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Volume 2009, Article ID 528454,22pages doi:10.1155/2009/528454

Research Article

Derivatives of Integrating Functions for

Orthonormal Polynomials with Exponential-Type

Weights

Hee Sun Jung

1

and Ryozi Sakai

2

1Department of Mathematics Education, Sungkyunkwan University, Seoul 110-745, South Korea

2Fukami 675, Ichiba-cho, Toyota-city, Aichi 470-0574, Japan

Correspondence should be addressed to Hee Sun Jung,[email protected]

Received 22 December 2008; Revised 26 February 2009; Accepted 22 April 2009

Recommended by Jozsef Szabados

Letwρx:|x|ρexpQx,ρ >1/2, whereQC2:−∞, 0,is an even function. In

2008 we have a relation of the orthonormal polynomialpnw2

ρ;xwith respect to the weight2x; pnx Anxpn−1xBnxpnx−2ρnpnx/x, whereAnxandBnxare some integrating

functions for orthonormal polynomialspnw2

ρ;x. In this paper, we get estimates of the higher derivatives ofAnxandBnx, which are important for estimates of the higher derivatives of pnw2

ρ;x.

Copyrightq2009 H. S. Jung and R. Sakai. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1. Introduction and Results

Let R −∞,∞. LetQC2 : R R 0, be an even function, and letwx

exp−Qxbe such that∞0xnw2xdx <for alln0,1,2, . . . .Forρ >1/2, we set

wρx:|x|ρwx, x∈R. 1.1

Then we can construct the orthonormal polynomials pn,ρx pnw2

ρ;xof degree nwith

respect tow2

ρx. That is,

−∞pn,ρxpm,ρxw 2

ρxdxδmn Kronecker’s delta,

pn,ρx γnxn· · ·, γnγn,ρ >0.

(2)

A functionf :R → Ris said to be quasi-increasing if there existsC >0 such that

fxCfyfor 0 < x < y. For any two sequences {bn}∞n1 and {cn}∞n1 of nonzero real numbersor functions, we writebn cnif there exists a constantC >0 independent ofnor

xsuch thatbnCcnfornlarge enough. We writebncnifbncnandcn bn. We denote the class of polynomials of degree at mostnbyPn.

Throughout C, C1, C2, . . . denote positive constants independent of n, x, t, and polynomials of degree at mostn. The same symbol does not necessarily denote the same constant in different occurrences.

We will be interested in the following subclass of weights from1.

Definition 1.1. LetQ:R → Rbe even and satisfy the following properties. aQxis continuous inR, withQ0 0.

bQxexists and is positive inR\ {0}. c

lim

x→ ∞Qx. 1.3

dThe function

Tx: xQ

x

Qx , x /0 1.4

is quasi-increasing in0,∞with

Tx≥Λ>1, x∈R\ {0}. 1.5

eThere existsC1 >0 such that

Qx |Qx| ≤C1

Qx

Qx , a.e. x∈R\ {0}. 1.6

Then we writew ∈ FC2. If there also exist a compact subintervalJ 0ofRandC2 > 0 such that

Qx |Qx|≥C2

Qx

Qx , a.e. x∈R\J, 1.7

then we writew∈ FC2.

In the following we introduce useful notations.

aMhaskar-Rahmanov-Saff MRSnumbersaxare defined as the positive roots of the following equations:

x 2

π

1

0

axuQaxu

(3)

bLet

ηx xTax−2/3, x >0. 1.9

cThe functionϕuxis defined as follows:

ϕux

⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩

a2 2ux2

uauxauηuauxauηu1/2 , |x| ≤au,

ϕuau, au<|x|.

1.10

In the rest of this paper we often denotepn,ρxsimply bypnx. Letρnρifnis odd,

ρn 0 otherwise and define the integrating functionsAnxandBnxwith respect topnx

as follows:

Anx:2bn

−∞p 2

nuQx, uw2ρudu,

Bnx:2bn

−∞pnupn−1uQx, uw 2

ρudu,

1.11

whereQx, u QxQu/xuandbn γn−1/γn. Then in2, Theorem 4.1we have a relation of the orthonormal polynomialpnxwith respect to the weightw2

ρx:

pnx Anxpn−1xBnxpnx−2ρn pnx

x , ρn

⎧ ⎨ ⎩

ρ, nis odd,

0, nis even, 1.12

and in 2, Theorem 4.2we already have the estimates of the integrating functions Anx

andBnxwith respect topnx. So, in this paper we will estimate the higher derivatives of

AnxandBnxfor the estimates of the higher derivatives ofpnwρ2;x, because the higher

derivatives ofpn,ρxplay an important role in approximation theory such as investigating convergence of Hermite-Fej´er and Hermite interpolation based on the zeros ofpnw2

ρ;x see

3,4.

