On Continuous Selection Sets of Non-Lipschitzian Quantum Stochastic Evolution Inclusions
Abstract
We establish existence of a continuous selection of multifunctions associated with quantum stochastic evolution inclusions under a general Lipschitz condition. The coefficients here are multifunctions but not necessarily Lipschitz.
1. Introduction
As observed by [2], problems of continuous selection, features of reachable sets, and the solution sets of classical differential inclusions have attracted considerable attention [3–6]. The existence and nonuniqueness of solutions of such inclusions have been investigated to a large extent. See [7] and the references therein.
Existence of continuous selections of multifunctions associated with the sets of solutions of Lipschitzian and non-Lipschitzian quantum stochastic differential inclusions (QSDIs) has been considered in [2, 8], while the existence of solution of quantum stochastic evolution arising from hypermaximal monotone coefficients was established in [9].
Also in [10, 11] several results have been established concerning some properties of the solution sets of QSDIs. Results concerning the topological properties of solution sets of Lipschitzian QSDI were also considered in [12]. In [1], results on continuous selections of solution sets of quantum stochastic evolution inclusions (QSEIs) were established under the Lipschitz condition defined in [2, 13].
In order to generalize the results in the literature concerning QSDI, in [8] existence of continuous selections of solutions sets of non-Lipschitzian quantum stochastic differential inclusions was considered. It was proved that certain inclusion problems do not necessarily satisfy the Lipschitz condition defined in [2, 13]. In [8], the map x → P(t, x)(η, ξ) satisfied a general Lipschitz condition with values that are closed but not necessarily convex or bounded subsets of the field of complex numbers. This work is concerned with similar results established in [8] where the coefficients are not necessarily Lipschitz. The results here generalize existing results in the literature [1] concerning quantum stochastic evolution inclusions (QSEIs).
The rest of this paper is organized as follows: in Section 2, we present the foundations for establishing the major results. In Section 3, we will establish the major results. Our method will be a blend of the methods applied in [1, 8].
2. Preliminaries
All through this work, as in [2, 8], we adopt the definitions and notations of the following spaces, subspaces, and sets: , , , , , , , and for a fixed Hilbert space r. , clos(S), (resp., Comp(S)), , ρ(A, B), , ak, aηξ,k, Φηξ,k(·), and so forth. For the completion of the space and the generated topology and many more we refer the reader to [2, 8].
For the definitions of lower semicontinuous multivalued map (l.s.c.) , measurability and measurability of a multifunction (t, x) → Φ(t, x)(η, ξ), decomposable subset of a space, and locally absolutely P-integrable and adapted multivalued stochastic process Φ, we refer the reader to [2, 8].
Motivated by the result in [8], we extend the results in [1], to a class of evolution inclusion that depends on a more general Lipschitz condition W(t) ≠ t. Hence the results here are weaker than the results in [1].
- (1)
The map (t, x)∈→P2(t, x)(η, ξ) is measurable.
- (2)
There exists a map lying in and the function increasing and continuous with W(0) = 0 such that
()a.e., t ∈ [0, T], and for each pair . - (3)
There exists a β which lies in such that
()
Remark 1. Conditions (1) and (3) are similar to conditions S(i) and S(iii) in [1], while condition S(ii) has been modified to accommodate the general Lipschitz condition defined above. If we take W(t) = t, then condition (2) reduces to condition S(ii) in [1].
We adopt the proof of the following results established in [1] since the proof of these results is independent of the Lipschitz function.
Lemma 2. Consider the multivalued stochastic process , and assume that
- (i)
the map (t, x) → P(t, x)(η, ξ) is measurable,
- (ii)
the map (t, ·) → P(t, ·)(η, ξ) is l.s.c.
Lemma 3. Let the multivalued stochastic process be l.s.c. Assume that
- (i)
and are continuous,
- (ii)
for every aηξ ∈ A(η, ξ) the set Φ(aηξ) defined by (10) in [1] is nonempty.
Definition 4. A function is called a solution of (Ha) if there exists , a selection of P2(·, x(·, a))(η, ξ) such that x(·, a) is a weak solution of the Cauchy problem Hp(·,a).
3. Major Results
In this section, we present our major results under the general Lipschitz condition defined above. We will establish the result by employing similar argument employed in the proof of Theorems 3.1 in [1] and 3.1 in [8] by highlighting the major changes due to condition (iii).
Theorem 5. Assume that the maps satisfy the following conditions:
- (i)
P1 is hypermaximal monotone.
- (ii)
(t, x) → P2(t, x)(η, ξ) is measurable.
- (iii)
There exists a map lying in , such that
()a.e. in I, where W(t) ≠ t. - (iv)
There exists such that
()
- (i)
〈η, x(·, a)ξ〉 ∈ ST(a)(η, ξ) for every a ∈ A0;
- (ii)
〈η, aξ〉 → 〈η, x(·, a)ξ〉 is continuous from A0(η, ξ) to .
Proof. Let a ∈ A0 and be the unique weak solution of the Cauchy problem
As in [8] we fix ϵ > 0 and set ϵ = ϵ/2n+1, . Define and by (14) and (15) in [1]. Using (16) and Lemma 2, ϕ0(·) is lower semicontinuous (l.s.c.) and for each aη,ξ ∈ A0(η, ξ), ϕ0(aηξ) ≠ 0, and W(t) ≠ t. Again by Lemma 3, there exists , a continuous selection of ϕ0(·). Set p0(t, a)(η, ξ) = φ0(aηξ)(t) as in [1]; then p0(·, a)(η, ξ) is continuous, p0(t, a)(η, ξ) ∈ P2(t, a)(η, ξ), and
If we set 〈η, pn+1(t, a)ξ〉 = φn+1(aηξ)(t) for aηξ ∈ A0(η, ξ), t ∈ I, we have that pn+1 satisfies the properties (a), (b) in [1] and (22); hence by (24), we obtain
Now if we use (23) and (26), we get
Conflict of Interests
The author declares that there is no conflict of interests.