Home Some inequalities and superposition operator in the space of regulated functions
Article Open Access

Some inequalities and superposition operator in the space of regulated functions

  • Leszek Olszowy EMAIL logo and Tomasz Zając
Published/Copyright: December 14, 2019

Abstract

Some inequalities connected to measures of noncompactness in the space of regulated function R(J, E) were proved in the paper. The inequalities are analogous of well known estimations for Hausdorff measure and the space of continuous functions. Moreover two sufficient and necessary conditions that superposition operator (Nemytskii operator) can act from R(J, E) into R(J, E) are presented. Additionally, sufficient and necessary conditions that superposition operator Ff : R(J, E) → R(J, E) was compact are given.

1 Introduction

When studying solvability of various non-linear equations, it is significant to properly choose the space in which the equation is considered. Knowledge about some properties of the space e.g. easy to calculate formulas for measures of noncompactness or characteristic of superposition operator etc. combined with fixed point theorems allow to obtain general conditions for solvability of studied equations.

The space of regulated functions R(J, E), where J = [a, b] ⊂ ℝ and E is a Banach space, is one of such spaces, recently intensively studied (see [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14]). So far except stating general properties of this space [1, 5, 7, 8, 9, 10, 11, 12] it is also possible to use formulas for measures of noncompactness, conditions sufficient for the superposition operator Ff to act from R(J, E) into R(J, E), and conditions for continuity of this operator [2, 3, 4, 5, 6, 12, 13]. However, so far non-trivial sufficient and necessary conditions for compactness of the superposition operator Ff : R(J, E) → R(J, E) were not known. There was also lack of any estimations of such measures, so often needed. This paper will try to fill these gaps.

In the third chapter several theorems dealing with various types of inequalities, integral, but not only integral, that hold in the spaces of regulated functions and are expressed in terms of measures of noncompactness, will be formulated. These inequalities are analogues of known and often used inequalities holding in the class of continuous functions. In the fourth chapter two theorems (Theorem 4.4 and Theorem 4.6) that give sufficient and necessary conditions that superposition operator acted from the space of regulated functions into that space, will be presented. Known so far results in this area usually give only sufficient conditions and the only known sufficient and necessary conditions are actually rather “tautological”. Moreover, sufficient and necessary conditions that superposition operator is compact in the space of regulated functions will be given (Theorem 4.9).

2 Notation, definitions and auxiliary facts

This section is focuses on recalling some facts which will be used in our investigations.

Assume that E is a real Banach space with the norm ∥⋅∥ and the zero element θ. Denote by BE(x, r) the closed ball centered at x and with radius r. The ball BE(θ, r) will be denoted by BE(r). We write X, Conv X to denote the closure and the convex closure of a set X, respectively. The symbol ∥X∥ will stand for the norm of the set XE i.e., we have ∥X∥ : = sup{∥x∥: xX}. Furthermore, let 𝔐E denote the family of all nonempty and bounded subsets of E and 𝔑E its subfamily consisting of all relatively compact sets. We accept the following definition of a measure of noncompactness [15].

Definition 2.1

A mapping μ : 𝔐E → ℝ+ = [0, ∞) is said to be a measure of noncompactness in E if it satisfies the following conditions:

  1. The family ker μ : = {X ∈ 𝔐E : μ(X) = 0} is nonempty and ker μ ⊂ 𝔑E.

  2. XYμ(X) ≤ μ(Y).

  3. μ(Conv X) = μ(X).

  4. μ(λX + (1 – λ)Y) ≤ λμ(X) + (1 – λ)μ(Y) for λ ∈ [0, 1].

  5. If (Xn) is a sequence of closed sets from 𝔐E such that Xn+1Xn (n = 1, 2, …) and if limn μ(Xn) = 0, then the intersection X : = n=1 Xn is nonempty.

Subsequently, we will use measures of noncompactness having some additional properties. Namely, a measure μ is said to be sublinear if it satisfies the following two conditions:

  1. μ(λX) = |λ|μ(X), λ ∈ ℝ.

  2. μ(X + Y) ≤ μ(X) + μ(Y).

A sublinear measure of noncompactness μ satisfying the condition (strong maximum property)

  1. μ(XY) = max{μ(X), μ(Y)}

and such that ker μ = 𝔑E is said to be regular.

Except condition 8o we can also consider the condition (weak maximum property)

  1. μ(X ∪ {y}) = μ(X), yE.

For a given nonempty bounded subset X of E, we denote by βE(X) the so-called Hausdorff measure of noncompactness of X. This quantity is defined by formula

βE(X):={r>0:XhasafiniternetinE}.

The function βE is an example of regular measure of noncompactness in E.

Now we recall some facts concerning regulated functions.

Definition 2.2

A function x : [a, b] → E, where E is a topological vector space, is said to be a regulated function if for every t ∈ [a, b) the right-sided limit x(t+) : = limst+ x(s) exists and for every t ∈ (a, b] the left-sided limit x(t) := limst x(s) exists.

From now on, real Banach space will be denoted by E.

Denote by R(J, E) the space consisting of all regulated functions defined on the interval J = [a, b] with values in a real Banach space E. Since every regulated function xR(J, E) is bounded on the interval J, then the space R(J, E) can be normed via the classical supremum norm

||x||:=sup{||x(t)||:tJ}.

It is easy to show that R(J, E) is a real Banach space. Moreover, every regulated function x : JE is Riemann integrable.

Now, we remind a criterion for relative compactness in the space R(J, E). To this end, we introduce the concept of a equiregulated subset of the space R(J, E) (cf. [3, 9]).

Definition 2.3

We will say that the set XR(J, E) is equiregulated on the interval J if the following two conditions are satisfied:

t(a,b]ε>0δ>0xXt1,t2(tδ,t)[a,b]||x(t2)x(t1)||ε,t[a,b)ε>0δ>0xXt1,t2(t,t+δ)[a,b]||x(t2)x(t1)||ε.

