Abstract

We consider the initial value problem for a functional differential inclusion with a Volterra multivalued mapping that is not necessarily decomposable in 𝐿𝑛1[π‘Ž,𝑏]. The concept of the decomposable hull of a set is introduced. Using this concept, we define a generalized solution of such a problem and study its properties. We have proven that standard results on local existence and continuation of a generalized solution remain true. The question on the estimation of a generalized solution with respect to a given absolutely continuous function is studied. The density principle is proven for the generalized solutions. Asymptotic properties of the set of generalized approximate solutions are studied.

1. Introduction

During the last years, mathematicians have been intensively studying (see [1, 2]) perturbed inclusions that are generated by the algebraic sum of the values of two multivalued mappings, one of which is decomposable. Many types of differential inclusions can be represented in this form (ordinary differential, functional differential, etc.). In the above-mentioned papers, the authors investigated the solvability problem for such inclusions. Estimates for the solutions were obtained similar to the estimates, which had been obtained by Filippov for ordinary differential inclusions (see [3, 4]). The concept of quasisolutions is introduced and studied. The density principle and the β€œbang-bang” principle are proven. In papers [5–8], the perturbed inclusions with internal and external perturbations are considered, and the conjecture that β€œsmall” internal and external perturbations can significantly change the solution set of the perturbed inclusion is proven. Let us remark that, in the cited papers, the proofs of the obtained results essentially depend on the assumption that the multivalued mapping, which generates the algebraic sum of the values, is decomposable. Therefore, these studies once again confirm V. M. Tikhomirov's conjecture that decomposability is a specific feature of the space 𝐿𝑛1[π‘Ž,𝑏] and plays the same role as the concept of convexity in Banach spaces. The decomposability is implicitly used in many fields of mathematics: optimization theory, differential inclusions theory, and so forth. If a multivalued mapping is not necessarily decomposable, then the methods known for multivalued mappings cannot even be applied to the solvability problem of the perturbed inclusion. Furthermore, in this case, the equality between the set of quasisolutions of the perturbed inclusion and the solution set of the perturbed inclusion with the decomposable hull of the right-hand side fails. This equality for the ordinary differential inclusions was proven by WaΕΌewski (see [9]). The point is that, in this case, the closure (in the weak topology of 𝐿𝑛1[π‘Ž,𝑏]) of the set of the values of this multivalued mapping does not coincide with the closed convex hull of this set. As a result, we have that fundamental properties of the solution sets (the density principle and β€œbang-bang” principle) do not hold any more (see [3, 10–13]). The situation cannot be improved even if the mapping in question is continuous.

In this paper, we consider the initial value problem for a functional differential inclusion with a multivalued mapping. We assume that this mapping is not necessarily decomposable. Some mathematical models can naturally be described by such an inclusion. For instance, so do certain mathematical models of sophisticated multicomponent systems of automatic control (see [14]), where, due to the failure of some devices, objects are controlled by different control laws (different right-hand sides) with the diverse sets of the control admissible values. This means that the object's control law consists of a set of the controlling subsystems. These subsystems may be linear as well as nonlinear. For example, this occurs in the control theory of the hybrid systems (see [15–20]). Due to the failure of a device, the control object switches from one control law to another. The control of an object must be guaranteed in spite of the fact that failures (switchings) may take place any time. Therefore, the mathematical model should treat all available trajectories (states) corresponding to all switchings. The generalized solutions of the inclusion make up the set of all such trajectories. The concept of a generalized solution should be then introduced and its properties should be studied.

We consider a functional differential inclusion with a Volterra-Tikhonov type (in the sequel simply Volterra type) multivalued mapping and we prove that for such an inclusion, the theorem on existence and continuation of a local generalized solution holds true. This justifies one of the requirements, which were formulated in the monograph of Filippov [4] for generalized solutions of differential equations with discontinuous right-hand sides. In the present paper, it is also proven that in the regular case, that is, when a multivalued mapping is decomposable, a generalized solution coincides with an ordinary solution. At the same time, the concept of a generalized solution discussed in the present paper does not satisfy all the requirements that are usually put on generalized (in the sense of the monograph [4]) solutions of differential equations with discontinuous right-hand sides. For instance, the limit of generalized (in the sense of the present paper) solutions is not necessarily a generalized solution itself. The reason for that is that a multivalued mapping that determines a generalized solution (the definition is given below) may not be closed in the weak topology of 𝐋𝑛1[π‘Ž,𝑏], as this mapping is not necessarily convex-valued.

2. Preliminaries

We start with the notation and some definitions. Let 𝑋 be a normed space with the norm ‖⋅‖𝑋. Let 𝐡𝑋[π‘₯,πœ€] be the closed ball in the space 𝑋 with the center at π‘₯βˆˆπ‘‹ and of radius πœ€>0; if πœ€=0, then 𝐡𝑋[π‘₯,0]≑π‘₯. Let π‘ˆβŠ‚π‘‹. Then π‘ˆ is the closure of π‘ˆ, coπ‘ˆ is the convex hull of π‘ˆ; coπ‘ˆβ‰‘coπ‘ˆ, extπ‘ˆ is the set of all extreme points of π‘ˆ; extπ‘ˆ=extπ‘ˆ. Let β€–π‘ˆβ€–π‘‹=supπ‘’βˆˆπ‘ˆβ€–π‘’β€–π‘‹. Let π‘ˆπœ€β‰‘β‹ƒπ‘’βˆˆπ‘ˆπ΅[𝑒,πœ€] if πœ€>0 and π‘ˆ0β‰‘π‘ˆ.

Let πœŒπ‘‹[π‘₯;π‘ˆ] be the distance from the point π‘₯βˆˆπ‘‹ to the set π‘ˆ in the space 𝑋; let β„Ž+𝑋[π‘ˆ1;π‘ˆ]≑supπ‘₯βˆˆπ‘ˆ1πœŒπ‘‹[π‘₯,π‘ˆ] be the Hausdorff semideviation of the set π‘ˆ1 from the set π‘ˆ; let β„Žπ‘‹[π‘ˆ1;π‘ˆ]=max{β„Ž+𝑋[π‘ˆ1;π‘ˆ];β„Ž+𝑋[π‘ˆ;π‘ˆ1]} be the Hausdorff distance between the subsets π‘ˆ1 and π‘ˆ of 𝑋.

We denote by comp[𝑋] (resp., comp[π‘‹βˆ—]) the set of all nonempty compact subsets of 𝑋 (resp., the set of all nonempty, bounded, closed in the space 𝑋, and relatively compact in the weak topology on the space 𝑋 subsets of 𝑋). Let 2𝑋 be the set of all nonempty bounded subsets of 𝑋.

Let 𝒫 be a system of subsets of 𝑋 (a subset of 𝑋). We denote by Ξ©(𝒫) the set of all nonempty convex subsets of 𝑋, belonging to the system 𝒫 (the set of all nonempty convex subsets of 𝑋, belonging to 𝒫).

Let ℝ𝑛 be the space of all 𝑛-dimensional column vectors with the norm |β‹…|. We denote by 𝐢𝑛[π‘Ž,𝑏] (resp., 𝐷𝑛[π‘Ž,𝑏]) the space of continuous (resp., absolutely continuous) functions π‘₯∢[π‘Ž,𝑏]→ℝ𝑛 with norm β€–π‘₯‖𝐢𝑛[π‘Ž,𝑏]=max{|π‘₯(𝑑)|βˆΆπ‘‘βˆˆ[π‘Ž,𝑏]} (resp., β€–π‘₯‖𝐷𝑛[π‘Ž,𝑏]∫=|π‘₯(π‘Ž)|+π‘π‘Ž|Μ‡π‘₯(𝑠)|𝑑𝑠). Let π’°βŠ‚[π‘Ž,𝑏] be a measurable set πœ‡(𝒰)>0 (πœ‡β€”the Lebesgue measure). We denote by 𝐿𝑛𝑝(𝒰) the space of all functions π‘₯βˆΆπ’°β†’β„π‘› such that (π‘₯(𝑠))𝑝 is integrable (if 𝑝<∞) and the space of all measurable, essentially bounded (if 𝑝=∞) functions π‘₯βˆΆπ’°β†’β„π‘› with the norms β€–β€–π‘₯‖‖𝐿𝑛𝑝(𝒰)=ξ‚€ξ€œπ’°||||||π‘₯(𝑠)𝑝𝑑𝑠1/𝑝,β€–β€–π‘₯β€–β€–πΏπ‘›βˆž(𝒰)=vraisupπ‘ βˆˆπ’°||||||π‘₯(𝑠),(2.1) respectively.

Let Ξ¦βŠ‚πΏπ‘›1[π‘Ž,𝑏]. The set Ξ¦ is called integrally bounded if there exists a function πœ‘Ξ¦βˆˆπ‹11[π‘Ž,𝑏] such that |π‘₯(𝑑)|β‰€πœ‘Ξ¦(𝑑) for each π‘₯∈Φ and almost all π‘‘βˆˆ[π‘Ž,𝑏]. The set Ξ¦ is said to be decomposable if for each π‘₯,π‘¦βˆˆΞ¦ and every measurable set π’°βŠ‚[π‘Ž,𝑏] the inclusion πœ’(𝒰)π‘₯+πœ’([π‘Ž,𝑏]⧡𝒰)π‘¦βˆˆΞ¦ holds, where πœ’(𝑉) is the characteristic function of the set 𝑉. We denote by 𝑄[𝐋𝑛1[π‘Ž,𝑏]] (resp., Ξ [𝐿𝑛1[π‘Ž,𝑏]]) the set of all nonempty, closed, and integrally bounded (resp., nonempty, bounded, closed, and decomposable) subsets of the space 𝐿𝑛1[π‘Ž,𝑏].

Let 𝐹∢[π‘Ž,𝑏]β†’comp[ℝ𝑛] be a measurable mapping. Then by definition, 𝑆(𝐹)={π‘¦βˆˆπΏπ‘›1[π‘Ž,𝑏]βˆΆπ‘¦(𝑑)∈𝐹(𝑑)foralmostallπ‘‘βˆˆ[π‘Ž,𝑏]}. By 𝐢1+[π‘Ž,𝑏] (resp., 𝐿1+[π‘Ž,𝑏]), denote the cone of all nonnegative functions of the space 𝐢11[π‘Ž,𝑏] (resp., 𝐿11[π‘Ž,𝑏]).

Let π‘“βˆΆπ‘ƒβ†’π‘„ be a mapping between two partially ordered sets 𝑃 and 𝑄 (the partial order of both sets is denoted by ≀). The mapping 𝑓 is isotonic if 𝑓(π‘₯)≀𝑓(𝑦), whenever π‘₯≀𝑦.

In this paper, the expression β€œmeasurability of a single-valued function” is always used in the sense of Lebesgue measurability and β€œmeasurability of a multivalued function” in the sense of [21]. Let (𝑇,Ξ£,πœ‡) be a space with finite positive measure and let 𝐹 be a multivalued mapping from 𝑇 to ℝ𝑛. A set {π‘₯𝜈(β‹…)} (πœˆβˆˆβ„•) of measurable mappings from 𝑇 to ℝ𝑛 is said to approximate the multivalued mapping 𝐹 if the set {π‘‘βˆˆπ‘‡βˆ£π‘₯𝜈(𝑑)∈𝐹(𝑑)} is measurable for any πœˆβˆˆβ„•, and the set 𝐹(𝑑) belongs to the closure of its intersection with the set β‹ƒπœˆβˆˆβ„•{π‘₯𝜈(𝑑)} for almost all π‘‘βˆˆπ‘‡. A multivalued mapping 𝐹 from 𝑇 to ℝ𝑛 is called measurable if there exists a countable set of measurable mappings from 𝑇 to ℝ𝑛 that approximates the mapping 𝐹.

Further, let us introduce the main characteristic properties of a set that is decomposable.

Lemma 2.1. Let Φ∈Π[𝐿𝑛1[π‘Ž,𝑏]]. Then there exists a function π‘’βˆˆπΏ11[π‘Ž,𝑏] such that |πœ‘(𝑑)|≀𝑒(𝑑) for each function πœ‘βˆˆΞ¦ and almost all π‘‘βˆˆ[π‘Ž,𝑏].

Proof. Let πœ‘π‘–βˆˆΞ¦, 𝑖=1,2,…, be a sequence of functions such that limπ‘–β†’βˆžβ€–β€–πœ‘π‘–β€–β€–πΏπ‘›1[π‘Ž,𝑏]=‖‖Φ‖‖𝐿𝑛1[π‘Ž,𝑏].(2.2)
Let us show that there exists a sequence of functions ξ‚πœ‘π‘–βˆˆΞ¦, 𝑖=1,2,…, such that the equality (2.2) holds and |||ξ‚πœ‘1|||≀|||(𝑑)ξ‚πœ‘2|||≀|||(𝑑)ξ‚πœ‘3||||||(𝑑)β‰€β‹―β‰€ξ‚πœ‘π‘–|||≀|||(𝑑)ξ‚πœ‘π‘–+1|||(𝑑)≀⋯(2.3) for almost all π‘‘βˆˆ[π‘Ž,𝑏].
Indeed, let ξ‚πœ‘1=πœ‘1 and ξ‚πœ‘π‘–+1=πœ’(𝒰𝑖)ξ‚πœ‘π‘–+πœ’([π‘Ž,𝑏⧡𝒰𝑖)πœ‘π‘–+1, 𝑖=1,2,…, where 𝒰𝑖={π‘‘βˆˆ[π‘Ž,𝑏]∢|ξ‚πœ‘π‘–(𝑑)|β‰₯|πœ‘π‘–+1(𝑑)|}. Since Φ∈Π[𝐿𝑛1[π‘Ž,𝑏]], we see that the sequence ξ‚πœ‘π‘–βˆˆΞ¦, 𝑖=1,2,…, has the following properties: for almost all π‘‘βˆˆ[π‘Ž,𝑏], the inequalities (2.3) hold and β€–ξ‚πœ‘π‘–β€–πΏπ‘›1[π‘Ž,𝑏]β‰₯β€–πœ‘π‘–β€–πΏπ‘›1[π‘Ž,𝑏] for each 𝑖=1,2,…. Hence, from this property and equality (2.2), it follows that the sequence ξ‚πœ‘π‘–, 𝑖=1,2,…, satisfies (2.2). Further, we consider a measurable function π‘’βˆΆ[π‘Ž,𝑏]β†’[0,∞) defined by 𝑒(𝑑)=limπ‘–β†’βˆž|||ξ‚πœ‘π‘–|||(𝑑).(2.4) Since the set Ξ¦ is bounded, we see, using Fatou's lemma (see [22]), that π‘’βˆˆπΏ11[π‘Ž,𝑏]. Moreover, by the definition of the function 𝑒 and due to (2.2), ξ€œπ’°β€–β€–Ξ¦β€–β€–π‘’(𝑑)𝑑𝑑=𝐿𝑛1(𝒰)(2.5) for every measurable set π’°βŠ‚[π‘Ž,𝑏]. Now, let us show that the function 𝑒 defined by (2.4) satisfies the assumptions of the lemma. Indeed, if the contrary is true, then there exist a function πœ‘βˆˆΞ¦ and a measurable set 𝒰1βŠ‚[π‘Ž,𝑏] (πœ‡(𝒰1)>0) such that |πœ‘(𝑑)|>𝑒(𝑑) for each π‘‘βˆˆπ’°1. This implies that βˆ«π’°1|πœ‘1∫(𝑑)|𝑑𝑑>𝒰1𝑒(𝑑)𝑑𝑑, which contradicts (2.5). This completes the proof.

Lemma 2.2. Let Φ∈Π[𝐿𝑛1[π‘Ž,𝑏]] and πœ‘π‘–βˆˆΞ¦, 𝑖=1,2,…, be a sequence that is dense in Ξ¦. Further, let a measurable set 𝐹∢[π‘Ž,𝑏]β†’comp[ℝ𝑛] be defined by 𝐹(𝑑)=ξ‚†πœ‘π‘–ξ‚‡(𝑑),𝑖=1,2,….(2.6) Then 𝑆(𝐹)=Ξ¦.

