X . It is easy to see that B C ( T , X ) with the norm x = sup t T x ( t ) X is a Banach space.

We give the following definition of trigonometric polynomials defined on T .

Definition 3.1

A function T : T X defined by

(3.1) T ( t ) = k = 1 n a k e i λ k t , t T ,

where for k = 1 , 2 , , n , λ k R , and a k X is called a trigonometric polynomial with values in X .

We denote by T the set of all trigonometric polynomials with values in X . It is obvious that T B C ( T , X ) .

Definition 3.2

A function f C ( T , X ) is said to be almost periodic if for every ε > 0 there exists a trigonometric polynomial T ( t ) T such that

f T < ε .

We denote the space of all such functions by A P ( T , X ) .

Remark 3.1

Obviously, the space A P ( T , X ) is the closure T ¯ of T in the sense of convergence in the norm .

Remark 3.2

A function f A P ( T , X ) iff there exists a sequence of trigonometric polynomials { T n ( t ) } T such that lim n T n ( t ) = f ( t ) uniformly on T .

Lemma 3.1

If T ( t ) T , then T is uniformly continuous on T .

Proof

Let T ( t ) = k = 1 n a k e i λ k t , where a k X , λ k R . For any ε > 0 , there exists δ ( ε ) = ε k = 1 n 2 λ k a k X such that for any t 1 , t 2 T with t 1 t 2 < δ ( ε ) , one has

T ( t 1 ) T ( t 2 ) X k = 1 n a k X e i λ k t 1 e i λ k t 2 k = 1 n a k X ( cos λ k t 1 cos λ k t 2 + sin λ k t 1 sin λ k t 2 ) k = 1 n 2 λ k a k X t 1 t 2 < ε .

Thus, T is uniformly continuous on T . This completes the proof.□

Theorem 3.1

If f A P ( T , X ) , then f is bounded and uniformly continuous on T .

Proof

By Definition 3.2, for any ε > 0 , there exists T ( t ) T such that

f ( t ) T ( t ) X f T < ε .

Let M = sup t T T ( t ) X , we have

f ( t ) X f ( t ) T ( t ) X + T ( t ) X ε + M .

Hence, f is bounded on T .

Now, we will prove f is uniformly continuous on T . Since f A P ( T , X ) , there exists a sequence of trigonometric polynomials { T n ( t ) ; n 1 } T such that

lim n T n ( t ) = f ( t )

uniformly on T . Hence, for any ε > 0 , one can choose n large enough such that

T n ( t ) f ( t ) X < ε 3 , t T .

By Lemma 3.1, T n is uniformly continuous on T . That is, for the previous ε > 0 , there exists δ ( ε ) such that for any t , s T with t s < δ ( ε ) , it is implied that

T n ( t ) T n ( s ) X < ε 3 .

Thus, for t s < δ ( ε ) , we have

f ( t ) f ( s ) X f ( t ) T n ( t ) X + T n ( t ) T n ( s ) X + T n ( s ) f ( s ) X < ε 3 + ε 3 + ε 3 = ε ,

which implies that f is uniformly continuous on T . This completes the proof.□

Theorem 3.2

If { f n ( t ) } A P ( T , X ) and f n ( t ) f ( t ) as n uniformly on T , then f A P ( T , X ) .

Proof

For any ε > 0 , there exists N = N ( ε ) > 0 such that

f ( t ) f n 0 ( t ) X < ε 2 , t T ,

for n 0 > N . Because f n 0 ( t ) A P ( T , X ) , there exists a trigonometric polynomial T ( t ) T such that

f n 0 ( t ) T ( t ) X < ε 2 , t T .

As a consequence,

f ( t ) T ( t ) X f ( t ) f n 0 ( t ) X + f n 0 ( t ) T ( t ) X < ε 2 + ε 2 = ε , t T .

This completes the proof.□

Theorem 3.3

If f , g A P ( T , X ) and λ R , then f + g , λ f A P ( T , X ) .

Proof

Let f , g A P ( T , X ) , for any ε > 0 , there exist two trigonometric polynomials T ( t ) , S ( t ) T such that

f T < ε 2 , g S < ε 2 .

Thus, one has

( f + g ) ( T + S ) f T + g S < ε .

From the above inequality, we derive f + g A P ( T , X ) due to the fact that T ( t ) + S ( t ) T .

The proof of λ f A P ( T , X ) follows immediately from the fact that if T ( t ) T , then λ T ( t ) T . This completes the proof.□

Theorem 3.4

If X is a Banach algebra and φ , ψ A P ( T , X ) , then φ ψ A P ( T , X ) .

Proof

Since φ , ψ A P ( T , X ) , there exist two sequences of trigonometric polynomials { T n 1 ( t ) } and { T n 2 ( t ) } T such that

(3.2) lim n T n 1 ( t ) = φ ( t )

uniformly on T and

(3.3) lim n T n 2 ( t ) = ψ ( t )

uniformly on T . Because X is a Banach algebra, T n 1 ( t ) T n 2 ( t ) and ψ ( t ) φ ( t ) are meaningful. Let T n 1 ( t ) T n 2 ( t ) = S n ( t ) , by (3.2) and (3.3), we obtain

lim n S n ( t ) = ψ ( t ) φ ( t )

uniformly on T . Because S n ( t ) is also a trigonometric polynomial, so φ ψ A P ( T , X ) . This completes the proof.□

In the sequel, we denote C n by the n -dimensional complex vector space with the norm C n .

Lemma 3.2

[24] If f is continuous on a bounded and closed subset Ω of C n , then for any ε > 0 , one can choose a polynomial P ε such that

f ( x ) P ε ( x ) C n < ε , x Ω .

Lemma 3.3

[24] Let P : C n C n be a polynomial and f 1 , f 2 , , f n A P ( R , C ) . Then the function F ( ) = P ( f 1 ( ) , , f n ( ) ) A P ( R , C n ) .

By Lemmas 3.2 and 3.3, the following statement is obvious.

Theorem 3.5

Let F : D C n be a uniformly continuous function, where D is a bounded subset of C n . If f 1 , f 2 , , f n A P ( T , C ) and for each t R , ( f 1 ( t ) , f 2 ( t ) , , f n ( t ) ) D , then f ( ) = F ( f 1 ( ) , f 2 ( ) , , f n ( ) ) A P ( T , C n ) .

Theorem 3.6

If f , g A P ( T , C ) and m inf t T g ( t ) C > 0 , then f g A P ( T , C ) .

Proof

Let M sup t T g ( t ) C , we note that G ( z ) = 1 z is continuous in the crown m z C M . According to Theorem 3.5, if z A P ( T , C ) , then G A P ( T , C ) . Hence, 1 g ( t ) is almost periodic. Consequently, based on Theorem 3.4, f ( t ) g ( t ) is almost periodic. This completes the proof.□

Theorem 3.7

If f C ( C n , C n ) satisfies the Lipschitz condition and x A P ( T , C n ) , then f ( x ( ) ) A P ( T , C n ) .

Proof

Let L represent the Lipschitz constant of f . Since x A P ( T , C n ) , for any ε > 0 , there exists a trigonometric polynomial S ( t ) such that

(3.4) x ( t ) S ( t ) C n < ε 2 L , t T .