To estimate of the higher derivatives ofAnxandBnxwe need further assumptions forQxas follows.

Definition 1.2. Letwx exp−Qx∈ FC2, and letνbe a positive integer. Assume that

Qxisν−times continuously differentiable onRand satisfies the followings. a1xexists andQix,i0,1, . . . , ν1 are nonnegative forx >0.

bThere exist positive constantsCi>0 such that forx∈R\ {0}

Qi1xCiQix

Qx

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cThere exist constants 0≤δ <1 andc1>0 such that on0, c1

1xC 1

x

δ

. 1.14

Then we writewx∈ FνC2.

Letνbe a positive integer. Define forν >0,m≥0, l≥1, andα≥0,

Ql,α,mx:|x|mexpl|x|αα∗expl0, 1.15

whereα∗0 ifα0, otherwiseα∗1 and define

Qαx: 1|x||x|α−1, α >1. 1.16

Here we let exp0x : xand for l ≥ 1, explx : expexp· · ·expx· · · denotes the

lth iterated exponential. In particular, explx expexpl1x. Then exp−Ql,α,mxand exp−Qαxare typical examples ofFνC2 see5.

In the following we improve the inequality4.3in2, Theorem 4.2.

Theorem 1.3. Letρ >−1/2andwx exp−Qx∈ FC2. Additionally assume thatQx

is nondecreasing. Then for|x| ≤εanwith0< ε <1/2one has

|Bnx|< λε, nAnx, 1.17

where

lim

ε→0nlim→ ∞λε, n 0. 1.18

In this paper our main theorem is as follows.

Theorem 1.4. Letρ >−1/2andwx exp−Qx∈ FνC2for positive integerν≥2. Assume that12ρδ≥0forρ <0and

ann1/1νδ, 1.19

where0≤δ <1is defined in1.14.

a If Qx/Qxis quasi-increasing on c2,, then one has for |x| ≤ an1ηnand

j0, . . . , ν−1

AnjxAnx Tan an

j

, BnjxAnx Tan an

j

(5)

Moreover, for any0< ε <1/2there existsεε, n>0such that for|x| ≤εanandj1, . . . , ν−1,

Anjxεε, nAnx n an

j

, Bnjxεε, nAnx n an

j

, 1.21

withεε, n → 0asn → ∞.

bIfQν1xis non-decreasing onc

2,, then one has1.20and1.21for the respective

ranges ofx.

cIf there exists a constant0 ≤δ <1such thatQν1xC1/xδonc2,, then one

has1.20and1.21for the respective ranges ofx.

The examples satisfying the conditionsa,b, orcofTheorem 1.4are given in5.

Remark 1.5. Under the assumptions ofTheorem 1.4, we have from2, Theorem 4.2that there existsC, n0>0 such that fornn0and|x| ≤an1Lηn,

Anx

2bnϕnx

−1a2

n12Lηn2−x2

1/2

, |Bnx|Anx, 1.22

becausewx exp−Qx∈ FνC2for positive integerν≥1 and 12ρδ≥0 forρ <0.

In addition, for our future work we estimateatandTatusingλC1in1.6for the weight classFC2.

Theorem 1.6. Letwx exp−Qx∈ FC2, and we assume

Qx |Qx|≤λ

Qx

Qx , |x| ≥b >0, 1.23

whereb >0is large enough.

aAssume thatTxis unbounded. Then for anyη >0there existsCη> 0such that for t≥1,

atCηtη. 1.24

bSuppose that there exist constantsη >0andC2>0such thatatC2tη. Then there exists

a constantCdepending only onλ,η, andC2such that forat≥1, ifλ >1

TatCt2ηλ−11, 1.25

and if0< λ≤1,

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Remark 1.7. aLevin and Lubinsky showed the following1, Lemma 3.7: there existsC >0 such that for someε >0, and for large enought,

TatCt2−ε. 1.27

If from1.25and1.26we set for any 0< η <2

ε

⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩

2−η, 0< λ≤1,

22−η

λ1 , λ >1,

1.28

then we have1.27in Levin and Lubinsky’s lemma.

bIfTxis unbounded, then1.19is trivially satisfied by1.24.

2. Proof of Theorems

In this section we will prove the theorems ofSection 1.

