Abstract

Using some techniques from vector integration, we prove the weak measurability of the adjoint of strongly continuous semigroups which factor through Banach spaces without isomorphic copy of 𝑙1; we also prove the strong continuity away from zero of the adjoint if the semigroup factors through Grothendieck spaces. These results are used, in particular, to characterize the space of strong continuity of {π‘‡βˆ—βˆ—(𝑑)}𝑑β‰₯0, which, in addition, is also characterized for abstract 𝐿- and 𝑀-spaces. As a corollary, it is proven that abstract 𝐿-spaces with no copy of 𝑙1 are finite-dimensional.

1. Introduction

The study of the adjoint of a strongly continuous semigroups was initiated by Phillips [1], who proved, among other things, that for the general case, the domain of continuity of the adjoint semigroup on a Banach space 𝑋 is different from π‘‹βˆ—. A systematic study of the adjoint semigroup {π‘‡βˆ—(𝑑)}𝑑β‰₯0 can be found in [2], where, among other things, the basic properties of {π‘‡βˆ—(𝑑)}𝑑β‰₯0 and of the canonical spaces π‘‹βŠ™ and π‘‹βŠ™βŠ™ associated with it are studied. Also, in [2], Neerven introduces the space π‘‹βŠ™βŠ™ and studies the relationship between π‘‹βŠ™βŠ™ and π‘‹βŠ™βŠ™, giving some conditions guaranteeing that π‘‹βŠ™βŠ™ must be equal to π‘˜π‘‹βŠ™βŠ™, where π‘˜βˆΆπ‘‹βŠ™βŠ™β†’π‘‹βˆ—βˆ— is a natural embedding of π‘‹βŠ™βŠ™ into π‘‹βˆ—βˆ—, defined by the formula βŸ¨π‘˜π‘₯βŠ™βŠ™,π‘₯βˆ—βŸ©βˆΆ

Some of the principal tools used by van Neerven come from vector measures, like Gelfand and Pettis integrals, in order to provide the reader with some examples where the above-mentioned equality holds.

In this paper, we also employ certain techniques from vector measures to show that semigroups factoring through Banach spaces without isomorphic copy of = have weakly measurable adjoint. On the other hand, we prove the strong continuity away from zero of the adjoint when the semigroup factors through Grothendieck spaces. These results have several applications; in particular, there is one related to our other main topic of interest: to find a characterization of the space limπœ†β†’βˆž of strong continuity of a given second dual semigroup ⟨π‘₯βŠ™βŠ™. This can be done in the case of spaces satisfying the above-mentioned hypotheses. This is also done when ,πœ†π‘…(πœ†,π΄βˆ—) is sun-reflexive and π‘₯βˆ—βˆ— is isomorphic to a dual Banach space. Additionally, we give a characterization of the strong continuity of ⟩,π‘₯βŠ™βŠ™βˆˆπ‘‹βŠ™βŠ™. for abstract 𝑙1- and π‘‹βŠ™βŠ™-spaces, and prove that abstract {π‘‡βˆ—βˆ—(𝑑)}𝑑β‰₯0-spaces with no copy of 𝑋 are finite-dimensional.

2. Preliminaries

2.1. The Semigroup Dual

Let π‘‹βŠ™ be a complex Banach space and let {π‘‡βˆ—βˆ—(𝑑)}𝑑β‰₯0 be a 𝐿-semigroup of bounded linear operators on 𝑀 The adjoint semigroup 𝐿 fails in general to be strongly continuous. The semigroup dual of 𝑙1with respect to 𝑋 notation {𝑇(𝑑)}𝑑β‰₯0 (pronounced 𝐢0-sun) is defined as the linear subspace of 𝑋. on which {π‘‡βˆ—(𝑑)}𝑑β‰₯0 acts in a strongly continuous way 𝑋 From this definition, we have that {𝑇(𝑑)}𝑑β‰₯0, is π‘‹βŠ™-invariant, that is, 𝑋 for all π‘‹βˆ—

It can also be shown (see, e.g., [2]) that {π‘‡βˆ—(𝑑)}𝑑β‰₯0 is a closed, weakβˆ—-dense linear subspace of π‘‹βŠ™={π‘₯βˆ—βˆˆπ‘‹βˆ—βˆΆlim𝑑↓0β€–β€–π‘‡βˆ—(𝑑)π‘₯βˆ—βˆ’π‘₯βˆ—β€–β€–=0}.(2.1).

2.2. The Space π‘‹βŠ™

Let π‘‡βˆ—(𝑑) denote the restriction of π‘‡βˆ—π‘‹βŠ™βŠ†π‘‹βŠ™, to the 𝑑β‰₯0.-invariant subspace π‘‹βŠ™ Since π‘‹βˆ— is closed, π‘‹βŠ™βŠ™ is a Banach space. Also, it is clear from the definition of {π‘‡βŠ™(𝑑)}𝑑β‰₯0 that {π‘‡βˆ—(𝑑)}𝑑β‰₯0 is a strongly continuous semigroup on π‘‡βˆ—(𝑑)

We can also define π‘‹βŠ™. to be the adjoint of π‘‹βŠ™ and write π‘‹βŠ™ for π‘‹βŠ™ (read as {π‘‡βŠ™(𝑑)}𝑑β‰₯0-sun-sun or π‘‹βŠ™.-bosom).

