R E S E A R C H
Open Access
The structure of fractional spaces
generated by multi-dimensional elliptic
difference operator
Allaberen Ashyralyev
1,2and Sema Akturk
3**Correspondence:
3Department of Mathematics, Fatih
University, Buyukcekmece, Istanbul, 34500, Turkey
Full list of author information is available at the end of the article
Abstract
In the present paper, the positivity of a multi-dimensional difference operator in the half-space is considered. The structure of fractional spaces generated by this operator is investigated. The equivalence of the norms of these fractional spaces and Hölder spaces is proved. In applications, the stability of difference schemes for elliptic differential equations is presented.
MSC: 35J25; 47E05; 34B27
Keywords: positive operator; fractional spaces; Green’s function; Hölder spaces
1 Introduction
The role played by the positivity of differential and difference operators in Banach spaces in the study of the stability of solutions of boundary value problems for partial differential equations and the stability of difference schemes for partial differential equations, and of summation Fourier series converging inC-norm is well known (see [–]).
Recall that an operatorAdensely defined in a Banach spaceEwith domainD(A) is called positive inE, if its spectrumσA lies in the interior of the sector of angleϕ, <ϕ<π,
symmetric with respect to the real axis, and, moreover, on the edges of this sectorS(ϕ) =
{ρeiϕ: ≤ρ≤ ∞}andS(ϕ) ={ρe–iϕ: ≤ρ≤ ∞}, and outside of the sector the resolvent (A–λI)–is subject to the bound (see [])
(A–λI)–E→E≤ M +|λ|,
whereI is the identity operator. The infimum of all such anglesϕ is called the spectral angle of the positive operatorAand is denoted byϕ(A) =ϕ(E,A).
Throughout the present work, we will indicate withMpositive constants which can be different from time to time and we are not interested in precise. We will writeM(α,β, . . .) to express the fact that the constant depends only onα,β, . . . .
The theory of differential and difference operators in Banach spaces and their related applications have been investigated by many scientists (see, for example, [–]).
Great progress has been made in the study of structure of interpolation spaces generated by positive operators from the view-point of the stability analysis of high-order accuracy
difference schemes for various partial differential equations. However, the positivity of difference operators and structure of fractional spaces generated by these operators in Banach spaces are not well investigated in general. Therefore, the investigation of structure of fractional spaces generated by positive difference operators in Banach spaces and its applications to the stability of difference schemes for various partial differential equations is an important subject.
For a positive operatorAin the Banach spaceE, let us introduce the fractional spaces Eα=Eα(E,A) ( <α< ) consisting of thosev∈Efor which the norms
vEα=sup
λ>
λαA(A+λI)–vE
are finite. Clearly, the positive operator commutesAand its resolvent (A–λI)–. By the definition of the norm in the fractional spaceEα=Eα(E,A) ( <α< ), we get
(A–λI)–E
α→Eα≤(A–λI) –
E→E. ()
Thus, from the positivity of operatorAin the Banach spaceEfollows the positivity of this operator in fractional spacesEα=Eα(E,A) ( <α< ).
In [], Simirnitskii and Sobolevskii considered the difference operatorAxhwhich is an elliptic difference operator of an arbitrary high order of accuracy approximating the multi-dimensional elliptic operatorAx=Bx+δI.
Let us define the grid spaceRn–
h ( <h≤h) as the set of all points of the Euclidean
spaceRn–whose coordinates are given by
xk=skh, sk= ,±,±, . . . ,k= , . . . ,n– .
The numberhis called the step of the grid space. A function defined onRn–
h will be called
a grid function. To the differential operatorBwith constant coefficients of the form
Bx=
|r|=m
br
∂r+···+rn– ∂xr
· · ·∂xrnn–– ,
we assign the difference operator
Bx h=h
–m
m≤|s|≤S
dss–
s +· · ·
sn– (n–)–
sn–
(n–)+, ()
which acts on functions defined on the entire spaceRn–
h . Here,s∈R(n–)is a vector with
nonnegative integer coordinates,
k±fh(x) =±
fh(x±ekh) –fh(x)
,
andekis the unit vector of the axisxk.
smooth function onRn–. Using the Taylor expansion ofϕ(y), one can show that
sup
x∈Rn–
h
h–k±ϕ(x) – ∂
∂yk
ϕ(x)≤M(ϕ)h.
