Research article Special Issues

Fractional resolvent family generated by normal operators

  • The main focus of this paper is on the relationship between the spectrum of generators and the regularity of the fractional resolvent family. We will give a counter-example to show that the point-spectral mapping theorem is not valid for {Sα(t)} if α1; and we show that if {Sα(t)} is stable, then we can determine the decay rate by σ(A) and some examples are given; we also prove that Sα(t)x has a continuous derivative of order αβ>0 if and only if xD(IA)β. The main method we used here is the resolution of identity corresponding to a normal operator A and spectral measure integral.

    Citation: Chen-Yu Li. Fractional resolvent family generated by normal operators[J]. AIMS Mathematics, 2023, 8(10): 23815-23832. doi: 10.3934/math.20231213

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  • The main focus of this paper is on the relationship between the spectrum of generators and the regularity of the fractional resolvent family. We will give a counter-example to show that the point-spectral mapping theorem is not valid for {Sα(t)} if α1; and we show that if {Sα(t)} is stable, then we can determine the decay rate by σ(A) and some examples are given; we also prove that Sα(t)x has a continuous derivative of order αβ>0 if and only if xD(IA)β. The main method we used here is the resolution of identity corresponding to a normal operator A and spectral measure integral.



    Let α(0,2], an α-time resolvent family Sα(t) gives the solution to the α-order Cauchy problems

    Dαtu(t)=Au(t),t>0,u(0)=x,( in addtion u(0)=0 if α>1)

    by u(t)=Sα(t)x, where Dαt is the Caputo derivative of order α. See [28] for definitions and properties of fractional derivatives and fractional differential equations. This definition of fractional resolvent calculus has many applications, such as [16,24] for abstract Cauchy problems and [30,31] for engineering applications, and some applications on numerical simulations are given in [32,33].

    The main results of this article are the following three aspects: First, we give a counter-example of the point-spectral mapping theorem; second, we give the constant estimate of decay estimate of fractional resolvent family, and some examples are given at the end of this section. Third, we prove that DαβtSα(t) exist and continuous iff xD((IA)β).

    The main method we used in this paper is the resolution of identity corresponding to a normal operator A. By [25, Theorem 13.33], every normal operator A has a unique spectral decomposition and

    A=σ(A)λdP(λ). (1.1)

    If A generates a bounded fractional resolvent family {Sα(t)}, by using the properties of P(λ) and Eα(t) we can represent {Sα(t)} as follows:

    Sα(t)=σ(A)Eα(λtα)dP(λ). (1.2)

    It should be noticed that the above representation is a special case of functional calculus [15,25], which has been widely used to deal with semigroup problems, such as decay estimate, continuation, approximation, and resolvent representation, etc. More details about these topics can be found in [3,6,10,11,12,13]. The main question addressed in this article are: How to use this integral representation to show the relationship between the spectrum of the generator and the regularity of the fractional resolvent family, and the main results can be summarized as follows.

    The first one is the spectral mapping theorem of the resolvent family. In [8, Section 4.3], the authors discuss this problem in semigroup sense in detail and give a large number of examples to show that the conditions of theorems are optimal in some cases. In [19], authors proved that the spectral inclusion theorem is valid for the fractional resolvent family.

    Theorem 1.1. [19, Theorem 3.2] Suppose that there is an α-times resolvent family {Sα(t)} for A, where α(0,2], then

    (1) Eα(tασ(A))σ(Sα(t)).

    (2) Eα(tασap(A))σap(Sα(t)).

    (3) Eα(tασp(A))σp(Sα(t)).

    (4) Eα(tασr(A))σr(Sα(t)).

    Since the spectral mapping theorem is closely connected with the stability of the resolvent family and the decay rate can be given by spectral bound by using spectral mapping theorem (for example, [8, Proposition 1.7, Lemma 1.9]), it is very important to prove the spectral mapping theorem or construct a counter-example. Our first result is that we constrcut a normal operator A, which generates a fractional resolvent family {Sα(t)}, such that λσap(A)/σp(A) but Eα(λ)σp(Sα(1)).