If {π‘‡βŠ™βˆ—(𝑑)}𝑑β‰₯0 is defined by {π‘‡βŠ™(𝑑)}𝑑β‰₯0 then π‘‹βŠ™βŠ™ and (π‘‹βŠ™)βŠ™ Moreover, 𝑋 is an embedding and we can identify 𝑋 isomorphically with the closed subspace π‘—βˆΆπ‘‹β†’π‘‹βŠ™βˆ— of βŸ¨π‘—π‘₯,π‘₯βŠ™βŸ©βˆΆ=⟨π‘₯βŠ™,π‘₯⟩,. If ‖𝑗‖≀1, then 𝑗(𝑋)βŠ†π‘‹βŠ™βŠ™. is said to be sun-reflexive or 𝑗-reflexive with respect to 𝑋.

The following results can be found in [2].

Theorem 2.1. Let 𝑗𝑋 be a complex Banach space, π‘‹βŠ™βŠ™ a 𝑗𝑋=π‘‹βŠ™βŠ™-semigroup on 𝑋 with infinitesimal generator βŠ™ satisfying {𝑇(𝑑)}𝑑β‰₯0, and let 𝑋 be the adjoint of {𝑇(𝑑)}𝑑β‰₯0

The formula 𝐢0 defines a natural embedding 𝑋 Moreover, 𝐴, and ‖𝑇(𝑑)‖≀𝑀𝑒𝑀𝑑 If π΄βˆ— is the natural map, then we have 𝐴.

We also have the following characterization of ξ‚¬π‘˜π‘₯βŠ™βŠ™,π‘₯βˆ—ξ‚­βˆΆ=limπœ†β†’βˆžξ‚¬π‘₯βŠ™βŠ™ξ‚€,πœ†π‘…πœ†,π΄βˆ—ξ‚π‘₯βˆ—ξ‚­,π‘₯βŠ™βŠ™βˆˆπ‘‹βŠ™βŠ™,(2.2).

Theorem 2.2. It holds that π‘˜βˆΆπ‘‹βŠ™βŠ™β†’π‘‹βˆ—βˆ—.

The former theorem suggests to define the following.

Definition 2.3. 1β‰€β€–π‘˜β€–β‰€π‘€

A natural question is: do the spaces π‘˜π‘₯βŠ™βŠ™|π‘‹βŠ™=π‘₯βŠ™βŠ™.and π‘–βˆΆπ‘‹β†’π‘‹βˆ—βˆ—coincide? Trivially, this is true if 𝑖=π‘˜π‘—. since then we have the coincidence of both definitions. It is also shown in [2] that π‘˜π‘‹βŠ™βŠ™ maps π‘˜π‘‹βŠ™βŠ™={π‘₯βˆ—βˆ—βˆˆπ‘‹βˆ—βˆ—βˆΆlimπœ†β†’βˆžπœ†π‘…(πœ†,𝐴)βˆ—βˆ—π‘₯βˆ—βˆ—=π‘₯βˆ—βˆ—}.(2.3) into π‘‹βŠ™βŠ™βˆΆ={π‘₯βˆ—βˆ—βˆˆπ‘‹βˆ—βˆ—βˆΆlim𝑑↓0π‘‡βˆ—βˆ—(𝑑)π‘₯βˆ—βˆ—=π‘₯βˆ—βˆ—}.(2.4), and so π‘‹βŠ™βŠ™ always holds, but this inclusion can be proper. More specifically, if π‘˜π‘‹βŠ™βŠ™ is the rotation group on π‘‹βˆ—=π‘‹βŠ™, the unit circle, then π‘˜ (see [2, page 99]).

In the following, we will be interested in giving conditions guaranteeing that π‘‹βŠ™βŠ™ is equal to π‘‹βŠ™βŠ™

2.3. The Gelfand and Pettis Integrals

Let π‘˜π‘‹βŠ™βŠ™βŠ†π‘‹βŠ™βŠ™ be finite measure space and let {𝑇(𝑑)}𝑑β‰₯0 be a Banach space. Suppose that 𝑋=𝐢(𝑇),𝑇 is weaklyβˆ—-π‘‹βŠ™βŠ™β‰ π‘˜π‘‹βŠ™βŠ™-measurable and suppose further that for each π‘‹βŠ™βŠ™ the function π‘˜π‘‹βŠ™βŠ™. belongs to (Ξ©,Ξ£,πœ‡) For each 𝑋 define a map π‘“βˆΆΞ©β†’π‘‹βˆ—, πœ‡ It can be easily shown that π‘₯βˆˆπ‘‹ is bounded. This implies that the linear map βŸ¨π‘“(β‹…),π‘₯⟩ defined by 𝐿1(πœ‡). is bounded. The element 𝐸∈Σ is called the weakβˆ—-integral or Gelfand integral of π‘‡πΈβˆΆπ‘‹β†’πΏ1(πœ‡)over 𝑇𝐸π‘₯=βŸ¨π‘“πœ’πΈ(β‹…),π‘₯⟩. with respect to 𝑇𝐸 notation π‘₯βˆ—πΈ