Here, the grid functionϕ(x) and∂y∂
kϕ(x) are the traces of the functionsϕ(y) and ∂ ∂ykϕ(y),
respectively. The last inequality means that the difference operatorh–
k±is a first-order
approximation for the differential operator ∂y∂
k.
We say that the difference operatorBx
h is aλth-order (λ> ) approximation of the
dif-ferential operatorBxif the inequality
sup
x∈Rnh–
Bxhϕ(x) –Bxϕ(x)≤M(ϕ)hλ
holds for any smooth functionϕ(y). We shall assume that the operatorBxhapproximates the differential operatorBxwith any prescribed order.
A function of a continuous [resp., discrete] argument that decays at infinity faster than any negative power of|y|[resp., |x|] is said to be rapidly decreasing. Let us define the Fourier transform of a grid functionfh(x) by the formula
˜
f(ξ) = (π)–(n–)
x∈Rnh–
exp–i(x,ξ)fh(x)hn–, ξ∈Rn–. ()
This formula defines a πh–-periodic smooth function of the continuous argumentξ wheneverfh(x) is a rapidly decreasing grid function. In this last case, () is just a Fourier
series expansion of the functionf˜(ξ) and the numbersfh(x) are the Fourier coefficients,
given by the formula
fh(x) =
|ξ|≤πh–
· · ·
|ξn–|≤πh–
expi(x,ξ)f˜(ξ)dξ· · ·dξn–. ()
The inverse Fourier transform of a πh–-periodic functionϕ(ξ) is defined to be the grid functionϕ˜h(x) given by the formula
˜
ϕh(x) =
|ξ|≤πh–
· · ·
|ξn–|≤πh–
expi(x,ξ)ϕ(ξ)dξ· · ·dξn–. ()
Equations () and () establish a one-to-one correspondence between rapidly decreasing grid functions of a continuous argument. In particular, iffh(x) is a rapidly decreasing grid
function, then
[f˜]h(x) =fh(x).
Iffh(x) is a rapidly decreasing grid function, then the grid functionBx
hfh(x) exists and is
given by () and we have the equality
Bx
The functionB(ξh,h) is obtained by replacing the operatork±in the right-hand side of
equality () with the expression±(exp{±iξkh}– ), respectively, and is called the symbol of
the difference operator. Sinceexp{±iξkh}is a bounded analytic πh–-periodic function,
the symbolB(ξh,h) is a bounded analytic πh–-periodic function. It follows that for large
|ξ|one has the estimate
B(ξh,h)≤M(h)|ξ|m, |ξ|=|ξ|+· · ·+|ξn–|.
Let us give the difference operatorAx
hby the formula
Axhuh(x) = m≤|r|≤S
axrDrhuh(x) +δuh(x). ()
The coefficients are chosen in such a way that the operatorAxhapproximates in a specified way the operator
|r|=m
ar(x)
∂|r|
∂xr · · ·∂x
rn–
n– +δ.
We shall assume that for|ξkh| ≤πand fixedxthe symbolAx(ξh,h) of the operatorAxh–δ
satisfies the inequalities
(–)mAx(ξh,h)≥M|ξ|m, argAx(ξh,h)≤φ<φ≤ π
.
In [], Danelich considered the difference elliptic operatorAx
hwhich is to an arbitrary
high order of accuracy approximating the multi-dimensional elliptic operatorAxdefined
by
Ax=
|r|=m
ar(x)
∂|r|
∂xr · · ·∂x
rn–
n–
+ (–)ma(x)∂ m
∂xm n
+δI ()
with the domain
DAx=
u∈CmR+n:u(x)|xn== ∂u(x)
∂N
xn=
=· · ·=∂
m–u(x)
∂Nm–
xn=
=
.