Theorem 2.4

[3, 4, 5, 9] A nonempty subset XR(J, E) is relatively compact in R(J, E) if and only if X is equiregulated on the interval J and the sets X(t) are relatively compact in E for tJ.

Now we are going to recall the construction of a measure of noncompactness in the space R(J, E). To this end, let us take a set X ∈ 𝔐R(J,E). For xX and ε > 0 let us denote the following quantities:

ω(x,t,ε):=sup{||x(t2)x(t1)||:t1,t2(tε,t)J},t(a,b],ω+(x,t,ε):=sup{||x(t2)x(t1)||:t1,t2(t,t+ε)J},t[a,b).

The quantities ω(x, t, ε) and ω+(x, t, ε) can be interpreted as left hand and right hand sided moduli of convergence of the function x at the point t. Furthermore, let us put:

ω(X,t,ε):=sup{ω(x,t,ε):xX},t(a,b],ω+(X,t,ε):=sup{ω+(X,t,ε):xX},t[a,b),ω(X,t):=limε0+ω(X,t,ε),t(a,b],ω+(X,t):=limε0+ω+(X,t,ε),t[a,b),ω(X):=supt(a,b]ω(X,t),ω+(X):=supt[a,b)ω+(X,t).

Finally, let us define the following quantity

μm(X):=max{ω(X),ω+(X)}+suptJβE(X(t)). (2.1)

Theorem 2.5

[13] The function μm given by formula (2.1) satisfies conditions 1o – 7o and 9o in the space R(J, E).

Remark 2.6

Above construction of the measure (2.1) addresses inaccuracies existent in the construction of measures given in [3, 4].

3 Inequalities including measures of noncompactness

This section we start with the proof of inequality which analogue for equicontinuous family of continuous functions is often used in studying solvability of nonlinear equations.

For a fixed nonempty subset XR(J, E), let us put

X(t):={x(t):xX},tJ,abX(t)dt:={abx(t)dt:xX}.

Theorem 3.1

Let XR(J, E) be nonempty, bounded and equiregulated. Then the function JtβE(X(t)) ∈ ℝ+ is regulated and the following inequality holds

βE(abX(t)dt)abβE(X(t))dt.

Proof

Let us fix ε > 0. The condition of X being equiregulated implies that

s[a,b)δs>0ω+(X,s,δs)<εand(s,s+δs)[a,b), (3.1)
s(a,b]δs>0ω(X,s,δs)<εand(sδs,s)(a,b]. (3.2)

Since the family of intervals {[a, a + δa), (b δb , b], (s δs , s + δs) : s ∈ (a, b)} is an open cover of compact interval J, then there is a finite subcover. Obviously it contains intervals [a, a + δa) and (b δb , b]. From this finite subcover we can choose following subcover

[s0,s0+δs0),(s1δs1,s1+δs1),(s2δs2,s2+δs2),...,
...,(sk1δsk1,sk1+δsk1),(skδsk,sk] (3.3)

such that a = s0 < s1 < … < sk = b and additionally every two consecutive intervals from (3.3) have nonempty intersection. Now we choose one point si belonging to each of those k intersections, i.e. we have the sequence of points

a=s0<s1<s1<s2<s2<...<sk1<sk<sk=b.

For simplicity let us denote them by ti, i = 0, …, n where n = 2k i.e.

t0=s0,t1=s1,t2=s1,t3=s2,t4=s2,...,tn1=sk,tn=sk.

From (3.1) and (3.2) we yield that

τ1,τ2(ti1,ti)xXx(τ2)x(τ1)ε,i=1,...,n. (3.4)

Hence

τ1,τ2(ti1,ti)|βE(X(τ2))βE(X(τ1))|ε,i=1,...,n, (3.5)

which means that the function JtβE(X(t)) is regulated, thus Riemann integrable. Let us choose arbitrary si ∈ (ti–1, ti), i = 1, …, n. Then by (3.5) we have

|abβE(X(t))dti=1n(titi1)βE(X(si))|i=1n(titi1)ε=(ba)ε. (3.6)

For each i = 1, …, n there exist vji E, j = 1, …, mi, such that

X(si)j=1miB(vji,βE(X(si))+ε).

Hence and by (3.4) we have

t(ti1,ti)X(t)j=1miB(vji,βE(X(si))+2ε),i=1,...,n. (3.7)

Let us set functions yj1,…,jnR(J, E), ji ∈ {1, …, mi}, i = 1, …, n by formulas

yj1,...,jn(t):=θfort=ti,i=0,1,...n,vjiifort(ti1,ti),i=1,...,n.

We prove that the set of vectors given by ab yj1,…,jn(t)dt for ji ∈ {1, …, mi}, i = 1, …, n is ( ab βE(X(t))dt + 3ε(ba))-net for ab X(t)dt. Let xX. Because of (3.7) there exists such a sequence j1, …, jn, that

x(t)vjiiβE(X(si))+2ε,t(ti1,ti),i=1,...,n. (3.8)

Then, using (3.8) and (3.6) we have

abx(t)dtabyj1,...,jn(t)dti=1nti1tix(t)yj1,...,jn(t)dt=i=1nti1tix(t)vjiidti=1n(titi1)(βE(X(si))+2ε)i=1n(titi1)βE(X(si))+2ε(ba)abβE(X(t))dt+3ε(ba),

which means that

βE(abX(t)dt)abβE(X(t))dt+3ε(ba),

which for ε → 0 proves the theorem.□

Without the assumption about XR(J, E) being equiregulated, the function JtβE(X(t)) does not have to be measurable in Lebesgue sense. However, for countable subsets of the space R(J, E) we have (see [16]).

Theorem 3.2

If {xn : n ∈ ℕ} ⊂ R(J, E) and there exists Lebesgue integrable function g : J → ℝ+ such thatxn(t)∥ ≤ g(t) for tJ, n ∈ ℕ, then the function JtβE({xn(t) : n ∈ ℕ}) is Lebesgue integrable on J and

βE({abxn(t)dt:nN})2abβE({xn(t):nN})dt.