In addition, by Lemma 3.2, for any ε > 0 , there exists a polynomial P ε ( S ( t ) ) such that

(3.5) f ( S ( t ) ) P ε ( S ( t ) ) C n < ε 2 , t T .

Obviously, P ε ( S ( t ) ) is also a trigonometric polynomial. Thus, it follows from (3.4) and (3.5) that

f ( x ( t ) ) P ε ( S ( t ) ) C n f ( x ( t ) ) f ( S ( t ) ) C n + f ( S ( t ) ) P ε ( S ( t ) ) C n < L x ( t ) S ( t ) C n + ε 2 < ε 2 + ε 2 = ε , t T .

Hence, f ( x ( ) ) A P ( T , X ) . This completes the proof.□

4 Almost periodic functions on almost periodic time scales

Definition 4.1

[4] A time scale T is called an almost periodic time scale if

Π = { τ R : τ ± t T , t T } { 0 } .

Lemma 4.1

[12] Let T be an almost periodic time scale, and let K = inf { α : α Π for α 0 } . Then, K = 0 iff T = R , and K > 0 iff T R . Moreover, Π = R if T = R , and Π = K Z if T R .

In this section, we always assume that T be an almost periodic time scale, we will study some basic properties of almost periodic functions on T .

Theorem 4.1

If f A P ( T , X ) and h Π , then f ( + h ) A P ( T , X ) .

Proof

By Definition 3.2, for any ε > 0 , there exists a trigonometric polynomial T ( t ) T such that

f T < ε .

It follows immediately from T ( t + h ) T that f ( + h ) A P ( T , X ) .

This completes the proof.□

4.1 Fourier series of almost periodic functions on almost periodic time scales

In order to introduce the Fourier series of an almost periodic function on time scales, we first define the mean value of such a function.

Lemma 4.2

[25] If λ R and λ 0 , then lim l 1 l α α + l e i λ t Δ t = 0 , where α T , l Π .

Definition 4.2

Let f C ( T , X ) , if

M { f } lim l 1 l α α + l f ( t ) Δ t , where α T , l Π ,

exists, then the number M { f } is called the mean value of f .

Theorem 4.2

If f A P ( T , X ) , then

M { f } = lim l 1 l α α + l f ( t ) Δ t , w h e r e α T , l Π

uniformly exists for α T . The number M { f } is independent of α and is called the mean value of f.

Proof

Let

R ( t ) = c 0 + k = 1 m c k e i λ k t , t T ,

where λ k 0 , k = 1 , 2 , , n . It follows from Lemma 4.2 that

lim l 1 l α α + l R ( t ) Δ t = c 0 + lim l k = 1 m c k l α α + l e i λ k t Δ t = c 0 .

That is, for any R ( t ) T , its mean value exists and is independent of α .

Since f A P ( T , X ) , for any ε > 0 , there exists a trigonometric polynomial T ( t ) T such that

(4.1) f ( t ) T ( t ) X < ε 3 , t T ,

and T takes on the following form:

T ( t ) = d 0 + k = 1 m d k e i λ k t , t T ,

where λ k 0 , k = 1 , 2 , , n . Because the mean value of T exists, we can choose N ( ε ) > 0 such that

(4.2) 1 l 1 α α + l 1 T ( t ) Δ t 1 l 2 α α + l 2 T ( t ) Δ t X < ε 3

for l 1 , l 2 Π with l 1 , l 2 N ( ε ) . By (4.1) and (4.2), one has

1 l 1 α α + l 1 f ( t ) Δ t 1 l 2 α α + l 2 f ( t ) Δ t X 1 l 1 α α + l 1 f ( t ) T ( t ) X Δ t + 1 l 1 α α + l 1 T ( t ) Δ t 1 l 2 α α + l 2 T ( t ) Δ t X + 1 l 2 α α + l 2 f ( t ) T ( t ) X Δ t < ε 3 + ε 3 + ε 3 = ε .

Thus, the mean value of f ( t ) exists.

Now, we will prove that M { f } is independent of α T . By Theorem 3.1, note that f = sup t T f ( t ) X < . Let α * , α T , for α * > α , by Lemma 2.4, we have

1 l α α + l f ( t ) Δ t 1 l α * α * + l f ( t ) Δ t X = 1 l α α * f ( t ) Δ t + α * α + l f ( t ) Δ t α * α + l f ( t ) Δ t α + l α * + l f ( t ) Δ t X = 1 l α α * f ( t ) Δ t α + l α * + l f ( t ) Δ t X 2 ( α * α ) f l .

For α * < α , again by Lemma 2.4, we obtain

1 l α α + l f ( t ) Δ t 1 l α * α * + l f ( t ) Δ t X = 1 l α α * + l f ( t ) Δ t + α * + l α + l f ( t ) Δ t α * α f ( t ) Δ t α α * + l f ( t ) Δ t X = 1 l α * + l α + l f ( t ) Δ t α * α f ( t ) Δ t X 2 ( α α * ) f l .

Hence, for any α , α * T , we have

lim l 1 l α α + l f ( t ) Δ t = lim l 1 l α * α * + l f ( t ) Δ t ,

which means that M { f } is independent of α T . This completes the proof.□

Theorem 4.3

Let f , g A P ( T , X ) and λ R , then

  1. M { f + g } = M { f } + M { g } ;

  2. M { λ f } = λ M { f } ;

  3. If f ( t ) 0 , M { f } 0 ;

  4. M { f } X M { f X } ;

  5. If lim n f n ( t ) = f ( t ) uniformly on T , then lim n M { f n } = M { f } .

Proof

By Theorem 4.2, the proofs of statements ( i ) ( i v ) are obvious. The proof of statement ( v ) follows from the fact that

M { f n } M { f } X = M { f n f } X M { f n f X } .

This completes the proof.□

Let f A P ( T , X ) , λ R , we note the fact that f ( t ) e i λ t A P ( T , X ) . Therefore, there exists the mean value of f ( t ) e i λ t . We write

a ( f , λ ) = M { f ( t ) e i λ t } .

The following result is particularly important for the concept of Fourier series corresponding to almost periodic functions.

Theorem 4.4

For each f A P ( T , X ) , there exists at most a countable set of values of λ R such that

a ( f , λ ) 0 .

Proof

For f A P ( T , X ) , there exists a sequence of trigonometric polynomials { R m ( t ) ; m 1 } T such that lim m R m ( t ) = f ( t ) uniformly on T . By Theorem 4.3, one has

lim m M { R m ( t ) e i λ t } = M { f ( t ) e i λ t } = a ( f , λ ) .

Next, we will prove that M { R m ( t ) e i λ t } 0 for each m 1 . Let R m ( t ) = k = 1 n a k e i λ k t , a k X , k = 1 , 2 , , n . Then, one can easily see that M { R m ( t ) e i λ t } 0 only for λ = λ k , k = 1 , 2 , , n . As a consequence, there exists only a countable set of values of λ such that M { R m ( t ) e i λ t } 0 for at least one m , which implies that a ( λ , t ) 0 for such values. This completes the proof.□

Definition 4.3

Let f A P ( T , X ) , and denote by the numbers λ k R , k = 1 , 2 , , such that

a k = a ( f , λ k ) 0 ,

then the series

k = 1 a k e i λ k t

is called the Fourier series of the function f . We will denote this fact by

f ( t ) k = 1 a k e i λ k t .