Here,δ> is the sufficiently large number anda(x) is a continuous function defined on
R+={x:x≥}with
<s≤a(x)≤s<∞. ()
Let us define the grid spaceR+
hn( <h≤h) as the set of all points of the spaceR+nwhose
coordinates are given by
The numberhis called the step of the grid space. A functionϕh(x) defined onR+
hnwill be
called a grid function. To the differential operatorAxdefined by (), we assign the
differ-ence operator
Axhϕh(x) =Axhϕh(x) +Axhϕh(x) +δϕh(x), x∈R+hn,
Ax
hϕh(x) =h–m
m≤|p|≤S
ax r
p –
p +· · ·
pn– (n–)–
pn–
(n–)+ϕh(x), x∈R+hn, ()
Axhϕh(x) = (–)mh–m m≤r+s≤S
s≤m
axr,srn+sn–ϕh(x), x∈R+hn,
which acts on functions defined on the entire spaceR+
hn. Here,p∈R+n– is a vector with nonnegative integers coordinates. The coefficientsax
r are chosen in such a way that the
operatorAxhapproximates in a specified way the operator
|r|=m
ar(x)
∂|r| ∂xr
· · ·∂x
rn–
n– .
We shall assume that for|ξkh| ≤π and fixedxthe symbolAx(ξh,h) of the operatorAxh
satisfies the inequalities
(–)mAxξh,h≥Mξ m
,
argAxξh,h≤φ<φ<π, ξ= (ξ, . . . ,ξn–).
()
For the definition of the operatorAx
h, we will defineϕh(x) which is extended toϕh(x)
defined onR+
hnand additionally on the points
x,xk
=x,kh∈/R+hn, x∈Rh(n–),k= –, –, . . . , –(m– ),
and
ϕhx, = , h–k –k≤s≤sk
αs,kϕh
x,sh= , k= ,m– ,α–k,k= . ()
The coefficientsαs,kare chosen in such a way that the expression
h–k
–k≤s≤sk
αs,kϕh
x,sh
approximates in a specified way the expressionϕ(k)(x, ). The coefficientsax
r,sare chosen in
such a way that the operatorh–k
–k≤s≤skαs,kϕ
h(x,sh) approximates in a specified way the
operatorAx. We shall assume that the operatorAxhapproximates the differential operator Axwith any prescribed order.
In the present paper, a Green’s function is assigned. The organization of the present paper is as follows. In Section , the main theorem on the structure of fractional spaces Eα(C˙h(Rhn+ ),Axh) generated byAxhis investigated. In Section , applications on theorems on
2 Green’s function
Theorem [] Suppose that assumptions().Let the function a(x)satisfy the estimate
a(x) –a(y)≤s|x–y|α
<α≤;x,y∈R+h. ()
Then,for sufficiently large positiveδ andReλ≥,there exists a unique solution of the resolvent equation
Axhuh(x) +λuh(x) =fh(x), x∈R+hn ()
and the following formula:
fh(y)hnAhx+λI–fh(x) =
y∈R+hn
Gh(x,y;λ) ()
holds.Here,Gh(x,y;λ)is the Green’s function of the resolvent equation().
Lemma The following identities hold:
where vh(x)is the solution of the following problem: ⎧
Proof We consider the problem
Then
y∈R+hn
Gh(x,y;λ)hn=
δ+λ
–vh(x), x∈R+hn.
Identity () is proved. Sincevh() = , we have
δ+λ=
y∈R+hn
Gh(,y;λ)hn+
δ+λ.
Thus follows (). Lemma is proved.
For anyx∈R+hn, we have
Gh(x,y;λ) =Ghx(x,y;λ) +
y∈R+hn
Gh(x,z;λ)
Ax
h –A z h
Gx
h (z,y;λ)h
n, ()
whereGx
h (x,y;λ) is the Green’s function of the operatorA x
h .