    Another topic we discussed here is decay estimate, which is also an important subject. There are numerous articles and books discussing this subject and giving very detailed results, but we only mentioned one of these results here,

    Theorem 1.2. [2, Theorem 5.1.9] Let T be a C0-semigroup on Banach space X with generator A. Then

    s(A)=hol(ˆT)ω1(T)=abs(T)s0(A)ω(T). (1.3)

    An important question is whether we can prove a similar theorem for fractional resolvent families. The decay estimate of the fractional resolvent family has been given in many pieces of literature ([20, Proposition 3.3] and [21, Proposition 3.1]) and they show this theorem does not hold for the fractional resolvent family in general. In this paper, we proved that if fractional resolvent family {Sα(t)} generated by a normal operator A is stable, then it is polynomial stable and the constants are determined by spectral bound s(A), which can be seen as the Datko-Pazy theorem for fractional resolvent family. Additionally, we give some applications of this decay estimate.

    The third one is the partial answer to the question: under which condition can Sα(t)x have a continuous derivative of order β>0? It was proved by [17] that tS1(t)x has a continuous fractional derivative of order α>0 if and only if x belongs to D(bIA)α. In [9], the author proved that for {S2(t)}, the strongly continuous cosine functions, if S2(t)x has a continuous Riemann-Liouville fractional derivative of order αn=12,n=0.1.2....., then xD(bIA)α.

    Theorem 1.3. [9, Theorem 3.1] Let α>0, αn+12, n=0,1,.... Then

    E2α,βFα,E+2α,βFα.

    If we consider the Caputo fractional derivatives and let α(0,2), suppose {Sα(t)} is the fractional resolvent family generated by normal operator A. Then, by using spectral measure presentation, we can prove that Sα(t)x has a continuous derivative of order αβ>0 if and only if xD(IA)β.

    This paper is organized as follows. In Section 2, we give some necessary definitions and properties of Mittag-Leffler functions and fractional resolvent families. Section 3 focuses on the conditions for the generation of resolvent families by normal operators and the representation of resolvent families. Proofs of the above main results are given in Section 4, together with some examples.

    Throughout this paper, H is a separable Hilbert space, and L(H) is the Banach algebra of all bounded linear operators on H. We always assume that A is a closed unbounded operator, densely defined on H. We will denote by N(A), D(A), and R(A) the kernel, domain, and range of A respectively. Additionally, by ρ(A), σ(A), σp(A), σr(A) we denote the resolvent set, spectrum, point spectrum and residual spectrum of A, respectively. R(λ,A):=(λA)1 means the resolvent of A at λ if λρ(A), and notation s(A) means the spectral bound of σ(A), s(A):=sup{(λ)|λσ(A)}; by the Hahn-Banach theorem σr(A)=σp(A), where A is the adjoint of A. By W(A) we denote the numerical range of A if A is defined on Hilbert space H,

    W(A)={Ax,xC|xD(A),x=1}.

    And sector Σθ is defined as

    Σθ={λC|λ0and|argλ|<θ}

    for θ(0,π) and Σ0=(0,).

    We recall two important functions in the theory of fractional calculus. For details of these special functions and the general theory of fractional calculus, we refer to [1,24] and the references therein.

    The Mittag-leffler function Eα,β(z) is defined by

    Eα,β(z):=n=0zβΓ(αn+β)=12πiHaμαβeμμαzdμ,zC,

    where α,β>0, Ha is the Hankel contour which starts and ends at , and encircles the disc |t||z|1α counter clockwise. We use Eα(t):=Eα,1(t) for short. The Mittag-Leffler function Eα(t) satisfies the fractional differential equation

    DαtEα(ωtα)=ωEα(ωtα),

    where Dαt is the Caputo derivative of α-order (see [4]). The most important properties of this function are associated with their Laplace integral

    0eλttβ1Eα,β(stα)dt=λαβλαs,(λ)>|s|1α,

    and their asymptotic expansion as z. For 0<α<2 and β=1,

    Proposition 2.1. [24, Proposition 3.5] Let α(0,2) and

    απ2<θ<min{π,απ}.