Proof. Since πœ‘π‘–βˆˆπ‘†(𝐹) and the sequence πœ‘π‘–, 𝑖=1,2,…, is dense in Ξ¦, we have, due to the closedness of the set Ξ¦, the relation Ξ¦βŠ‚π‘†(𝐹). Let us prove that 𝑆(𝐹)βŠ‚Ξ¦. Let π‘₯βˆˆπ‘†(𝐹). For each π‘˜, 𝑖=1,2,…, put πΈπ‘˜π‘–=|||π‘‘βˆˆ[π‘Ž,𝑏]∢π‘₯(𝑑)βˆ’πœ‘π‘–|||≀1(𝑑)π‘˜ξ‚‡,(2.7) which are measurable sets. For 𝑖=1, let ξ‚‹πΈπ‘˜1=πΈπ‘˜1, and for 𝑖=2,3,…, let ξ‚‹πΈπ‘˜π‘–=πΈπ‘˜π‘–β§΅β‹ƒπ‘–βˆ’1𝑗=1πΈπ‘˜π‘—. Then ξ‚‹πΈπ‘˜π‘–β‹‚ξ‚‹πΈπ‘˜π‘—=βˆ… if 𝑖≠𝑗. By the definition of the mapping 𝐹∢[π‘Ž,𝑏]β†’comp[ℝ𝑛], for each π‘˜=1,2,…, we have πœ‡(βˆžξšπ‘–=1ξ‚‹πΈπ‘˜π‘–)=π‘βˆ’π‘Ž.(2.8) Let π‘₯π‘˜βˆΆ[π‘Ž,𝑏]→ℝ𝑛, π‘˜=1,2,…, be a sequence of measurable functions such that π‘₯π‘˜βŽ§βŽͺβŽͺ⎨βŽͺβŽͺβŽ©πœ‘(𝑑)=𝑖𝐸(𝑑)ifπ‘‘βˆˆπ‘˜π‘–πœ‘,𝑖=1,2,…,π‘˜,1(𝑑)ifπ‘‘βˆˆ[π‘Ž,𝑏]β§΅π‘˜ξšπ‘–=1ξ‚‹πΈπ‘˜π‘–.(2.9) Since the set Ξ¦ is decomposable, we see that π‘₯π‘˜βˆˆΞ¦ for each π‘˜=1,2,…. Moreover, from Lemma 2.1 and the definition of the set ξ‚‹πΈπ‘˜π‘–, it follows that for the functions π‘₯π‘˜, π‘˜=1,2,…, we have the estimates β€–β€–π‘₯βˆ’π‘₯π‘˜β€–β€–πΏπ‘›1[π‘Ž,𝑏]β‰€π‘βˆ’π‘Žπ‘˜ξ€œ+2[π‘Ž,𝑏]⧡βˆͺπ‘˜π‘–=1ξ‚‹πΈπ‘˜π‘–π‘’(𝑑)𝑑𝑑,(2.10) where 𝑒 satisfies the assertions of Lemma 2.1. From (2.8) and (2.10), it follows that π‘₯π‘˜β†’π‘₯ in 𝐿𝑛[π‘Ž,𝑏] as π‘˜β†’βˆž. Since the set Ξ¦ is closed, we have that π‘₯∈Φ. Hence 𝑆(𝐹)βŠ‚Ξ¦. Thus 𝑆(𝐹)=Ξ¦.

Lemma 2.3. Let measurable sets πΉπ‘–βˆΆ[π‘Ž,𝑏]β†’comp[ℝ𝑛], 𝑖=1,2,…, be integrally bounded, then 𝑆(𝐹1(β‹…))βŠ‚π‘†(𝐹2(β‹…)) if and only if 𝐹1(𝑑)βŠ‚πΉ2(𝑑) for almost all π‘‘βˆˆ[π‘Ž,𝑏].

Proof. First of all, it is evident that if for almost all π‘‘βˆˆ[π‘Ž,𝑏], 𝐹1(𝑑)βŠ‚πΉ2(𝑑), then 𝑆(𝐹1(β‹…))βŠ‚π‘†(𝐹2(β‹…)).
Let 𝑆(𝐹1(β‹…))βŠ‚π‘†(𝐹2(β‹…)) and let πœ‘π‘–βˆˆπΏπ‘›1[π‘Ž,𝑏], 𝑖=1,2,…, be a countable set, which is dense in 𝑆(𝐹1) and which approximates 𝐹1∢[π‘Ž,𝑏]β†’comp[ℝ𝑛] (see [21]). Thus πœ‘π‘–βˆˆπ‘†(𝐹2(β‹…)) for each 𝑖=1,2,… and by the definition of the set 𝑆(𝐹2(β‹…)), we have that {πœ‘π‘–(𝑑)βˆΆπ‘–=1,2,…}βŠ‚πΉ2(𝑑) for almost all π‘‘βˆˆ[π‘Ž,𝑏]. Since the sequence πœ‘π‘–, 𝑖=1,2,…, approximates the map 𝐹1∢[π‘Ž,𝑏]β†’comp[ℝ𝑛], it follows from the previous inclusion that 𝐹1(𝑑)βŠ‚πΉ2(𝑑) for almost all π‘‘βˆˆ[π‘Ž,𝑏].

Corollary 2.4. Let Φ∈Π[𝐿𝑛1[π‘Ž,𝑏]] and let πΉπ‘–βˆΆ[π‘Ž,𝑏]β†’comp[ℝ𝑛], 𝑖=1,2, be measurable sets such that Ξ¦=𝑆(𝐹1)=𝑆(𝐹2). Then 𝐹1(𝑑)=𝐹2(𝑑) for almost all π‘‘βˆˆ[π‘Ž,𝑏].

Remark 2.5. If Φ∈Π[𝐿𝑛1[π‘Ž,𝑏]], then a measurable set 𝐹∢[π‘Ž,𝑏]β†’comp[ℝ𝑛], that satisfies 𝑆(𝐹)=Ξ¦, uniquely determines the set Ξ¦.

3. Decomposable Hull of a Set in the Space of Integrable Functions

We introduce the concept of the decomposable hull of a set in the space 𝐋𝑛1[π‘Ž,𝑏]. We consider a multivalued mapping that is not necessarily decomposable. For such a mapping, we construct its decomposable hull and investigate topological properties of this hull.

Definition 3.1. Let Ξ¦ be a nonempty subset of 𝐋𝑛1[π‘Ž,𝑏]. By decΞ¦, we denote the set of all finite combinations 𝒰𝑦=πœ’1π‘₯1𝒰+πœ’2π‘₯2𝒰+β‹―+πœ’π‘šξ‚π‘₯π‘š(3.1) of elements π‘₯π‘–βˆˆΞ¦, 𝑖=1,2,…,π‘š, where the disjoint measurable subsets 𝒰𝑖, 𝑖=1,2,…,π‘š, of the segment [π‘Ž,𝑏] are such that β‹ƒπ‘šπ‘–=1𝒰𝑖=[π‘Ž,𝑏].

Lemma 3.2. The set decΞ¦ is decomposable for any nonempty set Ξ¦βŠ‚π‹π‘›1[π‘Ž,𝑏].

Proof. Let 𝑦1,𝑦2∈decΞ¦. Let also π’°βŠ‚[π‘Ž,𝑏] be a measurable set. Without loss of generality, it can be assumed that 𝑦𝑖𝒰=πœ’π‘–1π‘₯𝑖1𝒰+πœ’π‘–2π‘₯𝑖2𝒰+β‹―+πœ’π‘–π‘šξ‚π‘₯π‘–π‘š,(3.2) where π‘₯π‘–π‘—βˆˆΞ¦, 𝑗=1,2,…,π‘š, 𝑖=1,2, and the measurable disjoint sets π’°π‘–π‘—βŠ‚[π‘Ž,𝑏], 𝑗=1,2,…,π‘š, 𝑖=1,2, are such that ⋃[π‘Ž,𝑏]=π‘šπ‘—=1𝒰𝑖𝑗, 𝑖=1,2, (if the number of summands in (3.2) is not the same, we may use arbitrary functions multiplied by the characteristic functions of the empty sets). Further, from the equality πœ’(𝒰)𝑦1𝑦+πœ’[π‘Ž,𝑏]⧡𝒰2=π‘šξ“π‘–=1πœ’ξ‚€π’°βˆ©π’°1𝑖π‘₯1𝑖+π‘šξ“π‘–=1πœ’ξ‚ξ‚€ξ‚€[π‘Ž,𝑏]β§΅π’°βˆ©π’°2𝑖π‘₯2𝑖,(3.3) it follows that πœ’(𝒰)𝑦1+πœ’([π‘Ž,𝑏]⧡𝒰)𝑦2∈decΞ¦. Hence, the set decΞ¦ is decomposable.

Remark 3.3. Note that even if a set Ξ¦βŠ‚π‹π‘›1[π‘Ž,𝑏] is bounded, the set decΞ¦ is not necessarily bounded. For example, let us check that 𝐡dec𝐋𝑛𝑝[π‘Ž,𝑏]ξ‚„[0,1]=𝐋𝑛𝑝[π‘Ž,𝑏]π‘βˆˆ[1,∞).(3.4) Indeed, let π‘§βˆˆπ‹π‘›π‘[π‘Ž,𝑏] and 𝑒𝑖, 𝑖=1,2,…,π‘š, be measurable sets with the following properties: π‘’π‘–βˆ©π‘’π‘—=βˆ… if 𝑖≠𝑗, 𝑖,𝑗=1,2,…,π‘š, β‹ƒπ‘šπ‘–=1𝑒𝑖=[π‘Ž,𝑏]; for each 𝑖=1,2,…,π‘š, the inequality ξ€œπ‘’π‘–||||||𝑧(𝑠)𝑝𝑑𝑠<1(3.5) holds. Then 𝑧𝑖=πœ’(𝑒𝑖)π‘§βˆˆπ΅π‹π‘›π‘[π‘Ž,𝑏][0,1], 𝑖=1,2,…,π‘š, and 𝑒𝑧=πœ’1𝑧1𝑒+πœ’2𝑧2𝑒+β‹―+πœ’π‘šξ‚π‘§π‘š.(3.6) Therefore, π‘§βˆˆdec[𝐡𝐋𝑛𝑝[π‘Ž,𝑏][0,1]] and consequently, the equality (3.4) holds.

Remark 3.4. From (3.4), it follows that if a set Ξ¦βŠ‚π‹π‘›1[π‘Ž,𝑏] is relatively compact in the weak topology of 𝐋𝑛1[π‘Ž,𝑏], then the set decΞ¦ does not necessarily possess this property.

Remark 3.5. Note that if a set is convex in 𝐋𝑛1[π‘Ž,𝑏], then this set is not necessarily decomposable. The ball 𝐡𝐋𝑛1[π‘Ž,𝑏][0,1] is an example of such a set.

Remark 3.6. If a set Ξ¦βŠ‚π‹π‘›1[π‘Ž,𝑏] is integrally bounded, then by Lemma 2.2, for the set decΦ∈Π[𝐋𝑛1[π‘Ž,𝑏]], there exists a measurable and integrally bounded mapping 𝐹decΦ∢[π‘Ž,𝑏]β†’comp[𝑅𝑛] such that 𝐹decΞ¦=𝑆decΦ(β‹…).(3.7)

Lemma 3.7. If a set Ξ¦βŠ‚π‹π‘›1[π‘Ž,𝑏] is decomposable, then decΞ¦=Ξ¦.

Proof. Evidently, Ξ¦βŠ‚decΞ¦. We claim that decΞ¦βŠ‚Ξ¦. The proof is made by induction over π‘š. By the definition of the switching convexity, any expression (3.1) including two elements π‘₯1,π‘₯2∈Φ and two measurable sets 𝒰1,𝒰2βŠ‚[π‘Ž,𝑏] belongs to Ξ¦.
Suppose now that for π‘š=π‘˜, the combination of the form (3.1) belongs to Ξ¦. Let π‘₯1,π‘₯2,…,π‘₯π‘š+1∈Φ and let 𝒰1,𝒰2,…,π’°π‘š+1βŠ‚[π‘Ž,𝑏] be disjoint measurable sets such that ⋃[π‘Ž,𝑏]=π‘š+1𝑖=1𝒰𝑖. Let 𝒰𝑧=πœ’2βˆͺ𝒰1π‘₯2𝒰+πœ’3π‘₯3𝒰+β‹―+πœ’π‘š+1π‘₯π‘š+1.(3.8) By the inductive assumption, π‘§βˆˆΞ¦ and therefore πœ’(𝒰1)π‘₯1+πœ’([π‘Ž,𝑏]⧡𝒰1)π‘§βˆˆΞ¦. Since πœ’ξ‚€[π‘Ž,𝑏]⧡𝒰1𝒰𝑧=πœ’2π‘₯2𝒰+πœ’3π‘₯3𝒰+β‹―+πœ’π‘š+1π‘₯π‘š+1,(3.9) we have that πœ’ξ‚€π’°1π‘₯1𝒰+πœ’2π‘₯2𝒰+β‹―+πœ’π‘š+1π‘₯π‘š+1∈Φ.(3.10) Hence decΞ¦βŠ‚Ξ¦. This concludes the proof.

Corollary 3.8. If Ξ¦βŠ‚π‹π‘›1[π‘Ž,𝑏], then the set decΞ¦ is the minimal set which is decomposable and which contains Ξ¦.

Proof. Consider any set π‘ˆβŠ‚π‹π‘›1[π‘Ž,𝑏] which is decomposable and which satisfies Ξ¦βŠ‚π‘ˆ. Then, by Lemma 3.7, we have Ξ¦βŠ‚decΞ¦βŠ‚decπ‘ˆ=π‘ˆ.

Lemma 3.9. If a set Ξ¦βŠ‚π‹π‘›1[π‘Ž,𝑏] is convex, then so is the set decΞ¦βˆˆπ‹π‘›1[π‘Ž,𝑏].

Proof. Let 𝑦1,𝑦2∈decΞ¦ be given by the formula (3.2). It follows from the convexity of the set Ξ¦βŠ‚π‹π‘›1[π‘Ž,𝑏] and the equality πœ†π‘¦1+(1βˆ’πœ†)𝑦2=π‘šξ“π‘–,𝑗=1πœ’ξ‚€π’°1π‘–βˆ©π’°2π‘—ξ‚ξ‚€πœ†π‘₯1𝑖+(1βˆ’πœ†)π‘₯2𝑗(3.11) that πœ†π‘¦1+(1βˆ’πœ†)𝑦2∈decΞ¦ for any πœ†βˆˆ[0,1]. Thus, the set decΞ¦ is convex.

Similar to the definition of the convex hull in a normed space, the set decΦ will, in the sequel, be called the decomposable hull of the set Φin the space of integrable functions, or simply the decomposable hull of the set Φ. Likewise, decΦ is addressed as the closed decomposable hull of the set Φ.

Remark 3.10. If Ξ¦βˆˆπ‘„[𝐋𝑛1[π‘Ž,𝑏]], then the closed decomposable hull of the set Ξ¦ (the set decΞ¦) can be constructed as described in Remark 3.6. To do it, one needs a measurable and integrally bounded (see Remark 3.6) mapping 𝐹decΦ∢[π‘Ž,𝑏]β†’comp[ℝ𝑛] that satisfies (3.7). Note that finding this mapping 𝐹decΞ¦ is easier than constructing the set decΞ¦. At the same time, when one studies the metrical relations between the sets Ξ¦1,Ξ¦2βŠ‚π‹π‘›1[π‘Ž,𝑏] and their decomposable hulls (see Lemma 3.12), it is more convenient to use Definition 3.1.

Lemma 3.11. Let π‘£βˆˆπ‹π‘›1(𝒰)(π’°βŠ‚[π‘Ž,𝑏]) and let a set Ξ¦βŠ‚π‹π‘›1[π‘Ž,𝑏] be decomposable. Then for any disjoint measurable sets 𝒰1,𝒰2βŠ‚π’° such that 𝒰1βˆͺ𝒰2=𝒰, one has πœŒπ‹π‘›1(𝒰)[𝑣;Ξ¦]=πœŒπ‹π‘›1(𝒰1)[𝑣;Ξ¦]+πœŒπ‹π‘›1(𝒰2)[𝑣;Ξ¦].(3.12)

Proof. Indeed, let πœ€>0 and π‘¦βˆˆΞ¦ satisfy β€–π‘£βˆ’π‘¦β€–π‹π‘›1(𝒰)<πœŒπ‹π‘›1(𝒰)[𝑣;Ξ¦]+πœ€. It follows from this estimate that πœŒπ‹π‘›1(𝒰1)[𝑣;Ξ¦]+πœŒπ‹π‘›1(𝒰2)β€–β€–β€–β€–[𝑣;Ξ¦]β‰€π‘£βˆ’π‘¦π‹π‘›1(𝒰1)+β€–β€–β€–β€–π‘£βˆ’π‘¦π‹π‘›1(𝒰2)<πœŒπ‹π‘›1(𝒰)[𝑣;Ξ¦]+πœ€.(3.13) This yields πœŒπ‹π‘›1(𝒰1)[𝑣;Ξ¦]+πœŒπ‹π‘›1(𝒰2)[𝑣;Ξ¦]β‰€πœŒπ‹π‘›1(𝒰)[𝑣;Ξ¦].(3.14)
Further, let us show that the opposite inequality is valid. Let π‘¦π‘–βˆˆΞ¦|𝒰𝑖, 𝑖=1,2, where Ξ¦|𝒰𝑖 is the set of of all mappings from Ξ¦, restricted to 𝒰𝑖, 𝑖=1,2, and suppose that the functions 𝑦𝑖, 𝑖=1,2, satisfy β€–β€–π‘£βˆ’π‘¦π‘–β€–β€–π‹π‘›1(𝒰𝑖)<πœŒπ‹π‘›1(𝒰𝑖)πœ€[𝑣;Ξ¦]+2,𝑖=1,2.(3.15) Since the set Ξ¦ is decomposable, it follows that the map π‘¦βˆΆπ’°β†’β„ defined by 𝑦𝑦(𝑑)=1(𝑑)ifπ‘‘βˆˆπ’°1,𝑦2(𝑑)ifπ‘‘βˆˆπ’°2(3.16) belongs to the set Ξ¦|𝒰. By (3.15), we have πœŒπ‹π‘›1(𝒰)β€–β€–β€–β€–[𝑣;Ξ¦]β‰€π‘£βˆ’π‘¦π‹π‘›1(𝒰)<πœŒπ‹π‘›1(𝒰1)[𝑣;Ξ¦]+πœŒπ‹π‘›1(𝒰2)[𝑣;Ξ¦]+πœ€.(3.17) This implies that πœŒπ‹π‘›1(𝒰)[𝑣;Ξ¦]β‰€πœŒπ‹π‘›1(𝒰1)[𝑣;Ξ¦]+πœŒπ‹π‘›1(𝒰2)[𝑣;Ξ¦].(3.18) Comparing (3.14) and (3.18), we obtain (3.12).

