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Some Conclusions about α-times Integrated C Semigroups
Chunjing Liu and Xiaoqiu SongMathematic Department of College of ScienceChina University of Mining and Technology
Jiangsu, Xuzhou,China, 221008
Tao WangDepartment of Mathematics
Jiangsu Houji Senior High SchoolJiangsu, Xuzhou,China, 221008
Abstract— This paper gets two main conclusions about α-times integrated C semigroups based on the Hille exponentialformulas of the other kinds of semigroups, the generationtheorem in terms of the Laplace transform and the propertiesof exponential bounded α-times integrated C semigroups. Oneis the representation theorem, the other is the Laplace inversetransform as well as two deductions.
Index Terms— Intelligent Control; α-times integrated C semi-groups; Representation theorem; Exponential formulas; Laplaceinverse transform
I. INTRODUCTION AND PRELIMINARIES
Functional analysis is one of the mathematics foundations
that control theory and system science develope on. The basic
concepts of functional analysis form at the end of the 19th
century and the beginning of the 20th century, after decades
of development, as an independent branch of mathematics,
it becomes mature enough and seepage in various fields
gradually, including mechanical, electromagnetic field theory,
control theory and system science, etc. Operator theory,
especially the linear operator theory, is the main theory of
the functional analysis, the solving of operator equations
and the reaserch on the solvability of linear operators, have
provided theory basis for the solving of all sorts of algebraic
equations, the differential equations and the comprehensive
control system. Almost all the problems in control theory
can be described in terms of space and operator involved in
functional analysis. For example, the theory of the dual space
and the adjoint operator can explain almost all the duality
theorems in control theory, and the discovery of all these
theorems is the result of the direct deduction of mathematics.
Semigroup of operator, as an important branch of the
operator theory, has an abroad application in partial differ-
ential equations system theory, distributed parameter control
theory, the approximation and quantum mechanics theory.
For example, the solution of the control system model that
represented in developing equation in Banach space mainly
depends on Hille Yosida semigroup and Goldstein semigroup
in distributed parameter control system.
∗This work is partially supported by The Fundamental Research Fundsfor the Central Universities(2010LKSXO8)
The classical theory of C0 semigroups of operators [1] is a
powerful method in studying the first order Cauchy problem.
Later, two kinds of generalizations of C0 semigroups were
developed by some authors. One is C semigroups, it was
studied first by Da Prato [2] and later by Davies and Pang
[3]. The other is n-times integrated semigroups, which was
introduce by Arendt [4] firstly, and further developed by
Kellerman and Hieber [5], further extension to fractionally
integrated semigroups were carried out by Hieber [6]. Re-
cently, Li Yuanchuan and Shaw SenYen [7] have studied
a nature generalization of above two notations to a wider
class of operator families, called n- times integrated Csemigroups, and then it was generalized to α- times integrated
C semigroups by Kuo Chungcheng and Shaw SenYen [8].Based on these results, this paper aims to study the
representation theorem and the Laplace inverse transform of
α-times integrated C semigroups which have considerable
practical significance.
Next, we give the notations that will be used the in the
following:
let X be a Banach space and B(X) be the set of all
bounded linear operators from X to itself, ρ(A) is the
resolvent set of A.
Let j−1 := δ0, the Dirac measure at 0, and for r > −1,
letjr(t) = tr
Γ(r+1) , where Γ(·) is the Gamma function.
Let f(·) be a continuous function, β ≥ −1, the convolution
is defined as follows:
(jβ ∗ f)(t) =
{ ∫ t
0
(t−s)β
Γ(β+1) f(s)ds, β>−1∫ t
0f(t−s)dδ0(s)=f(t), β=−1
,
For α > 0, let [α], (α) be the integer part, the decimal
part of α, and Cα([0, T ], X) be the functions that are αorder continuously differentiable on [0, T ]. Now we define
the fractional differential and integral of functions:
The α times repeated integral (Iαf)(t) = (jα−1 ∗ f)(t) (1)The α order derivative
(Dαf)(t) = (d
dt)[α]+1(j−(α) ∗ [f − f(0)])(t) (2)
DEFINITION1.1. let C ∈B(X) and α ≥ 0. A family
{S(t) : t ≥ 0} in B(X) is called an α-times integrated
C semigroup(see [7] for the case α = n ∈ N) if
2011 International Conference on Internet Computing and Information Services
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DOI 10.1109/ICICIS.2011.22
61
1) S(·)x :[0,∞)→X is continuous for each x∈X;
2) S(t)S(s)x = 1Γ(α) [
∫ s+t
s− ∫ t
0](s + t− r)α−1S(r)Cxdr
for x∈X and s, t ≥ 0, and CS(0) = S(0)C.
It is called a C semigroup(see [2][3]) if
2′) S(0) = C and S(t)S(s) = S(t + s)C for all s, t ≥ 0.