    Then we have the following asymptotics for formulas in which N is an arbitrary positive integer

    Eα(z)=1αexp(z1α)+ϵα(z),|argz|θ,|z|, (2.1)
    Eα(z)=ϵα(z),θ|arg(z)|π,|z|, (2.2)

    where

    ϵα(z)=N1n=1znΓ(1αn)+O(|z|N).

    From the asymptotic expansion one knows that Eα(ωtα)=O(tα) as t when ω>0.

    Here we define fractional resolvent families and list some basic properties [4,18].

    Definition 2.2. Let 0<α2, a family {Sα(t)}t0L(X) is called an α-times resolvent family generated by A if the following conditions are satisfied:

    (1) Sα(t) is strongly continuous for t0 and Sα(0)=I;

    (2) Sα(t)AASα(t) for t0;

    (3) for xD(A), the resolvent equation

    Sα(t)x=x+At0gα(ts)Sα(t)xds

    holds for all t0, where gα(t):=tα1Γ(α).

    By this definition, we know that a 1-times resolvent family is exactly a C0-semigroup, and a 2-times resolvent family is a cosine operator.

    Definition 2.3. An α-times resolvent family Sα(t) is said to be exponentially bounded if there exists a constant M1 and ω0 such that Sα(t)Meωt for every t0. Sα(t) is called bounded if ω can be taken as 0, i.e., Sα(t)M for all t0.

    Let θ0(0,π], an α-times resolvent family Sα(t) is called analytic of angle θ0 if Sα(t) admits an analytic extension to the sectorial sector Σθ0:={zC:z0and|argz|<θ0}. An analytic α-times resolvent family Sα(t) is called to be bounded if Sα(z) is uniformly bounded for zΣθ for any 0<θ<θ0.

    Lemma 2.4. [4, Theorems 2.8 and 2.9] Let 0<α2, Sα(t) be an α-times resolvent family generated by A. Then Sα(t)Meωt for every t0 if and only if (ωα,)ρ(A) and

    dndλn(λα1R(λα,A))Mn!(λω)n+1,λ>ω,nN0.

    In this case {λα:Reλ>ω}ρ(A) and

    λα1R(λα,A)x=0eλtSα(t)xdt,(λ)>ω

    for every xX. In particular, if Sα(t) is bounded, then supλ>0λR(λ,A)<.

    The relationship between the generator of the analytic bounded resolvent operator and the sectorial operator can be narrated as follows.

    Lemma 2.5. [5, Lemma 2.7] Let α(0,2) and θ0(0,min{π2,παπ2}). The following assertions are equivalent.

    (1) A generates a bounded analytic α-times resolvent operator of angle θ0.

    (2) Σα(π2+θ)ρ(A) and for every θ(0,θ0) there is a constant Mθ such that

    λR(λ,A)Mθ,λΣα(π2+θ).

    (3) Asect(πα(π2+θ0)).

    The following subordination principle is a very powerful tool. For a more general subordination principle for the fractional powers of the generators see [18], and for regularized resolvent families see [1].

    Lemma 2.6. (Subordination principle) Let 0<β<α2. If A generates an exponentially bounded α-times resolvent family Sα(t), then A generates exponentially bounded analytic β-times resolvent family Sβ(t) which is subordinated to Sα(t) by

    Sβ(t)=0tβαWβα,1βα(stβα)Sα(s)ds,t>0. (2.3)

    Moreover, if Sα(t) is bounded, then Sβ(t) is analytic and bounded in a sector with an angle smaller than (α/β1)π/2.

    Where Wβα,1βα(stβα) is the Wright-type function, for details of this function, we refer to [1,24,28].

    Let (Ω,Σ,μ) be a σ-finite measure space. Let 1p<, define Banach space X:=Lp(Ω,μ), and suppose q is a measurable function on X, define set qess(Ω):

    qess(Ω):={λC:μ({sΩ:|q(s)λ|<ϵ})0,ϵ>0}

    be the essential range of function q. Using function q we can define a multiplication operator Mq on X.