Lemma 2.1. Letρ >−1/2and letwx∈ FC2. Then uniformly forn1, a

sup

x∈R

pn,ρxwx |x|an n

ρ

x2−a2n

1/4

∼1. 2.1

b

sup

x∈R

pn,ρxwx |x|an n

ρ

an1/2nTan1/6. 2.2

cMarkov inequality. Let0< p≤ ∞. For any polynomialP ∈ Pn

Pwx |x|an n

ρ

LpR

nTan1/2 an

P wx |x|an n

ρ

LpR

. 2.3

dLetβ∈R,0 < p ≤ ∞, andr >1. Then there exist positive constantsL,δ, andC2such

that for any polynomialP ∈ Pn

P w)x |x|ann

β

Lparn≤|x|

exp−C2nδP wx |x|an

n

β

LpLan/n≤|x|≤an1−Lηn .

(7)

Proof. afollows from2, Theorem 2.3.bfollows from2, Theorem 2.4.cfollows form 6, Theorem 2.1b.dfollows form6, Theorem 2.3.

Lemma 2.2. Letρ >−1/2and letwx∈ FC2. Then one has forc >0,

0≤uc

pnwρ2udu 1

an. 2.5

Proof. Forρ ≥0, the results are immediate fromLemma 2.1a. So we assume−1/2 < ρ <0. First we see

0≤uan/n

pnwρ2udu

0≤uan/n

pnw2u |u|an n

2ρ | u|2ρ

|u|an/n2ρdu

C 1 an

0≤uan/n

|u|2ρ

|u|an/n2ρdu

C 1 an

n an

2ρ

0≤uan/n |u|2ρdu

C 1 an

n an

2ρ an

n

12ρ

C1 n,

2.6

because we know thatanonfrom1, Lemma 3.5c. Next we see byLemma 2.1a

an/nuc

pnwρ2uduC 1

an. 2.7

Therefore, we have the result.

Lemma 2.3. Letρ >−1/2and letwx∈ FC2. Then aone has

0≤u≤∞

pnw2u |u|an n

2ρ

Qudun

an, 2.8

bforx∈0, an/2one has

QxCn an

x an

Λ1

. 2.9

(8)

Proof ofTheorem 1.3. SinceBnxis an odd function, we prove only for 0≤ xεan. Letθ :

εΛ−1/. Then we have the following two lemmas.

Lemma 2.4. Uniformly forθandn

|u|≤θan

pnupn−1uw2ρuQx, udu

1

1

θΛ−1 n

a2

n

. 2.10

Proof. For|u| ≤θan, we have byLemma 2.1a

p2nuw2ρu

1

a2

nθan2

|u|2ρ

|u|an/n2ρ

1

an

|u|2ρ

|u|an/n2ρ. 2.11

Since Qx is nondecreasing and 1 − 1/2Λ1/2Λ ≤ θε/θ ≤ 1, we have using

Lemma 2.3b:

Qx, uQ

θanQx

θanx

Qθan

θεan θ

Λ−2 n

a2

n

. 2.12

Moreover we know that forρ >−1/2,

θan

0

|u|2ρ

|u|an/n2ρdx

|u|≤an/n

an/n≤|u|≤θan an

n θan. 2.13

Therefore, we have

|u|≤θan p2

nuwρ2uQx, udu

1

1

θΛ−1 n

a2

n

. 2.14

Consequently, we have the result using Cauchy-Schwartz inequality

|u|≤θan

pnupn−1uw2ρuQx, udu

1

1

θΛ−1 n a2

n

. 2.15

Lemma 2.5. Uniformly forθεΛ−1/and forn

θan≤|u|≤a2n

pnupn−1uwρ2uQx, udu

ε1−1/ΛΛ−1ε1/Λn a2

n

(9)

Proof. Forθan≤ |u| ≤a2n, we have similarly to2,4.6

Qx, uQx,u2uQ

xxQu x2−u2

an

QεanεanQu θan2

ε1−1/ΛΛ−1 n a2

n

ε1/Λ

an

Qu

2.17

seeLemma 2.3b. Therefore, we have byLemma 2.3a,

θan≤|u|≤a2n

pnupn−1uw2ρuQx, udu

θan≤|u|≤a2n

pnupn−1uw2ρuQx, uQx,udu

ε1−1/ΛΛ−1 n a2n

θan≤|u|≤a2n

pnupn1uw2

ρudu

ε1/Λ

an

θan≤|u|≤a2n

pnupn1uw2

ρuQ

udu

ε1−1/ΛΛ−1 n a2

n

ε1/Λ n a2

n .

2.18

Here we usedLemma 2.1b.

