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ISSN 2077–9879

Eurasian

Mathematical Journal

2016, Volume 7, Number 2

Founded in 2010 by

the L.N. Gumilyov Eurasian National University in cooperation with

the M.V. Lomonosov Moscow State University the Peoples’ Friendship University of Russia

the University of Padua

Supported by the ISAAC

(International Society for Analysis, its Applications and Computation) and

by the Kazakhstan Mathematical Society

Published by

the L.N. Gumilyov Eurasian National University

Astana, Kazakhstan

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EURASIAN MATHEMATICAL JOURNAL

Editorial Board

Editors–in–Chief

V.I. Burenkov, M. Otelbaev, V.A. Sadovnichy

Editors

Sh.A. Alimov (Uzbekistan), H. Begehr (Germany), T. Bekjan (China), O.V. Besov (Rus- sia), N.A. Bokayev (Kazakhstan), A.A. Borubaev (Kyrgyzstan), G. Bourdaud (France), A. Caetano (Portugal), M. Carro (Spain), A.D.R. Choudary (Pakistan), V.N. Chubarikov (Russia), A.S. Dzumadildaev (Kazakhstan), V.M. Filippov (Russia), H. Ghazaryan (Arme- nia), M.L. Goldman (Russia), V. Goldshtein (Israel), V. Guliyev (Azerbaijan), D.D. Haroske (Germany), A. Hasanoglu (Turkey), M. Huxley (Great Britain), M. Imanaliev (Kyrgyzstan), P. Jain (India), T.Sh. Kalmenov (Kazakhstan), B.E. Kangyzhin (Kazakhstan), K.K. Ken- zhibaev (Kazakhstan), S.N. Kharin (Kazakhstan), E. Kissin (Great Britain), V. Koki- lashvili (Georgia), V.I. Korzyuk (Belarus), A. Kufner (Czech Republic), L.K. Kussainova (Kazakhstan), P.D. Lamberti (Italy), M. Lanza de Cristoforis (Italy), V.G. Maz’ya (Swe- den), E.D. Nursultanov (Kazakhstan), R. Oinarov (Kazakhstan), K.N. Ospanov (Kaza- khstan), I.N. Parasidis (Greece), J. Peˇcari´c (Croatia), S.A. Plaksa (Ukraine), L.-E. Pers- son (Sweden), E.L. Presman (Russia), M.A. Ragusa (Italy), M.D. Ramazanov (Russia), M. Reissig (Germany), M. Ruzhansky (Great Britain), S. Sagitov (Sweden), T.O. Sha- poshnikova (Sweden), A.A. Shkalikov (Russia), V.A. Skvortsov (Poland), G. Sinnamon (Canada), E.S. Smailov (Kazakhstan), V.D. Stepanov (Russia), Ya.T. Sultanaev (Russia), I.A. Taimanov (Russia), T.V. Tararykova (Great Britain), J.A. Tussupov (Kazakhstan), U.U. Umirbaev (Kazakhstan), Z.D. Usmanov (Tajikistan), N. Vasilevski (Mexico), Dachun Yang (China), B.T. Zhumagulov (Kazakhstan)

Managing Editor

A.M. Temirkhanova

c

The Eurasian National University

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4

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TYNYSBEK SHARIPOVICH KAL’MENOV

(to the 70th birthday)

On May 5, 2016 was the 70th birthday of Tynysbek Sharipovich Kal’menov, member of the Editorial Board of the Eurasian Math- ematical Journal, general director of the Institute of Mathematics and Mathematical Modeling of the Ministry of Education and Sci- ence of the Republic of Kazakhstan, laureate of the Lenin Komsomol Prize of the Kazakh SSR (1978), doctor of physical and mathemat- ical sciences (1983), professor (1986), honoured worker of science and technology of the Republic of Kazakhstan (1996), academician of the National Academy of Sciences (2003), laureate of the State Prize in the field of science and technology (2013).

T.Sh. Kal’menov was born in the South-Kazakhstan region of the Kazakh SSR. He graduated from the Novosibirsk State University (1969) and completed his postgraduate studies there in 1972.

He obtained seminal scientific results in the theory of partial differential equations and in the spectral theory of differential operators.

For the Lavrentiev-Bitsadze equation T.Sh. Kal’menov proved the criterion of strong solvability of the Tricomi problem in the Lp-spaces. He described all well-posed boundary value problems for the wave equation and equations of mixed type within the framework of the general theory of boundary value problems.