Remark 3.3

Above theorem is also true given weaker assumption that functions xn are strongly measurable [16]. The example from [17] shows that factor 2 from the above theorem cannot be replaced by smaller even for the sequence {xn} of regulated functions.

In some applications of measures of noncompactness the following lemma can be useful.

Lemma 3.4

[18] If E is a Banach then for each non-empty and bounded set XE there exists such countable set X0X, that βE(X) ≤ 2βE(X0).

One can ask what can be an analogue of this lemma for measure μm and space R(J, E)? The answer is given in two following theorems.

Theorem 3.5

For each non-empty and bounded set XR(J, E), where E is a finite dimensional Banach space, there exists such countable set X0X that μm(X0) = μm(X).

Proof

Without loss of generality we can assume that max{ω(X), ω+(X)} = ω+(X). Let {tn} ⊂ J be such a sequence that ω+(X) = supnN ω+(X, tn). Let us arbitrarily fix n ∈ ℕ. Then for each i ∈ ℕ there exists such a function xinXthatlimiω+(xin,tn,1i)=ω+(X,tn). Denote X0 := { xin : i, n ∈ ℕ}. Then based on the above we have ω+(X0) = ω+(X), ω(X0) ≤ ω(X) and hence μm(X0) = μm(X).□

In the general case the assertion of the previous theorem has to be weakened.

Theorem 3.6

For each non-empty and bounded set XR(J, E) and any ε > 0, there exists such countable set X0X, that μm(X) ≤ 2 μm(X0) + ε. In the above estimation factor 2 cannot be replaced by smaller (see Example 3.7).

Proof

Let 0 be a countable set constructed the same way as in the proof of Theorem 3.5. Thus

max{ω(X),ω+(X)}=max{ω(X0~),ω+(X0~)}.

Let us arbitrarily fix ε > 0. There exists such a number t0J that

suptJ βE(X(t)) < βE(X(t0)) + ε. Using Lemma 3.4 we get that there exists such a sequence {xn} ⊂ X that

βE(X(t0))2βE({xn(t0):nN}).

Hence

suptJβE(X(t))2βE({xn(t0):nN})+ε2suptJβE({xn(t):nN})+ε.

Let X0 := 0 ∪ {xn : n ∈ ℕ}. Obviously X0 is countable and

suptJβE(X(t))2suptJβE(X0(t))+ε,max{ω(X),ω+(X)}=max{ω(X0),ω+(X0)}.

Hence

μm(X)=suptJβE(X(t))+max{ω(X),ω+(X)}2suptJβE(X0)(t))+max{ω(X0),ω+(X0)}+ε2μm(X0)+ε.

By 1A we denote the indicator function of a subset A. When the subset A = {a} is singleton, we will write 1a.

Additionally, for arbitrary uE let û denotes the function û : JE given by

u^(t)u,tJ. (3.9)

Example 3.7

Let E be a space consisting of all bounded functions x : ℝ+ → ℝ such that for each of them there exists such countable set Tx ⊂ ℝ+, that function x(t) tends to 0 as t → ∞ and t ∈ ℝ+Tx. We assume the supremum norm in E. Now we can define a subset AE by A := {1t : t ∈ ℝ+} and next we define a subset XR(J, E) by X := {â : aA} where â is defined in (3.9). Thus ω(X) = ω+(X) = 0, suptJ βE(X(t)) = βE(A) = 1 which means that μm(X) = 1 and for any countable subset X0 = { 1tn^ : n = 1, 2, …} ⊂ X we have ω(X0) = ω+(X0) = 0, suptJ βE(X0(t)) = βE({1tn : n = 1, 2, …}) = 12 because {1tn:n=1,2,...}BE(12n=11tn,12) which means that μm(X0) = 12 and that proves that factor 2 from the above theorem cannot be replaced by smaller.

4 Superposition operator

Consider a function f : J × EE. Then, to every function x : JE, we may assign the function (Ffx)(t) := f(t, x(t)), tJ. Operator Ff defined in such way is said to be superposition (or Nemytskii) operator generated by the function f (see [19, 20, 21]). In connection with the space R(J, E), the natural question appears: what properties must the function f satisfy in order for operator Ff to map the space R(J, E) into itself?

In the paper by Aziz [2] and Michalak [12] the following results were obtained.

Theorem 4.1

[12] A superposition operator Ff maps R(J, E) into itself if and only if the function f has the following properties:

  1. the limit lim[a,t)×E(s,v)(t,x) exists for every (t, x) ∈ (a, b] × E,

  2. the limit lim(t,b]×E(s,v)(t,x) exists for every (t, x) ∈ [a, b) × E.

Given the notation

gt(x):=lim(t,b]×E(s,v)(t,x)f(s,v),t[a,b),xE, (4.1)

condition (2) of Theorem 4.1 can be written in an equivalent form using quantifiers

xEt[a,b)gt(x)Eε>0δ>0τ>0vBE(x,δ)s(t,t+τ)gt(x)f(s,v)ε. (4.2)

Analogically condition (1) of Theorem 4.1 can be written - we omit the details.

Theorem 4.2

[2] Suppose that the function f(⋅, u) is regulated on [0, 1] for all uE, and the function f(t, ⋅) is continuous on E, uniformly with respect to tJ. Then the superposition operator Ff maps R(J, E) into itself and is (norm) bounded.

Theorem 4.3

[12] A superposition operator Ff maps R(J, E) into itself is continuous if and only if a function : Exf(⋅, x) ∈ R(J, E) is continuous.

Let us denote by EE the linear space consisted of all, not necessarily continuous functions h : EE. This space will become a linear topological space when we introduce a topology of almost uniform convergence through a family of pseudonorms {∥ ⋅ ∥K}K∈ᵊ given by ∥hK := supxK h(x)∥ for hEE, where ᵊ is is a family of all non-empty compact sets in E. So given family {hs}sJEE the convergence {hs} to hEE in this topology with stJ means uniform convergence hs to h on all compact subsets in E when st.