λ k R , k = 1 , 2 , , are called the Fourier exponents of the function f , and a k , k = 1 , 2 , , are called Fourier coefficients of f .

Theorem 4.5

Let f A P ( T , X ) . If f ( t ) k = 1 a k e i λ k t , then the following hold:

  1. f ( t + c ) k = 1 a k e i λ k c e i λ k t , where c T .

  2. e i λ t f ( t ) k = 1 a k e i ( λ + λ k ) t , where λ R .

  3. if f Δ A P ( T , X ) , then f Δ ( t ) k = 1 A k e i λ k t , where A k = M { f ( t ) ( e i λ k t ) Δ } ; in particular, if T = R , then

    f Δ ( t ) k = 1 i λ k a k e i λ k t ,

    if T = h Z , then

    f Δ ( t ) k = 1 M 1 e i λ k h h f ( t + h ) e i λ k t e i λ k t .

Proof

By Definition 4.3, the proofs of statements ( i ) and ( i i ) are obvious. Next, we will prove statement ( i i i ) . Note that

1 l α α + l f Δ ( t ) e i λ t Δ t = 1 l ( f ( α + l ) e i λ ( α + l ) f ( α ) e i λ α ) 1 l α α + l f ( t ) ( e i λ t ) Δ Δ t .

Letting l , one obtains

M { f Δ ( t ) e i λ t } = M { f ( t ) ( e i λ t ) Δ } ,

which means that the Fourier exponents of f Δ are the same as those of f , except for λ = 0 . We denote by A k the Fourier coefficients of f Δ , we have A k = M { f ( t ) ( e i λ k t ) Δ } . Hence, if T = R , then

f Δ ( t ) k = 1 i λ k a k e i λ k t .

If T = h Z , since

( e i λ t ) Δ = e i λ h 1 h e i λ t ,

A k = M 1 e i λ k h h f ( t + h ) e i λ k t . Consequently,

f Δ ( t ) k = 1 M 1 e i λ k h h f ( t + h ) e i λ k t e i λ k t .

This completes the proof.□

One can easily prove that

Theorem 4.6

Let f A P ( T , C ) . If f ( t ) k = 1 a k e i λ k t , then f ¯ ( t ) k = 1 a ¯ k e i λ k t .

Let f A P ( T , C ) , b k C , and β k R , k = 1 , 2 , , n . Denote

ϕ ( b 1 , b 2 , , b n ) = M f ( t ) k = 1 n b k e i β k t 2 , t T .

Theorem 4.7

Let f A P ( T , C ) . If b k = a ( f , β k ) , then min ϕ = M { f ( t ) 2 } k = 1 n a ( f , β k ) 2 .

Proof

Note that f ( t ) 2 = f ( t ) f ¯ ( t ) is almost periodic, where f ¯ ( t ) denotes the conjugate of f ( t ) . So, the mean value of f ( t ) 2 exists. Thus,

(4.3) M f ( t ) k = 1 n b k e i β k t 2 = M f ( t ) k = 1 n b k e i β k t f ¯ ( t ) k = 1 n b ¯ k e i β k t = M { f ( t ) f ¯ ( t ) } M f ( t ) k = 1 n b ¯ k e i β k t M f ¯ ( t ) k = 1 n b k e i β k t + M k = 1 n j = 1 n b k b ¯ j e i ( β k β j ) t = M { f ( t ) 2 } k = 1 n b ¯ k M { f ( t ) e i β k t } k = 1 n b k M { f ¯ ( t ) e i β k t } + k = 1 n j = 1 n b k b ¯ j M { e i ( β k β j ) t } .

If k j , by Lemma 4.2, we have

M { e i ( β k β j ) t } = 0 .

If k = j , M { e i ( β k β j ) t } = 1 . Therefore, one has

(4.4) l = 1 n j = 1 n b k b ¯ j M { e i ( β k β j ) t } = k = 1 n b k 2 .

By (4.3) and (4.4), it is easy to obtain that

M f ( t ) k = 1 n b k e i β k t 2 = M { f ( t ) 2 } k = 1 n b ¯ k a ( f , β k ) k = 1 n b k a ( f , β k ) ¯ + k = 1 n b k 2 = M { f ( t ) 2 } + k = 1 n b k a ( f , β k ) 2 k = 1 n a ( f , β k ) 2 ,

which implies that min ϕ is attained for b k = a ( f , β k ) and min ϕ = M { f ( t ) 2 } k = 1 n a ( f , β k ) 2 , k = 1 , 2 , , n . This completes the proof.□

Theorem 4.8

Let f A P ( T , C ) . If f ( t ) k = 1 a k e i λ k t , then the Bessel inequality

k = 1 a k 2 M { f ( t ) 2 }

holds.

Proof

Since min ϕ 0 , by Theorem 4.7,

(4.5) k = 1 n a ( f , β k ) 2 M { f ( t ) 2 } ,

that is,

k = 1 n a k 2 M { f ( t ) 2 } .

Since M { f ( t ) 2 } is a constant, let n , we immediately obtain that

k = 1 a k 2 M { f ( t ) 2 } .

This completes the proof.□

Theorem 4.9

Let f A P ( T , C ) . If f ( t ) k = 1 a k e i λ k t , then the Parseval equality

k = 1 a k 2 = M { f ( t ) 2 }

holds.

Proof

By Theorem 4.8, the following inequality holds:

k = 1 a k 2 M { f ( t ) 2 } .

Next we will prove that

M { f ( t ) 2 } k = 1 a k 2 .

Since f A P ( T , C ) , there exists a sequence of trigonometric polynomials { R n ; n 1 } T such that

f ( t ) R n ( t ) < 1 n , t T .

Thus, it follows from the above inequality that

(4.6) M { f R n 2 } = lim l 1 l α α + l f ( t ) R n ( t ) 2 Δ t 1 n , l Π , α T .

Let F n ( t ) be the polynomial, n 1 . Set F n ( t ) 0 , if none of the Fourier exponents of f ( t ) occurs in R n ( t ) , and F n ( t ) = a k e i λ k t , the summation is extended to those ks, where λ k is a common Fourier exponent to f ( t ) and R n ( t ) . So, one has

M { f F n 2 } = M { f 2 } a k 2 ,

where the summation is extended to those ks, λ k is a Fourier exponent to R n ( t ) . Thus, by (4.5) and (4.6), we have

M { f 2 } a k 2 M { f R n 2 } 1 n .

Hence,

M { f 2 } a k 2 + 1 n ,

where the summation is extended to those ks, λ k is a Fourier exponent to R n ( t ) . Furthermore, we can write the inequality

M { f 2 } k = 1 a k 2 + 1 n .

Let n , it follows that

M { f 2 } k = 1 a k 2 .

This completes the proof.□

Theorem 4.10

Let f , g A P ( T , C ) . If they have the same Fourier series, then f ( t ) g ( t ) for all t T .