He solved the problem of existence of an eigenvalue of the Tricomi problem for the Lavrentiev-Bitsadze equation and the general Gellerstedt equation on the basis of the new extremum principle formulated by him.

T.Sh. Kal’menov proved the completeness of root vectors of main types of Bitsadze- Samarskii problems for a general elliptic operator. Green’s function of the Dirichlet problem for the polyharmonic equation was constructed. He established that the spectrum of general differential operators, generated by regular boundary conditions, is either an empty or an infinite set. The boundary conditions characterizing the volume Newton potential were found. A new criterion of well-posedness of the mixed Cauchy problem for the Poisson equation was found.

On the whole, the results obtained by T.Sh. Kal’menov have laid the groundwork for new perspective scientific directions in the theory of boundary value problems for hyperbolic equations, equations of the mixed type, as well as in the spectral theory.

More than 50 candidate of sciences and 9 doctor of sciences dissertations have been defended under his supervision. He has published more than 120 scientific papers. The list of his basic publications can be viewed on the web-page

https://scholar.google.com/citations?user=Zay4f xkAAAAJ&hl=ru&authuser = 1 The Editorial Board of the Eurasian Mathematical Journal congratulates Tynysbek Sharipovich Kal’menov on the occasion of his 70th birthday and wishes him good health and new creative achievements!

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EURASIAN MATHEMATICAL JOURNAL ISSN 2077-9879

Volume 7, Number 2 (2016), 19 – 37

INTEGRAL REPRESENTATION OF FUNCTIONS AND EMBEDDING THEOREMS FOR MULTIANISOTROPIC SPACES

IN THE THREE-DIMENSIONAL CASE G.A. Karapetyan

Communicated by V.I. Burenkov

Key words: integral representation, embedding theorem, multianisotropic spaces, com- pletely regular polyhedron.

AMS Mathematics Subject Classification: 46E35.

Abstract. In this paper we obtain a special integral representation of functions with a set of multi-indices and use it to prove embedding theorems for multianisotropic spaces in three-dimensional case.

1 Introduction

The embedding theorems for multianisotropic spaces in two-dimensional case can be found in [4]. In this paper we prove embedding theorems for the Sobolev multianisotropic spaces in three-dimensional space when the completely regular polyhedron has one anisotropicity vertex. The obtained results generalize embedding theorems for isotropic and anisotropic spaces in [1-3, 5-9] (for an overview of the history of the problem and related results see [2]), and in the case of anisotropic spaces coincide with known theorems, although a method of integral representation of functions is applied, which is based on the usage of special multianisotropic kernels.

2 Multianisotropic kernels and their properties

LetR3 be the three-dimensional space, Z3+ the set of all three-dimensional multi-indices, i.e.

α= (α1, α2, α3)∈ Z3+, if α1, α2, α3 are non-negative integers. Forξ, η ∈R3, α ∈Z3+, t >0 let |α| = α123, ξα = ξ1α1ξ2α2ξ3α3, tη = (tη1, tη2, tη3), Dk = 1i∂x

k, k = 1,2,3, and let Dα =Dα11D2α2D3α3 be the weak derivative of order α.

For a set of multi-indices let N be the smallest convex polyhedron containing it. N is said to be completely regular if

a) it has vertices at the origin and further vertices on each coordinate axis

b) all components of the outer normals of all two-dimensional non-coordinate faces are positive. For a completely regular polyhedron N in R3 let N2i (i = 1, ..., M) be the two- dimensional non-coordinate faces. Let µi(i= 1, . . ., M) be the outer normal of the face N2i,

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20 G.A. Karapetyan

such that the equation of that face is(α;µi) = 1; (i= 1, ..., M). We study the case when the vertices ofNare multi-index: α1 = (l1,0,0), α2 = (0, l2,0), α3 = (0,0, l3), α4 = (α1, α2, α3).

Denote by µi (i= 1,2,3) the outer normal of N2i, which is the face N21 passing through all the vertices with the exception of αi (i=1,2,3), i.e. µ1 is the outer normal of the face passing through the vertices{α234}, and so on.

Forθ > 0and positive integer k denote

P (θ, ξ) = (θξ1l1)2k+ (θξ2l2)2k+ (θξ3l3)2k+ (θξ1α1ξ2α2ξ3α3)2k, (2.1)

G0(ξ;θ) = e−P(θ,ξ), (2.2)

G1,j(ξ, θ) = 2k(θξαj)2k−1eP(θ,ξ) , j = 1,2,3,4. (2.3) It is obvious that for any value of θ >0 G0, G1,j∈S,(j = 1,2,3,4), where S =S(Rn)is the Schwartz space of rapidly decreasing functions.