    Mqf:=qffD(Mq):={fX:qfX}. (3.1)

    Some properties of the multiplication operator are summarized as follows.

    Lemma 3.1. [8, Proposition 4.10] Let Mq be the multiplication operator on X=Lp(Ω,μ) defined by measurable function q and (3.1), the following conclusion is valid:

    (1) Mq is a closed operator with a dense domain.

    (2) Mq is a bounded operator if and only if q is an essential bounded function, that is, essential range qess(Ω) is a bounded set, and

    Mq=q:=sup{|λ|:λqess(Ω)}.

    (3) The spectral of Mq is equal to the essential range of q.

    Next, we give a conclusion about the generation of resolvent families by multiplication operators.

    Theorem 3.2. Let 0<α<2 and q is a measurable function, q:ΩC, if

    ˜q:=sup{(q(x)1α):q(x)qess(Ω)¯Σαπ2,xΩ}<.

    Then the operator family Sqα(t) defined by

    Sqα(t)g:=Eα(tαq)g,gLp(Ω,μ)

    is a α-times resolvent family generated by Mq. And Sqα(t) is uniformly bounded if and only if qessCΣαπ2.

    Proof. By asymptotic estimate of Mittag-Leffler function (2.2),

    sup{|Eα(z)|:|arg(z)|απ2}<,

    and when z,

    Eα(z)=O(e(z1α)),|arg(z)|απ2.

    Because ˜q<, by Lemma 3.1, operator family Sqα(t) is exponentially bounded,

    Sqα(t)=Eα(tαq)Met˜q.

    Since

    Sqα(t)ggp=Ω|Eα(tαq(x))1|p|g(x)|pdx,

    so the strong convergence of Sqα(t) can be proved directly by the dominant convergence theorem. Then it is easy to see that operator family Sqα(t) is an α-times resolvent family generated by Mq.

    The following unitary isomorphism theorem is a classical theorem describing normal operators.

    Theorem 3.3. [15, Appendix D, Spectral Theorem] Suppose operator A is a normal operator on H, then there exist a σ-finite measure space (Ω,Σ,μ) and measurable function q:ΩC, such that operator A is unitary isomorphic to a multiplication operator Mq defined on L2(Ω,μ). This means there exists a unitary operator UL(H,L2(Ω,μ)), such that

    A=UMqU=U1MqU,

    and σ(A)=σ(Mq)=qess(Ω).

    From the above discussion, it can be seen that if the normal operator A unitary isomorphic to the multiplication operator Mq which is defined on L2(Ω,μ), and qess(Ω)CΣα2π, then A generates a bounded α-times resolvent family. Additionally, the converse can be proved directly by Theorems 2.4 and 3.3.

    Recall that for a normal operator A, there is a unique resolution of identity P(λ), which satisfies

    Ax,y=σ(A)λdP(λ)x,y,xD(A),yH. (3.2)

    Then for every measureble function f:σ(A)C, we can define operator f(A) as follows:

    f(A):=σ(A)f(λ)dP(λ),

    with domain

    D(f(A)):={xH:σ(A)|f(λ)|dP(λ)x,x<}.

    For more information about the resolution of identity and proofs please refer to [25, Section 13], especially [25, Lemma 13.22, Theorems 13.23 and 13.24].

    Now suppose that A is a normal operator with σ(A)CΣα2π, since Eα(tαλ) is bounded in σ(A), therefore we can define an operator family {Eα(tαA)}t0 with domain D(Eα(tαA))=H,

    Eα(tαA):=σ(A)Eα(tαλ)dP(λ).

    The operator family {Eα(tαA)}t0 is uniformly bounded and for every μ>0,

    0Eα(tαA)eμtdt=σ(A)μα1μλdP(λ)=μα1R(μ,A).

    Since the strong continuity of Eα(tαA) can be easily deduced by the dominant convergence theorem, which means that {Eα(tαA)}t0 is the bounded α-times resolvent family generated by A.

    Combining the above discussion, we deduce the following proposition.