We have from the definition that the weakβˆ—-integral satisfies π‘₯βˆ—πΈξ‚­ξ€œ,π‘₯∢=𝐸𝑓(β‹…),π‘₯π‘‘πœ‡(2.5) for all π‘₯βˆ—πΈβˆˆπ‘‹βˆ— and 𝑓

Now, if 𝐸 is weakly πœ‡,-measurable and for each π‘₯βˆ—πΈ=weakβˆ—βˆ«πΈπ‘“π‘‘πœ‡., the function weakβˆ—ξ€œπΈξ‚­=ξ€œπ‘“π‘‘πœ‡,π‘₯𝐸𝑓(β‹…),π‘₯π‘‘πœ‡(2.6) belongs to 𝐸∈Σ then using the same argument as above, each π‘₯βˆˆπ‘‹. defines an element π‘“βˆΆΞ©β†’π‘‹ such that πœ‡ for all π‘₯βˆ—βˆˆπ‘‹βˆ— If for all ⟨π‘₯βˆ—,𝑓(β‹…)⟩ the element 𝐿1(πœ‡), belongs to 𝐸∈Σ then π‘₯βˆ—βˆ—βˆˆπ‘‹βˆ—βˆ— is said to be Pettis integrable with respect to π‘₯πΈβˆ—βˆ—,π‘₯βˆ—ξ‚­=ξ€œπΈξ‚¬π‘₯βˆ—ξ‚­,𝑓(β‹…)π‘‘πœ‡(2.7)

For a detailed study of the Gelfand and Pettis integrals, see [3–5].

Theorem 2.4. An element π‘₯βˆ—βˆˆπ‘‹βˆ—. belongs to 𝐸∈Σ if and only if for all π‘₯πΈβˆ—βˆ— and 𝑋, one has 𝑓

For a proof of this, see [2].

Corollary 2.5. πœ‡. if and only if for all π‘₯βŠ™βŠ™βˆˆπ‘‹βŠ™βŠ™, π‘˜π‘‹βŠ™βŠ™, and 𝑑>0 one has π‘₯βˆ—βˆˆπ‘‹βˆ—

Hence, if π‘₯βŠ™βŠ™,weakβˆ—ξ€œπ‘‘0π‘‡βˆ—(𝜎)π‘₯βˆ—ξ‚­=ξ€œπ‘‘πœŽπ‘‘0π‘₯βŠ™βŠ™,π‘‡βˆ—(𝜎)π‘₯βˆ—ξ‚­π‘‘πœŽ.(2.8) is Pettis integrable, that is, for all π‘‹βŠ™βŠ™=π‘˜π‘‹βŠ™βŠ™ and 𝑑>0, the map π‘₯βˆ—βˆˆπ‘‹βˆ— is Pettis integrable on π‘₯βŠ™βŠ™βˆˆπ‘‹βŠ™βŠ™ then π‘₯βŠ™βŠ™,weakβˆ—ξ€œπ‘‘0π‘‡βˆ—(𝜎)π‘₯βˆ—ξ‚­=ξ€œπ‘‘πœŽπ‘‘0π‘₯βŠ™βŠ™,π‘‡βˆ—(𝜎)π‘₯βˆ—ξ‚­π‘‘πœŽ.(2.9) In particular, this holds if {π‘‡βˆ—(𝑑)}𝑑β‰₯0 is strongly continuous away from zero (notation: π‘₯βˆ—βˆˆπ‘‹βˆ—).

Definition 2.6. Let 𝜏>0 be two weakly π‘‘β†’π‘‡βˆ—(𝑑)π‘₯βˆ—-measurable functions. One says that [0,𝜏], are weakly π‘‹βŠ™βŠ™=π‘˜π‘‹βŠ™βŠ™.-equivalent if {π‘‡βˆ—(𝑑)}𝑑β‰₯0𝐢>0- almost everywhere, for each 𝑓,π‘”βˆΆΞ©β†’π‘‹ If πœ‡ are weaklyβˆ—π‘“,𝑔-measurable, one says that πœ‡, ⟨π‘₯βˆ—,𝑓(β‹…)⟩=⟨π‘₯βˆ—,𝑔(β‹…)⟩ are weaklyβˆ—πœ‡-equivalent if π‘₯βˆ—βˆˆπ‘‹βˆ—. for each 𝑓,π‘”βˆΆΞ©β†’π‘‹βˆ—

Following [5], we will denote by πœ‡ the space of classes of weakly 𝑓-equivalent Pettis 𝑔-integrable πœ‡-valued functions. It is a linear space with ordinary algebraic operations.