Moreover, applying (), (), (), and () conditions, one proved the following point-wise estimates of the Green’s functionGh(x,y;λ) of the resolvent equation and its
differ-ence derivatives:
Gh(x,y;λ)≤Mexp
–b|λ+δ|p|x–y||λ+δ|np– ()
for m>n,
Gh(x,y;λ)≤Mexp
–b|λ+δ|p|x–y| +ln|x–y||λ+δ|p–+ ()
for m=n,
Gh(x,y;λ)≤Mexp
–b|λ+δ|p|x–y||x–y|m–n ()
for m<n, and its derivatives respect tox
DrhGh(x,y;λ)≤Mexp
–b|λ+δ|p|x–y||λ+δ|(n+r)p– ()
for m–r>n,
Dr
hGh(x,y;λ)≤Mexp
–b|λ+δ|p|x–y| +ln|x–y||λ+δ|p–+ ()
for m–r=n,
DrhGh(x,y;λ)≤Mexp
–b|λ+δ|p|x–y||x–y|m–n–r ()
for m–r<n, wherep=m,a> ,M> for <|λ| ≤Lh–m,λ∈Qψ∪ {}, and Gh(x,y;λ)≤Mexp
DrhGh(x,y;λ)≤Mexp
–bh–|x–y|hm–n–r|δ+λ|hm+ – ()
for|λ|>Lh–m. Herep=
m,b> ,M> .
Note that under assumptions () and () there exists a unique solutionvh(x) of problem
() and the following estimate holds:
vh(x)≤Mexp
–b|λ+δ|p|x|, ()
for <|λ| ≤Lh–m,λ∈Q
ψ∪ {}and vh(x)≤M
exp
–bh–|x||δ+λ|hm+ –, ()
for|λ|>Lh–m.
Lemma [] |λ|>Lh–m,where L> large enough.Then
Gh(x,y;λ)≤Mexp
–bh–|x–y|hm|δ+λ|hm+ –|x–y|–n, x=y. ()
By()and(),we obtain the estimate
Gh(x,y;λ)
≤Mexp
–bh–|x–y|h–+m(+μ)
×|δ+λ|hm+ –(+mμ)|x–y|–mμ, x=y. ()
Moreover, applying the Green’s function ofAxhthe following results were proved.
Theorem [] Ax
h is a positive operator in the spaceC˙(R+hn)of all mesh functionsϕh(x)
defined onR+hnwith the norm
ϕhC˙
h= sup x∈R+
hn ϕh(x)
with the spectral angleϕ(Ax
h,C˙h) =π–ψ.
LetCβh =Cβ(R+
hn) be the Hölder space of all mesh functionsϕh(x) defined onR+hn
satis-fying a Hölder condition with the indicatorβ∈(, ) with the norm
ϕhCβ
h= ϕhC
h+ sup x,y∈R+hn
x=y
|ϕh(x) –ϕh(y)| |x–y|β .
One proved the strong positivity ofAxhin the Banach spaceC˙h=C˙(R+hn) (difference
ana-log ofC˙(R+
n)) for sufficiently large positiveδ. Passing to limit whenh→, we can get the
strong positivity of differential operatorAxin the Banach spaceC˙(R+
3 The structure of fractional spacesEα(C˙h(R+hn),Axh)
Theorem Supposemα∈(, ).Then the norms of the spaces Eα(C˙h,Axh)andC˙mα(R+hn)
are equivalent.Here,
˙
Chmα=
ϕh:ϕh∈Chmα,ϕhx, = ,h–k –k≤s≤sk
αs,kϕh
x,sh= ,
k= ,m– ,α–k,k= ,x∈Rh(n–)
.
Proof Assume thatfh∈ ˙Cmα(R+
hn). Letx∈R+hnandλ> be fixed. Using equation ()
and identity (), we can write
AxhAxh+λ–fh(x)
= δ
λ+δf
h(x) +λ
y∈R+n
Gh(x,y;λ)
fh(x) –fh(y)hn
+ λ
λ+δv
h(x)fh(x) –fh(x, . . . ,x n–, )
+ λ
λ+δv
h(x)fh(x, . . . ,x n–, ).