    Proposition 3.4. Suppose A is a densely defined, closed normal operator on H, α(0,2). Then operator A generates an bounded α-times resolvent family {Sα(t)}t0 if and only if σ(A)CΣα2π. Moreover, if A generates a bounded fractional resolvent family {Sα(t)}t0, then it can be represented as:

    Sα(t)=σ(A)Eα(tαλ)dP(λ), (3.3)

    where P(λ) is the resolution of identity corresponding to A which satisfies the Eq (3.2).

    In this section, we give some applications of Proposition 3.4. We shall use the properties of zeros of the Mittag-Leffler function several times, then distributions of zeros of the Mittag-Leffler function can be found in [24, Sections 3.5 and 4.6].

    It has been proved that if A generates a strong-continuous semigroup {T(t)}, then we have

    σp(A){0}=etσp(A). (4.1)

    This equation is called the spectral mapping theorem for point spectral or point-spectral mapping theorem, the proof of this equation can be found in [8, Chapter 4, Section 3.7]. In paper [19], authors prove the point-spectral inclusion theorem for a fractional resolvent family

    Eα(σp(A)tα)σp(Sα(t)) (4.2)

    by using the following lemma.

    Lemma 4.1. [19, Lemma 3.1] Denote ma(t)=tα1Eα,α(atα), aC. Suppose {Sα(t)} is a fractional resolvent family generated by A with α(0,2], then

    (aA)t0ma(s)Sα(ts)xds=Eα(atα)xSα(t)x,xX. (4.3)
    t0ma(s)Sα(ts)(aA)xds=Eα(atα)xSα(t)x,xD(A). (4.4)

    Here, we will use Proposition 3.4, Lemma 4.1, and properties of resolution of identity to construct an operator A such that

    0λσap(A)σp(A),Eα(λtα)σp(Sα(t)),1α(0,2]. (4.5)

    Let A be a normal operator which satisfies Proposition 3.4, then the fractional resolvent family {Sα(t)} generated by A is given by

    Sα(t)=σ(A)Eα(tαλ)dP(λ), (4.6)

    where P(λ) is the resolution of identity corresponding to A. Moreover, suppose operator A satisfies the following condition.

    Condition 1: Let λ0σ(A)σp(A) and λ1σ(A){λ0} satisfies P(λ1)>0 and Eα,α+1(λ0)=Eα,α+1(λ1)=0.

    There indeed exists an operator A satisfies Condition 1, since there are infinitely zeros of Eα,α+1(λ) lies in the CΣα2π.

    Example 4.2 By using Lemma 4.1, [24, (4.4.10)] and let t=1, we have

    (λ0A)10mλ0(s)Sα(1s)xds=(λ0A)10mλ0(s)σ(A)Eα((1s)αλ)dP(λ)xds=(λ0A)σ(A)10mλ0(s)Eα((1s)αλ)dsdP(λ)x=(λ0A)σ(A)fλ0(λ)dP(λ)x=Eα(λ0)xSα(1)x,

    where

    fλ0(λ)=λEα,α+1(λ)λ0λ. (4.7)

    Then we have

    fλ0(λ1)=0,

    Since P(λ1)>0 we know that P(ω)>0, where ω={λσ(A):fλ0(λ)=0}.

    Then choose 0x0R(P(ω)), by using the proof of [25, Theorem 13.27(a)] we have

    σ(A)fλ0(λ)dP(λ)x0=0. (4.8)

    That is,

    Eα(λ0)x0Sα(1)x0=0, (4.9)

    this means Eα(λ0)σp(Sα(1)) with λ0σp(A).

    Since we construct this example in Hilbert space and A is a normal operator, then we can prove the following claim for A satisfies Condition 1 directly,

    Eα(σrtα)σr(Sα(t)). (4.10)

    One question is how to add some more conditions on normal generator A to ensure the correctness of the point-spectral mapping theorem. Notice that we prove Eα(λ0)x0Sα(1)x0=0 only for t=1, so if we want to prove the point-spectral mapping theorem for all fractional resolvent family, we at least should prove that for every t>0,

    σ(A)λ0Eα,α+1(λ0tα)λEα,α+1(λtα)λ0λtαdP(λ) (4.11)

    is an injective operator then the point-spectral mapping theorem is valid for the fractional resolvent family with this normal generator. However, this is difficult since instead of explicit representation of zeros, we only have the asymptotic behavior of zeros of Mittag-Leffler function Eα,α(λ) except α=1 [24, Sections 3.5 and 4.6], in this case, E1,1(λ)=eλ has no zeros and the fractional resolvent operator is a strongly continuous semigroup and satisfies the point-spectral mapping theorem.