Definition 2.7. βŸ¨π‘“(β‹…),π‘₯⟩=βŸ¨π‘”(β‹…),π‘₯⟩ has the π‘₯βˆˆπ‘‹.-weak Radon-Nikodym property (𝒫(πœ‡,𝑋)-WRNP) if for each πœ‡-valued πœ‡-continuous measure of 𝑋-finite variation 𝑋, there exists πœ‡ such that πœ‡ for each 𝑋 and πœ‡

𝜎 has the WRNP if it has the 𝛾-WRNP for every π‘“βˆˆπ’«(πœ‡,𝑋)

For more details about the WRNP, see [4, 5].

One of the principal tools used here is the following theorem.

Theorem 2.8. π‘₯βˆ—ξ‚­=ξ€œ,𝛾(𝐸)𝐸π‘₯βˆ—ξ‚­,π‘“π‘‘πœ‡(2.10) has the weak Radon-Nikodym property if and only if π‘₯βˆ—βˆˆπ‘‹βˆ— contains no isomorphic copy of 𝐸∈Σ.

3. Strong Continuity of the Adjoint Semigroup

It is well known that a semigroup is strongly continuous if and only if it is weakly continuous (see [6]). In [7], BΓ‘rcenas and Diestel have proved that if a 𝑋-semigroup πœ‡ is such that, for each πœ‡. factors through an Asplund space, then the adjoint semigroup π‘‹βˆ— is 𝑋 (A Banach space 𝑙1. is an Asplund space if and only if 𝐢0 has the Radon-Nikodym property.) Since weakly compact operators factor through reflexive Banach spaces (which are Asplund spaces), we see that the adjoint semigroup of a semigroup of weakly compact operators is strongly continuous away from {𝑇(𝑑)}𝑑β‰₯0 (see [8]). BΓ‘rcenas and Diestel used those results to get some applications in optimal control theory.

In this section, we get the same conclusion of BΓ‘rcenas-Diestel if a 𝑑>0,𝑇(𝑑)-semigroup {π‘‡βˆ—(𝑑)}𝑑β‰₯0 is such that, for each 𝐢>0., 𝑋 factors through a Grothendieck space.

We recall that a Banach space is a Grothendieck space if every weaklyβˆ—-convergent sequence in π‘‹βˆ— is also weakly convergent. Equivalently, 𝑂 is a Grothendieck space if every linear bounded operator from 𝐢0 to any separable space, Banach space is weakly compact. Among Grothendieck spaces, we list all reflexive Banach spaces and {𝑇(𝑑)}𝑑β‰₯0, where 𝑑>0 is a positive measure space. A Banach space isomorphic to a complemented subspace of a Grothendieck space is also a Grothendieck space. Several characterizations of Grothendieck spaces are found in [9].

A Banach space is said to have the Dunford-Pettis property if every weakly compact operator in 𝑇(𝑑) applies relatively weakly compact sets onto relatively norm compact sets. The most common examples of Banach spaces with the Dunford-Pettis property are π‘‹βˆ— and 𝑋 Complemented subspaces of a space with the Dunford-Pettis property have also the Dunford-Pettis property. For more details about this, see [10].

If 𝑋 is a Grothendieck space with the Dunford-Pettis property, Lotz (see [11]) has shown that every strongly continuous semigroup is uniformly continuous and so the adjoint semigroup is uniformly continuous.

We also recall that a bounded linear operator 𝐿∞(Ξ©,Ξ£,πœ‡) (where (Ξ©,Ξ£,πœ‡) and 𝐿(𝑋) are Banach spaces) factors through a Banach space 𝐿1(πœ‡) if there are bounded linear operators 𝐢(𝐾). and 𝑋 such that the following diagram: fig.001(3.1) commutes.

Theorem 3.1. Let π‘‡βˆΆπ‘‹β†’π‘Œ be a Banach space and 𝑋 a π‘Œ-semigroup defined on 𝑍 Suppose that for every π‘’βˆΆπ‘‹β†’π‘ there exists a Grothendieck space π‘£βˆΆπ‘β†’π‘Œ such that 𝑋 factors through {𝑇(𝑑)}𝑑β‰₯0 Then 𝐢0 is 𝑋.