Proof

In view of Theorem 4.9, one has

M { f ( t ) g ( t ) 2 } = 0 ,

which means that f ( t ) g ( t ) . Hence, we obtain that f ( t ) g ( t ) , t T . This completes the proof.□

4.2 Equivalent definitions of almost periodic functions on time scales

In this subsection, we first give definitions of almost periodic functions in Bochner’s sense and almost periodic functions in Bohr’s sense on T and then discuss some of their properties.

Definition 4.4

A function f B C ( T , X ) is said to be almost periodic in Bochner’s sense, if the family of translates = { f ( t + a ) ; a Π } is relatively compact in B C ( T , X ) . The set of all such functions will be denoted by A P N ( T , X ) .

Definition 4.5

A function f B C ( T , X ) is said to be almost periodic in Bohr’s sense, if for each ε > 0 , the ε -translation set of

E { ε , f } = { τ Π : f ( t + τ ) f ( t ) X < ε , t T }

is a relatively dense set in R , i.e., for any given ε > 0 , there exists a constant l ( ε ) > 0 such that every interval of length l ( ε ) contains at least one τ ( ε ) E { ε , f } such that

f ( t + τ ) f ( t ) X < ε , t T .

The l ( ε ) is called the inclusion length of E { ε , f } and the τ is called ε -translation number of f . The set of all such functions will be denoted by A P B ( T , X ) .

To prove the equivalence of Definitions 3.2, 4.4, and 4.5, the introduction of the Fourier series of almost periodic functions in Bohr’s sense is very critical. Therefore, we must first derive the existence of the mean value.

Theorem 4.11

If f A P B ( T , X ) , then

M { f } lim r 1 r β β + r f ( t ) Δ t , w h e r e β T , r Π

uniformly exists for β T . M { f } is independent of β and is called the mean value of f.

Proof

For any ε > 0 , there exists a constant l = l ( ε ) > 0 such that each interval ( β , β + l ) , β T contains at least one τ = τ ( ε ) Π such that

f ( t + τ ) f ( t ) X < ε 2 .

For a given a Π , one has

(4.7) 1 r β + a β + a + r f ( t ) Δ t = 1 r β + a β + τ f ( t ) Δ t + 1 r β + τ β + r + τ f ( t ) Δ t + 1 r β + r + τ β + a + r f ( t ) Δ t .

Denote M = sup t T f ( t ) X . Then, in view of (4.7), we have

(4.8) 1 r β β + r f ( t ) Δ t β + a β + a + r f ( t ) Δ t X 1 r β β + r f ( t ) Δ t β + τ β + r + τ f ( t ) Δ t X + 1 r β + a β + τ f ( t ) Δ t X + 1 r β + r + τ β + a + r f ( t ) Δ t X 1 r β β + r f ( t ) f ( t + τ ) X Δ t + 1 r β + a β + τ f ( t ) X Δ t + 1 r β + r + τ β + a + r f ( t ) X Δ t < ε 2 + 2 τ a M r .

Taking a = ( k 1 ) r , k = 1 , 2 , , n , from (4.8), one can deduce that

(4.9) 1 r β β + r f ( t ) Δ t β + ( k 1 ) r β + k r f ( t ) Δ t X < ε 2 + 2 τ a M r , k = 1 , 2 , , n .

It follows from inequalities (4.15) that

(4.10) 1 r β β + r f ( t ) Δ t 1 m β β + m r f ( t ) Δ t X = 1 r β β + r f ( t ) Δ t 1 m k = 1 m β + ( k 1 ) r β + k r f ( t ) Δ t X 1 r m k = 1 m β β + r f ( t ) Δ t β + ( k 1 ) r β + k r f ( t ) Δ t X < 1 m m ε 2 + 2 τ a M r = ε 2 + 2 τ a M r , k = 1 , 2 , , n .

Take r 1 , r 2 Π with r 1 , r 2 > 0 such that m 1 r 1 = m 2 r 2 , for some natural numbers m 1 and m 2 , according to (4.10), we can derive that

(4.11) 1 r 1 β β + r 1 f ( t ) Δ t 1 r 2 β β + r 2 f ( t ) Δ t X 1 r 1 β β + r 1 f ( t ) Δ t 1 m 1 β β + m 1 r 1 f ( t ) Δ t X + 1 r 2 1 m 2 β β + m 2 r 2 f ( t ) Δ t β β + r 2 f ( t ) Δ t X < ε + 2 τ a M 1 r 1 + 1 r 2 .

We choose r 1 , r 2 > 4 τ a M , it follows from (4.11) that

1 r 1 β β + r 1 f ( t ) Δ t 1 r 2 β β + r 2 f ( t ) Δ t X < 2 ε ,

which implies that the mean value of f ( t ) exists. From inequalities (4.8), choose r Π with r > 2 τ a M , for any β T and a Π , one has

1 r β β + r f ( t ) Δ t β + a β + a + r f ( t ) Δ t X < ε ,

which means that M { f } is independent of β T . This completes the proof.□

Remark 4.1

It is useful to point out the fact from Theorem 4.11 that the Fourier series of f A P B ( T , X ) exists, and if f ( t ) k = 1 a k e i λ k t , then, similar to the proof on page 28 of [26], one can easily prove that Parseval’s equality

k = 1 a k X 2 = M { f ( t ) X 2 }

is also valid.

Next we will prove the equivalence of Definitions 3.2, 4.4, and 4.5.

Theorem 4.12

If f A P ( T , X ) , then f A P N ( T , X ) .

Proof

Obviously, to prove the theorem, it is suffice to show that every sequence { f ( t + α n ) ; α n Π , n 1 } A P ( T , X ) contains a subsequence that converges in A P ( T , X ) .

Let R ( t ) = e i λ t , where λ R , t T . If { b k ; k 1 } Π is an arbitrary sequence, then one obtains that R ( t + b k ) = e i λ t e i λ b k , k 1 . Since e i λ b k = 1 , in view of the Bolzano-Weierstrass criterion, there exists a subsequence { b 1 k ; k 1 } { b k ; k 1 } such that { e i λ b 1 k ; k 1 } is convergent. Since

R ( t + b 1 j ) R ( t + b 1 k ) = e i λ b 1 j e i λ b 1 k ,

it follows from Cauchy’s criterion that { R ( t + b 1 k ) ; k 1 } is uniformly convergent on T .

Now, consider a trigonometric polynomial T ( t ) = k = 1 h a k e i λ k t , where a k X and λ k R . Let { β k ; k 1 } Π be an arbitrary sequence, then from the previous discussion, we know that there exists a subsequence { β k 1 ; k 1 } { β k ; k 1 } such that { a 1 e i λ 1 β k 1 ; k 1 } is uniformly convergent on T . Proceeding in the same way, there exists a subsequence { β k h ; k 1 } { β k m ; k 1 } such that { a n e i λ h β k h ; k 1 } is uniformly convergent on T , where 1 m < h . Consequently, we have proved that { T ( t + β k ) ; k 1 } contains a subsequence { T ( t + b k h ) ; k 1 } that is uniformly convergent on T .