S(·) is said to be nondegenerate if
3) S(t)x = 0 for all t > 0 implies x = 0.
S(·) is said to be exponentially bounded if
4) there are constants M, ω > 0 such that ‖S(t) ‖≤ Meωt
for all t ≥ 0When C = I , an α-times integrated C semigroup reduce to
an α-times integrated semigroup.
Let α ≥ 0, the generator A of a nondegenerate α-times
integrated C semigroup S(·) is defined as
5) x ∈ D(A) and for all t ≥ 0
Ax = y ⇔ S(t)x − jα(t)Cx =∫ t
0
S(s)yds
LEMMA1.2. Let C∈B(X) be an injection, α ≥ 0, a
strong continuous family {S(t) : t ≥ 0} in B(X) is called
an exponentially bounded α-times integrated C semigroup
with generator A, if and only if {S(t) : t ≥ 0} satisfies 4),S(0) = 0, CS(·) = S(·)C, and for each λ > ω, x ∈ X
R(λ,A)Cx = λα
∫ ∞
0
e−λtS(t)xdt
LEMMA1.3. Let A be the generator of an nondegenerate
α-times integrated C semigroup {S(t) : t ≥ 0}, then
1) S(t)x ∈ D(A) and AS(t)x = S(t)Ax for all x ∈ D(A)and t ≥ 0;
2)∫ t
0S(s)xds ∈ D(A) and A
∫ t
0S(s)xds = S(t)x −
jα(t)Cx for all x ∈ X and t ≥ 0.
II. REPRESENTATION THEOREM
In this section, first we get some properties about α-times
integrated C semigroup: then based on the Hille exponential
formulas of the other kinds of semigroups ([1], [9] − [11]),we deduce the representation theorem.
THEOREM2.1. Let [0,∞) ⊂ ρ(A), α, β ≥ 0, t ≥0, {S(t)} is an α-times integrated C semigroup, then T (t) =(jβ ∗ S)(t) is an α + β + 1-times integrated C semigroup.
Proof. When S(t) is an α-times integrated C semigroup,
R(λ,A)Cx = λα
∫ ∞
0
e−λtS(t)xdt for each λ > ω
so
∫ ∞
0
e−λtT (t)xdt =∫ ∞
0
e−λt(jβ ∗ S)(t)xdt
=1
λβ+1
∫ ∞
0
e−λtS(t)xdt
=1
λα+β+1R(λ,A)Cx
that is proved by lemma1.2.
THEOREM2.2. Let A be the generator of an exponentially
bounded α-times integrated C semigroup {S(t) : t ≥ 0},
then
1) S(t)x ∈ Ck(R+, X), and Sk(t)x = S(t)Akx +∑ki=1 jα−i(t)CAk−ix for all x ∈ D(Ak), k = 1, 2, · · · [α];2) S(t)x ∈ Cθ(R+, X), and (DθS)(t)x =∑[θ]+1j=1 jα−(θ)+1−j(t)CA[θ]+1−jx+(j−(θ)∗S)(t)A[θ]+1x for
all x ∈ D(A[θ]+1), 0 ≤ θ < α;
3) (DθS)(0)x = 0 for all x ∈ D(A[θ]+1), 0 ≤ θ < α,
and (DαS)(0)x = x when x ∈ D(A[α]+1)Proof. S(t)x ∈ Ck(R+, X) is obvious from [6], now
differentiate the equation 2) in lemma1.3 with respect to t,we obtain the following equalities:
S′(t)x =αtα−1
Γ(α + 1)Cx + S(t)Ax
= jα−1(t)Cx + S(t)Ax
S′′(t)x = jα−2(t)Cx + S′(t)Ax
= jα−2(t)Cx + jα−1(t)CAx + S(t)A2x
...
S(k)(t)x = S(t)Akx +k∑
i=1
jα−i(t)CAk−ix
Thus 1) is proved.
To prove 2), by equation (2) and S(0) = 0, we have
(DθS)(t)x =d[θ]+1
dt(j−(θ) ∗ [S − S(0)])(t)x
=d[θ]+1
dt(j−(θ) ∗ S)(t)x
yet (j−(θ) ∗ S)(t) is an α − (θ) + 1-times integrated Csemigroup by theorem 2.1, so 2) is obtained from 1)by taking S(t) = (j−(θ)∗S)(t), k = [θ]+1, α = α−(θ)+1.
3) is easily got by taking t = 0 in 2).LEMMA2.3. Let A be a closed operator, {S(t) : t ≥ 0}
is an n-times integrated C semigroup with generator A, and
there exist constants M ′ ≥ 0, ω′ ∈ R, such that ‖ S(n)(t) ‖≤M ′eω′t, then for any x ∈ X, and t ≥ 0, we have
S(n)(t)x = limm→∞(I − t
mA)−mCx
= limm→∞(
m
t)m(
m
t− A)−mCx
and the limit is uniform in t on any bounded interval.