Proof. More generally, we will prove that, given π‘Ž>0, the adjoint semigroup is strongly continuous for π‘Œπ‘Ž if the operator 𝑇(π‘Ž) factors through a Grothendieck space π‘Œπ‘Ž..
Let {π‘‡βˆ—(𝑑)}𝑑β‰₯0 be a positive number. There exist a Grothendieck space 𝐢>0. and bounded linear operators π‘Ž>0 and 𝑑β‰₯π‘Ž such that the following diagram is commutative:fig.002(3.2) For every 𝑇(π‘Ž), the following diagram also commutes, due to semigroup properties: fig.003(3.3) Hence π‘Œπ‘Ž is π‘Žβˆ—-continuous. If π‘Œπ‘Ž and π‘’βˆΆπ‘‹β†’π‘Œπ‘Ž then π‘£βˆΆπ‘Œπ‘Žβ†’π‘‹ But 𝑑>π‘Ž is a Grothendieck space, and consequently π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž)=(𝑇(π‘‘βˆ’π‘Ž)𝑣)βˆ— From this, we can deduce that 𝑀 is weakly continuous for (𝑑𝑛)∈(π‘Ž,+∞). Finally, 𝑑𝑛→𝑑, is π‘£βˆ—π‘‡βˆ—(π‘‘π‘›βˆ’π‘Ž)π‘€βˆ—β†’π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž).-continuous for π‘Œπ‘Ž, which implies that π‘£βˆ—π‘‡βˆ—(π‘‘π‘›βˆ’π‘Ž)π‘€β†’π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž). is strongly continuous.

Remark 3.2. Our proof that semigroups factorizing through Grothendieck spaces have adjoint semigroup π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž) can be adapted to prove that the adjoint of a 𝑑β‰₯π‘Ž-semigroup on a Grothendieck space is also a π‘’βˆ—(𝑇(π‘‘βˆ’π‘Ž)𝑣)βˆ—=(𝑇(π‘‘βˆ’π‘Ž)𝑣𝑒)βˆ—=𝑇(𝑑)βˆ—-semigroup. This result can also be obtained by combining the results of 2.3.2 and 2.3.3 from [12].

Remark 3.3. Since reflexive Banach spaces are Grothendieck spaces, this gives an alternative proof that 𝑀-semigroups of weakly compact operators have adjoint semigroups which are 𝑑β‰₯π‘Ž thanks to the Davis, Figiel, Johnson, and Pelczynski factorization scheme (see [8]).

Remark 3.4. Theorem 3.1 also has applications in optimal control theory. See [7] for details.

The following theorem shows, in the spirit of Remark 3.3, new examples of semigroups satisfying the hypotheses of Theorem 3.1.

Theorem 3.5. Let {π‘‡βˆ—(𝑑)}𝑑β‰₯π‘Ž be a strongly continuous semigroup on an 𝐢>0-space. If, for 𝐢0 does not contain any isomorphic copy of 𝐢0, then 𝐢0 is a compact semigroup.

Proof. Let 𝐢>0, be an {𝑇(𝑑)}𝑑β‰₯0-space and 𝐴𝐿 a strongly continuous semigroup such that for 𝑑>0,𝑇(𝑑)𝑋 does not contain any isomorphic copy of 𝑙1. Then {𝑇(𝑑)}𝑑β‰₯0 applies bounded sets onto sets which contain a weakly Cauchy sequence. Since 𝑋-spaces are weakly sequentially complete, 𝐴𝐿 applies bounded sets onto weakly compact sets, due to the Eberlein-Smulian theorem. Therefore 𝑇(𝑑)βˆΆπ‘‹β†’π‘‹ is weakly compact. Since 𝑑>0,𝑇(𝑑)𝑋-spaces have the Dunford-Pettis property, the square of a weakly compact operator is compact; hence for 𝑙1 we have 𝑇(𝑑) with 𝐴𝐿 being weakly compact, 𝑇(𝑑) is compact.

Corollary 3.6. Every infinite-dimensional 𝑇(𝑑)-space contains a copy of 𝐴𝐿.

Proof. If not, we consider the semigroup defined, for each 𝑑>0 by 𝑑𝑇(𝑑)=𝑇22;(3.4), the identity on 𝑇(𝑑/2), which is strongly continuous and hence compact, and, by the Riesz lemma, 𝑇(𝑑) is finite-dimensional.

We finish this section with two results related to the aim of finding a characterization of the space 𝐴𝐿 of strong continuity of 𝑙1.

Theorem 3.7. If 𝑑 is 𝑇(𝑑)∢=𝐼-reflexive under 𝑋 and 𝑋 is isomorphic to a dual Banach space, then π‘‹βŠ™βŠ™ is {π‘‡βˆ—βˆ—(𝑑)}𝑑β‰₯0

Proof. 𝑋 is βŠ™-reflexive if and only if {𝑇(𝑑)}𝑑β‰₯0 is π‘‹βŠ™-reflexive (see [2]). If {π‘‡βˆ—(𝑑)}𝑑β‰₯0 is 𝐢>0.-reflexive, then the resolvent 𝑋 is weakly compact. Since βŠ™ we can conclude that each π‘‹βŠ™-reflexive Banach space is necessarily weakly compactly generated.
Then βŠ™ is weakly compactly generated and therefore 𝑋 has the Radon-Nikodym property since weakly compactly generated dual Banach spaces have that property (see [13]). Now [2, Corollary 6.2.4] is applied.