Finally, since f A P ( T , X ) , there exists a sequence of trigonometric polynomials { T n ( t ) ; n 1 } T such that

(4.12) lim n T n ( t ) = f ( t )

uniformly on T . Let { α n ; n 1 } Π be a sequence. Based on the above proof, from the sequence { T 1 ( t + α n ) ; n 1 } , one can extract a subsequence { α n 1 ; n 1 } Π such that { T 1 ( t + α n 1 ) ; n 1 } is uniformly convergent on T . From the sequence { α n 1 ; n 1 } Π , one can extract a subsequence { α n 2 ; n 1 } Π such that { T 2 ( t + α n 2 ) ; n 1 } is uniformly convergent on T . Going on like this, for any integer p , for a sequence of { α n p ; n 1 } Π , we can obtain that { T q ( t + β n p ) ; n 1 } is uniformly convergent on T , q = 1 , 2 , , p . This means that { T n ( t + β m m ) ; m 1 } with fixed n is uniformly convergent on T . In the view of (4.12), for any ε > 0 , we can choose n large enough such that

f ( t ) T n ( t ) X < ε 3 , for all t T .

Hence, there exists N = N ( ε ) > 0 such that

T n ( t + b m m ) T n ( t + α p p ) X < ε 3 , for all t T ,

for m , p N ( ε ) . Thus, for m , p N ( ε ) , we have

f ( t + α m m m ) f ( t + α p p ) X f ( t + α m m ) T ( t + α m m ) X + T n ( t + α m m ) T n ( t + α p p ) X + f ( t + α p p ) T n ( t + α p p ) X < ε 3 + ε 3 + ε 3 = ε , for all t T ,

which means that the sequence { f ( t + α m m ) ; m 1 } is uniformly convergent on T . Thus, f A P N ( T , X ) . This completes the proof.□

Theorem 4.13

If f A P N ( T , X ) , then f A P B ( T , X ) .

Proof

On the contrary, if this is not true, then there exists ε > 0 such that for any sufficiently large l ( ε ) > 0 , one can find an interval with length of l ( ε ) that contains no ε -translation numbers of f . That is, every point in this interval is not in E { ε , f } .

According to Lemma 4.1, we can take a number β 1 Π and an interval ( c 1 , d 1 ) with

(4.13) d 1 c 1 > 2 β 1

such that ( c 1 , d 1 ) contains no ε -translation numbers of f , where c 1 , d 1 T with d 1 + c 1 2 Π . Next, denote

(4.14) β 2 = d 1 + c 1 2 .

By (4.13) and (4.14), we obtain β 2 β 1 ( c 1 , d 1 ) . Hence, β 2 β 1 E { ε , f } . Again, by Lemma 4.1, take an interval ( c 2 , d 2 ) with d 2 c 2 > 2 ( β 1 + β 1 ) such that ( c 2 , d 2 ) contains no ε -translation numbers of f , where c 2 , d 2 T with d 2 + c 2 2 Π . Next, denote β 3 = d 2 + c 2 2 , obviously, β 3 β 2 E { ε , f } and β 3 β 1 E { ε , f } . Proceeding similarly, one can find β 4 , β 5 , such that β i β j E { ε , f } , i > j . Thus, for i > j , i , j = 1 , 2 , 3 , , we have

sup t T f ( t + β i ) f ( t + β j ) X = sup t T f ( t + β i β j ) f ( t ) X ε , t T ,

which contradicts relative compactness of the family = { f ( t + a ) ; a Π } . By Theorem 4.12, the conclusion is valid. Thus, f A P B ( T , X ) . This completes the proof.□

Theorem 4.14

If f A P B ( T , X ) , then f A P ( T , X ) .

Proof

Let f ( t ) k = 1 a k e i λ k t and

(4.15) F n ( t ) = f ( t ) k = 1 n a k e i λ k t .

According to Remark 4.1,

M { F n ( t ) X 2 } = k = n + 1 + a k X 2 .

Because k = 1 a k 2 is convergent, so for any ξ > 0 , we can find n such that

(4.16) M { F n ( t ) X 2 } < ξ .

Moreover, by Theorem 4.11, there exists T 0 Π such that

(4.17) 1 T α α + T F n ( t + s ) X 2 Δ t M { F n ( t ) X 2 } < ξ , α T ,

for all T Π with T > T 0 and for all s Π . Hence, it follows from (4.16) and (4.17) that

(4.18) 1 T α α + T F n ( t + s ) X 2 Δ t < 2 ξ , α T .

Let l ( ε 3 ) be the inclusion length of E { ε 3 , f } . Take T = Z ( l ( ε 3 ) + 1 ) , Z is a nature number. Since f A P B ( T , X ) , every interval ( α + m ( l ( ε 3 ) + 1 ) , α + m ( l ( ε 3 ) + 1 ) + l ( ε 3 ) ) contains a τ m E { ε 3 , f } , m = 0 , 2 , , Z 1 such that

(4.19) f ( τ m + s ) f ( s ) X < ε 3 .

Then, by Theorem 3.1, we can take a δ Π such that for t 1 , t 2 T with t 1 t 2 < δ ,

f ( t 1 ) f ( t 2 ) X < ε 3 .

Define a function h ( t ) in the interval ( α , α + T ) by

h ( t ) = 1 , t ( α + τ m , α + τ m + δ ) , m = 0 , 2 , , Z 1 ; 0 , t ( α , α + T ) \ ( α + τ m , α + τ m + δ ) , m = 0 , 2 , , Z 1 .

Thus,

(4.20) α α + T h ( t ) X 2 Δ t = m = 1 Z 1 α + τ m α + τ m + δ h ( t ) X 2 Δ t = Z δ .

Based on (4.18), (4.20), and the Schwarz inequality, we obtain that

(4.21) α α + T F n ( t + s ) h ( t ) Δ t X 2 α α + T F n ( t + s ) X 2 Δ t α α + T h ( t ) X 2 Δ t 2 T ξ Z δ .

Observing that

α α + T F n ( t + s ) h ( t ) Δ t = m = 1 Z 1 α + τ m α + τ m + δ F n ( t + s ) Δ t = m = 1 Z 1 α α + δ F n ( t + τ m + s ) Δ t ,

we conclude from (4.21) that

m = 1 Z 1 α α + δ F n ( t + τ m + s ) Δ t X < 2 T ξ Z δ .

Thus, taking ξ < ε 2 δ 18 ( l ( ε 3 ) + 1 ) , from T = Z ( l ( ε 3 ) + 1 ) , we have

(4.22) 1 Z δ m = 1 Z 1 α α + δ F n ( t + τ m + s ) Δ t X < 2 ξ T Z δ < 2 ξ ( l ( ε 3 ) + 1 ) δ < ε 3 .

It follows from (4.15) that

(4.23) 1 Z δ α α + δ F n ( t + τ m + s ) Δ t X = 1 Z δ α α + δ f ( t + τ m + s ) Δ t P m ( s ) X ,

where

P m ( s ) = 1 Z δ α α + δ k = 1 n a k e i λ k ( t + τ m + s ) Δ t = 1 Z δ k = 1 n e i λ k s α α + δ a k e i λ k ( t + τ m ) Δ t .

Thus, P m is a trigonometric polynomial. Based on (4.22) and (4.23), one has

(4.24) 1 Z δ m = 1 Z 1 α α + δ f ( t + τ m + s ) Δ t P ( s ) X < ε 3 ,

where P ( s ) = m = 1 Z 1 P m ( s ) . We can choose value of δ Π such that

f ( t + τ m + s ) f ( τ m + s ) X < ε 3 ,

for t T with 0 t δ . Consequently,

1 δ α α + δ f ( t + τ m + s ) Δ t f ( τ m + s ) X < ε 3 .