Lemma 3.12. If Ξ¦1,Ξ¦2βˆˆπ‘„[𝐋𝑛1[π‘Ž,𝑏]] and there exists a function πœ”βˆˆπ‹1+[π‘Ž,𝑏] such that β„Ž+𝐋𝑛1(𝒰)Φ1;Ξ¦2ξ‚„β‰€ξ€œπ’°πœ”(𝑠)𝑑𝑠(3.19) for any measurable set π’°βŠ‚[π‘Ž,𝑏], then β„Ž+𝐋𝑛1(𝒰)decΞ¦1;decΞ¦2ξ‚„β‰€ξ€œπ’°πœ”(𝑠)𝑑𝑠(3.20) for any measurable set π’°βŠ‚[π‘Ž,𝑏].

Proof. Let π’°βŠ‚[π‘Ž,𝑏] be a measurable set, πœ‡(𝒰)>0. Let π‘§βˆˆdecΞ¦1 and π‘§π‘–βˆˆΞ¦1, 𝑖=1,2,…,π‘š. Suppose also that the functions 𝑧𝑖 and disjoint measurable sets ξ‚π‘’π‘–βŠ‚[π‘Ž,𝑏], 𝑖=1,2,…,π‘š, such that ⋃[π‘Ž,𝑏]=π‘šπ‘–=1𝑒𝑖, satisfy the equality 𝑧=πœ’ξ‚π‘’1𝑧1ξ‚€+πœ’ξ‚π‘’2𝑧2ξ‚€+β‹―+πœ’ξ‚‹π‘’π‘šξ‚π‘§π‘š.(3.21)
Further, by 𝑧,𝑧𝑖, 𝑖=1,2,…,π‘š, we denote the restrictions of these functions to 𝒰 and put 𝑒𝑖=ξ‚π‘’π‘–βˆ©π’°, 𝑖=1,2,…,π‘š.
From (3.21) and Lemma 3.11, it follows that πœŒπ‹π‘›1(𝒰)𝑧;decΞ¦2ξ‚„=π‘šξ“π‘–=1πœŒπ‹π‘›1(𝑒𝑖)𝑧𝑖;decΞ¦2ξ‚„β‰€π‘šξ“π‘–=1πœŒπ‹π‘›1(𝑒𝑖)𝑧𝑖;Ξ¦2ξ‚„.(3.22)
From (3.19), we obtain that πœŒπ‹π‘›1(𝑒𝑖)𝑧𝑖;Ξ¦2ξ‚„β‰€ξ€œπ‘’π‘–πœ”(𝑠)𝑑𝑠(3.23) for each 𝑖=1,2,…,π‘š.
Therefore, (3.22) and (3.23) imply πœŒπ‹π‘›1(𝒰)𝑧;decΞ¦2ξ‚„β‰€ξ€œπ’°πœ”(𝑠)𝑑𝑠.(3.24) Since (3.24) holds for any π‘§βˆˆdecΞ¦1, it follows from (3.24) that (3.20) holds as well.

Remark 3.13. Note that the function πœ”βˆˆπ‹1+[π‘Ž,𝑏] (see (3.19)) provides a uniform with respect to measurable sets π’°βŠ‚[π‘Ž,𝑏] estimate for the Hausdorff semideviation of the set Ξ¦1 from the set Ξ¦2.

Remark 3.14. The inequality (3.20) holds true even if the set decΦ𝑖 is replaced with its closure decΦ𝑖, 𝑖=1,2.

We say that a multivalued mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] is integrally bounded on a set πΎβŠ‚π‚π‘›[π‘Ž,𝑏] if the image Ξ¦(𝐾) is integrally bounded.

Let Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]]. We introduce an operator ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] by the formula Φ(π‘₯)=decΞ¦(π‘₯).(3.25)

Note that even if a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] is continuous, the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25) may be discontinuous. To illustrate this, let us consider an example.

Example 3.15. We define an integrable function πœ‘βˆΆ[0,2]Γ—[0,1]Γ—[0,2]→ℝ1 by ⎧βŽͺβŽͺ⎨βŽͺβŽͺβŽ©πœ‘(π‘₯,π‘Ÿ)(𝑑)=1ifπ‘‘βˆˆ[π‘₯,π‘₯+π‘Ÿ]∩[0,2],π‘Ÿβ‰ 0,0ifπ‘‘βˆˆ[π‘₯,π‘₯+π‘Ÿ]∩[0,2],π‘Ÿβ‰ 0,0ifπ‘Ÿ=0.(3.26)
We also define a multivalued mapping Φ∢[0,1]→𝑄[𝐿11[0,2]] by the formula ⎧βŽͺ⎨βŽͺ⎩Φ(π‘Ÿ)=π‘₯∈[0,2]πœ‘(π‘₯,π‘Ÿ)ifπ‘Ÿβ‰ 0,0ifπ‘Ÿ=0.(3.27)
Note that β„ŽπΏ11[0,2]ξ‚ƒΞ¦ξ‚€π‘Ÿ1ξ‚ξ‚€π‘Ÿ;Ξ¦2=|||π‘Ÿξ‚ξ‚„1βˆ’π‘Ÿ2|||(3.28) for any π‘Ÿ1,π‘Ÿ2∈[0,1], but at the same time, β„ŽπΏ11ξ€Ί0,2]Φ(0);Ξ¦(π‘Ÿ)=2(3.29) for any π‘Ÿβˆˆ(0,1].

Using Lemma 3.12, we obtain the following continuity conditions for the operator ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25).

Definition 3.16. Let π‘ˆβŠ‚πΆπ‘›[π‘Ž,𝑏]. One says that a mapping π‘ƒβˆΆπ‘ˆΓ—π‘ˆβ†’πΏ1+[π‘Ž,𝑏] is symmetric on the set π‘ˆ if 𝑃(π‘₯,𝑦)=𝑃(𝑦,π‘₯) for any π‘₯,π‘¦βˆˆπ‘ˆ. One says that a mapping π‘ƒβˆΆπ‘ˆΓ—π‘ˆβ†’πΏ1+[π‘Ž,𝑏] is continuous in the second variable at a point (π‘₯,π‘₯) belonging to the diagonal of π‘ˆΓ—π‘ˆ if for any sequence π‘¦π‘–βˆˆπ‘ˆ such that 𝑦𝑖→π‘₯ as π‘–β†’βˆž it holds that 𝑃(π‘₯,π‘₯)=limπ‘–β†’βˆžπ‘ƒ(π‘₯,𝑦𝑖). One says that a mapping π‘ƒβˆΆπ‘ˆΓ—π‘ˆβ†’πΏ1+[π‘Ž,𝑏] is continuous in the second variable on the diagonal of π‘ˆΓ—π‘ˆ if 𝑃 is continuous in the second variable at each point of this diagonal. Continuity in the fist variable is defined similarly.

Definition 3.17. Let π‘ˆβŠ‚πΆπ‘›[π‘Ž,𝑏]. Suppose also that 𝑃(π‘₯,π‘₯)=0 for any π‘₯βˆˆπ‘ˆ. One says that a mapping π‘ƒβˆΆπ‘ˆΓ—π‘ˆβ†’πΏ1+[π‘Ž,𝑏] has property π’œ on the set π‘ˆ if it is continuous in the second variable on the diagonal of π‘ˆΓ—π‘ˆ; it has property ℬ on the set π‘ˆ if it is continuous in the first variable on the diagonal of π‘ˆΓ—π‘ˆ; it has property π’ž on the set π‘ˆ if it is continuous on the diagonal of π‘ˆΓ—π‘ˆ and symmetric on the set π‘ˆ.

Theorem 3.18. Let π‘ˆβŠ‚πΆπ‘›[π‘Ž,𝑏]. Suppose also that for a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] there exists a mapping π‘ƒβˆΆπ‘ˆΓ—π‘ˆβ†’πΏ1+[π‘Ž,𝑏] such that β„Ž+𝐿𝑛1(𝒰)≀‖‖‖‖Φ(π‘₯),Ξ¦(𝑦)𝑃(π‘₯,𝑦)𝐿11(𝒰)(3.30) for any π‘₯,π‘¦βˆˆπ‘ˆ and any measurable set π’°βŠ‚[π‘Ž,𝑏]. Then for the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25), the inequality (3.30), where Φ(β‹…)≑Φ(β‹…), is satisfied as well as for any π‘₯,π‘¦βˆˆπ‘ˆ and any measurable set π’°βŠ‚[π‘Ž,𝑏].

Corollary 3.19. If the mapping π‘ƒβˆΆπ‘ˆΓ—π‘ˆβ†’πΏ1+[π‘Ž,𝑏] in Theorem 3.18 has property π’œ (resp., ℬ, π’ž) on the set π‘ˆβŠ‚πΆπ‘›[π‘Ž,𝑏], then the operator ξ‚Ξ¦βˆΆπΆπ‘›[π‘Ž,𝑏]β†’Ξ [𝐿𝑛1[π‘Ž,𝑏]] given by (3.25) is Hausdorff lower semicontinuous (resp., Hausdorff upper semicontinuous, Hausdorff continuous) on the set π‘ˆβŠ‚πΆπ‘›[π‘Ž,𝑏].

We say that the mapping π‘ƒβˆΆπ‘ˆΓ—π‘ˆβ†’πΏ1+[π‘Ž,𝑏] satisfying the inequality (3.30) for any measurable set π’°βŠ‚[π‘Ž,𝑏] is a majorant mapping for Ξ¦βˆΆπΆπ‘›[π‘Ž,𝑏]→𝑄[𝐿𝑛1[π‘Ž,𝑏]] on the set π‘ˆ.

Let a mapping πΉπ‘–βˆΆ[π‘Ž,𝑏]×ℝ𝑛→comp[ℝ𝑛], 𝑖=1,2, be measurable as a composite function for every π‘₯βˆˆπΆπ‘›[π‘Ž,𝑏]. Let also 𝐹𝑖 be integrally bounded for every bounded set πΎβŠ‚β„π‘›. Consider a mapping β„³βˆΆπΆπ‘›[π‘Ž,𝑏]→𝑄[𝐿𝑛1[π‘Ž,𝑏]] given by β„³(π‘₯)=𝒩1(π‘₯)βˆͺ𝒩2(π‘₯),(3.31) where the mapping π’©π‘–βˆΆπΆπ‘›[π‘Ž,𝑏]β†’Ξ [𝐿𝑛1[π‘Ž,𝑏]], 𝑖=1,2, is the Nemytskii operator generated by the mapping πΉπ‘–βˆΆ[π‘Ž,𝑏]×ℝ𝑛→comp[ℝ𝑛], 𝑖=1,2. For the operator β„³βˆΆπΆπ‘›[π‘Ž,𝑏]→𝑄[𝐿𝑛1[π‘Ž,𝑏]] given by (3.31), the majorant mapping ξ‚π‘ƒβˆΆπΆπ‘›[π‘Ž,𝑏]×𝐢𝑛[π‘Ž,𝑏]→𝐿1+[π‘Ž,𝑏] can be defined as ξ‚ξ‚†β„Žπ‘ƒ(π‘₯,𝑦)(𝑑)=max+𝐹1𝑑,π‘₯(𝑑);𝐹1𝑑,𝑦(𝑑);β„Ž+𝐹2𝑑,π‘₯(𝑑);𝐹2𝑑,𝑦(𝑑).(3.32)

It follows from Theorem 3.18 that the operator 𝑃(β‹…,β‹…) given by (3.32) is also a majorant mapping for the mapping ξ‚‹β„³βˆΆπΆπ‘›[π‘Ž,𝑏]β†’Ξ [𝐿𝑛1[π‘Ž,𝑏]] given by (3.25), where Ξ¦(β‹…)≑ℳ(β‹…). If the mapping πΉπ‘–βˆΆ[π‘Ž,𝑏]×ℝ𝑛→comp[ℝ𝑛], 𝑖=1,2, is Hausdorff lower semicontinuous (resp., Hausdorff upper semicontinuous and Hausdorff continuous) in the second variable, then by Corollary 3.19, the mapping ξ‚‹β„³βˆΆπΆπ‘›[π‘Ž,𝑏]β†’Ξ [𝐿𝑛1[π‘Ž,𝑏]] given by (3.25) is Hausdorff lower semicontinuous (resp., Hausdorff upper semicontinuous and Hausdorff continuous).

Definition 3.20. One says that a multivalued mapping Ξ¦βˆΆπΆπ‘›[π‘Ž,𝑏]→𝑄[𝐿𝑛1[π‘Ž,𝑏]]has Property π’œ (resp., ℬ and π’ž) if for this mapping there exists a majorant mapping π‘ƒβˆΆπΆπ‘›[π‘Ž,𝑏]×𝐢𝑛[π‘Ž,𝑏]→𝐿1+[π‘Ž,𝑏] satisfying Property π’œ (resp., ℬ and π’ž).

4. Basic Properties of Generalized Solutions of Functional Differential Inclusions

Using decomposable hulls, we introduce in this section the concept of a generalized solution of a functional differential inclusion with a right-hand side which is not necessarily decomposable. Using, as mentioned in Section 3, basic topological properties of a mapping given by (3.25), we study the properties of a generalized solution of the initial value problem.

Consider the initial value problem for the functional differential inclusion Μ‡π‘₯∈Φ(π‘₯),π‘₯(π‘Ž)=π‘₯0ξ‚€π‘₯0βˆˆβ„π‘›ξ‚,(4.1) where the mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] satisfies the following condition: for every bounded set π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏], the image Ξ¦(π‘ˆ) is integrally bounded. Note that the right-hand side of the inclusion (4.1) is not necessarily decomposable. Note also that Μ‡π‘₯ in (4.1) is not treated as a derivative at a point but as an element of 𝐋𝑛1[π‘Ž,𝑏] (see [10, 23–25]). When we study such a problem, there may appear some difficulties described in the introduction. In this connection, we will introduce the concept of a generalized solution of the problem (4.1) and study the properties of this solution. Using the Nemytskii operator, which is decomposable, the initial value problem for a classical differential inclusion, that is, one without delay (see [10, 23–25]), can be reduced to (4.1).

Definition 4.1. An absolutely continuous function π‘₯∢[π‘Ž,𝑏]→ℝ𝑛 is called a generalized solution of the problem (4.1) if Μ‡π‘₯∈decΞ¦(π‘₯),π‘₯(π‘Ž)=π‘₯0ξ‚€π‘₯0βˆˆβ„π‘›ξ‚.(4.2)

Note that from Lemma 3.7, it follows that if the set Ξ¦(π‘₯) (see(4.1)) is decomposable, then a generalized solution of the problem (4.1) coincides with a classical solution.

Example 4.2. Consider an ordinary differential equation, π‘₯∈[0,1],Μ‡π‘₯=π‘˜π‘₯,π‘₯(0)=1.(4.3) Its solution is the function π‘₯=π‘’π‘˜π‘‘.
We assume that the parameter π‘˜ may take two values: 1 or 2. Then the trajectories of such a system are described by the differential inclusion Μ‡π‘₯∈Φ(𝑑)π‘₯(𝑑),π‘₯(0)=1,(4.4) where Ξ¦(𝑑) is a multivalued function with the values from the set {1,2}. Note that decΞ¦(𝑑)=Ξ¦(𝑑), that is, the set in the right-hand side of the inclusion is decomposable. In this case, a generalized solution of the inclusion coincides with a classical solution.
The latter differential inclusion describes the model that is controlled by the differential equation either with the parameter value π‘˜=1 or with the parameter value π‘˜=2. In this model, switchings from one law (equation) to another may take place any time.
In the limit case, all possible solutions fill entirely the set of all points between the graphs of the functions 𝑒𝑑 and 𝑒2𝑑.