Furthermore given fixed function f : J × EE we shall denote: for each tJ let

f¯t(x):=f(t,x),xE.

Thus we have ftEE for tJ.

Now we can formulate a theorem that gives (in terms of the function ft) necessary conditions for any space E and sufficient ones when dim E < ∞ such that superposition operator Ff maps R(J, E) into itself.

Theorem 4.4

Let the superposition operator Ff maps R(J, E) into itself. Then the family of functions {ft}tJEE satisfies the following conditions:

  1. The mapping JtftEE is a regulated function.

  2. The following limits of pointwise convergence exist and

    1. limst+ fs is continuous in E for t ∈ [a, b),

    2. limst fs is continuous in E for t ∈ (a, b].

Conversely, if additionally E is a finitely dimensional Banach space and conditions (a) and (b) are satisfied then the superposition operator Ff maps R(J, E) into itself.

Proof

(⇒) Let us fix t ∈ [a, b). Using condition (2) of Theorem 4.1 and based on notation (4.1) we have the following equality

gt(x)=limst+f¯s(x),xE.

First we prove (b1). Let us fix xE and ε > 0. Because of (4.2) we have the existence of δ > 0 and τ > 0 such that

gt(x)f¯s(v)ε,s(t,t+τ),vB(x,δ).

Now going from st+ we have ∥gt(x) – gt(v)∥ ≤ ε which proves continuity of gt in x and thereby on E. Analogically we can prove (b2).

We will now prove (a) i.e. that fs converges to gt almost uniformly on E when st+. Let us fix non-empty and compact set KE and ε > 0. Then, because of (4.2) and already proven continuity of gt, we have that for each xK there exist δx > 0, τx > 0 such that concurrently

s(t,t+τx)vBE(x,δx)gt(x)f¯s(v)ε2 (4.3)

and

gt(x)gt(v)ε2,vBE(x,δx). (4.4)

Out of family {BE(x, δx)}xK covering compact set K we choose a finite subcover {BE(xi,δxi)}i=1n. Let τ := min{τi : i = 1, …, n}. Let us fix arbitrary vK. Then there exists such i that vBE(xi, δi). Thus for s ∈ (t, t + τ) based on (4.3) and (4.4) we have the following estimation

gt(v)f¯s(v)gt(v)gt(xi)+gt(xi)f¯s(v)ε2+ε2=ε

for any vK, i.e. we have uniform convergence on K. Similarly we can prove the existence of the limit limst fs in the topology of almost uniform convergence.

(⇐) Assume that E has a finite dimension and fix t ∈ [a, b). Condition (a) assures the existence of the limit gt := limst+ fs which, based on (b) is continuous on E. Let us fix xE and ε > 0. Continuity of gt means that for some r > 0 we have

gt(x)gt(v)ε2,vBE(x,r). (4.5)

Moreover (a) implies that for a compact set BE(x, r) there exists τ > 0 such that

gt(v)f¯s(v)ε2,vB¯E(x,r),s(t,t+τ).

When we combine it with (4.5), for vBE(x, r), s ∈ (t, t + τ) we have

gt(x)f(s,v)gt(x)gt(v)+gt(x)f(s,v)ε2+ε2=ε

i.e. condition (4.2) is satisfied and thereby (2) in Theorem 4.1 holds. Similarly we can prove (1) in Theorem 4.1, so actually Ff acts from R(J, E) into R(J, E).□

Corollary 4.5

If E is a finitely dimensional Banach space then superposition operator Ff acts from R(J, E) into R(J, E) if and only if both conditions (a) and (b) in Theorem 4.4 are satisfied.

Now we give further sufficient and necessary conditions that superposition operator Ff acts from R(J, E) into R(J, E).

To this end, let us recall so-called module of continuity of a mapping h : EE at a point vE given by

ν(h,v,δ):=sup{h(v)h(u):uBE(v,δ)},δ>0. (4.6)

For a fixed mapping f : J × EE and vE let us denote

Dv:={tJ:themappingf¯tisnotcontinuousatv}. (4.7)

For any subset SJ, in the space R(J, E) we will use a pseudonorm ∥⋅∥S given by

xS:=sup{x(t):tS},xR(J,E).

Now we can give another sufficient and necessary criterion that superposition operator Ff acts from R(J, E) into R(J, E).

Theorem 4.6

Superposition operator Ff acts from R(J, E) into R(J, E) if and only if the following four conditions are satisfied:

  1. vE f(⋅, v) ∈ R(J, E).

  2. For each vE set Dv is finite or countable.

  3. For each vE, if the set Dv = {tn} is infinite then

    lim(n,δ)(,0+)ν(f¯tn,v,δ)=0.
  4. The mapping Euf(⋅, u) ∈ R(J, E) is continuous in every point vE in regard to pseudonorm ∥⋅∥JDv, i.e. for each vE and each sequence vnv we havef(⋅, v) – f(⋅, vn)∥JDv → 0 when n → ∞.

Before we prove Theorem 4.6 we give technical lemma, necessary in the next part of the paper.

Lemma 4.7

If there exist a number ε0 > 0, a sequence {tn} ⊂ J convergent to a point t0J from one side and a sequence {vn} ⊂ E convergent to vector vE, such that

f(tn,v)f(tn,vn)ε0,n=1,2,... (4.8)

then superposition operator Ff does not act from R(J, E) into R(J, E).

Proof

We give a proof by contradiction. Let us assume that Ff acts from R(J, E) into R(J, E). Hence we have

vEf(,v)R(J,E). (4.9)

Let assume that {tn} is convergent to some t0J from one side, for example tn t0+ , and moreover {tn} is strictly decreasing (we can have that choosing a proper subsequence). Let us put

y(t):=θfort[a,t0](t1,b],vnfort(tn+1,tn],n=1,2,....

Obviously yR(J, E). Since FfyR(J, E), then there exists a limit

limtt0+(Ffy)(t)=limnf(tn,vn).