It follows from the above inequality and (4.19) that

(4.25) 1 δ α α + δ f ( t + τ m + s ) Δ t f ( s ) X < 2 ε 3 .

Hence, based on (4.24) and (4.25), one has

f ( s ) P ( s ) X = 1 δ α α + δ f ( t + τ m + s ) Δ t f ( s ) X + 1 δ α α + δ f ( t + τ m + s ) Δ t P ( s ) X < 2 ε 3 + 1 Z δ m = 1 Z 1 α α + δ f ( t + τ m + s ) Δ t P ( s ) X < 2 ε 3 + ε 3 = ε .

This completes the proof.□

Remark 4.2

According to Theorems 4.12, 4.13, and 4.14, it is obvious that Definitions 3.2, 4.4, and 4.5 are equivalent.

Theorem 4.15

Let f A P ( T , X ) be a non-negative function. If f ( t ) 0 , then M { f } > 0 .

Proof

At some point t 0 T , let f ( t 0 ) = β > 0 . Then, take a number δ Π with δ > 0 such that

f ( t ) f ( t 0 ) < β 3 ,

for t t 0 < δ . Since f A P ( T , X ) , there exist a positive number l 1 > 0 such that any interval of length l 1 contains β 3 -translation numbers of f . Let c , l 1 Π , then τ ( c t 0 + δ , c t 0 + δ + l 1 ) is a β 3 -translation number. Thus, t 0 + τ ( c + δ , c + δ + l 1 ) . Since t t 0 < δ , it is easy to see that t + τ ( c , c + l 1 + 2 δ ) . Therefore, one has

f ( t + τ ) f ( t 0 ) f ( t ) f ( t 0 ) f ( t + τ ) f ( t ) > β β 3 β 3 = β 3 .

One can take l = l 1 + 2 δ and conclude that any interval of length l on T contains a subinterval of length 2 δ at all points of which f ( t ) > β 3 . Thus,

1 n l α α + n l f ( t ) Δ t = 1 n l k = 1 n α + ( k 1 ) l α + k l f ( t ) Δ t > δ β 3 l .

Letting n , one can obtain M { f } δ β 3 l > 0 . This completes the proof.□

Theorem 4.16

Let f , g A P ( T , X ) . If they have the same Fourier series, then f ( t ) g ( t ) for t T .

Proof

If f ( t ) g ( t ) and they have the same Fourier series, then by Theorem 4.9, one has

M { f ( t ) g ( t ) 2 } = 0 ,

which is a contradiction by Theorem 4.15. Hence, we obtain that f ( t ) g ( t ) for t T . This completes the proof.□

5 Conclusion

In this study, we have proposed a concept of almost periodic functions on arbitrary time scales defined by the closure of the set of trigonometric polynomials in the supremum norm and investigated some their basic properties. Moreover, we have introduced the concepts of mean-value and Fourier series associated with an almost periodic function on time scales and present some relative results. Finally, we have given the definitions of almost periodic functions on time scales in Bohr’s sense and in Bochner’s sense, and discussed the relationship among them. The research in this work lays a foundation for further study of almost periodic function theory on time scales and almost periodic solutions of dynamic equations.

  1. Funding information: The research was supported by the National Natural Science Foundation of China (No. 12261098).

  2. Author contributions: All the authors contributed equally to this work.

  3. Conflict of interest: The authors state no conflicts of interest.

  4. Data availability statement: Data sharing is not applicable to this article as no datasets were generated or analyzed during this study.

References

[1] S. Hilger, Analysis on measure chains - a unified approach to continuous and discrete calculus, Results Math. 18 (1990), no. 1, 18–56, DOI: https://doi.org/10.1007/BF03323153. 10.1007/BF03323153Search in Google Scholar

[2] M. Bohner and A. Peterson, Dynamic Equations on Time Scales, An Introduction with Applications, Birkhäuser, Boston, 2001. 10.1007/978-1-4612-0201-1Search in Google Scholar

[3] H. Bohr, Zur theorie der fast periodischen funktionen, Acta Math. 45 (1925), no. 1, 29–127, DOI: https://doi.org/10.1007/BF02395468. 10.1007/BF02395468Search in Google Scholar

[4] Y. Li and C. Wang, Uniformly almost periodic functions and almost periodic solutions to dynamic equations on time scales, Abstr. Appl. Anal. 2011 (2011), 341520, DOI: https://doi.org/10.1155/2011/341520. 10.1155/2011/341520Search in Google Scholar

[5] Y. Li and W. Chao, Almost periodic functions on time scales and applications, Discrete Dyn. Nat. Soc. 2011 (2011), 727068, DOI: https://doi.org/10.1155/2011/727068. 10.1155/2011/727068Search in Google Scholar

[6] J. Gao, Q. R. Wang, and L. W. Zhang, Existence and stability of almost-periodic solutions for cellular neural networks with time-varying delays in leakage terms on time scales, Appl. Math. Comput. 237 (2014), 639–649, DOI: https://doi.org/10.1016/j.amc.2014.03.051. 10.1016/j.amc.2014.03.051Search in Google Scholar

[7] B. Du, Y. Liu, H. A. Batarfi, and F. E. Alsaadi, Almost periodic solution for a neutral-type neural networks with distributed leakage delays on time scales, Neurocomputing 173 (2016), 921–929, DOI: https://doi.org/10.1016/j.neucom.2015.08.047. 10.1016/j.neucom.2015.08.047Search in Google Scholar

[8] S. Hong and Y. Peng, Almost periodicity of set-valued functions and set dynamic equations on time scales, Inf. Sci. 330 (2016), 157–174, DOI: https://doi.org/10.1016/j.ins.2015.10.008. 10.1016/j.ins.2015.10.008Search in Google Scholar

[9] C. H. Tang and H. X. Li, The connection between pseudo almost periodic functions defined on time scales and on the real line, Bull. Aust. Math. Soc. 95 (2017), no. 482–494, DOI: https://doi.org/10.1017/S0004972717000041. 10.1017/S0004972717000041Search in Google Scholar

[10] Q. Wang and Z. Liu, Existence and stability of positive almost periodic solutions for a competitive system on time scales, Math. Comput. Simulation 138 (2017), 65–77, DOI: https://doi.org/10.1016/j.matcom.2016.09.016. 10.1016/j.matcom.2016.09.016Search in Google Scholar

[11] Z. Yao, Existence and exponential stability of unique almost periodic solution for Lasota-Wazewska red blood cell model with perturbation on time scales, Math. Methods Appl. Sci. 40 (2017), no. 13, 4709–4715, DOI: https://doi.org/10.1002/mma.4337. 10.1002/mma.4337Search in Google Scholar

[12] C. H. Tang and H. X. Li, Bochner-like transform and Stepanov almost periodicity on time scales with applications, Symmetry 10 (2018), no. 11, 566, DOI: https://doi.org/10.3390/sym10110566. 10.3390/sym10110566Search in Google Scholar