Example 4.3. Consider a simple pendulum. It consists of a mass π‘š hanging from a string of length 𝑙 and fixed at a pivot point 𝑃. When displaced to an initial angle and released, the pendulum will swing back and forth with periodic motion. The equation of motion for the pendulum is given by ̈π‘₯=βˆ’π‘Žsinπ‘₯,(4.5) where π‘₯(𝑑) is the angular displacement at the moment 𝑑, π‘Ž=𝑔/𝑙, 𝑔 is the acceleration of gravity, and 𝑙 is the length of the string.
If the amplitude of angular displacement is small enough that the small angle approximation holds true, then the equation of motion reduces to the equation of simple harmonic motion ̈π‘₯=βˆ’π‘Žπ‘₯.(4.6) Let us now assume that the length of the string 𝑙 may change, that is, it may take an value from a finite set {𝑙1,…,π‘™π‘š}. In this case, the equation of simple harmonic motion transforms to the differential inclusion with a multivalued mapping ̈π‘₯∈Φ(π‘₯),(4.7) where ⋃Φ(π‘₯)=π‘šπ‘–=1βˆ’(𝑔/𝑙𝑖)π‘₯.
We assume that switching from one length (equation) to another may take place any time. Then the generalized solutions of the inclusion treat all available trajectories (states) corresponding to all switchings.

Definition 4.4. An operator Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] is called a Volterra-Tikhonov (or simply a Volterra) operator (see [26]) if the equality π‘₯=𝑦 on [π‘Ž,𝜏], 𝜏∈(π‘Ž,𝑏], implies (Ξ¦(π‘₯))|𝜏=(Ξ¦(𝑦))|𝜏, where (Ξ¦(𝑧))|𝜏 is the set of all functions from Ξ¦(𝑧) restricted to [π‘Ž,𝜏].

In what follows, we assume that the operator Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] (the right-hand side of the inclusion (4.1)) is a Volterra operator. This implies that the operator ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] given by (3.25) is also a Volterra operator.

Let 𝜏∈(π‘Ž,𝑏]. Let us determine the continuous mapping π‘‰πœβˆΆπ‚π‘›[π‘Ž,𝜏]→𝐂𝑛[π‘Ž,𝑏] by ξ‚€π‘‰πœπ‘₯=ξƒ―π‘₯(𝑑)ifπ‘‘βˆˆ[π‘Ž,𝜏],π‘₯(𝜏)ifπ‘‘βˆˆ(𝜏,𝑏].(4.8)

Definition 4.5. One says that an absolutely continuous function π‘₯∢[π‘Ž,𝜏]→ℝ𝑛 is a generalized solution of the problem (4.1) on the interval [π‘Ž,𝜏], 𝜏∈(π‘Ž,𝑏], if π‘₯ satisfies Μ‡π‘₯∈(decΞ¦(π‘‰πœ(π‘₯)))|𝜏 and π‘₯(π‘Ž)=π‘₯0, where the continuous mapping π‘‰πœβˆΆπ‚π‘›[π‘Ž,𝜏]→𝐂𝑛[π‘Ž,𝑏] is given by (4.8).

A function π‘₯∢[π‘Ž,𝑐)→ℝ𝑛, which is absolutely continuous on any interval [π‘Ž,𝜏]βŠ‚[π‘Ž,𝑐), π‘βˆˆ(π‘Ž,𝑏], is called a generalized solution of the problem (4.1) on the interval [π‘Ž,𝑐) if for each 𝜏∈(π‘Ž,𝑐) the restriction of π‘₯ to [π‘Ž,𝜏] is a generalized solution of the problem (4.1) on the interval [π‘Ž,𝜏].

A generalized solution π‘₯∢[π‘Ž,𝑐)→ℝ𝑛 of the problem (4.1) on the interval [π‘Ž,𝑐) is said to be nonextendable if there is no generalized solution 𝑦 of the problem (4.1) on any larger interval [π‘Ž,𝜏] (here, 𝜏∈(𝑐,𝑏] if 𝑐<𝑏 and 𝜏=𝑏 if 𝑐=𝑏) such that π‘₯(𝑑)=𝑦(𝑑) for each π‘‘βˆˆ[π‘Ž,𝑐).

In Theorems 4.6–4.12 below, we assume that the mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property π’œ. Due to Corollary 3.19, the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25) is lower semicontinuous. Due to [27, 28], the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] admits a continuous selection. Therefore, the following propositions on local solutions of the problem (4.1) are straightforward.

Theorem 4.6. There exists 𝜏∈(π‘Ž,𝑏] such that a generalized solution of the problem (4.1) is defined on the interval [π‘Ž,𝜏].

Theorem 4.7. A generalized solution π‘₯∢[π‘Ž,𝑐)→ℝ𝑛 of the problem (4.1) admits a continuation if and only if  limπ‘‘β†’π‘βˆ’0|π‘₯(𝑑)|<∞.

Theorem 4.8. If 𝑦 is a generalized solution of the problem (4.1) on the interval [π‘Ž,𝜏], 𝜏∈(π‘Ž,𝑏), then there exists a nonextendable solution π‘₯ of the problem (4.1) defined on the interval [π‘Ž,𝑐)(π‘βˆˆ(𝜏,𝑏]), or on the entire interval [π‘Ž,𝑏], such that π‘₯(𝑑)=𝑦(𝑑) for each π‘‘βˆˆ[π‘Ž,𝜏].

Let 𝐻(π‘₯0,𝜏) be the set of all generalized solutions of the problem (4.1) on the interval [π‘Ž,𝜏](𝜏∈(π‘Ž,𝑏]).

We say that generalized solutions of the problem (4.1) admit a uniform a priori estimate if there exists a number π‘Ÿ>0 such that for every 𝜏∈(π‘Ž,𝑏], there is no generalized solution π‘¦βˆˆπ»(π‘₯0,𝜏) satisfying ‖𝑦‖𝐂𝑛[π‘Ž,𝜏]>π‘Ÿ.

Theorems 4.6–4.8 yield the following result.

Theorem 4.9. Let the generalized solutions of the problem (4.1) admit a uniform a priori estimate. Then 𝐻(π‘₯0,𝜏)β‰ βˆ… for any 𝜏∈(π‘Ž,𝑏] and there exists a number π‘Ÿ>0 such that ‖𝑦‖𝐂𝑛[π‘Ž,𝜏]β‰€π‘Ÿ for any 𝜏∈(π‘Ž,𝑏], π‘¦βˆˆπ»(π‘₯0,𝜏).

Definition 4.10. One says that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property Ξ“1 if there exists an isotonic continuous operator Ξ“1βˆΆπ‚1+[π‘Ž,𝑏]→𝐋1+[π‘Ž,𝑏] satisfying the following conditions:(i)for any function π‘₯βˆˆπ‚π‘›[π‘Ž,𝑏] and any measurable set π’°βŠ‚[π‘Ž,𝑏], one hasβ€–β€–β€–β€–Ξ¦(π‘₯)𝐋𝑛1(𝒰)≀‖‖Γ1β€–β€–(𝑍π‘₯)𝐋11(𝒰),(4.9) where the continuous mapping π‘βˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂1+[π‘Ž,𝑏] is given by ||||||(𝑍π‘₯)(𝑑)=π‘₯(𝑑);(4.10)(ii)the local solutions of the problem ̇𝑦=Ξ“1|||π‘₯(𝑦),𝑦(π‘Ž)=0|||(4.11) admit a uniform a priori estimate.

Lemma 4.11. Suppose that a multivalued mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property Ξ“1. Then so does the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25).

Proof. It suffices to show that β€–β€–β€–β€–decΞ¦(π‘₯)𝐋𝑛1(𝒰)≀‖‖Γ1β€–β€–(𝑍π‘₯)𝐋11(𝒰)(4.12) for any function π‘₯βˆˆπ‚π‘›[π‘Ž,𝑏] and any measurable set π’°βŠ‚[π‘Ž,𝑏]. Indeed, let a function π‘¦βˆˆdecΞ¦(π‘₯) be as in (3.1). By (4.9), ξ€œπ’°π‘–βˆ©π’°|||π‘₯𝑖|||β€–β€–Ξ“(𝑠)𝑑𝑠≀1β€–β€–(𝑍π‘₯)𝐋11(π’°π‘–βˆ©π’°)(4.13) for each 𝑖=1,2,…,π‘š. Hence, we have that for the function π‘¦βˆˆdecΞ¦(π‘₯), the estimate ξ€œπ’°||||||‖‖Γ𝑦(𝑠)𝑑𝑠≀1β€–β€–(𝑍π‘₯)𝐋11(𝒰)(4.14) is satisfied as well. This gives the inequality (4.12). The proof is complete.

Let a continuous operator Ξ˜βˆΆπƒπ‘›[π‘Ž,𝑏]→𝐂1+[π‘Ž,𝑏] be given by ||||||+ξ€œ(Ξ˜π‘§)(𝑑)=𝑧(π‘Ž)π‘‘π‘Ž||||||̇𝑧(𝑠)𝑑𝑠.(4.15)

Theorem 4.12. Suppose that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property Ξ“1. Then the set 𝐻(π‘₯0,𝜏) is nonempty for any 𝜏∈(π‘Ž,𝑏] and there exists a number π‘Ÿ>0 such that ‖𝑦‖𝐂𝑛[π‘Ž,𝜏]β‰€π‘Ÿ for any π‘¦βˆˆπ»(π‘₯0,𝜏), 𝜏∈(π‘Ž,𝑏].

Proof. Indeed, let π‘₯∈𝐻(π‘₯0,𝜏) (𝜏∈(π‘Ž,𝑏]). From Lemma 4.11, it follows that for any π‘‘βˆˆ[π‘Ž,𝜏], |||π‘₯(Θπ‘₯)(𝑑)≀0|||+ξ€œπ‘‘π‘Žξ‚€Ξ“1|||π‘₯(𝑍π‘₯)(𝑠)𝑑𝑠≀0|||+ξ€œπ‘‘π‘Žξ‚€Ξ“1(Θπ‘₯)(𝑠)𝑑𝑠,(4.16) where the function Θπ‘₯ is given by (4.15). Due to the theorem on integral inequalities for an isotonic operator (see [29]), this implies that we actually have Θπ‘₯β‰€πœ‰0, where πœ‰0 is the upper solution of the problem (4.11). Thus, there is no π‘₯∈𝐻(π‘₯0,𝜏) satisfying the inequality β€–π‘₯‖𝐂𝑛[π‘Ž,𝜏]>β€–πœ‰0‖𝐂1[π‘Ž,𝑏]. From this, it follows that the set of all local generalized solutions of the problem (4.1) admits a uniform a priori estimate. Applying Theorem 4.9 completes the proof.

Let a linear continuous operator Ξ›βˆΆπ‹π‘›1[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] be given by ξ€œ(Λ𝑧)(𝑑)=π‘‘π‘Žπ‘§(𝑠)𝑑𝑠,π‘‘βˆˆ[π‘Ž,𝑏].(4.17) We say that Ξ›βˆΆπ‹π‘›1[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] is the operator of integration.

Theorem 4.13. Let the set of all local generalized solutions of the problem (4.1) admit a uniform a priori estimate. Suppose also that Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property π’ž. Then for any function π‘£βˆˆπ‹π‘›1[π‘Ž,𝑏] and any πœ€>0, there exists a generalized solution π‘₯βˆˆπƒπ‘›[π‘Ž,𝑏] of the problem (4.1) such that β€–β€–β€–β€–Μ‡π‘₯βˆ’π‘£π‹π‘›1(𝒰)β‰€πœŒπ‹π‘›1(𝒰)𝑣,ξ‚„decΞ¦(π‘₯)+πœ€πœ‡(𝒰)(4.18) for any measurable set π’°βŠ‚[π‘Ž,𝑏].
If Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(𝑄[𝐋𝑛1[π‘Ž,𝑏]]), then the theorem is also valid for πœ€=0.

Proof. Let Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] have Property π’ž. Then by Corollary 3.19, the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25) is continuous. Therefore (see [30–32]), given a number πœ€>0 and a function π‘£βˆˆπ‹π‘›1[π‘Ž,𝑏], there exists a continuous mapping πœ‘βˆΆπ‚π‘›[π‘Ž,𝑏]→𝐋𝑛1[π‘Ž,𝑏] satisfying ξ‚πœ‘(𝑦)∈Φ(𝑦) and β€–β€–β€–β€–πœ‘(𝑦)βˆ’π‘£π‹π‘›1(𝒰)β‰€πœŒπ‹π‘›1(𝒰)𝑣,ξ‚„decΞ¦(𝑦)+πœ€πœ‡(𝒰)(4.19) for any π‘¦βˆˆπ‚π‘›[π‘Ž,𝑏] and any measurable set π’°βŠ‚[π‘Ž,𝑏]. It follows from Theorem 4.9 that 𝐻(π‘₯0,𝜏)β‰ βˆ… for any 𝜏∈(π‘Ž,𝑏], and that there exists a number π‘Ÿ>0 such that ‖𝑦‖𝐂𝑛[π‘Ž,𝜏]β‰€π‘Ÿ for each 𝜏∈(π‘Ž,𝑏], π‘¦βˆˆπ»(π‘₯0,𝜏). Now, we show that there exists π‘₯∈𝐻(π‘₯0,𝑏) satisfying (4.18). Consider the problem Μ‡π‘₯βˆˆξ‚€π‘ŠdecΞ¦π‘Ÿξ‚(π‘₯),π‘₯(π‘Ž)=π‘₯0ξ‚€π‘₯0βˆˆβ„π‘›ξ‚,(4.20) where the continuous mapping π‘Šπ‘ŸβˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] is given by ξ‚€π‘Šπ‘Ÿπ‘₯ξ‚βŽ§βŽͺβŽͺ⎨βŽͺβŽͺ⎩||||||(𝑑)=π‘₯(𝑑)ifπ‘₯(𝑑)β‰€π‘Ÿ+2,π‘Ÿ+2||||||||||||π‘₯(𝑑)π‘₯(𝑑)ifπ‘₯(𝑑)>π‘Ÿ+2.(4.21) We denote by 𝐻(π‘Š) the set of all solutions of the problem (4.20). Let us show that 𝐻(π‘Š)=𝐻(π‘₯0,𝑏). It follows from the definition of the mapping π‘Šπ‘ŸβˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] (see (4.21)) that 𝐻(π‘₯0,𝑏)βŠ‚π»(π‘Š). Let us prove that 𝐻(π‘Š)βŠ‚π»(π‘₯0,𝑏). Assume the converse. Then there exists π‘¦βˆˆπ»(π‘Š) such that ‖𝑦‖𝐂𝑛[π‘Ž,𝑏]>π‘Ÿ+2. Since 𝑦(π‘Ž)=π‘₯0, we have |𝑦(π‘Ž)|<π‘Ÿ+2. This implies that there exists a number 𝜏∈(π‘Ž,𝑏] such that ‖𝑦|πœβ€–π‚π‘›[π‘Ž,𝜏]=π‘Ÿ+1 (𝑦|𝜏 is the restriction of the function 𝑦 to [π‘Ž,𝜏]). By (4.21), we have 𝑦|𝜏∈𝐻(π‘₯0,𝜏). This contradicts to the definition of the number π‘Ÿ. Hence, 𝐻(π‘₯0,𝑏)=𝐻(π‘Š). Consider a continuous operator Ξ¨βˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] given by Ξ¨(π‘₯)=π‘₯0ξ‚€π‘Š+Ξ›πœ‘π‘Ÿξ‚(π‘₯),(4.22) where the operator Ξ›βˆΆπ‹π‘›1[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] is the operator of integration defined by (4.17), and πœ‘βˆΆπ‚π‘›[π‘Ž,𝑏]→𝐋𝑛1[π‘Ž,𝑏] is a continuous selection of the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25). The function πœ‘ ia also assumed to satisfy (4.19). Since the operator π‘Šπ‘ŸβˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] is bounded, we obtain that the image Ξ¨(𝐂𝑛[π‘Ž,𝑏]) is a relatively compact subset of 𝐂𝑛[π‘Ž,𝑏]. Hence, the set π‘ˆ=coΞ¨(𝐂𝑛[π‘Ž,𝑏]) is a convex compact set. Since the operator Ξ¨βˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] given by (4.22) takes the set π‘ˆ into itself, we have, by Schauder theorem, that the mapping Ξ¨(β‹…) has a fixed point. This fixed point π‘₯ is the solution of the problem (4.20). It follows from the above equality 𝐻(π‘Š)=𝐻(π‘₯0,𝑏) that this solution π‘₯∈𝐻(π‘Š) is a generalized solution of the problem (4.1). Since Μ‡π‘₯=πœ‘(π‘₯), we see that (4.19) implies (4.18).