    It should be noticed that in strong continuous semigroup sense (α=1), the spectral mapping theorem holds if this semigroup is eventually norm-continuous [8, Chapter 4, 3.10], but we can find an operator satisfies Condition 1 which generates an analytic fractional resolvent family (α(0,2),α1), so we conclude that the point-spectral mapping theorem does not hold for the fractional resolvent family in general, even if for analytic fractional resolvent family or vector-valued cosine function.

    The method we used in the above example can be used to construct another example that shows that there exists a fractional resolvent family {Sα(t)} and a positive constant t0 such that

    Sα(t0)=0.

    It is well known that if there is a t0 and a semigroup {T(t)} such that

    T(t0)=0,

    then

    T(t)=0,tt0,

    then we conclude that for any postive constant ω, we can find another constant M such that

    T(t)Meωt,

    then we conclude that the generator of {T(t)} has an empty spectrum set, which is impossible if {T(t)} is a semigroup of normal operator,

    Example 4.3. Denote set B={λ:Eα(λ)=0,λCΣαπ2} and let A be the normal operator with σ(A)=B. Then we know that A generates a fractional resolvent family {Sα(t)} with representation

    Sα(t)=σ(A)Eα(λtα)dP(λ). (4.12)

    Then we have

    Sα(1)=BEα(λ)dP(λ)=0. (4.13)

    This construction can not be applied on semigroup because E1(λ)=eλ has no zeros.

    It has been proved that if A generates a stable semigroup, then this semigroup is exponentially stable and there exists a constant ω<0 such that

    σ(A){λ:(λ)<ω}.

    But a similar property has not been proved for the general fractional resolvent family. By using Proposition 3.4 we can prove the following theorem.

    Theorem 4.4. Suppose A is a normal operator which generates a stable fractional resolvent family {Sα(t)}, then there exists a constant ω>0 such that

    ω+σ(A)CΣαπ2, (4.14)

    and

    Sα(t)1ωΓ(1α)tα+o(t2α),t. (4.15)

    Proof. We prove the first claim by a contradiction. If there is no such a constant ω satisfies the Eq (4.14), then there must be a sequence {zn}σ(A) such that

    (z1αn)0,asn. (4.16)

    Since {Sα(t)} is stable, then 0ρ(A) and we can choose t0 big enough and ϵ<13α such that Sα(t)ϵ, and tα0zn satisfies Proposition 2.1,

    Eα(tα0zn)=1αexp((tα0zn)1α)+ϵα((tα0zn)).

    Since (z1αn)0, we can choose n0 big enough and t1>t0 such that Sα(t1)<ϵ and

    |Eα(tα1zn0)|>12α. (4.17)

    By spectral inclusion theorem [19, Theorem 3.2] we have

    Eα(tα1zn0)σ(Sα(t1)). (4.18)

    Thus

    13α>ϵ>Sα(t1)|Eα(tα1zn0)|>12α. (4.19)

    This is a contradiction. Then there exists a constant ω>0 such that

    ω+σ(A)CΣαπ2.

    The second claim can be proved by Propositions 2.1 and 3.4 directly. Since

    Sα(t)=σ(A)Eα(λtα)dP(λ), (4.20)

    then for t big enough, we have

    Sα(t)max{Eα(λtα),λσ(A)}1αexp((ωtα)1α)+ϵα(ωtα)1ωΓ(1α)tα+o(t2α).

    We shall give some examples to show how to use Theorem 4.4, suppose Δ is the n-dimension Laplace operator. More details about the following operators can be found in [26,29].