Sincefh(x
, . . . ,xn–, ) = , we have
AxhAxh+λ–fh(x) = δ λ+δf
h(x) +λ
y∈R+n
Gh(x,y;λ)
fh(x) –fh(y)hn
+ λ
λ+δv
h(x)fh(x) –fh(x, . . . ,x n–, )
. ()
Using equation () and the triangle inequality, and the definition of theC˙mα(R+
hn)-norm,
we have
λαAxhAxh+λ–fh(x)
≤
λαδ
λ+δ +λ
α+
y∈R+n
Gh(x,y;λ)|x–y|mαhn+
λα+
λ+δv(x)|x|
mαfh
˙
Cmα(R+
hn)
= [I+I+I]fhC˙mα(R+
hn).
We will estimateIi,i= , , , separately. First, let us estimateI. Clearly, using the estimate
λαδ–α
λ+δ ≤
we get
I≤δα ()
We will consider two cases:λ>Lh–mandλ≤Lh–m. First, letλ>Lh–m. Using estimate
(), we have
I≤Mλα+
y∈R+n
e–bh–|x–y|h–n+m(+α)(λ+δ)hm+ –(+mα)hn
≤M
(λhm)αλ
((λ+δ)hm)mα(λ+δ)≤M ()
for anyλ> andx∈R+hn. From estimate () and the following inequality:
(at)θe–at≤M, a> ,θ∈[, ], ()
it follows that
I≤M λα+ λ+δe
–ah–|x|(λ+δ)hm+ –| x|mα
≤M
λα+hmα
(λ+δ)((λ+δ)hm+ )≤M ()
for anyλ> andx∈R+hn. Combining estimates ()-(), we get
λαAxhAxh+λ–fh(x)≤M(α) ()
for anyλ> andx∈R+
hn.
Second, letλ≤Lh–m. We consider three cases: m>n, m=n, and m<n.
In the first case, using estimate (), applying inequality (), and the definition of the
˙
Cmα(R+
hn)-norm, we have
I≤Mλα+
y∈R+
hn
e–b(λ+δ)m|x–y|(λ+δ)n
m–
≤M
λα+ (λ+δ)–nm+α+
β m+nm
≤M ()
for anyλ> andx∈R+hn.
In the second case, applying estimate (), and inequality (), we have
I≤Mλα+
y∈R+hn
e–b(λ+δ)m|x–y| +ln|x–y|(λ+δ)
m–+ |x–y|mα+βhn
≤M
λα+ (λ+δ)α+nm+
β m
≤M ()
for anyλ> andx∈R+hn.
In the third case, using estimate () we obtain
I≤Mλα+
y∈R+hn
e–b(λ+δ)m|x–y|(λ+δ)n
m–|x–y|m–n|x–y|mα+βhn
≤M
λα+ (λ+δ)m–n+mmα+β–nm
for anyλ> andx∈R+hn. Estimates ()-() result in
I≤M ()
for anyλ> andx∈R+hn. From estimate () and inequality () it follows that
I≤M λα+ λ+δe
–b(λ+δ)m|x||x|mα+β≤
M ()
for anyλ> andx∈R+
hn. Combining estimates (), (), and (), we have
λαAxhAxh+λ–fh(x)≤M(α)fhC˙mα ()
for anyλ> andx∈R+
hn.
Combining estimates () and (), we get
sup
λ> sup
x∈R+hn
λαAxhAhx+λ–fh(x)≤M(α)fhC˙mα. ()
Now, we will prove the opposite inequality. Using the definition ofEα(C˙h,Axh), we obtain
sup
x∈R+
n
fh(x)≤fhE
α(C˙h,Axh) ()
for anyx∈R+
hn. By Theorem ,Axhis a positive operator in the Banach spaceEα(C˙h,Axh).