Let us prove the second statement of the theorem. Let Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(𝑄[𝐋𝑛1[π‘Ž,𝑏]]). Suppose also that Ξ¦ has Property π’ž. Then by Lemma 3.9, ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(Ξ [𝐋𝑛1[π‘Ž,𝑏]]). Hence for each 𝑖=1,2,…, there exists a generalized solution π‘₯π‘–βˆˆπƒπ‘›[π‘Ž,𝑏] of the problem (4.1) such that for any measurable set π’°βŠ‚[π‘Ž,𝑏], the inequality (4.18) is valid for Μ‡π‘₯=Μ‡π‘₯𝑖 and πœ€=1/𝑖. Since the set 𝐻(π‘₯0,𝑏) is bounded, we see that the sequence {Μ‡π‘₯𝑖} is weakly compact in 𝐋𝑛1[π‘Ž,𝑏]. Without loss of generality, it can be assumed that Μ‡π‘₯𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] and π‘₯𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž. Let us show that π‘₯ is a generalized solution of the problem (4.1). In other words, we have to prove that Μ‡π‘₯∈decΞ¦(π‘₯). Assume that the functions π‘¦π‘–βˆˆdecΞ¦(π‘₯), 𝑖=1,2,…, satisfy β€–β€–π‘¦π‘–βˆ’Μ‡π‘₯𝑖‖‖𝐋𝑛1[π‘Ž,𝑏]=πœŒπ‹π‘›1[π‘Ž,𝑏]̇π‘₯𝑖;ξ‚„decΞ¦(π‘₯)(4.23) (as decΞ¦(π‘₯)∈Π[𝐋𝑛1[π‘Ž,𝑏]], these functions do exist). It follows from (4.23) that β€–β€–π‘¦π‘–βˆ’Μ‡π‘₯𝑖‖‖𝐋𝑛1[π‘Ž,𝑏]β‰€β„Žπ‹π‘›1[π‘Ž,𝑏]π‘₯decΦ𝑖;ξ‚„decΞ¦(π‘₯).(4.24) Since the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(Ξ [𝐋𝑛1[π‘Ž,𝑏]]) given by (3.25) is continuous, we obtain, by (4.24), that π‘¦π‘–βˆ’Μ‡π‘₯𝑖→0 in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž. Since Μ‡π‘₯𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž, we have that 𝑦𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž. Therefore, the convexity of the set decΞ¦(π‘₯) implies that Μ‡π‘₯∈decΞ¦(π‘₯) (see [21]). Thus, π‘₯ is a generalized solution of the problem (4.1).

Further, let us show that (4.19) holds for the solution π‘₯ and for πœ€=0. Since Μ‡π‘₯𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž, we have, by [21], that for each π‘š=1,2,…, there exist numbers 𝑖(π‘š), πœ†π‘šπ‘—β‰₯0, 𝑗=1,2,…,𝑖(π‘š), satisfying the following conditions: βˆ‘π‘–(π‘š)𝑗=1πœ†π‘šπ‘—=1; the sequence {π›½π‘š=βˆ‘π‘–(π‘š)𝑗=1πœ†π‘šπ‘—Μ‡π‘₯𝑗+π‘š} tends to Μ‡π‘₯ in 𝐋𝑛1[π‘Ž,𝑏]. Since β€–β€–β€–β€–Μ‡π‘₯βˆ’π‘£π‹π‘›1[π‘Ž,𝑏]≀‖‖̇π‘₯βˆ’π›½π‘šβ€–β€–π‹π‘›1[π‘Ž,𝑏]+𝑖(π‘š)𝑗=1πœ†π‘šπ‘—β€–β€–Μ‡π‘₯𝑗+π‘šβ€–β€–βˆ’π‘£π‹π‘›1[π‘Ž,𝑏](4.25) for each π‘š=1,2,…, it follows, due to the choice of the sequence {Μ‡π‘₯𝑖}, that β€–β€–β€–β€–Μ‡π‘₯βˆ’π‘£π‹π‘›1[π‘Ž,𝑏]≀‖‖̇π‘₯βˆ’π›½π‘šβ€–β€–π‹π‘›1[π‘Ž,𝑏]+𝑖(π‘š)𝑗=1πœ†π‘šπ‘—πœŒπ‹π‘›1[π‘Ž,𝑏]𝑣;ξ‚€π‘₯decΦ𝑗+π‘šξ‚ξ‚„+(π‘βˆ’π‘Ž)𝑖(π‘š)𝑗=1πœ†π‘šπ‘—1𝑗+π‘š(4.26) for each π‘š=1,2,….

Since limπ‘–β†’βˆžπœŒπ‹π‘›1[π‘Ž,𝑏]𝑣;ξ‚€π‘₯decΦ𝑖=πœŒπ‹π‘›1[π‘Ž,𝑏]𝑣;ξ‚„decΞ¦(π‘₯),(4.27) it follows that letting π‘šβ†’βˆž in the previous inequality, we obtain β€–β€–β€–β€–Μ‡π‘₯βˆ’π‘£π‹π‘›1[π‘Ž,𝑏]=πœŒπ‹π‘›1[π‘Ž,𝑏]𝑣;ξ‚„decΞ¦(π‘₯).(4.28) Finally, note that by the decomposability of the set decΞ¦(π‘₯), this equality holds for any measurable set π’°βŠ‚[π‘Ž,𝑏]. This completes the proof.

Theorems 4.12 and 4.13 yield the following result.

Corollary 4.14. Suppose that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Properties Ξ“1 and π’ž. Then for any function π‘£βˆˆπ‹π‘›1[π‘Ž,𝑏] and any πœ€>0, there exists a generalized solution π‘₯βˆˆπƒπ‘›[π‘Ž,𝑏] of the problem (4.1) such that (4.18) holds for any measurable set π’°βŠ‚[π‘Ž,𝑏].
If Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(𝑄[𝐋𝑛1[π‘Ž,𝑏]]), then the corollary is also valid for πœ€=0.

Remark 4.15. Consider the convex compact set π‘ˆ=coΞ¨(𝐂𝑛[π‘Ž,𝑏])βŠ‚π‚π‘›[π‘Ž,𝑏], where the mapping ξ‚Ξ¨βˆΆπ‚π‘›[π‘Ž,𝑏]β†’2𝐂𝑛[π‘Ž,𝑏] is given by Ψ(π‘₯)=π‘₯0ξ‚Ξ¦ξ‚€π‘Š+Ξ›π‘Ÿξ‚(π‘₯).(4.29) Here, the operators ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] and π‘Šπ‘ŸβˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] are determined by (3.25) and (4.21), respectively. If a number π‘Ÿ>0 is such that ‖𝑦‖𝐂𝑛[π‘Ž,𝜏]β‰€π‘Ÿ for any 𝜏∈(π‘Ž,𝑏], π‘¦βˆˆπ»(π‘₯0,𝜏), then due to the the coincidence of the sets 𝐻(π‘Š) and 𝐻(π‘₯0,𝑏) (see the proof of Theorem 4.13), 𝐻(π‘₯0,𝑏)βŠ‚π‘ˆ.

Definition 4.16. Given πœ€β‰₯0, 𝑝β‰₯0, π‘’βˆˆπ‹1+[π‘Ž,𝑏], one says that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property Ξ“2𝑒,πœ€,𝑝 if there exists an isotonic and continuous Volterra operator Ξ“2βˆΆπ‚1+[π‘Ž,𝑏]→𝐋1+[π‘Ž,𝑏] satisfying the following conditions:(i)Ξ“2(0)=0;(ii)for any functions π‘₯,π‘¦βˆˆπ‚π‘›[π‘Ž,𝑏] and any measurable set π’°βŠ‚[π‘Ž,𝑏], one has β„Žπ‹π‘›1(𝒰)≀‖‖ΓΦ(π‘₯);Ξ¦(𝑦)2‖‖𝑍(π‘₯βˆ’π‘¦)𝐋11(𝒰),(4.30) where the continuous mapping π‘βˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂1+[π‘Ž,𝑏] is determined by (4.10);(iii)the set of all local solutions of the problem ̇𝑦=𝑒+πœ€+Ξ“2(𝑦),𝑦(π‘Ž)=𝑝,(4.31) admits a uniform a priori estimate.

Given π‘¦βˆˆπƒπ‘›[π‘Ž,𝑏] and πœ˜βˆˆπ‹1+[π‘Ž,𝑏], the following estimate will be used in the sequel: πœŒπ‹π‘›1(𝒰)ξ‚ƒξ‚„β‰€ξ€œΜ‡π‘¦;Ξ¦(𝑦)π’°πœ˜(𝑠)𝑑𝑠(4.32) for each measurable set π’°βŠ‚[π‘Ž,𝑏].

Theorem 4.17. Let functions π‘¦βˆˆπƒπ‘›[π‘Ž,𝑏] and πœ˜βˆˆπ‹1+[π‘Ž,𝑏] satisfy the inequality (4.32) for each measurable set π’°βŠ‚[π‘Ž,𝑏]. Suppose that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property Ξ“2𝜘,πœ€,𝑝, where πœ€β‰₯0, 𝑝=|π‘₯0βˆ’π‘¦(π‘Ž)|, and π‘₯0 is the initial condition of the problem (4.1). Then for any generalized solution of the problem (4.1) satisfying β€–β€–β€–β€–Μ‡π‘₯βˆ’Μ‡π‘¦π‹π‘›1(𝒰)β‰€πœŒπ‹π‘›1(𝒰)̇𝑦;ξ‚„decΞ¦(π‘₯)+πœ€πœ‡(𝒰)(4.33) for any measurable set π’°βŠ‚[π‘Ž,𝑏], the following conditions are satisfied: (1)Θ(π‘₯βˆ’π‘¦)(𝑑)β‰€πœ‰(𝜘,πœ€,𝑝)(𝑑)(4.34) for each π‘‘βˆˆ[π‘Ž,𝑏], where the function πœ‰(𝜘,πœ€,𝑝)βˆˆπƒ1[π‘Ž,𝑏] is the upper solution of the problem (4.31) for 𝑒=𝜘 and 𝑝=|π‘₯0βˆ’π‘¦(π‘Ž)|, and the mapping Ξ˜βˆΆπƒπ‘›[π‘Ž,𝑏]→𝐂1+[π‘Ž,𝑏] is given by (4.15);(2)||||||ξ‚€Ξ“Μ‡π‘₯(𝑑)βˆ’Μ‡π‘¦(𝑑)β‰€πœ˜(𝑑)+πœ€+2ξ‚€πœ‰(𝜘,πœ€,𝑝)(𝑑)(4.35) for almost all π‘‘βˆˆ[π‘Ž,𝑏].

Proof. First, note that since the mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property Ξ“2𝜘,πœ€,𝑝, it follows from Theorem 3.18 that so does the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] determined by (3.25). Further, the inequality (4.33) yields that β€–β€–β€–β€–Μ‡π‘₯βˆ’Μ‡π‘¦π‹π‘›1(𝒰)β‰€πœŒπ‹π‘›1(𝒰)̇𝑦;ξ‚„decΞ¦(𝑦)+β„Žπ‹π‘›1(𝒰)decΞ¦(𝑦);ξ‚„decΞ¦(π‘₯)+πœ€πœ‡(𝒰)(4.36) for any measurable set π’°βŠ‚[π‘Ž,𝑏].
Remark 4.15 and relations (4.36), (4.32), and (4.30) imply that for any measurable set π’°βŠ‚[π‘Ž,𝑏], we obtain the inequality β€–β€–β€–β€–Μ‡π‘₯βˆ’Μ‡π‘¦π‹π‘›1(𝒰)β‰€ξ€œπ’°ξ‚€πœ˜(𝑠)+πœ€+Ξ“2𝑍(π‘₯βˆ’π‘¦)(𝑠)𝑑𝑠,(4.37) where the mapping π‘βˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂1+[π‘Ž,𝑏] is given by (4.10). It follows from this inequality that ||||||Μ‡π‘₯(𝑑)βˆ’Μ‡π‘¦(𝑑)β‰€πœ˜(𝑑)+πœ€+Ξ“2𝑍(π‘₯βˆ’π‘¦)(𝑑)(4.38) for almost all π‘‘βˆˆ[π‘Ž,𝑏]. Since 𝑍(π‘₯βˆ’π‘¦)(𝑑)β‰€Ξ˜(π‘₯βˆ’π‘¦)(𝑑) for all π‘‘βˆˆ[π‘Ž,𝑏] (see (4.10), (4.15)) and the operator Ξ“2βˆΆπ‚1+[π‘Ž,𝑏]→𝐋1+[π‘Ž,𝑏]] (see (4.38)) is isotonic, we have that ||||||=Μ‡Μ‡π‘₯(𝑑)βˆ’Μ‡π‘¦(𝑑)Θ(π‘₯βˆ’π‘¦)(𝑑)β‰€πœ˜(𝑑)+πœ€+Ξ“2ξ‚€ξ‚Ξ˜(π‘₯βˆ’π‘¦)(𝑑)(4.39) for almost all π‘‘βˆˆ[π‘Ž,𝑏]. Therefore, (4.39) and the theorem on differential inequalities with an isotonic operator (see [29]) imply (4.34) for any π‘‘βˆˆ[π‘Ž,𝑏]. The inequality (4.35) follows from (4.34) and (4.39). The proof is complete.

Theorems 4.13 and 4.17 yield the following result.

Theorem 4.18. Let functions π‘¦βˆˆπƒπ‘›[π‘Ž,𝑏] and πœ˜βˆˆπ‹1+[π‘Ž,𝑏] satisfy (4.32) for each measurable set π’°βŠ‚[π‘Ž,𝑏]. Suppose that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property Ξ“2𝜘,πœ€,𝑝, where πœ€β‰₯0, 𝑝=|π‘₯0βˆ’π‘¦(π‘Ž)|, π‘₯0 is the initial condition in the problem (4.1). Let the set of all local generalized solutions of the problem (4.1) admit a uniform a priori estimate. Then for πœ€>0, there exists a generalized solution π‘₯βˆˆπƒπ‘›[π‘Ž,𝑏] of the problem (4.1) which satisfies (4.34) and (4.35) for all π‘‘βˆˆ[π‘Ž,𝑏] and for almost all π‘‘βˆˆ[π‘Ž,𝑏], respectively.
If Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(𝑄[𝐋𝑛1[π‘Ž,𝑏]]), then the theorem is also valid for πœ€=0.

Corollary 4.19. Let functions π‘¦βˆˆπƒπ‘›[π‘Ž,𝑏] and πœ˜βˆˆπ‹1+[π‘Ž,𝑏] satisfy (4.32) for each measurable set π’°βŠ‚[π‘Ž,𝑏]. Suppose that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has properties Ξ“1 and Ξ“2𝜘,πœ€,𝑝, where πœ€β‰₯0, 𝑝=|π‘₯0βˆ’π‘¦(π‘Ž)|, π‘₯0 is the initial condition in the problem (4.1). Then for πœ€>0, there exists a generalized solution π‘₯βˆˆπƒπ‘›[π‘Ž,𝑏] of the problem (4.1) which satisfies (4.34) and (4.35) for all π‘‘βˆˆ[π‘Ž,𝑏] and for almost all π‘‘βˆˆ[π‘Ž,𝑏], respectively.
If Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(𝑄[𝐋𝑛1[π‘Ž,𝑏]]), then the corollary is also valid for πœ€=0.

Remark 4.20. It follows from the proof of Theorem 4.17 that Theorems 4.17, 4.18, and Corollary 4.19 are also valid if the functions π‘¦βˆˆπƒπ‘›[π‘Ž,𝑏] and πœ˜βˆˆπ‹1+[π‘Ž,𝑏] satisfy πœŒπ‹π‘›1(𝒰)̇𝑦;ξ‚„β‰€ξ€œdecΞ¦(𝑦)π’°πœ˜(𝑠)𝑑𝑠(4.40) for each measurable set π’°βŠ‚[π‘Ž,𝑏].

Definition 4.21. An absolutely continuous function π‘₯βˆˆπƒπ‘›[π‘Ž,𝑏] is called a generalized quasisolution of the problem (4.1) if there exists a sequence of functions π‘₯π‘–βˆˆπƒπ‘›[π‘Ž,𝑏], 𝑖=1,2,…, such that the following conditions hold:(i)π‘₯𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž;(ii)Μ‡π‘₯π‘–βˆˆdecΞ¦(π‘₯) and π‘₯𝑖(π‘Ž)=π‘₯0 for each 𝑖=1,2,….

Note that by Lemma 3.7, if the set Ξ¦(π‘₯) mentioned in Definition 4.21 is decomposable, then a generalized quasisolution coincides with a quasisolution defined in [9, 33], where Ξ¦(β‹…) is the Nemytskii operator. Note also that this definition of a generalized quasisolution differs from the definition of a quasitrajectory given in [9, 33, 34] due to the condition Μ‡π‘₯π‘–βˆˆdecΞ¦(π‘₯). Using Definition 4.21, we can obtain more general results on the properties of quasisolutions (see Remark 4.23). Moreover, this definition is more suitable for applications.

Let β„‹(π‘₯0) be the set of all generalized quasisolutions of the problem (4.1).

We define a mapping ΦcoβˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(Ξ [𝐋𝑛1[π‘Ž,𝑏]]) by the formula Φco(π‘₯)=ξ‚€codecΞ¦(π‘₯).(4.41)

We call ΦcoβˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(Ξ [𝐋𝑛1[π‘Ž,𝑏]]) the convex decomposable hull.

Consider the problem (4.1) with the convex decomposable hull ΦcoβˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(Ξ [𝐋𝑛1[π‘Ž,𝑏]]) given by (4.41) leading to Φ̇π‘₯∈co(π‘₯),π‘₯(π‘Ž)=π‘₯0ξ‚€π‘₯0βˆˆβ„π‘›ξ‚.(4.42)

Let 𝐻co(π‘₯0,𝜏) be the set of all solutions of the problem (4.42) on the interval [π‘Ž,𝜏](𝜏∈(π‘Ž,𝑏]).