Theorem 3.8. If βŠ™ is an 𝑅(πœ†,𝐴)-space or an 𝑋=𝐷(𝐴)=linspan𝑅(πœ†,𝐴)𝐡𝑋,(3.5)-space, and βŠ™ is a π‘‹βŠ™-semigroup on π‘‹βŠ™, then 𝑋 is strongly continuous if and only if 𝐴𝑀 has bounded generator.

Proof. If 𝐴𝐿 is an {𝑇(𝑑)}𝑑β‰₯0-space, then 𝐢0 is an 𝑋-space and therefore there exists {π‘‡βˆ—βˆ—(𝑑)}𝑑β‰₯0 such that {𝑇(𝑑)}𝑑β‰₯0 is isometrically isomorphic to 𝑋 (see [14, page 18] for details). So 𝐴𝑀 is isometrically isomorphic to π‘‹βˆ—, which is a Grothendieck space with the Dunford-Pettis property. Since 𝐴𝐿 is a (Ξ©,Ξ£,πœ‡)-semigroup, it has bounded generator, by the Lotz theorem. So 𝑋 has bounded generator.
Now we suppose that 𝐿1(πœ‡) is an π‘‹βˆ—βˆ—-space and 𝐿∞(πœ‡) is strongly continuous. By [12, Lemma II.3.2], {π‘‡βˆ—βˆ—(𝑑)}𝑑β‰₯0 is strongly continuous. Since 𝐢0 is a Grothendieck space with the Dunford-Pettis property, it has bounded generator. Therefore {𝑇(𝑑)}𝑑β‰₯0 has bounded generator.

3.1. The Weak Measurability of the Adjoint Semigroup

Definition 3.9. Let 𝑋 be a compact Hausdorff space. A function 𝐴𝐿 is said to be universally measurable if it is {π‘‡βˆ—βˆ—(𝑑)}𝑑β‰₯0-measurable for all finite positive regular Borel measures {π‘‡βˆ—(𝑑)}𝑑β‰₯0 on π‘‹βˆ— A function {𝑇(𝑑)}𝑑β‰₯0 with 𝐾 a Banach space, is universally weakly measurable if πœ™βˆΆπΎβ†’β„‚ is universally measurable for all πœ‡ is called universally Pettis integrable if it is Pettis integrable with respect to every πœ‡

The following theorem of Riddle-Saab and Uhl (see [15]) is useful in providing examples of 𝐾.-semigroups for which πœ“βˆΆπΎβ†’π‘‹,

Theorem 3.10. Let 𝑋 be a separable Banach space and suppose that ⟨π‘₯βˆ—,πœ“(β‹…)⟩ is a bounded, universally weakly measurable function. Then π‘₯βˆ—βˆˆπ‘‹βˆ—.πœ“ is universally Pettis integrable.

Remark 3.11. If πœ‡. is weakly Borel measurable, that is, for all 𝐢0 and π‘‹βŠ™βŠ™=π‘˜π‘‹βŠ™βŠ™. the map 𝑋 is weakly Borel measurable on πœ“βˆΆπΎβ†’π‘‹βˆ— it follows from Theorem 3.10 that πœ“ is Pettis integrable. Combining this with Corollary 2.5 and the notes immediately following it, we get.

Corollary 3.12. Suppose that {π‘‡βˆ—(𝑑)}𝑑β‰₯0 is separable. If π‘₯βˆ—βˆˆπ‘‹βˆ— is weakly Borel measurable, then 𝜏>0.

Remark 3.13. It should be pointed out that weak measurability does not imply strong measurability. For example, let JF be the James function space, defined as the completion of the linear span of the characteristic functions of subintervals of π‘‘β†’π‘‡βˆ—(𝑑)π‘₯βˆ— with respect to the norm [0,𝜏], where the supremum runs over all partitions {π‘‡βˆ—(𝑑)}𝑑β‰₯0 of 𝑋. Define {π‘‡βˆ—(𝑑)}𝑑β‰₯0 on JF by π‘‹βŠ™βŠ™=π‘˜π‘‹βŠ™βŠ™ It is shown [2, pages 159-160] that the adjoint semigroup [0,1] is weakly Borel measurable (and hence Pettis integrable) but not ‖‖𝑓‖‖=sup(π‘˜βˆ’1𝑖=0|||ξ€œπ‘‘π‘–+1𝑑𝑖|||𝑓(𝑑)𝑑𝑑2)1/2,(3.6). In particular, it cannot be strongly measurable.