Hence, forfh∈Eα(C˙h,Axh), we have
fh=
∞
AxhAxh+λ–V dλ. ()
It follows from equation () and equation () that
fh(x) =
∞
Axh+λ–AxhAxh+λ–fh(x)dλ
=
∞
y∈R+
hn
Gh(x,y;λ)Axh
Axh+λ–fh(y)hndλ. ()
Letx,τ ∈R+hn be fixed. We will consider two cases:λ>Lh–m andλ≤Lh–m. First, let λ>Lh–m. Using equation () and Lemma , we have
fh(x+τ) –fh(x) |τ|mα =
∞
y∈R+
hn
[Gh(x+τ,y;λ) –Gh(x,y;λ)] |τ|mαλα A
x h
From the triangle inequality and the definition of theEα(C˙h,Axh)-norm it follows that
We will estimateLandL. Let us estimateL. From the Lagrange theorem and estimate (), we have, for somex∗betweenx,x+τ, the inequality () yield
for anyλ> andx∈R+hn. Third, let m<n. Using the triangle inequality, estimate (), we have
L≤M
∞
|τ|m
y∈R+
hn
e–b(λ+δ)m|x+τ–y|
|τ|mαλα |x+τ–y|
m–nhndλ
+
∞
|τ|m
y∈R+
hn
e–b(λ+δ)m|x–y| |τ|mαλα |x–y|
m–nhndλ
≤M
∞
|τ|m
|τ|mαλα+dλ≤M(α). ()
Then, combining estimates ()-(), we have
L≤M(α). ()
Estimates () and () yield
fh(x+τ) –fh(x) |τ|mα
≤M(α)fhE
α. ()
Combining estimates () and (), we obtain
sup
x∈R+
hn τ=(,...,)
fh(x+τ) –fh(x) |τ|mα
≤M(α)fhE
α. ()
From estimates () and () it follows that
Eα ˙
Ch,Axh
⊂ ˙CmαR+hn.
This is the end of the proof of Theorem .
From Theorem and Theorem follows the following result.
Theorem Ax
his a positive operator in the spaceC˙ β(R+
hn),β∈(, ).
4 Applications
Now, we present some applications of Theorems -.
First, we consider the difference schemes for the approximate solution of problem
⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩
–∂∂tu(t,x)+
|r|=mar(x) ∂ |r|u(t,x) ∂xr···∂xrnn––
+ (–)ma(x)∂∂xmum(t,x)+δu(t,x) =f(t,x), <t<T,x∈R+n,
u(,x) =ϕ(x), u(T,x) =ψ(x), x∈R+
n,
u(t,x)|xn==∂u∂N(t,x)|xn==· · ·=∂
m–u(t,x)
∂Nm– |xn== , x∈R+n, ≤t≤T.
()
Here,ar(x),a(x),ϕ(x),ψ(x), andf(t,x) are sufficiently smooth functions and they satisfy all
Assume that uniform ellipticity holds. Note that problem () can be written in the form of the abstract boundary value problem
⎧ ⎨ ⎩
–u(t) +Au(t) =f(t), <t<T,
u() =ϕ, u(T) =ψ ()
in a Banach spaceE=C˙hwith positive operatorA=Axhdefined by () and (). The
dis-cretization of problem () is carried out in two steps. In the first step, let us give the difference operatorAx
h by equation (). With the help of Axh we arrive at the boundary
value problem
⎧ ⎨ ⎩
–dudth(t,x)+Axhuh(t,x) =fh(t,x), <t<T,x∈R+hn,
uh(,x) =ϕh(x), uh(T,x) =ψh(x), x∈R+hn,
()
for an infinite system of ordinary differential equations.
In the second step, we replace problem () by the difference scheme
⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩
–τ(uhk+(x) – uhk(x) +ukh–(x)) +Axhukh(x) =fkh(x), fkh(x) =fh(t
k,x), tk=kτ, ≤k≤N– ,Nτ =T,x∈R+hn,
uh
(x) =ϕh(x), uhN(x) =ψh(x), x∈R+hn,
()
for the approximate solution of boundary value problem ().