Let Gˆ0(t, θ), Gˆ1,j(t, θ) (j = 1,2,3,4) be the corresponding Fourier transform of G0, G1,j (j = 1,2,3,4).

Note that Gˆ0 ,Gˆ1,j ∈ S,(j = 1,2,3,4), because the Fourier transform is an automor- phism on S.

Suppose that the inequality α1 < α2 < α3 < l3 holds forα=α4 = (α1, α2, α3). Consider the intersection of planesN21T

N22, i.e. the line passing through the pointsα3 = (0; 0;l3)and α4 = (α1, α2, α3). The parametric equation of that line isx =α1t; y=α2t; z =l3−t(l3−α3).

Let β = (β1, β2,0) be the point of intersection of that line with the XOY plane. Note that β1 = lα1l3

3−α3, β2 = lα2l3

3−α3, β ∈ N21T

N22 (i.e. (β;µ1) = 1; (β;µ2) = 1), also β1 < β2 which follows from α1 < α2.

Consider the pointγ = (γ1,0,0), such thatγ ∈N21. Let N be an even number, such that all components of multi-indices N α, N β, N γ are even. (A) Such N exists, because all components ofα, β, γ are rational. Let us prove the following lemma (an analogue of Lemma 2.1 in [4]).

Lemma 2.1. Let α4 = (α1, α2, α3)∈Z3+, α1 < α2 < α3 and θ ∈(0; 1). Then for any multi- index m = (m1, m2, m3) and for any even N satisfying (A) there exist constants Ci, (i = 0,1,2), such that

|Dm1,j(t, θ)| ≤ θi=1,2,3max(|µi|+(m,µi))

C0(lnθ)2+C1|lnθ|+C2

1 +θ−N(tN α1 1tN α2 2tN α3 3 +tN β1 1tN β2 2 +tN γ1 1) . (2.4) An analogous inequality is true for Gˆ0(t, θ).

Proof. As in the proof of Lemma 2.1 in [4], for any multi-indexm= (m1, m2, m3)we estimate the following integral:

I = Z

0

Z 0

Z 0

ξm1 1ξ2m2ξ3m3e−P(θ,ξ)123. Consider mαi

i+1 (i= 1,2,3). Leti0 be an index, such that max

i=1,2,3 αi

mi+1 = mαi0

i0+1 . There are 3 possible cases:

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Integral representation of functions and embedding theorems for multianisotropic spaces 21 1. The maximum is obtained only at one index i0 , i.e. mαi

i+1<mαi0

i0+1 i6=i0, i= 1,2,3.

2. The maximum is obtained at two indices (e.g. i0 = 2 Рё i0 = 3), i.e. mα1

1+1 <

α3

m3+1 ,mα2

2+1 = mα3

3+1

3. All the ratios are equal, i.e. mα1

1+1 = mα2

2+1 = mα3

3+1.

Consider the first case. Let i0 = 3. Note that it suffices to estimate the integral only on the closed upper half-space. By substituting ξ=θ−µ3η in I, we have

I =θ(|µ3|+(m,µ3))Z 0

Z 0

Z 0

η1m1ηm2 2η3m3e−η2kl1 1e−η2kl2 2e−η2kα1 1η22kα2η2kα3 3123

(|µ3|+(m,µ3))Z +∞

0

e

η1

α1 α3η2

α2 α3η3

2kα3

1

α1 α3η2

α2

α3η3)m3d η1

α1 α3η2

α2 α3η3

· Z

0

ηm1

α1 α3m3αα1

3

1 e−η2kl1 11 Z

0

ηm2

α2 α3m3αα2

3

2 e−η2kl2 22

=Cθ(|µ3|+(m,µ3)) =Cθi=1,2,3max (|µi|+(m,µi))

. (2.5) The last relation follows from the convergence of the three integrals and from inequalities m1αα1

3m3αα1

3 >−1, m2αα2

3m3αα2

3 >−1, which are in turn inferred from αα1

3 < mm1+1

3+1 ,αα2

3 <

m2+1 m3+1.