[13] C. H. Tang and H. X. Li, Stepanov-like pseudo almost periodic functions on time scales and applications to dynamic equations with delay, Open Math. 16 (2018), no. 1, 826–841, DOI: https://doi.org/10.1515/math-2018-0073. 10.1515/math-2018-0073Search in Google Scholar

[14] S. Dhama and S. Abbas, Existence and stability of square-mean almost automorphic solution for neutral stochastic evolution equations with Stepanov-like terms on time scales, Rev. R. Acad. Cienc. Exactas Fís. Nat. Ser. A Mat. RACSAM 113 (2019), 1231–1250, DOI: https://doi.org/10.1007/s13398-018-0547-3. 10.1007/s13398-018-0547-3Search in Google Scholar

[15] K. R. Prasad and M. Khuddush, Existence and global exponential stability of positive almost periodic solutions for a time-scales model of Hematopoiesis with multiple time-varying variable delays, Int. J. Difference Equ. 14 (2019), no. 2, 149–167, DOI: https://doi.org/10.37622/IJDE/14.2.2019.149-167. 10.37622/IJDE/14.2.2019.149-167Search in Google Scholar

[16] Y. Xue, X. Xie, and Q. Lin, Almost periodic solutions of a commensalism system with Michaelis-Menten type harvesting on time scales, Open Math. 17 (2019), no. 1, 1503–1514, DOI: https://doi.org/10.1515/math-2019-0134. 10.1515/math-2019-0134Search in Google Scholar

[17] X. Yu and Q. Wang, Weighted pseudo-almost periodic solutions for shunting inhibitory cellular neural networks on time scales, Bull. Malays. Math. Sci. Soc. 42 (2019), no. 5, 2055–2074, DOI: https://doi.org/10.1007/s40840-017-0595-4. 10.1007/s40840-017-0595-4Search in Google Scholar

[18] C. Xu, M. Liao, P. Li, and Z. Liu, Almost automorphic solutions to cellular neural networks with neutral type delays and leakage delays on time scales, Int. J. Comput. Intell. Syst 13 (2020), no. 1, 1–11, DOI: https://doi.org/10.2991/ijcis.d.200107.001. 10.2991/ijcis.d.200107.001Search in Google Scholar

[19] S. Dhama, S. Abbas, and R. Sakthivel, Stability and approximation of almost automorphic solutions on time scales for the stochastic Nicholson’s blowflies model, J. Integral Equations Appl. 33 (2021), no. 1, 31–51, DOI: https://doi.org/10.1216/jie.2021.33.31. 10.1216/jie.2021.33.31Search in Google Scholar

[20] J. Gao, Q. R. Wang, and Y. Lin, Existence and exponential stability of almost-periodic solutions for MAM neural network with distributed delays on time scales, Appl. Math. J. Chinese Univ. 36 (2021), no. 1, 70–82, DOI: https://doi.org/10.1007/s11766-021-3606-z. 10.1007/s11766-021-3606-zSearch in Google Scholar

[21] A. Arbi and N. Tahri, New results on time scales of pseudo Weyl almost periodic solution of delayed QVSICNNs, Comput. Appl. Math. 41 (2022), 293, DOI: https://doi.org/10.1007/s40314-022-02003-0. 10.1007/s40314-022-02003-0Search in Google Scholar

[22] M. Khuddush and K. R. Prasad, Global exponential stability of almost periodic solutions for quaternion-valued RNNs with mixed delays on time scales, Bol. Soc. Mat. Mex. 28 (2022), 75, DOI: https://doi.org/10.1007/s40590-022-00467-y. 10.1007/s40590-022-00467-ySearch in Google Scholar

[23] Y. Li and X. Huang, Besicovitch almost periodic solutions to stochastic dynamic equations with delays, Qual. Theory Dyn. Syst. 21 (2022), 74, DOI: https://doi.org/10.1007/s12346-022-00606-w. 10.1007/s12346-022-00606-wSearch in Google Scholar

[24] C. Corduneanu, Almost Periodic Functions, Wiley, New York, 1968. Search in Google Scholar

[25] Y. Li and C. Wang, Pseudo almost periodic functions and pseudo almost periodic solutions to dynamic equations on time scales, Adv. Differential Equations 2012 (2012), 77, DOI: https://doi.org/10.1186/1687-1847-2012-77. 10.1186/1687-1847-2012-77Search in Google Scholar

[26] A. B. Besicovitch, Almost Periodic Functions, Dover, New York, 1954. Search in Google Scholar

Received: 2024-06-10
Revised: 2024-11-17
Accepted: 2024-11-24
Published Online: 2024-12-16