Moreover, by (4.9), there exists a limit limn f(tn, v). Hence, by (4.8) we get

||limnf(tn,vn)limnf(tn,v)||ε0. (4.10)

Now let us define next function zR(J, E) as follows

z(t):=θfort[a,t0](t1,b],vfort(t2n,t2n1],n=1,2,...,vnfort(t2n+1,t2n],n=1,2,....

Since FfzR(J, E) then there is a limit limtt0+ (Ffz)(t) which means that

limnf(t2n,v2n)=limnf(t2n1,v).

However it is in contradiction with (4.10).□

Proof of Theorem 4.6

(⇒) Take an arbitrary vE and put x(t) ≡ v, tJ. Since FfxR(J, E), then (a) is satisfied.

Let us assume that the set Dv is uncountable. Since

Dv=k=1{tJ:ν(f¯t,v)>1k}

then there exists such k ∈ ℕ, that the set {tJ : ν(ft, v) > 1k } is uncountable. Let us put ε0 := 1k and choose an arbitrary injective sequence {tn} ⊂ {tJ : ν(ft, v) > 1k }. Since ν(ftn, v) > ε0 for n = 1, 2, … it follows that for each n ∈ ℕ we can choose such vnE, that ∥ftn(v) – ftn(vn) ∥ ≥ ε0 and ∥vvn∥ ≤ 1n . Choosing from the sequence {tn} a subsequent (also denoted as {tn}) which converges from one side to some tJ we have vnv and

f(tn,v)f(tn,vn)ε0,n=1,2,.... (4.11)

However then, by Lemma 4.7 operator Ff would not act from R(J, E) into R(J, E) which proves (b).

Analogically negating conditions (c) and (d) we would have the existence of ε0 > 0, a sequence {tn} ⊂ Dv for condition (c) or {tn} ⊂ JDv for condition (d), convergent from one side to some tJ, a vector vE and a sequence {vn} ⊂ E, such that vnv and (4.11) holds which, by Lemma 4.7 contradicts the hypothesis and thereby prove conditions (c) and (d).

(⇐) Let us fix xR(J, E). To prove that FfxR(J, E) we will show that for fixed t ∈ [a, b) there exists a limit limst+ (Ffx)(s) (we omit the proof of the existence of left-hand side limit as similar to the following). Let us fix such a sequence {tn} ⊂ (t, b], that tnt+ and define vn := x(tn). Since xR(J, E), then there exists a limit v := limn vn. By (a) there exists also a limit limn f(tn, v). To prove the existence of the limit limst+ (Ffx)(s) it is enough to show the existence of the limit limn f(tn, vn). Additionally we show that

limnf(tn,vn)=limnf(tn,v). (4.12)

Let us consider 3 cases:

Case (i): the sequence {tn}, outside a finite number of terms is contained in JDv.

Therefore, by (d), for each ε > 0 and for sufficiently large n we have ∥f(tn, vn) – f(tn, v) ∥ ≤ ε. When n → ∞ we have

lim supnf(tn,vn)limnf(tn,v)ε

which considering that ε > 0 is arbitrary implies (4.12).

Case (ii): The sequence {tn}, outside a finite number of terms is contained in Dv.

Let us fix ε > 0. By (b) and (c) there exists such n0 ∈ ℕ and δ0 > 0, that for nn0 and for 0 < δ < δ0 we have ν(ftn, v, δ) < ε, i.e. for large enough n we have ∥f(tn, vn) – f(tn, v) ∥ ≤ ε. When n → ∞ using similar reasoning as in case (i) we also get that (4.12) holds.

Case (iii): Infinitely many terms of the sequence {tn} is contained in Dv as well as infinitely many terms of the sequence {tn} is contained in JDv.

Dividing the sequence {tn} into two adequate subsequences the case can be reduced to previous cases (i) and (ii). □

Remark 4.8

The above Theorems 4.4 and 4.6 improve some mistake contained in [13] (Theorem 5.1).

We now give a criterion of compactness for the superposition operator Ff.

Theorem 4.9

Let E be a separable Banach space and let the superposition operator Ff : R(J, E) → R(J, E) be continuous and compact (i.e. Ff transforms bounded sets in relatively compact sets). Then

  1. there exists a function gR(J, E),

  2. there exists a countable or finite set T = {tn} ⊂ J,

  3. there exist a countable or finite sequence of functions hn : EE, n = 1, 2, … that are continuous, compact and when it is infinite

    r>0limnhn(BE(r))=0 (4.13)

    such that

    f(t,x)=g(t)+n=11tn(t)hn(x),tJ,xE. (4.14)

Conversely, if the conditions (H1)-(H3) are satisfied and E is a Banach space then the formula (4.14) gives such a function f(t, x), that operator Ff : R(J, E) → R(J, E) and it is continuous and compact.

Remark 4.10

Obviously the case when all hn functions in the previous theorem are equal to θ, that is when f(t, x) = g(t), or only a finite number of them is not equal to θ is also allowed.

The proof of the theorem will be preceded by two lemmas. Before that however we will give a useful notation. For each xR(J, E) we will put

suppx:={tJ:x(t)θ}.

In contrast to standard definition of a support we do not require the closure.

Lemma 4.11

If Ff : R(J, E) → R(J, E) is compact, then for each x, yR(J, E) the set supp (FfxFfy) is countable or finite and for each injective sequence {tn} ⊂ J, we have

limnf(tn,x(tn))f(tn,y(tn))=θ. (4.15)

Proof

If the set supp(FfxFfy) was uncountable or if (4.15) was not satisfied, then there would exist a injective sequence {sn} ⊂ J and a number ε0 > 0, such that

f(sn,x(sn))f(sn,y(sn))ε0,n=1,2,...

Let us define the sequence of functions un : JE, n = 1, 2, … by

un(t):=x(sn)for t=sn,y(t)for tsn.