Consider the second case. We have αα1

3 < mm1+1

3+1 ,αα2

3 = mm2+1

3+1 and thus αα1

2 < mm1+1

2+1

The polyhedron N is completely regular, thus αl1

1 + αl2

2 + αl3

3 > 1 and µ33 < µ23. We can split I into 8 integrals:

I = Z θ−µ31

0

1

Z θ−µ32 0

2

Z θ−µ33 0

. . . dξ3+ Z θ−µ31

0

1

Z θ−µ32 0

2

Z θ−µ33

. . . dξ3

+ Z θ−µ31

0

1 Z

θ−µ32

2 Z θ−µ33

0

. . . dξ3+ Z

θ−µ31

1 Z θ−µ32

0

2 Z θ−µ33

0

. . . dξ3

+ Z θ−µ31

0

1 Z

θ−µ32

2 Z

θ−µ33

. . . dξ3+ Z

θ−µ31

1 Z

θ−µ32

2 Z θ−µ33

0

. . . dξ3

+ Z

θ−µ31

1 Z θ−µ32

0

2 Z

θ−µ33

. . . dξ3 + Z

θ−µ31

1 Z

θ−µ32

2 Z

θ−µ33

. . . dξ3 =I1+· · ·+I8. We will estimate each integral separately. The substitution ξ =θ−µ3η in I1 yields I1 ≤ Cθ(|µ3|+(m,µ3)).

By substituting ξ =θ−µ2η inI2, we get

I2 ≤Cθ(|µ2|+(m,µ2))Z 0

1 Z

0

2 Z

θ−µ33

η1m1ηm2 2η3m3e−η12kl1e−η32kl3e−η2kα1 1η2kα2 2η32kα33

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22 G.A. Karapetyan

=Cθ(|µ2|+(m,µ2))Z 0

ηm1

α1 α2m2α1

α2

1 e−η2kl1 11 Z

θ−µ3323

e−η2kl3 3 η3

3

· Z

0

η

α1 α2

1 η2η

α3 α2

3

m2

e

η

α1 α2 1 η2η

α3 α2 3

!2kα2

d(η

α1 α2

1 η2η

α3 α2

3 )≤θ(|µ2|+(m,µ2)) (C1|lnθ|+C2). The first integral converges, because αα1

3 < mm1+1

3+1. By substituting t=η

α1 α2

1 η2η

α3 α2

3 , it follows that the third integral is convergent. The second integral can be estimated via(C1|lnθ|+C2).

By substituting ξ =θ−µ3η inI3, we get

I3(|µ3|+(m,µ3))Z 1 0

1 Z

0

2 Z 1

0

m1 1η2m2ηm3 3e−η2kl1 1e−η2kl2 2e−η12kα1η2kα2 2η2kα3 3)dη3

≤Cθ(|µ3|+(m,µ3)).

We substitute ξ =θ−µ3η inI4 and estimate it similarly to I3. By substituting ξ =θ−µ3η inI5, we get

I5 ≤Cθ(|µ3|+(m,µ3))Z 1 0

ηm1

α1 α3m2αα1

3

1 e−η2kl1 11 Z

1

e−η22kl2 η22

Z 0

tm3e−t2kα3dt

≤Cθ(|µ3|+(m,µ3)). By substituting ξ =θ−µ2η inI6, we get

I6 ≤Cθ(|µ2|+(m,µ2))Z 0

ηm1

α1 α2m2α1

α2

1 e−η2kl1 11 Z

1

e−η32kl3 η33

Z 0

tm2e−t2kα2dt

≤θ(|µ2|+(m,µ2)) (C1|lnθ|+C2). By substituting ξ =θ−µ3η inI7, we get

I7 ≤Cθ(|µ3|+(m,µ3))Z 1 0

ηm1

α1 α3m2α1

α3

1 e−η2kl1 11 Z

1

e−η22kl2 η22

Z 0

tm3e−t2kα3dt

≤Cθ(|µ3|+(m,µ3)). Finally, by substituting ξ =θ−µ3η inI8, we get

I8 ≤Cθ(|µ3|+(m,µ3)). As a result, if αα1

3 < mm1+1

3+1 ,αα2

3 = mm2+1

3+1 then for some constants C1, C2 the following inequality holds:

I ≤θi=1,2,3max (i|+(m,µi))

(C1|lnθ|+C2). (2.6) Consider the third case, i.e. αα1

3 = mm1+1

3+1 ,αα2

3 = mm1+1

3+1, thus αα2

3 = mm2+1

3+1.

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Integral representation of functions and embedding theorems for multianisotropic spaces 23 Let

µ0i = min

j=1,2,3µji.