As it has been noted by van Neerven, as a consequence of the theorem of Odell-Rosenthal (see [16]), if 0=𝑑0<𝑑1<β‹―<π‘‘π‘˜=1 is separable and does not contain a closed subspace isomorphic to [0,1] then each 𝑇(𝑑) is the weakβˆ—-limit of some sequence in 𝑇(𝑑)𝑓=𝑓(π‘₯+𝑑mod1).(3.7)

If {π‘‡βˆ—(𝑑)}𝑑β‰₯0 is a 𝐢>0-semigroup on such a space, then 𝑋 is the pointwise limit of the continuous functions 𝑙1, which implies that it is Borel measurable. From this, we can deduce that π‘₯βˆ—βˆ—βˆˆπ‘‹βˆ—βˆ—

Now, using the WRNP of the dual space of any space with no copy of 𝑋. we will prove that if {𝑇(𝑑)}𝑑β‰₯0 factors through a separable space without copy of 𝐢0 then ⟨π‘₯βˆ—βˆ—,π‘‡βˆ—(𝑑)π‘₯βˆ—βŸ© is weakly measurable, thus giving some generality to the former results.

We will begin with a weakβˆ— version of the theorem of Riddle-Saab and Uhl.

Theorem 3.14. Let βŸ¨π‘‡βˆ—(𝑑)π‘₯βˆ—,π‘₯π‘›βŸ©, be a Banach space with no copy of π‘‹βŠ™βŠ™=π‘˜π‘‹βŠ™βŠ™. and suppose that 𝑙1, is a bounded, universally weakly measurable function. Then 𝑇(𝑑) is weak*-equivalent to a Pettis integrable function.

Proof. Let 𝑙1, be the weakβˆ—-integral of {π‘‡βˆ—(𝑑)}𝑑β‰₯0 that is, 𝑋 for each 𝑙1 and πœ“βˆΆπΎβ†’π‘‹βˆ—. πœ“ is weaklyβˆ—-countably additive. π›Ύπœ“βˆΆΞ£β†’π‘‹βˆ— does not contain a subspace isomorphic to πœ“, Then, by a classic result of Bessaga and Pelczynski (see [17, pages 48-49]), π‘₯,π›Ύπœ“ξ‚­=ξ€œ(𝐸)𝐸⟨π‘₯,πœ“βŸ©π‘‘πœ‡(3.8) does not contain a copy of π‘₯βˆˆπ‘‹ By [5, Theorem 4.2, pages 197-198] (see also [3, I.4.7]), 𝐸∈Σ is a measure in the strong topology of π›Ύπœ“
Now we use the WRNP of 𝑋: there exists an 𝑙1.-Pettis integrable function π‘‹βˆ— such that π‘™βˆž. By (3.8) and (3.9), we conclude that π›Ύπœ“β€‰β€‰π‘‹βˆ—.-almost everywhere, for all π‘‹βˆ—

Theorem 3.15. Let πœ‡ be a Banach space and let 𝑔 be a π‘₯,π›Ύπœ“ξ‚­=ξ€œ(𝐸)𝐸⟨π‘₯,π‘”βŸ©π‘‘πœ‡.(3.9)-semigroup defined on ⟨π‘₯,πœ“βŸ©=⟨π‘₯,π‘”βŸ© If for every πœ‡ factors through a separable Banach space with no copy of π‘₯βˆˆπ‘‹. then 𝑋 is weakly Borel measurable.

Proof. Let {𝑇(𝑑)}𝑑β‰₯0 be any closed and bounded interval contained in 𝐢0 There exists a Banach space 𝑋. with no copy of 𝑑>0,𝑇(𝑑) and bounded linear operators 𝑙1, and {π‘‡βˆ—(𝑑)}𝑑β‰₯0 such that the following diagram is commutative: fig.004(3.10) For every [π‘Ž,𝑏] the following diagram also commutes, due to semigroup property: fig.005(3.11) Then (0,∞). is weakβˆ—-continuous and hence Gelfand integrable with respect to the Lebesgue measure on π‘Œπ‘Ž
For each 𝑙1, we define π‘’βˆΆπ‘‹β†’π‘Œπ‘Ž where π‘£βˆΆπ‘Œπ‘Žβ†’π‘‹ is a countably additive vector measure which is also a vector measure in the strong topology, by the same argument used in the proof of Theorem 3.14. On the other hand, we have that π‘‘βˆˆ[π‘Ž,𝑏], is absolutely continuous with respect to the Lebesgue measure on π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž)
By the WRNP of [π‘Ž,𝑏]. there exists a Pettis-integrable function πΈβŠ†[π‘Ž,𝑏], such that ξ€œπ›Ύ(𝐸)=πΈπ‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž)π‘₯βˆ—π‘‘π‘‘,(3.12) Let 𝛾(𝐸) be a dense subset in 𝛾 From (3.12) and (3.13), we have [π‘Ž,𝑏]. for each π‘Œβˆ—π‘Ž,
Let 𝑓 denote the Lebesgue measure on ξ€œπ›Ύ(𝐸)=𝐸𝑓(𝑑)𝑑𝑑.(3.13) According to (3.14), there exists {𝑦𝑛}π‘›βˆˆβ„•, π‘Œπ‘Ž. such that π‘¦π‘›ξ€œπ›Ύ(𝐸)=πΈπ‘¦π‘›ξ€œπ‘“(𝑑)𝑑𝑑=πΈπ‘¦π‘›π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž)π‘₯βˆ—π‘‘π‘‘(3.14) for every π‘›βˆˆβ„•.
Now, take πœ‡ then [π‘Ž,𝑏]. and 𝑁𝑛 for every πœ‡(𝑁𝑛)=0 and 𝑦𝑛𝑓(𝑑)=π‘¦π‘›π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž)π‘₯βˆ—(3.15)
Since π‘‘βˆˆ[π‘Ž,𝑏]⧡𝑁𝑛. is dense in ⋃𝑁=βˆžπ‘›=1𝑁𝑛;, we have that πœ‡(𝑁)=0 for every 𝑦𝑛𝑓(𝑑)=π‘¦π‘›π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž)π‘₯βˆ—(3.16) and hence π‘‘βˆˆ[π‘Ž,𝑏]⧡𝑁𝑛 is weakly Borel measurable. Finally π‘›βˆˆβ„•. is also weakly Borel measurable.