THEOREM2.4. Let A be a closed operator, {S(t) : t ≥0} is an α-times integrated C semigroup with generator
A and there exist constants M ′ ≥ 0, ω′ ∈ R, such that
‖ (DαS)(t) ‖≤ M ′eω′t, then for any x ∈ X, and t ≥ 0, we
have
(DαS)(t)x = limm→∞(I − t
mA)−mCx
= limm→∞(
m
t)m(
m
t− A)−mCx
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and the limit is uniform in t on any bounded interval.
Proof. Theorem2.1 and 2.2 yields that, for any x ∈X, and t ≥ 0
(DαS)(t)x =d[α]+1
dt(j−(α) ∗ S)(t)x
and (j−(α) ∗ S)(t) is [α] + 1-times integrated C semigroup.
According to lemma 2.3, we completes the proof by
replacing n with [α] + 1 and S(t) with (j−(α) ∗ S)(t).COROLLARY2.5. The condition is the same as theo-
rem2.4, then for any x ∈ D(A[α]+1) and t ≥ 0, we have
1) (j−(α) ∗ S)(t)x
= limm→∞J [α]+1((I − t
mA)−mCx)
= limm→∞J [α]+1((
m
t)m(
m
t− A)−mCx)
which J(f(t)) =∫ t
0f(r)dr, f : [0,∞) → X is continuous.
and 2) S(t)x
= limm→∞
1Γ(α)
∫ t
0
(t − s)α−1(I − s
mA)−mCxds
= limm→∞
1Γ(α)
∫ t
0
(t − s)α−1(m
s)m(
m
s− A)−mCxds
and the limit is uniform in t on any bounded interval.
Proof. In order to prove these two equalities, we only have
to repeatedly integrate the equality in theorem2.4 by [α] +1 and α times respectively, now we only prove 2):
S(t)x = (Iα(DαS))(t)x
= (jα−1 ∗ (DαS))(t)x = (tα−1
Γ(α)∗ (DαS)(t)x
= limm→∞
1Γ(α)
∫ t
0
(t − s)α−1(I − s
mA)−mCxds
= limm→∞
1Γ(α)
∫ t
0
(t − s)α−1(m
s)m(
m
s− A)−mCxds
III. LAPLACE INVERSE TRANSFORM
Shi Deming and Yang Deshan[12] have given the Laplace
inverse transform of C semigroups in 1944, then Laplace
inverse transform of n times integrated semigroups was
introduced by two different approaches, Cao Dexia[13] get
it based on the relations among these semigroups, recently
Rong Rong[14] obtain it with the results that Hening B. and
Neubrander[15] have got. In this section, we try to study the
two kinds of the Laplace inverse transform as well as two
deductions of exponentially bounded α times integrated Csemigroups, based on the generation theorem in terms of the
Laplace transform, the properties and the Gamma function.
LEMMA3.1. Let A be the infinitesimal generator of an
exponentially bounded C semigroup, ‖S(t)‖ ≤ Meωt, γ >max{0, ω}, then for all x ∈ D(A), we have∫ t
0
S(s)xds =1
2πi
∫ γ+i∞
γ−i∞eλt(λ − A)−1Cx
dλ
λ
and the integral on the right hand converges uniformly in tfor t in bounded intervals.
LEMMA3.2. Let α ≥ 0, C ∈ B(X) be an injection, then
the following are equivalent:
1) A generates an exponentially bounded α-times inte-
grated C semigroup {S(t) : t ≥ 0.
2) There exist ω > 0, that (ω,∞) ⊂ ρ(A), and for all
μ > ω, A generates an exponentially bounded (μ − A)−αCsemigroup {T (t) : t ≥ 0, and
T (t) = (μ − A)−α(d
dt)[α]+1(j−(α) ∗ S)(t)
LEMMA3.3. ω ≥ 0, F [λ] : (ω,∞) → X, let F [λ]satisfies: F (λ) = λ
∫ ∞0
e−λtα(t)dt, α(t) = 0, and ‖α(t +h) − α(t)‖ ≤ Mheω(t+h), t, h ≥ 0, then
α(t) =i
2πi
∫ γ+i∞
γ−i∞eλtF (λ)
dλ
λ(γ > ∞)
and the integral on the right hand converges uniformly in tfor t in bounded intervals.
THEOREM3.4. Let A be a closed operator, C ∈ B(X)is injective, ρ(A) �= ∅, λ ∈ ρ(A), and A is the gen-
erator of an exponentially bounded α-times integrated Csemigroup,‖S(t)‖ ≤ Meωt(ω ≥ 0), γ > ω, then for all
x ∈ D(A), we obtain∫ t
0
S(s)xds =1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)Cx
λα
dλ
λ
=1
2πi
∫ γ+i∞
γ−i∞Iα(eλtR(λ,A)Cx)
dλ
λ
and the integral on the right hand converges uniformly in tfor t in bounded intervals.