Then µ01 = µ11, µ02 = µ22, µ03 = µ33. As in the first case, we split I into 8 integrals by µ01, µ0203. We consider each integral separately. By substituting ξ=θ−µ3η in I1, we get

I1 ≤Cθ(|µ3|+(m,µ3)). By substituting ξ =θ−µ2η inI2, we get

I2 ≤Cθ(|µ2|+(m,µ2))Z 0

η1m1e−η12kl11 Z 1

0

η1m2e−η12kα1η22kα2η32kα32 Z

0

η3m3e−η32kl33

≤Cθ(|µ2|+(m,µ2)).

By substitutingξ=θ−µ3η inI3 and I4 and estimating them similarly toI2, an analogous estimate can be obtained.

By substituting ξ =θ−µ1η inI5, we get I5 ≤Cθ(|µ1|+(m,µ1))Z 1

0

1 Z

0

2 Z

0

e−η22kl2e−η32kl3e−η12kα1η22kα2η32kα3η1m1η2m2η3m33

≤Cθ(|µ1|+(m,µ1)).

Similarly, we make the substitutions ξ =θ−µ2η and ξ=θ−µ3η in I6 and I7, respectively.

Let us estimate I8. By substituting ξ =θ−µ3η, we get I8 ≤Cθ(|µ3|+(m,µ3))Z

θ−µ0131

e−η12kl1 η11

Z θ−µ0232

e−η22kl2 η22

Z 1

tm3e2kα3dt

≤ C0(lnθ)2+C1|lnθ|+C2

θ(|µ3|+(m,µ3)).

Finally, we get that in the third case there exist constants C0, C1, C2, such that I ≤(C0(lnθ)2+C1|lnθ|+C2i=1,2,3max |µi|+(m,µi)

. (2.7)

Using inequalities (2.5), (2.6) and (2.7), we proceed with the proof of Lemma 2.1. Let us estimate Gˆ1,j(t, θ), j = 1,2,3,4. For any multi-index m= (m1, m2, m3)

Dm1,j(t, θ) = 1 (2π)32

Z

R3

ξ1m1ξ2m2ξ3m3e−i(t,ξ)2k(θξαj)2k−1e−P(θ,ξ)123. (2.8)

Consider the vertexα = (α1, α2, α3)ofN, and the multi-index(m1j1, m2j2, m33j).

Suppose that:

αi

αr 6= miji + 1

mrjr+ 1, i, r= 1,2,3. (2.9) Leti0 be the index, for which the following relation holds:

i=1,2,3max

αi

miji + 1 = αi0 mi0ji0 + 1.

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24 G.A. Karapetyan

Then let us substitute ξ=θ−µi0η in integral (2.8).

According to (2.9), αi

miji+1 < αi0

mi0ji

0+1 i6=i0. Considering 1−l1µi10 ≥0, 0< θ <1

|Dm1,j(t, θ)| ≤Cθ−(|µi0|+(m,µi0)). (2.10) In the second case, i.e. when there is one equality in (2.9), (2.6) is obtained for

|Dm1,j(t, θ)|. In the third case, i.e. when there are only equalities in (2.9), (2.7) is obtained for |Dm1,j(t, θ)|.

Let us estimatetN α1 1 tN α2 2 tN α3 3Dm1,j(t, θ). Using the properties of the Fourier transform we have

θ−NtN α1 1 tN α2 2 tN α3 3Dm1,j(t, θ)

= θ−N (2π)32

Z

R3

DN αξ 1

1 DξN α2

2 DξN α3

3 e−i(t,ξ)ξ1m1ξm2 2ξ3m32k(θξαj)2k−1e−P(θ,ξ)123. Integration by parts makes it suffice to estimate the integral

θ−N Z

0

Z 0

Z 0

DξN α1

1 DN αξ 2

2 DξN α3

31m1ξm2 2ξ3m3(θξαj)2k−1e−P(θ,ξ))dξ123.

As in [4], we apply the following formula for the derivative of Φ(ξ)e−P(θ,ξ) of order N α, whereΦ(ξ) = ξm1 1ξ2m2ξ3m3

θξαj2k−1

θ−N X

β+γ=N α

C|N α||β|

Z 0

Z 0

Z 0

Dβξ1m1ξ2m2ξ3m3(θξαj)2k−1·

· X

σ1+···+σ|γ|

e−P(θ,ξ)

|γ|

Y

j=1

DσξjP(θ, ξ)dξ123,

(2.11)

where the product is taken over all σj, satisfying |σj|>0.