Theorem 4.22. β„‹(π‘₯0)=𝐻co(π‘₯0,𝑏).

Proof. First, we will show that 𝐻co(π‘₯0,𝑏)βŠ‚β„‹(π‘₯0). Let π‘₯∈𝐻co(π‘₯0,𝑏). By [35], for Μ‡π‘₯βˆˆπ‹π‘›1[π‘Ž,𝑏], there exists a sequence π‘¦π‘–βˆˆdecΞ¦(π‘₯), 𝑖=1,2,…, such that 𝑦𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž. This implies that π‘₯𝑖=π‘₯0+Λ𝑦𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž, where Ξ›βˆΆπ‹π‘›1[π‘Ž,𝑏]→𝐂𝑛[π‘Ž,𝑏] is the operator of integration (see (4.17)). Hence, 𝐻co(π‘₯0,𝑏)βŠ‚β„‹(π‘₯0).
Let us now prove that β„‹(π‘₯0)βŠ‚π»co(π‘₯0,𝑏). Let π‘₯βˆˆβ„‹(π‘₯0). Then there exists a sequence π‘₯π‘–βˆˆπƒπ‘›[π‘Ž,𝑏], 𝑖=1,2,…, satisfying the following conditions: (1) Μ‡π‘₯π‘–βˆˆdecΞ¦(π‘₯) (see (4.41)) and π‘₯𝑖(π‘Ž)=π‘₯0 for each 𝑖=1,2,…; (2) π‘₯𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž. Since the sequence Μ‡π‘₯𝑖, 𝑖=1,2,…, is weakly compact, we can assume without loss of generality that Μ‡π‘₯𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž. Since Μ‡π‘₯π‘–βˆˆξ‚Ξ¦co(π‘₯) (see (4.41)), it follows that Φ̇π‘₯∈co(π‘₯) (see [21]). Hence π‘₯∈𝐻co(π‘₯0,𝑏) and therefore β„‹(π‘₯0)βŠ‚π»co(π‘₯0,𝑏).

Remark 4.23. Theorem 4.22 may still remain valid even if the mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] is discontinuous and its image Ξ¦(ℬ) is not integrally bounded for every bounded set β„¬βŠ‚π‚π‘›[π‘Ž,𝑏]. The proof of Theorem 4.22 is only based on the fact that every value of this mapping is integrally bounded, rather than on the assumption that Ξ¦ is a Volterra operator.

Definition 4.24. One says that a compact convex set π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏] has Property π’Ÿ if β„‹(π‘₯0)βŠ‚π‘ˆ, and for any π‘₯βˆˆβ„‹(π‘₯0), there exists a sequence of absolutely continuous functions π‘₯π‘–βˆΆ[π‘Ž,𝑏]→ℝ𝑛, 𝑖=1,2,…, such that(i)π‘₯𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž;(ii)π‘₯π‘–βˆˆπ‘ˆ, Μ‡π‘₯π‘–βˆˆdecΞ¦(π‘₯) and π‘₯𝑖(π‘Ž)=π‘₯0 for each 𝑖=1,2,….

Lemma 4.25. Suppose that the set of all local solutions of the problem (4.41) admits a uniform a priori estimate. Then, there exists a set π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏] satisfying Property π’Ÿ.

Proof. It follows from Theorem 4.22 and Remark 4.15 that the set π‘ˆ=coΞ¨(𝐂𝑛[π‘Ž,𝑏]) has Property π’Ÿ. Here, the mapping ξ‚Ξ¨βˆΆπ‚π‘›[π‘Ž,𝑏]β†’2𝐂𝑛[π‘Ž,𝑏] is determined by (4.29), where ΦΦ(β‹…)≑co(β‹…).

Lemma 4.26. Let sets Ξ¦π‘–βˆˆΞ [𝐋𝑛1[π‘Ž,𝑏]], 𝑖=1,2, satisfy Φ𝑖=𝑆(𝐹𝑖(β‹…)), 𝑖=1,2, where πΉπ‘–βˆΆ[π‘Ž,𝑏]β†’comp[ℝ𝑛] are measurable mappings. Then for any measurable set π’°βŠ‚[π‘Ž,𝑏], one has β„Žπ‹π‘›1(𝒰)Φ1;Ξ¦2ξ‚„β‰€ξ€œπ’°β„Žξ‚ƒπΉ1(𝑑);𝐹2ξ‚„(𝑑)𝑑𝑑≀2β„Žπ‹π‘›1(𝒰)Φ1;Ξ¦2ξ‚„.(4.43)

Proof. Let π’°βŠ‚[π‘Ž,𝑏] be a measurable set. Put 𝒰=π‘‘βˆˆπ’°βˆΆβ„Ž+𝐹1(𝑑);𝐹2ξ‚„(𝑑)β‰₯β„Ž+𝐹2(𝑑);𝐹1(𝑑).(4.44) The set ξ‚π’°βŠ‚π’° is measurable. Since ξ€œπ’°β„Žξ‚ƒπΉ1(𝑑);𝐹2ξ‚„ξ€œ(𝑑)𝑑𝑑=ξ‚π’°β„Ž+𝐹1(𝑑);𝐹2ξ‚„ξ€œ(𝑑)𝑑𝑑+ξ‚π’°π’°β§΅β„Ž+𝐹2(𝑑);𝐹1ξ‚„(𝑑)𝑑𝑑,(4.45) we have ξ€œπ’°β„Žξ‚ƒπΉ1(𝑑);𝐹2ξ‚„(𝑑)𝑑𝑑=β„Ž+𝐋𝑛1(𝒰)Φ1;Ξ¦2ξ‚„+β„Ž+𝐋𝑛1(𝒰⧡𝒰)Φ2;Ξ¦1ξ‚„.(4.46) This implies (4.43), and the proof is completed.

Let 𝐹∢[π‘Ž,𝑏]β†’comp[ℝ𝑛] be a measurable mapping. Let a mapping co𝐹∢[π‘Ž,𝑏]β†’comp[ℝ𝑛] be defined by (co𝐹)(𝑑)=co𝐹(𝑑).(4.47)

Corollary 4.27. Let sets Ξ¦π‘–βˆˆΞ [𝐋𝑛1[π‘Ž,𝑏]], 𝑖=1,2, satisfy Φ𝑖=𝑆(𝐹𝑖(β‹…)), 𝑖=1,2, where πΉπ‘–βˆΆ[π‘Ž,𝑏]β†’comp[ℝ𝑛] are measurable mappings. Then for any measurable set π’°βŠ‚[π‘Ž,𝑏], one has β„Žπ‹π‘›1(𝒰)Φco1;ξ‚€Ξ¦co2≀2β„Žπ‹π‘›1(𝒰)Φ1;Ξ¦2ξ‚„.(4.48)

Proof. By [35], we have that co(Φ𝑖)=𝑆(co𝐹𝑖(β‹…)), 𝑖=1,2. Therefore, β„Žπ‹π‘›1(𝒰)Φco1;ξ‚€Ξ¦co2β‰€ξ€œξ‚ξ‚„π’°β„Žξ‚ƒξ‚€co𝐹1(𝑑);co𝐹2(𝑑)𝑑𝑑(4.49) for any measurable set π’°βŠ‚[π‘Ž,𝑏]. Since, for any measurable set π’°βŠ‚[π‘Ž,𝑏], ξ€œπ’°β„Žξ‚ƒξ‚€co𝐹1(𝑑);co𝐹2ξ‚ξ‚„ξ€œ(𝑑)π‘‘π‘‘β‰€π’°β„ŽπΉξ‚ƒξ‚€1𝐹(𝑑);2(𝑑)𝑑𝑑,(4.50) we obtain, due to (4.43), the inequality (4.48).

Definition 4.28. One says that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property Ξ“3 if Property Ξ“20,0,0 is satisfied and the following conditions hold:(i)Ξ“2(0)=0;(ii)on every interval [π‘Ž,𝜏] (𝜏∈(π‘Ž,𝑏]), there exists a unique zero solution of the problem (4.31), where 𝑒=0, πœ€=0, 𝑝=0.

Theorem 4.29. Suppose that the set of all local generalized solutions of the problem (4.1) admits a uniform a priory estimate. Suppose also that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] satisfies Property Ξ“3. Then, 𝐻(π‘₯0,𝑏)β‰ βˆ… and 𝐻π‘₯0,𝑏=𝐻coξ‚€π‘₯0,𝑏,(4.51) where 𝐻(π‘₯0,𝑏) is the closure of the set 𝐻(π‘₯0,𝑏) in 𝐂𝑛[π‘Ž,𝑏].

Proof. Let us first prove that the set 𝐻co(π‘₯0) is closed in 𝐂𝑛[π‘Ž,𝑏]. Indeed, suppose that a sequence π‘₯π‘–βˆˆπ»co(π‘₯0), 𝑖=1,2,…, tends to π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž. Since the sequence {Μ‡π‘₯𝑖} is integrally bounded, it follows that π‘₯π‘–βˆˆπƒπ‘›[π‘Ž,𝑏] and Μ‡π‘₯𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž. For each 𝑖=1,2,…, let the function π‘§π‘–βˆˆξ‚Ξ¦co(π‘₯) satisfy β€–β€–Μ‡π‘₯π‘–βˆ’π‘§π‘–β€–β€–π‹π‘›1[π‘Ž,𝑏]=πœŒπ‹π‘›1[π‘Ž,𝑏]̇π‘₯𝑖;Φcoξ‚„(π‘₯),(4.52) where ΦcoβˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(Ξ [𝐋𝑛1[π‘Ž,𝑏]]) is the convex decomposable hull given by (4.41). Since the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25) is Hausdorff continuous, it follows from (4.48) that so is the mapping Φco(π‘₯)βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ©(Ξ [𝐋𝑛1[π‘Ž,𝑏]]). Therefore, (4.52) implies that Μ‡π‘₯π‘–βˆ’π‘§π‘–β†’0 in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž. Hence, 𝑧𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž. Since the set Φco(π‘₯) is convex, we have (see [21]) that Φ̇π‘₯∈co(π‘₯). Therefore, the set 𝐻co(π‘₯0) is closed in 𝐂𝑛[π‘Ž,𝑏].
Now, let us prove the equality (4.51). The closedness of the set 𝐻co(π‘₯0) yields that 𝐻(π‘₯0,𝑏)βŠ‚π»co(π‘₯0). Further, let us show that 𝐻co(π‘₯0)βŠ‚π»(π‘₯0,𝑏). Suppose π‘₯∈𝐻co(π‘₯0). Then from Theorem 4.22, it follows that there exists a sequence π‘¦π‘–βˆˆπƒπ‘›[π‘Ž,𝑏], 𝑖=1,2,…, such that π‘¦π‘–βˆˆξ‚Ξ¦(π‘₯), 𝑦𝑖(π‘Ž)=π‘₯0, 𝑖=1,2,… (π‘₯0 is the initial condition in the problem (4.1)) and 𝑦𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž. Since the mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property Ξ“3, we see that, due to (4.30), πœŒπ‹π‘›1(𝒰)̇𝑦𝑖𝑦;Ξ¦π‘–ξ‚ξ‚„β‰€β„Žπ‹π‘›1(𝒰)𝑦Φ(π‘₯);Ξ¦π‘–β‰€ξ€œξ‚ξ‚„π’°ξ‚€Ξ“2𝑍π‘₯βˆ’π‘¦π‘–ξ‚ξ‚ξ‚(𝑠)𝑑𝑠(4.53) for each 𝑖=1,2,… and any measurable set π’°βŠ‚[π‘Ž,𝑏]. Here, the operator π‘βˆΆπ‚π‘›[π‘Ž,𝑏]→𝐂1+[π‘Ž,𝑏] is given by (4.10). Since the mapping Ξ“2βˆΆπ‚1+[π‘Ž,𝑏]→𝐋1+[π‘Ž,𝑏] is continuous and Ξ“2(0)=0, we have that πœ˜π‘–=Ξ“2(𝑍(π‘₯βˆ’π‘¦π‘–))β†’0 in 𝐋11[π‘Ž,𝑏] as π‘–β†’βˆž. Since the problem (4.31) with 𝑒=0, πœ€=0, and 𝑝=0 only has the zero solution on each interval [π‘Ž,𝜏] (𝜏∈(π‘Ž,𝑏]), we see that the set of all local solutions of the problem (4.31) with 𝑒=πœ˜π‘–, πœ€=1/𝑖, and 𝑝=0 admits a uniform a priori estimate starting from some 𝑖=1,2,… (see [36]). Renumerating, we may assume without loss of generality that this holds true for all 𝑖=1,2,…. This implies (see [29]) that for each 𝑖=1,2,…, there exists the upper solution πœ‰(πœ˜π‘–,1/𝑖,0) of the problem (4.31) with 𝑒=πœ˜π‘–, πœ€=1/𝑖, and 𝑝=0. Hence, it follows from Theorem 4.18 that for each 𝑖=1,2,…, there exists a generalized solution π‘₯π‘–βˆˆπƒπ‘›[π‘Ž,𝑏] of the problem (4.1) satisfying Θ(π‘₯π‘–βˆ’π‘¦π‘–)β‰€πœ‰(πœ˜π‘–,1/𝑖,0), where the continuous operator Ξ˜βˆΆπƒπ‘›[π‘Ž,𝑏]→𝐂1+[π‘Ž,𝑏] is given by (4.15). Since πœ‰(πœ˜π‘–,1/𝑖,0)β†’0 in 𝐂1[π‘Ž,𝑏] as π‘–β†’βˆž, we have that Θ(π‘₯π‘–βˆ’π‘¦π‘–)β†’0 as π‘–β†’βˆž. Since 𝑦𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž, we see that π‘₯𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž. Therefore, π‘₯∈𝐻(π‘₯0,𝑏) and consequently 𝐻co(π‘₯0)βŠ‚π»(π‘₯0,𝑏). This yields (4.51). The proof is complete.

Corollary 4.30. Suppose that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Properties Ξ“1 and Ξ“3. Then 𝐻(π‘₯0,𝑏)β‰ βˆ… and the equality (4.51) is satisfied.

Remark 4.31. If the solution set of a differential inclusion with nonconvex multivalued mapping is dense in the solution set of the convexified inclusion, then such a property is called the density principle. The density principle is a fundamental property in the theory of differential inclusions (see [13]). Many papers (e.g., [3, 4, 6, 10–12, 23, 24, 25, 29, 30, 31, 32, 37, 38, 39]) deal with the justification of the density principle. Theorem 4.29 and Corollary 4.30 justify the density principle for the generalized solutions of the problem (4.1).

5. Generalized Approximate Solutions of the Functional Differential Equation

Approximate solutions are of great importance in the study of differential equations and inclusions (see [4, 40–43]). They are used in the theorems on existence (e.g., Euler curves) as well as in the study of the dependence of a solution on initial conditions and the right-hand side of the equation. In [40, 41], the definition of an approximate solution of a differential equation with piecewise continuous right-hand side was given, using so-called internal and external perturbations. This definition not only deals with small changes of the right-hand side within its domain of continuity, but also with the small changes in the boundaries of these domains. A more general definition of an approximate solution, which can be used not only for the study of functional differential equations with discontinuous right-hand sides but also for differential inclusions with upper semicontinuous convex right-hand sides, was given in [4]. In this paper, the following important property was justified for such an inclusion: the limit of approximate solutions is again a solution of functional differential inclusion. In the present paper, we introduce various definitions of generalized approximate solutions of a functional differential inclusion. The main difference of our definitions from the one given in [4] is that the values of a multivalued mapping are not convexified. Due to this, the topological properties of the sets of generalized approximate solutions are studied and the density principle is proven.

Since a generalized solution of the problem (4.1) is determined by the closed decomposable hull of a set, it is natural to raise the following question: how robust is the set of the generalized solutions of (4.1) with respect to small perturbations of decΞ¦(π‘₯)? It follows from Remark 3.10 that constructing decΞ¦(π‘₯) for each fixed π‘₯βˆˆπ‚π‘›[π‘Ž,𝑏] is equivalent to finding a measurable, integrally bounded mapping Ξ”π‘₯∢[π‘Ž,𝑏]β†’comp[ℝ𝑛] satisfying ξ‚€Ξ”decΞ¦(π‘₯)=𝑆π‘₯(β‹…).(5.1) The mapping Ξ”π‘₯∢[π‘Ž,𝑏]β†’comp[ℝ𝑛] is, in the sequel, written as Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛] and called a mapping generating the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25).

Denote by 𝐾([π‘Ž,𝑏]Γ—[0,∞)) the set of all continuous functions πœ‚βˆΆ[π‘Ž,𝑏]Γ—[0,∞)β†’[0,∞) satisfying the following conditions:(1)for each 𝛿β‰₯0, πœ‚(β‹…,𝛿)βˆˆπ‹11[π‘Ž,𝑏];(2)for each 𝛿β‰₯0, there exists a function 𝛽𝛿(β‹…)βˆˆπ‹11[π‘Ž,𝑏] such that πœ‚(𝑑,𝜏)≀𝛽𝛿(𝑑) for almost all π‘‘βˆˆ[π‘Ž,𝑏] and all 𝜏∈[0,𝛿];(3)lim𝛿→0+0πœ‚(𝑑,𝛿)=πœ‚(𝑑,0)=0 for almost all π‘‘βˆˆ[π‘Ž,𝑏].