© 2024 the author(s), published by De Gruyter

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

Articles in the same Issue

  1. Special Issue on Contemporary Developments in Graph Topological Indices
  2. On the maximum atom-bond sum-connectivity index of graphs
  3. Upper bounds for the global cyclicity index
  4. Zagreb connection indices on polyomino chains and random polyomino chains
  5. On the multiplicative sum Zagreb index of molecular graphs
  6. The minimum matching energy of unicyclic graphs with fixed number of vertices of degree two
  7. Special Issue on Convex Analysis and Applications - Part I
  8. Weighted Hermite-Hadamard-type inequalities without any symmetry condition on the weight function
  9. Scattering threshold for the focusing energy-critical generalized Hartree equation
  10. (pq)-Compactness in spaces of holomorphic mappings
  11. Characterizations of minimal elements of upper support with applications in minimizing DC functions
  12. Some new Hermite-Hadamard-type inequalities for strongly h-convex functions on co-ordinates
  13. Global existence and extinction for a fast diffusion p-Laplace equation with logarithmic nonlinearity and special medium void
  14. Extension of Fejér's inequality to the class of sub-biharmonic functions
  15. On sup- and inf-attaining functionals
  16. Regularization method and a posteriori error estimates for the two membranes problem
  17. Rapid Communication
  18. Note on quasivarieties generated by finite pointed abelian groups
  19. Review Articles
  20. Amitsur's theorem, semicentral idempotents, and additively idempotent semirings
  21. A comprehensive review of the recent numerical methods for solving FPDEs
  22. On an Oberbeck-Boussinesq model relating to the motion of a viscous fluid subject to heating
  23. Pullback and uniform exponential attractors for non-autonomous Oregonator systems
  24. Regular Articles
  25. On certain functional equation related to derivations
  26. The product of a quartic and a sextic number cannot be octic
  27. Combined system of additive functional equations in Banach algebras
  28. Enhanced Young-type inequalities utilizing Kantorovich approach for semidefinite matrices
  29. Local and global solvability for the Boussinesq system in Besov spaces
  30. Construction of 4 x 4 symmetric stochastic matrices with given spectra
  31. A conjecture of Mallows and Sloane with the universal denominator of Hilbert series
  32. The uniqueness of expression for generalized quadratic matrices
  33. On the generalized exponential sums and their fourth power mean
  34. Infinitely many solutions for Schrödinger equations with Hardy potential and Berestycki-Lions conditions
  35. Computing the determinant of a signed graph
  36. Two results on the value distribution of meromorphic functions
  37. Zariski topology on the secondary-like spectrum of a module
  38. On deferred f-statistical convergence for double sequences
  39. About j-Noetherian rings
  40. Strong convergence for weighted sums of (α, β)-mixing random variables and application to simple linear EV regression model
  41. On the distribution of powered numbers
  42. Almost periodic dynamics for a delayed differential neoclassical growth model with discontinuous control strategy
  43. A new distributionally robust reward-risk model for portfolio optimization
  44. Asymptotic behavior of solutions of a viscoelastic Shear beam model with no rotary inertia: General and optimal decay results
  45. Silting modules over a class of Morita rings
  46. Non-oscillation of linear differential equations with coefficients containing powers of natural logarithm
  47. Mutually unbiased bases via complex projective trigonometry
  48. Hyers-Ulam stability of a nonlinear partial integro-differential equation of order three
  49. On second-order linear Stieltjes differential equations with non-constant coefficients
  50. Complex dynamics of a nonlinear discrete predator-prey system with Allee effect
  51. The fibering method approach for a Schrödinger-Poisson system with p-Laplacian in bounded domains
  52. On discrete inequalities for some classes of sequences
  53. Boundary value problems for integro-differential and singular higher-order differential equations
  54. Existence and properties of soliton solution for the quasilinear Schrödinger system
  55. Hermite-Hadamard-type inequalities for generalized trigonometrically and hyperbolic ρ-convex functions in two dimension
  56. Endpoint boundedness of toroidal pseudo-differential operators
  57. Matrix stretching
  58. A singular perturbation result for a class of periodic-parabolic BVPs
  59. On Laguerre-Sobolev matrix orthogonal polynomials
  60. Pullback attractors for fractional lattice systems with delays in weighted space
  61. Singularities of spherical surface in R4
  62. Variational approach to Kirchhoff-type second-order impulsive differential systems
  63. Convergence rate of the truncated Euler-Maruyama method for highly nonlinear neutral stochastic differential equations with time-dependent delay
  64. On the energy decay of a coupled nonlinear suspension bridge problem with nonlinear feedback
  65. The limit theorems on extreme order statistics and partial sums of i.i.d. random variables
  66. Hardy-type inequalities for a class of iterated operators and their application to Morrey-type spaces
  67. Solving multi-point problem for Volterra-Fredholm integro-differential equations using Dzhumabaev parameterization method
  68. Finite groups with gcd(χ(1), χc (1)) a prime
  69. Small values and functional laws of the iterated logarithm for operator fractional Brownian motion
  70. The hull-kernel topology on prime ideals in ordered semigroups
  71. ℐ-sn-metrizable spaces and the images of semi-metric spaces
  72. Strong laws for weighted sums of widely orthant dependent random variables and applications
  73. An extension of Schweitzer's inequality to Riemann-Liouville fractional integral
  74. Construction of a class of half-discrete Hilbert-type inequalities in the whole plane
  75. Analysis of two-grid method for second-order hyperbolic equation by expanded mixed finite element methods
  76. Note on stability estimation of stochastic difference equations
  77. Trigonometric integrals evaluated in terms of Riemann zeta and Dirichlet beta functions
  78. Purity and hybridness of two tensors on a real hypersurface in complex projective space
  79. Classification of positive solutions for a weighted integral system on the half-space
  80. A quasi-reversibility method for solving nonhomogeneous sideways heat equation
  81. Higher-order nonlocal multipoint q-integral boundary value problems for fractional q-difference equations with dual hybrid terms
  82. Noetherian rings of composite generalized power series
  83. On generalized shifts of the Mellin transform of the Riemann zeta-function
  84. Further results on enumeration of perfect matchings of Cartesian product graphs
  85. A new extended Mulholland's inequality involving one partial sum
  86. Power vector inequalities for operator pairs in Hilbert spaces and their applications
  87. On the common zeros of quasi-modular forms for Γ+0(N) of level N = 1, 2, 3
  88. One special kind of Kloosterman sum and its fourth-power mean
  89. The stability of high ring homomorphisms and derivations on fuzzy Banach algebras
  90. Integral mean estimates of Turán-type inequalities for the polar derivative of a polynomial with restricted zeros
  91. Commutators of multilinear fractional maximal operators with Lipschitz functions on Morrey spaces
  92. Vector optimization problems with weakened convex and weakened affine constraints in linear topological spaces
  93. The curvature entropy inequalities of convex bodies
  94. Brouwer's conjecture for the sum of the k largest Laplacian eigenvalues of some graphs
  95. High-order finite-difference ghost-point methods for elliptic problems in domains with curved boundaries
  96. Riemannian invariants for warped product submanifolds in Q ε m × R and their applications
  97. Generalized quadratic Gauss sums and their 2mth power mean
  98. Euler-α equations in a three-dimensional bounded domain with Dirichlet boundary conditions
  99. Enochs conjecture for cotorsion pairs over recollements of exact categories
  100. Zeros distribution and interlacing property for certain polynomial sequences
  101. Random attractors of Kirchhoff-type reaction–diffusion equations without uniqueness driven by nonlinear colored noise
  102. Study on solutions of the systems of complex product-type PDEs with more general forms in ℂ2
  103. Dynamics in a predator-prey model with predation-driven Allee effect and memory effect
  104. A note on orthogonal decomposition of 𝔰𝔩n over commutative rings
  105. On the δ-chromatic numbers of the Cartesian products of graphs
  106. Binomial convolution sum of divisor functions associated with Dirichlet character modulo 8
  107. Commutator of fractional integral with Lipschitz functions related to Schrödinger operator on local generalized mixed Morrey spaces
  108. System of degenerate parabolic p-Laplacian
  109. Stochastic stability and instability of rumor model
  110. Certain properties and characterizations of a novel family of bivariate 2D-q Hermite polynomials
  111. Stability of an additive-quadratic functional equation in modular spaces
  112. Monotonicity, convexity, and Maclaurin series expansion of Qi's normalized remainder of Maclaurin series expansion with relation to cosine
  113. On k-prime graphs
  114. On the existence of tripartite graphs and n-partite graphs
  115. Classifying pentavalent symmetric graphs of order 12pq
  116. Almost periodic functions on time scales and their properties
  117. Some results on uniqueness and higher order difference equations
  118. Coding of hypersurfaces in Euclidean spaces by a constant vector
  119. Cycle integrals and rational period functions for Γ0+(2) and Γ0+(3)
  120. Degrees of (L, M)-fuzzy bornologies
  121. A matrix approach to determine optimal predictors in a constrained linear mixed model
  122. On ideals of affine semigroups and affine semigroups with maximal embedding dimension
  123. Solutions of linear control systems on Lie groups
  124. A uniqueness result for the fractional Schrödinger-Poisson system with strong singularity
  125. On prime spaces of neutrosophic extended triplet groups
  126. On a generalized Krasnoselskii fixed point theorem
  127. On the relation between one-sided duoness and commutators
  128. Non-homogeneous BVPs for second-order symmetric Hamiltonian systems
  129. Erratum
  130. Erratum to “Infinitesimals via Cauchy sequences: Refining the classical equivalence”
  131. Corrigendum
  132. Corrigendum to “Matrix stretching”
  133. Corrigendum to “A comprehensive review of the recent numerical methods for solving FPDEs”
Downloaded on 11.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/math-2024-0107/html
Scroll to top button