Obviously unR(J, E). For nm we have snsm and therefore

FfunFfum(Ffun)(sn)(Ffum)(sn)=f(sn,x(sn))f(sn,y(sn))ε0

i.e. the sequence {Ffun} is ε0-separable, hence Ff is not compact, which ends the proof.□

Lemma 4.12

If E is a separable Banach space and Ff : R(J, E) → R(J, E) is compact and continuous, then there exists a countable or finite set T = {tn} ⊂ J, such that

xEsupp(Ffx^Ffθ^)T. (4.16)

Proof

Let A = {an : n ∈ ℕ} ⊂ E be a countable dense subset of E. Let us put T := n=1supp(Ffan^Ffθ^). By the previous Lemma 4.11, the set T is countable or finite. If there existed xE such that (4.16) did not hold then there would exist sJ such that s ∈ supp(FfFfθ̂)∖T. Thus ∥(FfFfθ̂)(s) ∥ = ε0 for some ε0 > 0 and additionally (Ff an^ Ffθ̂)(s) = θ for n ∈ ℕ. If we took such a subsequence {akn}, that aknx in E we would have

Ffx^Ffakn^(Ffx^Ffθ^)(s)(Ffakn^Ffθ^)(s)=ε0

which is in contradiction with continuity Ff.□

Proof of Theorem 4.9

Let us assume first that E is separable and Ff is compact and continuous. Let the set T = {tn} be like in Lemma 4.12. We define the function g : JE and the sequence of functions hn : EE, n = 1, 2, … by

g(t):=f(t,θ),tJ,hn(x):=f(tn,x)f(tn,θ),xE,nN.

By Lemma 4.12, for each xE the mapping Jtf(t, x) – f(t, θ) can be non-zero only on the set T and its formula is given by n=11tn(t)hn(x). Therefore

f(t,x)=f(t,θ)+f(t,x)f(t,θ)=g(t)+n=11tn(t)hn(x).

Since Ff is continuous the functions hn must be continuous and since Ff is compact also the functions hn must be compact. Moreover it results from Lemma 4.11 that limn f(tn, x) – f(tn, θ) = θ for xE i.e.

limnhn(x)=θ,xE. (4.17)

We have only (4.13) left to prove. Let us assume that it is not satisfied. Then there would exist r > 0, a number ε0 > 0 and such a subsequence of the sequence {hn}, (also denoted by {hn}), that

hn(BE(r))ε0,n=1,2,... (4.18)

Let k1 = 1. We choose x1BE(r), such that ∥hk1(x1)∥ ≥ ε02 . By (4.17) we know that there exists k2 ∈ ℕ, such that k2 > k1 i ∥hi(x1)∥ ≤ ε04 for ik2. By (4.18) we conclude that there exists x2BE(r), such that ∥hk2(x2)∥ ≥ ε02 . By (4.17) we know that there exists k3 ∈ ℕ, such that k3 > k2 and ∥hi(x2)∥ ≤ ε04 for ik3. Continuing this procedure we get an strictly increasing sequence {kn} ⊂ ℕ and the sequence {xn} ⊂ BE(r) such that

hkn(xn)ε02,n=1,2,...hi(xn)ε04,ikn+1,n=1,2,...

Let n > m. Then

Ffxn^Ffxm^(Ffxn^)(tkn)(Ffxm^)(tkn)=hkn(xn)hkn(xm)hkn(xn)hkn(xm)ε02ε04=ε04

i.e. {Ff xn^ } is positively separated and Ff is not compact which contradicts the assumptions.

Let us assume now that the conditions (H1)-(H3) are satisfied and the function f(t, x) is given by the formula (4.14). First we prove that Ff : R(J, E) → R(J, E). Let us fix xR(J, E), tJ and the sequence { tj } convergent to t from one side, e.g. tj t+. Since the sequence {x( tj )} is bounded, then by (4.13) we have limjn=11tn(tj)hn(x(tj))=θ and in virtue of (4.14) we get limj(Ffx)(tj)=limjg(tj)=g(t+) i.e. FfxR(J, E).

Now we prove that the operator Ff is compact. Let us fix a bounded sequence {xn} ⊂ BR(J,E)(r), where r > 0. Since the operator h1 is compact we are able to choose such a subsequence {xn,1} of a sequence {xn} that the sequence {h1(xn,1(t1))} is convergent. Since the operator h2 is compact we are able to choose such a subsequence {xn,2} of the sequence {xn,1} that the sequence {h2(xn,2(t2))} is convergent. Obviously {h1(xn,2(t1))} is also convergent. Continuing this procedure we get a sequence of sequences {xn,i}n=1 , i = 1, 2, … which has a property that {xn,i+1}n=1 is a subsequence of the sequence {xn,i}n=1 and that there exists a limit limn hj(xn,i(tj)) for i = 1, 2, …, j = 1, 2, …, i. Now, using a diagonal method we can define the sequence {yn} by yn : = xn,n, n = 1, 2, …. Obviously {yn} is a subsequence of {xn}. Moreover the limit limn hi(yn(ti)) exists for each i = 1, 2, …. Thus as well as from the fact that (Ffyn)(t) = g(t) for tT we conclude that the limit limn (Ffyn)(t) exists for each tJ. We are able now to define a function z : JE by z(t) := limn (Ffyn)(t) i.e.

z(t)=g(t)for tJT,g(ti)+limnhi(yn(ti))for t=ti,i=1,2,...

By (4.13) we have

z(ti)g(ti)=limnhi(yn(ti))hi(BE(r))i0.

This means that zR(J, E). Using (4.14) we get

zFfyn=suptiTlimnhi(yn(ti))hi(yn(ti)). (4.19)

Let us fix ε > 0. By (4.13) there exists m ∈ ℕ such that for i > m we have ∥hi(BE(r))∥ ≤ ε and therefore supi>mlimnhi(yn(ti))hi(yn(ti))2ε. Since there exists limit limn hi(yn(ti)), i = 1, 2, …, then there is n0 ∈ ℕ such that for nn0 and for i = 1, 2, …, m we have

limnhi(yn(ti))hi(yn(ti))ε.

Combining the above and (4.19) we get for nn0 the inequality ∥zFfyn ≤ 2ε which proves that Ffynz in R(J, E).