Since the mappings Ξ”(β‹…,β‹…) and Ξ¦(β‹…) are related by the equality (5.1), we have that the robustness of the set of the generalized solutions of (4.1) with respect to small perturbations of decΞ¦(π‘₯) can be studied via the robustness properties of Ξ”. Assume that the perturbation Ξ”πœ‚(𝑑,π‘₯,𝛿) (e.g., an error in measurements of Ξ”(𝑑,π‘₯)) is given by Ξ”πœ‚ξ‚€ξ‚(𝑑,π‘₯,𝛿)=Ξ”(𝑑,π‘₯)πœ‚(𝑑,𝛿),(5.2) where πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)) (here, (Ξ”(𝑑,π‘₯))πœ‚(𝑑,𝛿) is an πœ‚-neighborhood of the set Ξ”(𝑑,π‘₯), see Preliminaries).

Note that (5.2) yields β„Žξ‚ƒΞ”(𝑑,π‘₯);Ξ”πœ‚ξ‚„(𝑑,π‘₯,𝛿)=πœ‚(𝑑,𝛿)(5.3) for all (𝑑,π‘₯)∈[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]. Thus, (5.3) implies that lim𝛿→+0β„Žξ‚ƒΞ”(𝑑,π‘₯);Ξ”πœ‚ξ‚„(𝑑,π‘₯,𝛿)=0(5.4) for each function πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)), almost all π‘‘βˆˆ[π‘Ž,𝑏], and all π‘₯βˆˆπ‚π‘›[π‘Ž,𝑏]. Therefore, all mappings Ξ”πœ‚βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)β†’comp[ℝ𝑛] defined by (5.2) and depending on πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)) are close (in the sense of (5.4)) to the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛]. The mapping Ξ”πœ‚βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)β†’comp[ℝ𝑛] is called the approximating operator.

We define a mapping ξ‚Ξ¦πœ‚βˆΆπ‚π‘›[π‘Ž,𝑏]Γ—[0,∞)β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] by the formula ξ‚Ξ¦πœ‚ξ‚€Ξ”(π‘₯,𝛿)=π‘†πœ‚ξ‚(β‹…,π‘₯,𝛿),(5.5) where the operator Ξ”πœ‚βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)β†’comp[ℝ𝑛] is given by (5.2). The equalities (5.3) and (5.5) imply that β„Žπ‹π‘›1[π‘Ž,𝑏]ξ‚ƒξ‚Ξ¦πœ‚ξ‚ξ‚„=ξ€œ(π‘₯,𝛿);Ξ¦(π‘₯)π‘π‘Žπœ‚(𝑑,𝛿)𝑑𝑑(5.6) for any π‘₯βˆˆπ‚π‘›[π‘Ž,𝑏].

It follows from (5.6) and the Lebesgue theorem that lim𝛿→0+0β„Žπ‹π‘›1[π‘Ž,𝑏]ξ‚ƒξ‚Ξ¦πœ‚ξ‚ξ‚„(π‘₯,𝛿);Ξ¦(π‘₯)=0.(5.7)

Thus, all mappings ξ‚Ξ¦πœ‚βˆΆπ‚π‘›[π‘Ž,𝑏]Γ—[0,∞)β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] defined by (5.2) and (5.5) and depending on πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)) are close (in the sense of (5.7)) to the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25).

Lemma 5.1 (see [6]). Let 𝑋 be a normed space and let π‘ˆβŠ‚π‘‹ be a convex set. Then β„Žπ‘‹ξ‚ƒπ΅π‘‹ξ‚ƒπ‘₯1,π‘Ÿ1ξ‚„βˆ©π‘ˆ;𝐡𝑋π‘₯2,π‘Ÿ2≀‖‖π‘₯βˆ©π‘ˆ1βˆ’π‘₯2‖‖𝑋+|||π‘Ÿ2βˆ’π‘Ÿ1|||(5.8) for all π‘₯1,π‘₯2βˆˆπ‘ˆ and all π‘Ÿ1,π‘Ÿ2>0.

Denote by 𝑃(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)) the set of all continuous functions πœ”βˆΆπ‚π‘›[π‘Ž,𝑏]Γ—[0,∞)β†’[0,∞) such that πœ”(π‘₯,0)=0 for any π‘₯βˆˆπ‚π‘›[π‘Ž,𝑏] and πœ”(π‘₯,𝛿)>0 for any (π‘₯,𝛿)βˆˆπ‚π‘›[π‘Ž,𝑏]Γ—(0,∞).

Let π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏] be a closed convex set and let πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)). We define a multivalued mapping π‘€π‘ˆ(πœ”)βˆΆπ‘ˆΓ—[0,∞)β†’Ξ©(π‘ˆ) by π‘€π‘ˆ(πœ”)(π‘₯,𝛿)=𝐡𝐂𝑛[π‘Ž,𝑏]π‘₯,πœ”(π‘₯,𝛿)βˆ©π‘ˆ.(5.9)

The inequality (5.8) yields the following result.

Lemma 5.2. Let π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏] be a closed convex set and let πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)). Then, a multivalued mapping π‘€π‘ˆ(πœ”)βˆΆπ‘ˆΓ—[0,∞)β†’Ξ©(π‘ˆ) given by (5.9) is Hausdorff continuous.

We define a mapping πœ‘π‘ˆ(πœ”)∢[π‘Ž,𝑏]Γ—π‘ˆΓ—[0,∞)β†’[0,∞) by the formula πœ‘π‘ˆ(πœ”)(𝑑,π‘₯,𝛿)=supπ‘¦βˆˆπ‘€π‘ˆ(πœ”)(π‘₯,𝛿)β„Žξ‚ƒξ‚„Ξ”(𝑑,π‘₯);Ξ”(𝑑,𝑦),(5.10) where the mapping π‘€π‘ˆ(πœ”)βˆΆπ‘ˆΓ—[0,∞)β†’Ξ©(π‘ˆ) is given by (5.9) and the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛] generates the mapping Φ given by (3.25).

It is natural to address the value of the function πœ‘π‘ˆ(πœ”)(β‹…,β‹…,β‹…) at the point (𝑑,π‘₯,𝛿)∈[π‘Ž,𝑏]Γ—π‘ˆΓ—[0,∞) as the modulus of continuity of the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛] at the point (𝑑,π‘₯) with respect to the variable π‘₯βˆˆπ‘ˆ. We call the function πœ”(β‹…,β‹…) the radius of continuity, while the function πœ‘π‘ˆ(β‹…,β‹…,β‹…) itself is called the modulus of continuity of the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛]with respect to the radius of continuity πœ”(β‹…,β‹…).

Definition 5.3. One says that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛[π‘Ž,𝑏]] has Property 𝐢 if the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛] generating the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25) is Hausdorff continuous in the second variable for almost all π‘‘βˆˆ[π‘Ž,𝑏].

Lemma 5.4. Suppose that for a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛[π‘Ž,𝑏]], there exists an isotonic continuous operator Ξ“βˆΆπ‚1+[π‘Ž,𝑏]→𝐋1+[π‘Ž,𝑏] satisfying the following conditions: (i)Ξ“(0)=0;(ii)the inequality (4.30), where Ξ“2≑Γ, is satisfied for any π‘₯,π‘¦βˆˆπ‚π‘›[π‘Ž,𝑏] and any measurable set π’°βŠ‚[π‘Ž,𝑏].
Then the mapping Ξ¦(β‹…) has Property ξ‚π’ž.

Proof. Let π‘₯𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž. Let us show that limπ‘–β†’βˆžβ„Žξ‚ƒΞ”ξ‚€π‘‘,π‘₯𝑖;Ξ”(𝑑,π‘₯)=0(5.11) for almost all π‘‘βˆˆ[π‘Ž,𝑏].
For each 𝑖=1,2,…, put 𝑦𝑖=sup𝑗β‰₯𝑖‖π‘₯π‘—βˆ’π‘₯‖𝐂𝑛[π‘Ž,𝑏]. Due to Theorem 3.18, (4.43), and the isotonity of the operator Ξ“βˆΆπ‚1+[π‘Ž,𝑏]→𝐋1+[π‘Ž,𝑏], for each 𝑖=1,2,… and almost all π‘‘βˆˆ[π‘Ž,𝑏], we have β„Žξ‚ƒΞ”ξ‚€π‘‘,π‘₯𝑖𝑍π‘₯;Ξ”(𝑑,π‘₯)≀2Ξ“π‘–ξ‚€π‘¦βˆ’π‘₯(𝑑)≀2Γ𝑖(𝑑).(5.12) Since the sequence Ξ“(𝑦𝑖), 𝑖=1,2,…, decreases, we obtain, due to the continuity of the mapping Ξ“(β‹…) and the equality Ξ“(0)=0, the equality (5.11). This completes the proof.

Lemma 5.5. Let π‘ˆ be a nonempty, convex, compact set in the space 𝐂𝑛[π‘Ž,𝑏] and let πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)). Suppose also that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property 𝐢. Then the mapping πœ‘π‘ˆ(πœ”)∢[π‘Ž,𝑏]Γ—π‘ˆΓ—[0,∞) given by (5.10) has the following properties: (i)πœ‘π‘ˆ(πœ”)(β‹…,π‘₯,𝛿) is measurable for any (π‘₯,𝛿)βˆˆπ‘ˆΓ—[0,∞);(ii)πœ‘π‘ˆ(𝑑,β‹…,β‹…) is continuous on π‘ˆΓ—[0,∞) for almost all π‘‘βˆˆ[π‘Ž,𝑏];(iii)for any π‘₯βˆˆπ‘ˆ and for almost all π‘‘βˆˆ[π‘Ž,𝑏], lim𝑧→π‘₯,𝛿→0+0πœ‘π‘ˆ(πœ”)(𝑑,π‘₯,𝛿)=0;(5.13)(iv)there exists an integrable function π‘π‘ˆβˆΆ[π‘Ž,𝑏]β†’[0,∞) such that πœ‘π‘ˆ(πœ”)(𝑑,π‘₯,𝛿)β‰€π‘π‘ˆ(𝑑) for almost all π‘‘βˆˆ[π‘Ž,𝑏], any π‘₯βˆˆπ‘ˆ, and all π›Ώβˆˆ[0,∞).

Definition 5.6. Let π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏]. One says that the function πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)) provides on π‘ˆ a uniform with respect to the radius of continuity πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)) estimate from above for the modulus of continuity of the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛]; if for any πœ€>0 there exists 𝛿(πœ€)>0 such that for almost all π‘‘βˆˆ[π‘Ž,𝑏], all π‘₯βˆˆπ‘ˆ, and π›Ώβˆˆ(0,𝛿(πœ€)], one has πœ‘π‘ˆ(πœ”)(𝑑,π‘₯,𝛿)β‰€πœ‚(𝑑,πœ€),(5.14) where πœ‘π‘ˆβˆΆ[π‘Ž,𝑏]Γ—π‘ˆΓ—[0,∞)β†’[0,∞) is given by (5.10).

Let π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏] and πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)). One defines a function πœ†π‘ˆ(πœ”)∢[π‘Ž,𝑏]Γ—[0,∞)β†’[0,∞) by πœ†π‘ˆ(πœ”)(𝑑,𝛿)=supπ‘₯βˆˆπ‘ˆπœ‘π‘ˆ(πœ”)(𝑑,π‘₯,𝛿).(5.15)

Lemma 5.1 yields the following result.

Corollary 5.7. Let π‘ˆ be a nonempty, convex, compact set in the space 𝐂𝑛[π‘Ž,𝑏] and let πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)). Suppose also that a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property 𝐢. Then the mapping πœ†π‘ˆ(πœ”)∢[π‘Ž,𝑏]Γ—[0,∞)β†’[0,∞) given by (5.15) belongs to the set 𝐾([π‘Ž,𝑏]Γ—[0,∞)) and provides a uniform (in the sense of Definition 5.6) estimate from above for the modulus of continuity of the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛].

Remark 5.8. Corollary 5.7 yields that if π‘ˆ is a nonempty, convex, compact set in the space 𝐂𝑛[π‘Ž,𝑏] and a mapping Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]→𝑄[𝐋𝑛1[π‘Ž,𝑏]] has Property 𝐢, then for a given πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)), there exists at least one function πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)) that provides a uniform (in the sense of Definition 5.6) estimate from above for the modulus of continuity of the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛].

Let πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)). For each π›Ώβˆˆ[0,∞), consider the initial value problem Φ̇π‘₯βˆˆπœ‚(π‘₯,𝛿),π‘₯(π‘Ž)=π‘₯0ξ‚€π‘₯0βˆˆβ„π‘›ξ‚,(5.16) where the mapping ξ‚Ξ¦πœ‚βˆΆπ‚π‘›[π‘Ž,𝑏]Γ—[0,∞)β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] is given by (5.1) and (5.5).

Since the operator ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25) is a Volterra operator, we see that the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛] has the following property: if π‘₯=𝑦 on [π‘Ž,𝜏] (𝜏∈(π‘Ž,𝑏]), then Ξ”(𝑑,π‘₯)=Ξ”(𝑑,𝑦) for almost all π‘‘βˆˆ[π‘Ž,𝜏]. This property, (5.1), and (5.4) imply that the operator ξ‚Ξ¦πœ‚βˆΆπ‚π‘›[π‘Ž,𝑏]Γ—[0,∞)β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] is a Volterra operator for each π›Ώβˆˆ[0,∞).

Any solution of the problem (5.16) with a given 𝛿>0 is said to be a generalized 𝛿-solution (a generalized approximate solution with external perturbations) of the problem (4.1). We denote by π»πœ‚(𝛿)(π‘ˆ) the set of all generalized 𝛿-solutions of (4.1) belonging to π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏].

Theorem 5.9. Suppose that a set π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏] has Property π’Ÿ. Then for any function πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)) that provides a uniform (in the sense of Definition 5.6) estimate from above for the modulus of continuity of the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛], one has 𝐻coξ‚€π‘₯0=,𝑏𝛿>0π»πœ‚(𝛿)(π‘ˆ),(5.17) where π»πœ‚(𝛿)(π‘ˆ) is the closure of π»πœ‚(𝛿)(π‘ˆ) in 𝐂𝑛[π‘Ž,𝑏].