Theorem 3.16. Let {𝑦𝑛}π‘›βˆˆβ„• and π‘Œπ‘Ž be as in Theorem 3.15. Then 𝑓(𝑑)=π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž)π‘₯βˆ—(3.17).

Proof. We are going to prove that π‘‘βˆˆ[π‘Ž,𝑏]⧡𝑁, is Pettis integrable.
As in Theorem 3.15, Let π‘£βˆ—π‘‡βˆ—π‘‘βˆ’π‘Ž by any closed bounded interval. We have the following factorization scheme: fig.006(3.19)we also have fig.007(3.20)Then, using the same argument, we conclude that there exists a Pettis-integrable function π‘’βˆ—ξ‚€ξ‚π‘‡(π‘‘βˆ’π‘Ž)π‘£βˆ—=𝑇(π‘‘βˆ’π‘Ž)π‘£π‘’βˆ—=𝑇(π‘‘βˆ’π‘Ž)𝑇(π‘Ž)βˆ—=π‘‡βˆ—(𝑑)(3.18) such that 𝑋 but then {𝑇(𝑑)}𝑑β‰₯0 and it is easy to see that π‘‹βŠ™βŠ™=π‘˜π‘‹βŠ™βŠ™ is Pettis integrable.

Remark 3.17. A Banach space {π‘‡βˆ—(𝑑)}𝑑β‰₯0 is said to have the Lotz property if every strongly continuous semigroup on [π‘Ž,𝑏]βŠ†(0,∞) has bounded generator. It is noticeable that Leung [18] has found a Lotz space without the Dunford-Pettis property, and it is also noticeable that to be a Grothendieck space is not enough to ensure the Lotz property, since in π‘“βˆΆ[π‘Ž,𝑏]β†’π‘‹βˆ—, π‘£βˆ—π‘‡βˆ—(π‘‘βˆ’π‘Ž)π‘₯βˆ—=𝑓(𝑑)almosteverywhere(3.21), we can easily define a π‘‡βˆ—(𝑑)π‘₯βˆ—=π‘’βˆ—ξ‚€ξ‚π‘“(𝑑)(3.22)-semigroup which is not uniformly continuous by means of π‘’βˆ—(𝑓(𝑑)) where 𝑋 is the standard unit basis.
Reworking on van Neerven results, we can show the relationship that exists among some of them (note that they were stated separately), thus giving necessary and sufficient conditions to ensure the uniform continuity of the adjoint of a strongly continuous semigroup defined on a Banach space whose dual has the Lotz property. This can be done as follows.
Let 𝑋 be a complex Banach space such that 𝑙𝑝 has the Lotz property, and let 1<𝑝<∞ be a 𝐢0-semigroup on 𝑇(𝑑)βˆΆπ‘™π‘β†’π‘™π‘,π‘₯∢=βˆžβˆ‘π‘›=1𝛼𝑛π‘₯𝑛↦𝑇(𝑑)π‘₯∢=βˆžβˆ‘π‘›=1π›Όπ‘›π‘’βˆ’π‘›π‘‘π‘₯𝑛,(3.23) with infinitesimal generator {π‘₯𝑛}
The following statements are equivalent.(1)𝑋 is uniformly continuous. (2)π‘‹βˆ— is strongly continuous. (3){𝑇(𝑑)}𝑑β‰₯0 for all 𝐢0(4)𝑋 for all 𝐴. where {𝑇(𝑑)}𝑑β‰₯0 is the Gelfand integral of {π‘‡βˆ—(𝑑)}𝑑β‰₯0 on limπœ†β†’βˆžβ€–πœ†π‘…(πœ†,π΄βˆ—)π‘₯βˆ—βˆ’π‘₯βˆ—β€–=0 with respect to the Lebesgue measure. (5)The quotient semigroup on π‘₯βˆ—βˆˆπ‘‹βˆ—. is strongly continuous.

Acknowledgment

This work is partially supported by CDCH of ULA under Project C-1335-05-05-A and by Universidad SimΓ³n Bolivar, Caracas, Venezuela.