Theorem Let≤μ< .Then the solution of difference scheme()satisfies the following
stability estimate:
max ≤k≤N
uhkC˙μ
h ≤M(μ)
ϕhC˙μ
h + ϕhC˙μ
h +≤maxk≤N–
fkhC˙μ
h
.
The proof of Theorem is based on Theorem and Theorem , on the positivity of the difference operatorAxhin the Banach spaceC˙hμfor ≤μ< , and on the following abstract theorem on the stability of the difference scheme
⎧ ⎨ ⎩
–τ(uk+– uk+uk–) +Auk=fk,
fk=f(tk), tk=kτ, ≤k≤N– ,Nτ=T,u=ϕ,uN=ψ,
()
for the approximate solution of the abstract boundary value problem ().
Theorem [] Let A be a positive operator in a Banach space E.Then,for the solution of difference scheme(),the following stability inequality holds:
max
≤k≤NukEα≤M(α)
ϕEα+ψEα+ max ≤k≤N–fkEα
Theorem The solution of difference scheme()satisfies the following almost coercive
The proof of Theorem is based on Theorem on the positivity of an elliptic difference operatorAx
and on the following theorems on the almost coercive stability of difference scheme () and on the almost coercive stability of the elliptic difference problem.
Theorem [] Let A be a positive operator in a Banach space E.Then,for the solution of difference scheme(),the following almost coercive stability inequality holds:
max
Theorem Under assumptions()and(),the solution of the difference elliptic problem
Axhuh(x) =fh(x), x∈R+hn, ()
satisfies the following almost coercive inequality:
h–m
Theorem Let < mα< .Then,for the solution of difference scheme(),the following coercive stability estimate holds:
max
The proof of Theorem is based on Theorem on the structure of the fractional spaces Eα(C˙h,Axh), on Theorem on the positivity of an elliptic difference operator Axh in the
Banach spaceC˙h, and on the following theorems on the structure of the fractional space
Eα=Eα(E,A/), on the coercive stability of difference scheme (), and on the coercive
stability of the elliptic difference problem.
Theorem [] The spaces Eα(E,A)and Eα(A/,E)coincide for any <α<,and their norms are equivalent.
Theorem [] Let A be a strongly positive operator in a Banach space E.Then,for the solution of difference scheme(),the following coercive stability inequality:
max ence elliptic problem(),we have the following coercive inequality:
The proof of Theorem uses the techniques introduced in [] and it is based on esti-mates for the Green’s function of operatorAxhdefined by ().
Second, we consider the difference schemes for the approximate solution of problem
⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩
–∂∂tu(t,x)+
|r|=mar(x) ∂ |r|u(t,x) ∂xr···∂xrnn––
+ (–)ma(x)∂mu(t,x)
∂xm +δu(t,x) =f(t,x), <t<T,x∈R+n,
u(,x) =u(T,x), ut(,x) =ut(T,x), x∈R+n,
u(t,x)|xn==∂u∂N(t,x)|xn==· · ·=∂
m–u(t,x)
∂Nm– |xn== , x∈R+n, ≤t≤T.
()
Here,ar(x),a(x), andf(t,x) are sufficiently smooth functions and they satisfy every
com-patibility conditions which guarantee that problem () has a smooth solutionu(t,x). As-sume that the assumption of the uniform ellipticity holds. The discretization of problem () is carried out in two steps. In the first step, let us give the difference operatorAx
hby
equation (). With the help ofAxhwe arrive at the boundary value problem
⎧ ⎨ ⎩
–dudth(t,x)+Axhuh(t,x) =fh(t,x), <t<T,x∈R+hn,
uh(,x) =uh(T,x), uh
t(,x) =uht(T,x), x∈R+hn,
()
for an infinite system of ordinary differential equations.