Proof. First, let us prove that 𝐻coξ‚€π‘₯0ξ‚βŠ‚ξ™,𝑏𝛿>0π»πœ‚(𝛿)(π‘ˆ).(5.18) Let π‘₯∈𝐻co(π‘₯0,𝑏). Let us show that π‘₯ is a limit point of the set π»πœ‚(𝛿)(π‘ˆ) for any 𝛿>0. By Theorem 4.22, π‘₯ is a generalized quasisolution of the problem (4.1). Moreover, π‘₯βˆˆπ‘ˆ. Since the set π‘ˆ has Property π’Ÿ, we see that there exists a sequence of absolutely continuous functions π‘₯π‘–βˆΆ[π‘Ž,𝑏]→ℝ𝑛, 𝑖=1,2,…, such that the following conditions hold: π‘₯𝑖→π‘₯ in 𝐂𝑛[π‘Ž,𝑏] as π‘–β†’βˆž; π‘₯π‘–βˆˆπ‘ˆ, Μ‡π‘₯π‘–βˆˆdecΞ¦(π‘₯), and π‘₯𝑖(π‘Ž)=π‘₯0 for each 𝑖=1,2,…. Suppose that πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)) provides a uniform (in the sense of Definition 5.6) estimate from above for the modulus of continuity of the mapping Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛]. Then there exists 𝑖1 such that β€–π‘₯βˆ’π‘₯𝑖‖𝐂𝑛[π‘Ž,𝑏]<πœ”(π‘₯,𝛿) for each 𝑖β‰₯𝑖1. This implies that π‘₯π‘–βˆˆπ΅π‚π‘›[π‘Ž,𝑏][π‘₯,πœ”(π‘₯,𝛿)] for each 𝑖β‰₯𝑖1. Therefore, π‘₯π‘–βˆˆπ‘€π‘ˆ(πœ”)(π‘₯,𝛿) for each 𝑖β‰₯𝑖1. By Definition 5.6, there exists a number 𝑖2β‰₯𝑖1 such that πœ‘π‘ˆξ‚€β€–β€–(πœ”)𝑑,π‘₯,π‘₯βˆ’π‘₯𝑖‖‖𝐂𝑛[π‘Ž,𝑏]ξ‚β‰€πœ‚(𝑑,𝛿)(5.19) for any 𝑖β‰₯𝑖2 and almost all π‘‘βˆˆ[π‘Ž,𝑏].
The inequality (5.19) yields that πœŒξ‚ƒΜ‡π‘₯𝑖𝑑);Δ𝑑,π‘₯π‘–ξ‚ƒξ‚€ξ‚ξ‚„β‰€β„ŽΞ”(𝑑,π‘₯);Δ𝑑,π‘₯π‘–ξ‚ξ‚„β‰€πœ‘π‘ˆξ‚€β€–β€–(πœ”)𝑑,π‘₯,π‘₯βˆ’π‘₯𝑖‖‖𝐂𝑛[π‘Ž,𝑏]ξ‚ξ€Έβ‰€πœ‚(𝑑,𝛿(5.20) for each 𝑖β‰₯𝑖2 and almost all π‘‘βˆˆ[π‘Ž,𝑏]. By (5.20), π‘₯π‘–βˆˆπ»πœ‚(𝛿)(π‘ˆ) for each 𝑖β‰₯𝑖2. This implies that π‘₯ is a limit point of the set π»πœ‚(𝛿)(π‘ˆ). Therefore, π‘₯βˆˆπ»πœ‚(𝛿)(π‘ˆ), and consequently (5.18), is satisfied.
Let us prove the opposite inclusion 𝛿>0π»πœ‚(𝛿)(π‘ˆ)βŠ‚π»coξ‚€π‘₯0,𝑏.(5.21) Let β‹‚π‘₯βˆˆπ›Ώ>0π»πœ‚(𝛿)(π‘ˆ). This implies that for each 𝑖=1,2,…, there exists π‘₯π‘–βˆˆπ»πœ‚(1/𝑖)(π‘ˆ) satisfying β€–π‘₯βˆ’π‘₯𝑖‖𝐂𝑛[π‘Ž,𝑏]<1/𝑖. Suppose that functions π‘§π‘–βˆˆdecΞ¦(π‘₯) satisfy |||Μ‡π‘₯𝑖(𝑑)βˆ’π‘§π‘–|||(𝑑)=πœŒΜ‡π‘₯𝑖(𝑑);Ξ”(𝑑,π‘₯)(5.22) for each 𝑖=1,2,… and almost all π‘‘βˆˆ[π‘Ž,𝑏]. Let us show that limπ‘–β†’βˆžβ€–β€–Μ‡π‘₯π‘–βˆ’π‘§π‘–β€–β€–π‹π‘›1[π‘Ž,𝑏]=0.(5.23) Since πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)), by the Lebesgue theorem, we have that limπ‘–β†’βˆžξ€œπ‘π‘Žπœ‚ξ‚€1𝑑,𝑖𝑑𝑑=0.(5.24) By (5.22), the estimates |||Μ‡π‘₯𝑖(𝑑)βˆ’π‘§π‘–|||ξ‚€(𝑑)β‰€β„Ž[Δ𝑑,π‘₯π‘–ξ‚πœ‚(𝑑,1/𝑖)ξ‚€1;Ξ”(𝑑,π‘₯)]β‰€πœ‚π‘‘,𝑖+β„ŽΞ”(𝑑,π‘₯);Δ𝑑,π‘₯𝑖(5.25) are satisfied for each 𝑖=1,2,… and almost all π‘‘βˆˆ[π‘Ž,𝑏]. Therefore, ξ€œπ‘π‘Ž|||Μ‡π‘₯𝑖(𝑑)βˆ’π‘§π‘–|||ξ€œ(𝑑)π‘‘π‘‘β‰€π‘π‘Žπœ‚ξ‚€1𝑑,𝑖𝑑𝑑+2β„Žπ‹π‘›1[π‘Ž,𝑏]decΞ¦(π‘₯);ξ‚€π‘₯decΦ𝑖(5.26) for each 𝑖=1,2,…. By (5.24) and due to the continuity of the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25), we have (5.23).
Since Μ‡π‘₯𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž, we have that 𝑧𝑖→̇π‘₯ weakly in 𝐋𝑛1[π‘Ž,𝑏] as π‘–β†’βˆž. Therefore, by [21], Φ̇π‘₯∈co(π‘₯) and hence π‘₯∈𝐻(π‘₯0,𝑏). Thus, (5.21) is valid. Hence, (5.17) holds and the proof is complete.

Theorem 5.10. Suppose that a set π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏] has Property π’Ÿ. Then, 𝐻π‘₯0=,𝑏𝛿>0π»πœ‚(𝛿)(π‘ˆ)(5.27) for any πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)) if and only if the equality (4.51) is satisfied.

Proof. Let us prove the sufficiency. Assume that (4.51) holds. Let us show that the equality (5.27) is satisfied for any function πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)). By the definition of the problem (5.16), the inclusion 𝐻π‘₯0,π‘βŠ‚π»πœ‚(𝛿)(π‘ˆ)(5.28) is satisfied for any 𝛿>0. Therefore, for any 𝛿>0, we have the inclusion 𝐻π‘₯0ξ‚βŠ‚,π‘π»πœ‚(𝛿)(π‘ˆ)(5.29) and consequently the inclusion 𝐻π‘₯0ξ‚βŠ‚ξ™,𝑏𝛿>0π»πœ‚(𝛿)(π‘ˆ)(5.30) holds. Now, let us check that the opposite relation 𝛿>0π»πœ‚(𝛿)(π‘ˆ)βŠ‚π»ξ‚€π‘₯0,𝑏,(5.31) which is, by (4.51), equivalent to the inclusion 𝛿>0π»πœ‚(𝛿)(π‘ˆ)βŠ‚π»coξ‚€π‘₯0,𝑏,(5.32) holds as well. The latter relation can be proven similarly to Theorem 5.9.
The necessity follows readily from Theorem 5.9. The proof is complete.

Remark 5.11. Note that the equality (5.27) describes the robustness property of the set 𝐻(π‘₯0,𝑏) with respect to external perturbations πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)). These external perturbations (e.g., πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞))) characterize an error in measurements of the values of the mapping ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25).

On the other hand, each generalized solution π‘₯∢[π‘Ž,𝑏]→ℝ𝑛 of the problem (4.1) may also be measured with a certain error. This error may be described by a function belonging to the set 𝑃(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)) and it may be characterized by so-called internal perturbations, which are defined below. Let us show further that internal perturbations influence essentially the properties of generalized solutions of the problem (4.1).

We define a mapping Ξ”ext∢[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛] by Ξ”ext(𝑑,π‘₯)=extcoΞ”(𝑑,π‘₯),(5.33) where Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛] is the mapping generating the operator ξ‚Ξ¦βˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by (3.25); see the definition of ext(coΞ”(𝑑,π‘₯)) in Section 2. Let us remark that the mapping Ξ”ext(β‹…,π‘₯) is measurable (see [25]) and integrally bounded for each π‘₯βˆˆπ‚π‘›[π‘Ž,𝑏].

Consider the operator ΦextβˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]] given by Φextξ‚€Ξ”(π‘₯)=𝑆ext(β‹…,π‘₯),(5.34) where the mapping Ξ”ext∢[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛] is given by (5.33).

Remark 5.12. Note that for each π‘₯βˆˆπ‚π‘›[π‘Ž,𝑏], the set Φext(π‘₯) has the following property Φcoext=(π‘₯)ξ‚€codecΞ¦(π‘₯).(5.35) Also, Φext(π‘₯) is the minimal set among all nonempty closed in 𝐋𝑛1[π‘Ž,𝑏] decomposable subsets of decΞ¦(π‘₯) satisfying (5.35).

Consider the problem Φ̇π‘₯∈ext(π‘₯),π‘₯(π‘Ž)=π‘₯0ξ‚€π‘₯0βˆˆβ„π‘›ξ‚.(5.36) We call any solution (resp., quasisolution) of (5.36) a generalized extreme (in the sense of the definition in Section 2) solution (resp., generalized extreme quasisolution) of the problem (4.1).

Let β„‹ext(π‘₯0) be the set of all generalized extreme quasisolutions of the problem (4.1). Theorem 4.22, Remark 4.23, and equality (5.35) imply the following result.

Corollary 5.13. β„‹ext(π‘₯0)=𝐻co(π‘₯0,𝑏).

Let πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)), πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)). Let also π‘ˆ be a convex closed set in 𝐂𝑛[π‘Ž,𝑏]. We define mappings ξ‚Ξ¦πœ‚,πœ”βˆΆπ‘ˆΓ—[0,∞)β†’comp[𝐋𝑛1[π‘Ž,𝑏]βˆ—], Ξ”ext,πœ‚βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)β†’comp[ℝ𝑛], Φext,πœ‚βˆΆπ‚π‘›[π‘Ž,𝑏]Γ—[0,∞)β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]], Φext,πœ‚,πœ”βˆΆπ‚π‘›[π‘Ž,𝑏]Γ—[0,∞)β†’comp[𝐋𝑛1[π‘Ž,𝑏]βˆ—] by the formulas ξ‚Ξ¦πœ‚,πœ”ξ‚Ξ¦(π‘₯,𝛿)=πœ‚π‘€ξ‚€ξ‚€π‘ˆξ‚ξ‚,ξ‚€Ξ”(πœ”)(π‘₯,𝛿),𝛿ext,πœ‚ξ‚ξ‚€Ξ”(𝑑,π‘₯,𝛿)=ext(𝑑,π‘₯)πœ‚(𝑑,𝛿),Φext,πœ‚ξ‚ξ‚€Ξ”(π‘₯,𝛿)=𝑆ext,πœ‚ξ‚,Φ(β‹…,π‘₯,𝛿)ext,πœ‚,πœ”ξ‚Ξ¦(π‘₯,𝛿)=ext,πœ‚π‘€ξ‚€ξ‚€π‘ˆξ‚ξ‚,(πœ”)(π‘₯,𝛿),𝛿(5.37) where the mappings ξ‚Ξ¦πœ‚βˆΆπ‚π‘›[π‘Ž,𝑏]Γ—[0,∞)β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]], π‘€π‘ˆ(πœ”)βˆΆπ‘ˆΓ—[0,∞)β†’Ξ©(π‘ˆ), Ξ”ext∢[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)β†’comp[ℝ𝑛] are given by the equalities (5.5), (5.9), and (5.33), respectively.

For each 𝛿>0, consider the following problems on π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏]: Φ̇π‘₯βˆˆπœ‚,πœ”(π‘₯,𝛿),π‘₯(π‘Ž)=π‘₯0ξ‚€π‘₯0βˆˆβ„π‘›ξ‚ξ‚Ξ¦,(5.38)Μ‡π‘₯∈ext,πœ‚,πœ”(π‘₯,𝛿),π‘₯(π‘Ž)=π‘₯0ξ‚€π‘₯0βˆˆβ„π‘›ξ‚,(5.39)ξ‚Ξ¦πœ‚,πœ”βˆΆπ‘ˆΓ—[0,∞)β†’comp[𝐋𝑛1[π‘Ž,𝑏]βˆ—] where the mappings Φext,πœ‚,πœ”βˆΆπ‘ˆΓ—[0,∞)β†’, comp[𝐋𝑛1[π‘Ž,𝑏]βˆ—]𝛿>0 are given by (5.37).

We call any solution of the problem (5.38) with a fixed 𝛿 a generalized 𝛿>0-solution of the problem (4.1), or a generalized approximate solution of (4.1) with external and internal perturbations. For each π»πœ‚(𝛿),πœ”(𝛿)(π‘ˆ), we denote by 𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ) (π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏].) the set of all solutions of the problem (5.38) ((5.39)) on Φext,πœ‚,πœ”ξ‚Ξ¦(π‘₯,𝛿)βŠ‚πœ‚,πœ”(π‘₯,𝛿) Since 𝛿>0 for any π‘₯βˆˆπ‘ˆ, and any 𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ)βŠ‚π»πœ‚(𝛿),πœ”(𝛿)(π‘ˆ) we see that 𝛿>0 for any π‘ˆβŠ‚π‚π‘›[π‘Ž,𝑏].

Theorem 5.14. Let the set π’Ÿ. have Property πœ‚(β‹…,β‹…)∈𝐾([π‘Ž,𝑏]Γ—[0,∞)) Then for any πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)), 𝐻coξ‚€π‘₯0=,𝑏𝛿>0𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ)=𝛿>0π»πœ‚(𝛿),πœ”(𝛿)(π‘ˆ),(5.40), one has 𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ) where π»πœ‚(𝛿),πœ”(𝛿)(π‘ˆ) and 𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ) are the closures of the sets π»πœ‚(𝛿),πœ”(𝛿)(π‘ˆ), and 𝐂𝑛[π‘Ž,𝑏]. respectively, in the space 𝐻coξ‚€π‘₯0ξ‚βŠ‚ξ™,𝑏𝛿>0𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ).(5.41)

Proof. First of all, let us check that π‘₯∈𝐻(π‘₯0,𝑏). Let π‘₯ We show that 𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ) is a limit point of the set 𝛿>0. for any π‘₯ By Corollary 5.13, π‘ˆ is a generalized extreme quasisolution of the problem (4.1). Since the set π’Ÿ, has Property π‘₯βˆˆπ‘ˆ we see that π‘₯π‘–βˆΆ[π‘Ž,𝑏]→ℝ𝑛 and there exists a sequence of absolutely continuous functions 𝑖=1,2,…,, π‘₯𝑖→π‘₯ with the following properties: 𝐂𝑛[π‘Ž,𝑏] in π‘–β†’βˆž as π‘₯π‘–βˆˆπ‘ˆ; Μ‡π‘₯π‘–βˆˆξ‚Ξ¦ext(π‘₯),, π‘₯𝑖(π‘Ž)=π‘₯0 and 𝑖=1,2,… for each ΦextβˆΆπ‚π‘›[π‘Ž,𝑏]β†’Ξ [𝐋𝑛1[π‘Ž,𝑏]]. Here, the operator 𝑖0 is given by (5.33) and (5.34).
Let us prove also that there exists a number 𝑖β‰₯𝑖0 such that for each π‘₯π‘–βˆˆπ»ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ).(5.42), πœ”(β‹…,β‹…)βˆˆπ‘ƒ(𝐂𝑛[π‘Ž,𝑏]Γ—[0,∞)), Since 𝑖0 we see that there exists a number 𝑖β‰₯𝑖0 such that for each π‘₯βˆˆπ΅π‚π‘›[π‘Ž,𝑏][π‘₯𝑖;πœ”(π‘₯𝑖,𝛿)]., 𝑖β‰₯𝑖0 This implies that for each π‘₯βˆˆπ‘€π‘ˆ(π‘₯𝑖,𝛿), we have that 𝑖β‰₯𝑖0 (see (5.9)). Therefore, for each ΦextΦ(π‘₯)βŠ‚ext,πœ‚,πœ”(π‘₯𝑖,𝛿), the inclusion 𝑖β‰₯𝑖0 holds. Hence, for each π‘₯, we have (5.42). This means that 𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ). is a limit point of the set π‘₯∈𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ) Therefore, 𝛿>0𝐻ext,πœ‚(𝛿),πœ”(𝛿)(π‘ˆ)βŠ‚π»coξ‚€π‘₯0,𝑏(5.43) and (5.41) is satisfied.
The relation Ξ”βˆΆ[π‘Ž,𝑏]×𝐂𝑛[π‘Ž,𝑏]β†’comp[ℝ𝑛] can be proven similarly to (5.21) (see the proof of Theorem 5.9). The second equality of (5.40) can be proven in the same way. This completes the proof of the theorem.

Remark 5.15. Theorem 5.14 says that no measurement accuracy of the values of the mapping 𝐻(π‘₯0,𝑏) could guarantee the β€œreconstruction” of the set π»πœ‚(𝛿),πœ”(𝛿)(π‘ˆ). by means of 𝛿 That is only possible if the density principle holds for the generalized solutions.

6. Conclusion

The main results of the paper can be summarized as follows. For the decomposable hull of a mapping, we have obtained the conditions for the property of the Hausdorff lower semicontinuity (resp., upper semicontinuity and continuity). We considered a functional differential inclusion with a Volterra multivalued mapping which is not necessarily decomposable. The concept of a generalized solution of the initial value problem for such an inclusion was introduced and its properties were studied. Conditions for the local existence and continuation of a generalized solution to the initial value problem were obtained. We have offered some estimates, which characterize the closeness of generalized solutions and a given absolutely continuous function. These estimates were derived from the conditions for the existence of a generalized solution satisfying the inequality (4.18) (see Theorem 4.13 and Corollary 4.14).

The concept of a generalized quasisolution of the initial value problem was introduced. We proved that the set of all generalized quasisolutions of the initial value problem coincides with the solution set of the functional differential inclusion with the convex decomposable hull of the right-hand side. Using this fact as well as the estimates characterizing the closeness of generalized solutions and a given absolutely continuous function, we obtained the density principle for the generalized solutions.

Asymptotic properties of the set of generalized approximate solutions (generalized 𝛿-solutions) were studied. It was proven that the limit of the closures of the sets of generalized approximate solutions coincides with the closure of the set of the generalized solutions if and only if the density principle holds for the generalized solutions.

Acknowledgments

The first author is supported by CIGENE (Center for Integrative Genetics) and by LΓ₯nekassen (Norwegian State Educational Loan Fund). The second author is supported by CIGENE and partially supported by the Russian FBR Grant no. 07-01-00305. The third author is partially supported by the Russian FBR Grant no. 07-01-00305.