Suppose that the substitution ξ = θ−µiη is made in (2.11) for some i(i= 1,2,3), then, considering the equalities (αN, µi) = N(i= 1,2,3), Dξβi,β)Dβη, we find that the "con- tribution" of θ to (2.11) is

θ(2k−1)(1−(αji))

|γ|

Y

j=1

θ(2k)(1−(αri))θ−(|µi|+(m,µi)).

As (αN, µi) = N,(αr, µi) ≤ 1 , r = 1,2,3,4 , i = 1,2,3, the exponent of θ is at least

−(|µi|+ (m, µi)).

Let ρi be an exponent of ξi in (2.11) (i = 1,2,3). Consider ρ = (ρ123) and α = (α123). For the ratios ραi

i+1 (i = 1,2,3) cases 1-3 may arise. Then (2.5) is true for

|tN α1 1 tN α2 2 tN α3 3Dm1,j(t, θ)|in the first case, (2.6) in the second case, and (2.7) in the third case.

To estimate θ−N|tN β1 1tN β2 2tN β3 3Dm1,j(t, θ)| a similar argument can be used. The expo- nent of θ will be at least − max

i=1,2,3(|µi|+ (m, µi)), because the multi-index (β1, β2,0) lies

(13)

Integral representation of functions and embedding theorems for multianisotropic spaces 25 on the intersection of the plane passing through the points {α2, α3, α4} and the plane passing through the points {α1, α3, α4}. Thus, a substitution by µ1 or µ2 will yield (N β;µ1) = (N β;µ2) =N, and a substitution by µ3 will yield (N β;µ3)>N.

The estimate for θ−N

tN γ1 1 Dm1,j(t, θ)

is done similarly, taking into account that γ = (γ1,0,0) lies on the plane, passing through the points {α2, α3, α4}, and (N γ;µ1) = N, (N γ;µ2)> N, (N γ;µ3)> N.

In either case, one of (2.5), (2.6), (2.7) holds.

Remark 1. If (2.9) holds, then in (2.4) the constants C0 and C1 are 0. If there is at least one equality in (2.9), then C0 = 0.

Lemma 2.2. Let 0< θ <1, α1 < α2 < α3. Then there is a constant РЎ, such that Z

R3

dt1dt2dt3

1 +θ−N

tN α1 1tN α2 2tN α3 3 +tN β1 1tN β2 2 +tN γ1 1 =Cθ|µ1|. (2.12) Proof. Recall, thatβ1 = lα1l3

3−α3, β2 = lα2l3

3−α3, and thus ββ1

2 = αα1

2, β1 < β2.

By substituting t =θµ1η in (2.12) (note that it suffices to estimate the integral only on the closed upper half-space), we have

I = Z

0

Z 0

Z 0

dt1dt2dt3 1 +θ−N

tN α1 1tN α2 2tN α3 3 +tN β1 1tN β2 2 +tN γ1 1

1| Z

0

Z 0

Z 0

123

1 +

η

α1 α3

1 η

α2 α3

2 η3 N α3

+

η

β1 β2

1 η2 N β2

1N γ1

!.

By applying the change of variables τ11, τ2

α1 α2

1 η2, τ3

α1 α3

1 η

α2 α3

2 η3, we get I =Cθ1|

Z 0

Z 0

Z 0

123 τ

α1 α2

1 τ

α2 α3

2

1 +τ3N α32N β21N γ1. (2.13) Since αα1

2 <1, αα2

3 <1, the integral converges and I =Cθ1|.

Lemma 2.3. Let 0< θ <1, α1 < α23. Then for any multi-index

m= (m1, m2, m3) and any N satisfying (A) there are constants Ci(i= 0,1,2), such that

Dm1,j(t, θ)

≤θi=1,2,3max(i|+(m,µi)) C0(lnθ)2+C1|lnθ|+C2 1 +θ−N

tN α1 1tN α2 2tN α3 3 +tN β1 1tN β2 2 +tN γ1 1

· 1

1 +θ−N

tN α1 1tN α2 2tN α3 3 +tN σ1 1tN σ3 3 +tN γ1 1 ,

(2.14)

where γ = (γ1, γ2,0) is the point of intersection of the planes µ2 and µ3 and XOY, σ = (σ1,0, σ3) is the point of intersection of the planes µ1 and µ3 andXOZ, γ = (γ1,0,0) is the point of intersection of the µ3 plane with the x-axis.

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