Proof. For ‖S(t)‖ ≤ Meωt(ω ≥ 0), we let α(t) =∫ t
0S(s)xds, F (λ) = (λ−A)−1Cx
λα ,∀x ∈ D(A), obviously,
α(t) satisfies the conditions of Lemma3.3, and
F (λ) =(λ − A)−1Cx
λα=
∫ ∞
0
e−λtS(t)xdt
=∫ ∞
0
e−λtxd
∫ t
0
S(s)ds
= λ
∫ ∞
0
e−λt(∫ t
0
S(s)ds)xdt (λ > ω)
also satisfies the conditions of Lemma3.3, so we have∫ t
0
S(s)xds =1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)Cx
λα
dλ
λ(γ > ω)
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the former part is proved now.
On the other hand, Lemma3.2 implies that A also generates
an exponentially bounded (μ−A)−αC semigroup {T (t) : t ≥0}, together with Lemma3.1, we get∫ t
0
T (s)xds
=1
2πi
∫ γ+i∞
γ−i∞eλt(λ − A)−1(μ − A)−αCx
dλ
λ
=1
2πi
∫ γ+i∞
γ−i∞eλt(λ − A)−1R(μ,A)αCx
dλ
λ
=R(μ,A)α
2πi
∫ γ+i∞
γ−i∞eλt(λ − A)−1Cx
dλ
λ
It follows from Lemma3.2 that
S(t) = (μ − A)α(IαT )(t) (3)
so∫ t
0S(s)xds
= (μ − A)α
∫ t
0
(IαT )(s)xds
= (μ − A)αIα(∫ t
0
T (s)xds)
= (μ − A)α R(μ,A)α
2πi
∫ γ+i∞
γ−i∞Iα(eλt(λ − A)−1Cx)
dλ
λ
=1
2πi
∫ γ+i∞
γ−i∞Iα(eλtR(λ,A)Cx)
dλ
λ
that is proved.
COROLLARY3.5. The condition is the same as theo-
rem3.4, then for all x ∈ X
S(t)x =1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)Cx
λαdλ
=1
2πi
∫ γ+i∞
γ−i∞Iα(eλtR(λ,A)Cx)dλ
and the integral on the right hand converges uniformly in tfor t in bounded intervals.
Proof. By theorem3.4,∫ t
0
S(s)xds =1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)Cx
λα
dλ
λ
multiply this equation by A that
A
∫ t
0
S(s)xds =1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)ACx
λα
dλ
λ
then it is seen from Lemma1.3 and
tα
Γ(α + 1)=
12πi
∫ γ+i∞
γ−i∞eλtλ−α−1dλ
that S(t)x
=tα
Γ(α + 1)Cx +
12πi
∫ γ+i∞
γ−i∞eλt R(λ,A)ACx
λα
dλ
λ
=1
2πi
∫ γ+i∞
γ−i∞eλtλ−α−1Cxdλ
+1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)ACx
λα
dλ
λ
=1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)Cx
λα(λ − A + A)
dλ
λ
=1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)Cx
λαdλ
this completes the former part of the corollary, together with
theorem(3.4) and (3), the other part can be proved in the
same way.
COROLLARY3.6. The condition is the same as theo-
rem3.4, then all x ∈ X∫ t
0
(t − s)S(s)xds =1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)Cx
λα
dλ
λ2
=1
2πi
∫ γ+i∞
γ−i∞Iα(eλtR(λ,A)Cx)
dλ
λ2
and the integral on the right hand converges uniformly in tfor t in bounded intervals.
Proof. Theorem3.4 shows∫ t
0
S(s)xds =1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)Cx
λα
dλ
λ
integrating the equation from 0 to t, we get∫ t
0
(t − s)S(s)xds =1
2πi
∫ t
0
∫ γ+i∞
γ−i∞eλs R(λ,A)Cx
λα
dλ
λds
=1
2πi
∫ γ+i∞
γ−i∞(eλt − 1)
R(λ,A)Cx
λα
dλ
λ2
and for1
2πi
∫ γ+i∞
γ−i∞
R(λ,A)Cx
λα
dλ
λ= 0
so∫ t
0
(t − s)S(s)xds =1
2πi
∫ γ+i∞
γ−i∞eλt R(λ,A)Cx
λα
dλ
λ2
the other part of this corollary can be got similarly from
theorem(3.4) and (3).
ACKNOWLEDGMENT
The authors would like to thank the referees for their
valuable suggestions, this paper is supported in part by
The Fundamental Research Funds for the Central Univer-
sities(2010LKSXO8).
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