    Example 4.5. Let H=L2(Rn),n>3 and operator A=12Δ+λV,λ>1. Then, by [26, Theorem B5.2] we know that if 0VLpLq,p<n2<q, and

    α2(1)=lneA=0,

    then

    limtetA

    exists, then for every ω>0, A+ω=12Δ+λV+ω generates a exponentially stable semigroup. Since operator A+ω is a normal operator, by using Theorem 4.4 we know that the solution of fractional differential equation with α<1,

    iαDαtu(t,x)=(12Δ+λV(x))u(t,x)+ωu(t,x),t>0u(0,x)=f(x)L2(Rn)

    satisfies the Eq (4.15), that is

    u(t,x)L2(Rn)cos(απ2)ωtαΓ(1α)+o(t2α),t. (4.21)

    Example 4.6. Let ΔS be the Laplace operator on Sn,n>1, the n-dimension sphere, and define operator A on L2(Sn) as

    A=(ΔS+(n1)24)12.

    Then by [29, Proposition 4.1] we know that A is self-adjoint and

    σ(A){12(n1)+k:k=0,1,2,...}

    Thus, for every α(0,2), the equation

    iαDαtu(t,x)=(ΔS+(n1)24)12u(t,x),t>0u(0,x)=f(x)L2(Sn)

    has a solution u(t,x) satisfies

    u(t,x)L2(Sn)2cos(απ2)n1tαΓ(1α)+o(t2α),t. (4.22)

    Example 4.7. Let ΔS be the Laplace operator on Hn,n>1, the n-dimension hyperbolic space, defined as

    Hn={vRn+1:v,v=1,vn+1>0},

    Since Hn is a compact Riemannian manifold, then by [29, Proposition 2.1] and the proof of [29, Proposition 5.1] we know that Δ is self-adjoint and

    σ(Δ)(,14(n1)2].

    Then we know that for every α(0,2), the equation

    iαDαtu(t,x)=Δu(t,x),t>0u(0,x)=f(x)L2(Hn)

    has a solution u(t,x) satisfies

    u(t,x)L2(Hn)4cos(απ2)(n1)2tαΓ(1α)+o(t2α),t. (4.23)

    It has been proved in [17] that for every exponentially bounded semigroup {T(t)} with generator A and xA, that T(t)x has a continuous fractional derivative of order α>0 if and only if x belongs to D((bIA)α) for some bρ(A). More precisely, in [9], the following theorem has been proved.

    Theorem 4.8. [9, Theorem 2.1] Let α>0 and {T(t)} be the exponentially bounded semigroup generated by A which satisfies

    T(t)Meωt.

    Then

    E+α,β=Fα. (4.24)

    Where Fα:=D((bIA)α) with bρ(A) and β>ω, xE+α,β means there exists a continuous function f such that

    eβtT(t)x=eiπαΓ(α)t(st)α1f(s)ds.

    And similar results for vector-valued cosine function family are also proved in [9]. It should be noticed that the fractional derivative used in these papers are Riemann-Liouville fractional derivative, which is different from the Caputo fractional derivative we used here, by using Proposition 3.4 we can prove a similar result for fractional resolvent family generated by the normal operator.

    Theorem 4.9. Let {Sα(t)} be the bounded fractional resolvent family generated by normal operator A. Fβ=D((IA)β),β>0 and xEα,β means there exists a continuous operator family {f(t)} such that

    DαβtSα(t)x=f(t)x, (4.25)

    then the following two assertions hold:

    (1) if αβ<1, then

    Fβ=Eα,β.

    (2) If αβ1, then

    FβEα,β.

    Proof. We only need to prove this theorem for β<1. If β1, then xD(Aβ)D(A) means AxD(Aβ1), by definition of fractional resolvent family we know that

    xD(A)iffDαtSα(t)x=ASα(t)x=Sα(t)Ax. (4.26)

    Now we assume β<1 and xFβ, then Sα(x)=(IA)βSα(t)(IA)βx, since 1(1λ)β is bounded in σ(A) and (IA)β is a bound operator, then we have

    Sα(t)x=(IA)βSα(t)(IA)βx=σ(A)1(1λ)βEα(λtα)dP(λ)(IA)βx.