In the second step, we replace problem () by the first order of approximation in thet difference scheme
⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩
–τ(uhk+(x) – uhk(x) +ukh–(x)) +Axhukh(x) =fkh(x), fkh(x) =fh(t
k,x), tk=kτ, ≤k≤N– ,Nτ =T,x∈R+hn,
uh
(x) =uhN(x), uh(x) –uh(x) =uhN(x) –uhN–(x), x∈R+hn,
()
and the second order of approximation in thetdifference scheme
⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩
–τ(uhk+(x) – uhk(x) +ukh–(x)) +Axhukh(x) =fkh(x),
fkh(x) =fh(tk,x), tk=kτ, ≤k≤N– ,Nτ =T,x∈R+hn,uh(x) =uhN(x),
–uh
(x) + uh(x) – uh(x) =uhN–(x) – uhN–(x) + uNh(x), x∈R+hn,
()
for the approximate solution of boundary value problem ().
Theorem Let≤μ< .Then the solution of the difference schemes()and()
sat-isfies the following stability estimate:
max ≤k≤N
uh
kC˙μh ≤M(μ)
ϕhC˙μ
h + ϕhC˙μ
h +≤maxk≤N–
fh kC˙μh
.
Theorem [] Let A be a positive operator in a Banach space E.Then,for the solution of difference schemes()and(),the following stability inequality holds:
max
Theorem For the solution of difference schemes ()and(),the following almost coercive stability estimate holds:
max
The proof of Theorem is based on Theorem , on the positivity of an elliptic difference operatorAx
and on the following theorem on the almost coercive stability of difference schemes () and () and on Theorem on the almost coercive stability of elliptic difference problem ().
Theorem [] Let A be a positive operator in a Banach space E.Then,for the solution of
difference schemes()and(),the following almost coercive stability inequality holds:
max satisfies the following coercive stability estimate:
+h–m m≤r+s≤S
s≤m
r+s–uhC˙mα
h
≤M(α)
h–m
m≤|p|≤S p
–
p +· · ·
pn– (n–)–
pn–
(n–)+ϕhC˙mα
h
+h–m m≤r+s≤S
s≤m
r+s–ϕhC˙mα
h
+h–m m≤|p|≤S
p –
p +· · ·
pn– (n–)–
pn– (n–)+ψ
h
˙
Cmα
h
+h–m m≤r+s≤S
s≤m
r+s–ψhC˙mα
h
+M(α) max ≤k≤N–
fh kC˙mα
h .
The proof of Theorem is based on Theorem , on the structure of the fractional spaces Eα(C˙h,Axh), on Theorem , on the structure of the fractional spaceEα =Eα(E,A/), on
Theorem , on the positivity of an elliptic difference operatorAxhin the Banach spaceC˙h,
and on the following theorem on the coercive stability of difference schemes () and () and on Theorem on the coercive stability of elliptic difference problem ().
Theorem [] Let A be a strongly positive operator in a Banach space E.Then,for the
solution of difference schemes()and(),the following coercive stability inequality:
max ≤k≤N–
τ(uk+– uk+uk–)
Eα
+ max
≤k≤NAukEα≤M(α)≤maxk≤N–fkEα is valid.
5 Conclusion
In the present article, the structure of the fractional spacesEα(C˙(R+hn),Axh) generated by
the multi-dimensional elliptic difference operatorAxhis investigated.
Competing interests
The authors declare that they have no competing interests.
Authors’ contributions
All authors read and approved the final manuscript.
Author details
1Department of Elementary Mathematics Education, Fatih University, Buyukcekmece, Istanbul, 34500, Turkey. 2Department of Mathematics, ITTU, Ashgabat, Turkmenistan.3Department of Mathematics, Fatih University,
Buyukcekmece, Istanbul, 34500, Turkey.
Acknowledgements
The authors would like to thank Prof. Pavel Sobolevskii (Universidade Federal do Ceará, Brasil). The second author would also like to thank The Scientific and Technological Research Council of Turkey (TUB˙ITAK) for the financial support.
Received: 24 August 2015 Accepted: 3 December 2015 References
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