Continuity of the operator Ff is a consequence of condition (H3) - we omit a simple proof of this fact. □

Corollary 4.13

Let Banach space E be separable. Then Ff(R(J, E)) ⊂ R(J, E) and the superposition operator Ff : R(J, E) → R(J, E) is continuous and compact if and only if the conditions (H1)-(H3) of Theorem 4.9 are satisfied.

Problem 4.14

Are the conditions (H1)-(H3) of Theorem 4.9 necessary in case when the space E is not separable?

References

[1] G. Aumann, Reelle Funktionen, Springer, Berlin, 1954.10.1007/978-3-662-42636-4Search in Google Scholar

[2] W. Aziz, N. Merentes and J.L. Sanchez, A note on the composition of regular functions, Z. Anal. Anwend. 33 (2014), 119–123.10.4171/ZAA/1502Search in Google Scholar

[3] J. Banaś, T. Zając, On a measure of noncompactness in the space of regulated functions and its applications, Adv. Nonlinear Anal. 8 (2019), 1099-1110.10.1515/anona-2018-0024Search in Google Scholar

[4] K. Cichoń, M. Cichoń and M.M.A. Metwali, On some parameters in the space of regulated functions and their applications, Carpathian J. Math. 34 (2018), no. 1, 17-30.10.37193/CJM.2018.01.03Search in Google Scholar

[5] K. Cichoń, M. Cichoń and B. Satco, On regulated functions, Fasc. Math. 60 (2018) (in press).10.1515/fascmath-2018-0003Search in Google Scholar

[6] K. Cichoń, M. Cichoń and B. Satco, Measure Differential Inclusions Through Selection Principles in the Space of Regulated Functions, Mediterr. J. Math. (2018) 15:148 https://doi.org/10.1007/s00009-018-1192-y-1660-5446/18/040001-1910.1007/s00009-018-1192-ySearch in Google Scholar

[7] J. Dieudonné, Foundations of Modern Analysis, Academic Press, New York, 1969.Search in Google Scholar

[8] L. Drewnowski, On Banach spaces of regulated functions, Comment. Math. vol. 57, no. 2 (2017), 153-167.10.14708/cm.v57i2.4373Search in Google Scholar

[9] D. Fraňkova, Regulated functions, Math. Bohemica 116 (1991), 20-59.10.21136/MB.1991.126195Search in Google Scholar

[10] L.A.O. Fernandes and R. Arbach, Integral functionals on C-algebra of vector-valued regulated functions, Ann. Funct. Anal. 3(2012), 21-31.10.15352/afa/1399899930Search in Google Scholar

[11] C. Goffman, G. Moran and Waterman, D., The structure of regulated functions, Proc. Amer. Math. Soc. 57 (1976), 61–65.10.1090/S0002-9939-1976-0401993-5Search in Google Scholar

[12] A. Michalak, On superposition operators in spaces of regular and of bounded variation functions, Z. Anal. Anwend. 35 (2016), 285–308.10.4171/ZAA/1566Search in Google Scholar

[13] L. Olszowy, Measures of noncompactness in the space of regulated functions, J. Math. Anal. Appl. 476 (2019), 860–874.10.1016/j.jmaa.2019.04.024Search in Google Scholar

[14] B. Satco, Regulated solutions for nonlinear measure driven equations, Nonlinear Anal. Hybrid Syst. 13 (2014), 22–31.10.1016/j.nahs.2014.02.001Search in Google Scholar

[15] J. Banaś and K. Goebel, Measures of Noncompactness in Banach Spaces, Lect. Notes in Pure and Appl. Math. 60, Marcel Dekker, New York, 1980.Search in Google Scholar

[16] W. Orlicz and S. Szufla, On some classes of nolinear Volterra integral equations in Banach spaces, Bull. Pol. Acad. Sci. Math. 30 (1982) no 5-6, 239-250.Search in Google Scholar

[17] H-P. Heinz, On the behaviour of measures of noncompactness with respect to differentiations and integration of vector-valued functions, Nonlinear Anal. Vol 7 No 12 (1983), 1351-1371.10.1016/0362-546X(83)90006-8Search in Google Scholar

[18] P. Chen and Y. Li, Monotone iterative technique for a class of semilinear evolution equations with nonlocal conditions, Results Math. 63 (2013), 731-744.10.1007/s00025-012-0230-5Search in Google Scholar

[19] N. Ackermann, Uniform continuity and Brezis-Lieb-type splitting for superposition operators in Sobolev space, Adv. Nonlinear Anal. 7 (2018), no. 4, 587-599.10.1515/anona-2016-0123Search in Google Scholar

[20] J. Appell and P.P. Zabrejko, Nonlinear Superposition Operators, in: Cambridge Tracts in Mathematics, vol. 95, Cambridge University Press, 1990.10.1017/CBO9780511897450Search in Google Scholar

[21] N.S. Papageorgiou, V.D. Radulescu and D.D. Repovs, Nonlinear analysis - theory and methods, Springer Monographs in Mathematics, Springer, Berlin, 2019.10.1007/978-3-030-03430-6Search in Google Scholar