    Since we have ([24, Equation 4.4.5])

    1Γ(β)t0(ts)β1Eα(λsα)ds=tβEα,β+1(λtα). (4.27)

    Then we can define the operator h(t) as

    h(t):=tα(1β)σ(A)λ(1λ)βEα,α(1β)+1(λtα)dP(λ). (4.28)

    Now using the asymptotic formula of Mittag-Leffler function [24, Theorem 4.3] and dominant convergence theorem, we deduce that h(t) is a strongly continuous operator, and for every xD((IA)β),

    (gαh)(t)(IA)βx=σ(A)gα(t)(gα(1β)(t)λ(1λ)βEα(λtα))dP(λ)(IA)βx=σ(A)gα(1β)(t)1(1λ)β(Eα(λtα)+k(t))dP(λ)(IA)βx=(gα(1β)(IA)βSα)(t)(IA)βx(gα(1β)k)(t)(IA)βx=(gα(1β)Sα)(t)x(gα(1β)k)(t)(IA)βx,

    where k(t) are defined as

    k(t)=1ifα<1,ork(t)=tΓ(α+1),if1<α<2. (4.29)

    Thus

    Sα(t)x=((gαβh)(t)+k(t))(IA)βx, (4.30)

    this shows that Sα(t)x is continuous differentiable of order αβ.

    Next we suppose that αβ<1 and Sα(t)x is continuous differentiable of order αβ, thus there exists a continuous operator f(t) such that

    Sα(t)x=(gαβf)(t)x. (4.31)

    Since

    Eα(λtα)=gαβ(t)tαβEα,1αβ(λtα),

    thus by the uniqueness of Laplace transform we deduce that

    f(t)x=tαβσ(A)Eα,1αβ(λtα)dP(λ)x. (4.32)

    Then we can prove that

    h(t)x=σ(A)λβ+11λEα(λtα)dP(λ)x (4.33)

    is well defined too, by using the asymptotic formulas of Eα,1αβ(λtα) and λβEα(λtα). Then

    (gαh)(t)x=σ(A)Eα(λtα)λβ1λ+k(t)dP(λ)x=SαAβ(IA)1x+k(t)x, (4.34)

    this shows that SαAβ(IA)1x is continuous differentiable of order α, then Aβ(IA)1xD(A) and xD(Aβ).

    There is proof of assertion (2) without using Proposition 3.4, instead, we use the Theorem 3.3. By using this theorem and the uniqueness of the Laplace transform we deduce that

    0eλtSα(t)xdt=λα1(λαA)1x=λα1(λαUqU)1x=Uλα1(λαq)1Ux=U0eλtEα(qtα)dtUx=0eλtUEα(qtα)Uxdt,

    that is

    Sα(t)x=UEα(qtα)Ux. (4.35)

    Since we know that Sα(t)x is continuous differentiable of order αβ, then

    DαβtSα(t)x=UDαβtEα(qtα)Ux=UtαEα.1αβ(qtα)Ux, (4.36)

    this means for every t>0, tαEα.1αβ(qtα)UxL2(Ω,μ), then by using asymptotic beheavior of Mittag-Leffler function we have

    qβ+1(1q)Eα(qtα)UxL2(Ω,μ),

    and

    Uqβ+1(1q)Eα(qtα)UxH,

    thus

    gα(t)Uqβ+1(1q)Eα(qtα)Ux=Ugα(t)qβ+1(1q)Eα(qtα)Ux=Uqβ(1q)Eα(qtα)Ux+k(t)x=Sα(t)Aβ(IA)1x+k(t)x.

    This shows Sα(t)Aβ(IA)1x is continuous diffenertiable of order α and xD(Aβ).

    By using the resolution of identity of a normal operator A, we deduce an integral representation of the fractional resolvent family generated by A. And then by using this representation, some applications are given here, especially, we show that the spectral mapping theorem does not hold for the fractional resolvent family.

    The author declares he has not used Artificial Intelligence (AI) tools in the creation of this article.

    The author declares no conflict of interest.



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