Received: 2019-08-06
Accepted: 2019-10-02
Published Online: 2019-12-14

© 2019 Jizheng Huang et al., published by De Gruyter

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

Articles in the same Issue

  1. Frontmatter
  2. On the moving plane method for boundary blow-up solutions to semilinear elliptic equations
  3. Regularity of solutions of the parabolic normalized p-Laplace equation
  4. Cahn–Hilliard equation on the boundary with bulk condition of Allen–Cahn type
  5. Blow-up solutions for fully nonlinear equations: Existence, asymptotic estimates and uniqueness
  6. Radon measure-valued solutions of first order scalar conservation laws
  7. Ground state solutions for a semilinear elliptic problem with critical-subcritical growth
  8. Generalized solutions of variational problems and applications
  9. Existence and non-existence results for Kirchhoff-type problems with convolution nonlinearity
  10. Nonlinear Sherman-type inequalities
  11. Global regularity for systems with p-structure depending on the symmetric gradient
  12. Homogenization of a net of periodic critically scaled boundary obstacles related to reverse osmosis “nano-composite” membranes
  13. Noncoercive resonant (p,2)-equations with concave terms
  14. Evolutionary quasi-variational and variational inequalities with constraints on the derivatives
  15. Sharp estimates on the first Dirichlet eigenvalue of nonlinear elliptic operators via maximum principle
  16. Localization and multiplicity in the homogenization of nonlinear problems
  17. Remarks on a nonlinear nonlocal operator in Orlicz spaces
  18. A Picone identity for variable exponent operators and applications
  19. On the weakly degenerate Allen-Cahn equation
  20. Continuity results for parametric nonlinear singular Dirichlet problems
  21. Construction of type I blowup solutions for a higher order semilinear parabolic equation
  22. Singularly perturbed Choquard equations with nonlinearity satisfying Berestycki-Lions assumptions
  23. Comparison results for nonlinear divergence structure elliptic PDE’s
  24. Constant sign and nodal solutions for parametric (p, 2)-equations
  25. Monotonicity formulas for coupled elliptic gradient systems with applications
  26. Berestycki-Lions conditions on ground state solutions for a Nonlinear Schrödinger equation with variable potentials
  27. A class of semipositone p-Laplacian problems with a critical growth reaction term
  28. The role of superlinear damping in the construction of solutions to drift-diffusion problems with initial data in L1
  29. Reconstruction of Tesla micro-valve using topological sensitivity analysis
  30. Lewy-Stampacchia’s inequality for a pseudomonotone parabolic problem
  31. Global well-posedness of nonlinear wave equation with weak and strong damping terms and logarithmic source term
  32. Regularity Criteria for Navier-Stokes Equations with Slip Boundary Conditions on Non-flat Boundaries via Two Velocity Components
  33. Homoclinics for singular strong force Lagrangian systems
  34. A constructive method for convex solutions of a class of nonlinear Black-Scholes equations
  35. On a class of nonlocal nonlinear Schrödinger equations with potential well
  36. Superlinear Schrödinger–Kirchhoff type problems involving the fractional p–Laplacian and critical exponent
  37. Regularity for minimizers for functionals of double phase with variable exponents
  38. Boundary blow-up solutions to the Monge-Ampère equation: Sharp conditions and asymptotic behavior
  39. Homogenisation with error estimates of attractors for damped semi-linear anisotropic wave equations
  40. A-priori bounds for quasilinear problems in critical dimension
  41. Critical growth elliptic problems involving Hardy-Littlewood-Sobolev critical exponent in non-contractible domains
  42. On the Sobolev space of functions with derivative of logarithmic order
  43. On a logarithmic Hartree equation
  44. Critical elliptic systems involving multiple strongly–coupled Hardy–type terms
  45. Sharp conditions of global existence for nonlinear Schrödinger equation with a harmonic potential
  46. Existence for (p, q) critical systems in the Heisenberg group
  47. Periodic traveling fronts for partially degenerate reaction-diffusion systems with bistable and time-periodic nonlinearity
  48. Some hemivariational inequalities in the Euclidean space
  49. Existence of standing waves for quasi-linear Schrödinger equations on Tn
  50. Periodic solutions for second order differential equations with indefinite singularities
  51. On the Hölder continuity for a class of vectorial problems
  52. Bifurcations of nontrivial solutions of a cubic Helmholtz system
  53. On the exact multiplicity of stable ground states of non-Lipschitz semilinear elliptic equations for some classes of starshaped sets
  54. Sign-changing multi-bump solutions for the Chern-Simons-Schrödinger equations in ℝ2
  55. Positive solutions for diffusive Logistic equation with refuge
  56. Null controllability for a degenerate population model in divergence form via Carleman estimates
  57. Eigenvalues for a class of singular problems involving p(x)-Biharmonic operator and q(x)-Hardy potential
  58. On the convergence analysis of a time dependent elliptic equation with discontinuous coefficients
  59. Multiplicity and concentration results for magnetic relativistic Schrödinger equations
  60. Solvability of an infinite system of nonlinear integral equations of Volterra-Hammerstein type
  61. The superposition operator in the space of functions continuous and converging at infinity on the real half-axis
  62. Estimates by gap potentials of free homotopy decompositions of critical Sobolev maps
  63. Pseudo almost periodic solutions for a class of differential equation with delays depending on state
  64. Normalized multi-bump solutions for saturable Schrödinger equations
  65. Some inequalities and superposition operator in the space of regulated functions
  66. Area Integral Characterization of Hardy space H1L related to Degenerate Schrödinger Operators
  67. Bifurcation of time-periodic solutions for the incompressible flow of nematic liquid crystals in three dimension
  68. Morrey estimates for a class of elliptic equations with drift term
  69. A singularity as a break point for the multiplicity of solutions to quasilinear elliptic problems
  70. Global and non global solutions for a class of coupled parabolic systems
  71. On the analysis of a geometrically selective turbulence model
  72. Multiplicity of positive solutions for quasilinear elliptic equations involving critical nonlinearity
  73. Lack of smoothing for bounded solutions of a semilinear parabolic equation
  74. Gradient estimates for the fundamental solution of Lévy type operator
  75. π/4-tangentiality of solutions for one-dimensional Minkowski-curvature problems
  76. On the existence and multiplicity of solutions to fractional Lane-Emden elliptic systems involving measures
  77. Anisotropic problems with unbalanced growth
  78. On a fractional thin film equation
  79. Minimum action solutions of nonhomogeneous Schrödinger equations
  80. Global existence and blow-up of weak solutions for a class of fractional p-Laplacian evolution equations
  81. Optimal rearrangement problem and normalized obstacle problem in the fractional setting
  82. A few problems connected with invariant measures of Markov maps - verification of some claims and opinions that circulate in the literature
Downloaded on 31.10.2025 from https://www.degruyterbrill.com/document/doi/10.1515/anona-2020-0050/html
Scroll to top button