Since for a constantC >0

a2n≤|u|

pnupn−1uwρ2uQx, udu

O

enC

, 2.19

see2, page 233, there existsλn>0 such that

a2n≤|u|

pnupn−1uw2ρuQx, udu

λnan2

n

, 2.20

and λn → 0 asn → ∞. We know from2, Lemma 4.7that bn γn−1/γnan. From 1.22we haveAnx/bnn/a2

nfor|x| ≤εanand from the preceding considerations and the

definition ofBnxit follows that for|x| ≤εan

|Bnx|

bn

λε, nn a2n

λε, nAnx

(10)

where for some positive constantC >0

λε, n:C·max 1

1

θΛ−1, ε1−1/ΛΛ−1, ε1/Λ, λn

. 2.22

Consequently,1.17is proved, and we can obtain that limε→0limn→ ∞λε, n 0. Now, we have for|x| ≤εan

Anxn

an, |Bnx|< λε, n n

an. 2.23

Proof ofTheorem 1.4. First, we see that for 1≤jν−1

Anjx 2bn

−∞pnwρ 2

u d j

dxjQx, udu. 2.24

We split proof of1.20into some lemmas as follows:

1Lemma 2.6is for 0≤xan1ηn,a4nu, and 1≤jν−1;

2Lemma 2.9is foran/2≤xan1ηn, 0≤ua4n, and−1;

3Lemma 2.10is for 0≤xan/2, 0≤ua4n, and−1;

4Lemma 2.11is for 0≤xan1ηn, 0≤ua4n, and 1≤jν−2;

on the other hand,1.21will be proved by Lemmas2.13and2.6. For 1≤jν−1 there existsηbetweenuandxsuch that

dj dxjQx, u

j! xuj1

j

k0 −1kQ

j1−kx

jk! xu

jk 1j1

Qu

Qj1xQj1

η

xu .

2.25

Then forx≥0 andu≥0, sinceQj1uis increasing for 1jν1, we have

0≤ d

j

dxjQx, u

Qj1xQj1u

xu . 2.26

Ifu <0 andx >0, then since|Qj1η| ≤Qj1uforη <0,

d

j

dxjQx, u

Qj1xQj1η

xu

Qj1x Qj1−u

xu

Qj1xQj1−u

x−−u 2

Qj1uQj10

u−0 .

(11)

So, for this case we can prove the result similarly to the casex, u > 0. For the other cases, we can prove it by the symmetry of Q, similarly. Therefore, we assume that u and xare nonnegative, and we will prove this theorem only for nonnegativexandu. Moreover, for simplicity, we letc1c2without loss of generality, because we know by1.13that1u is bounded for anyubetweenc1andc2.

On the other hand, ifQj2uis increasing, then

Qj1uQj1x

ux 2.28

is also increasing forubecause there exists a pointξbetweenxandusuch that

d du

Qj1uQj1x

ux

Qj2u

Qj1uQj1x/ux

ux

Qj2uQj2ξ

ux ≥0.

2.29

Moreover, if1tC1/tδfor

tbetweenxandu, then we see

uQνx

ux

1

ux

u

x

1tdtC ux

u1−δx1−δC 1 u

δ

. 2.30

To complete the proof ofTheorem 1.4we prove a series of lemmas.

Lemma 2.6. Let0≤xan1ηnand1≤jν−1:

a4n<u

pnwρ2u d j

dxjQx, udu

Tan an

jAnx

an . 2.31

Proof. Since

Anjx

2bn

0≤ua4n

a4n<u

pnwρ2u d j

dxjQx, udu, 2.32

we have to estimate

a4n<u

pnwρ2u d j

dxjQx, udu:

a4n<u

. 2.33

First, we see forx >0 large enough,

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is decreasing because

Qj1xeQxQj2xQj1xQxeQx, 2.35

and so from our assumption,

Qj2xQj1xQxCQj1xQ

x QxQ

j1xQx

Qj1xQx C Qx−1

<0,

2.36

ifC < Qx. We use this fact. Let 2ρ βiwhereβ <0, and letibe a nonnegative integer, and letPu p2

nuui. Letu >0. Then since

Qj1a

4n Qa4nC

Tan an

j

, 2.37

by1.13, we have for someξbetweenxandu

a4n<u

a4n<u

pnwρ2uQj2ξdu

a4n<u

pnwρ2uQj2udu

CQ j1a

4nwa4n

Qa4n a

β

4n

a4n<u

PuwuQudu by2.34

Tan an

j

wa4naβ4n

a4n

Pu d

duwudu,

a4n Pu d

duwudu P wa4n

a4n

Ptwudu.

2.38

ApplyingLemma 2.1dwithL∞,L1-norm andLemma 2.1c,

|P wa4n| ≤exp−C2nαP wxL∞Lan/n≤|x|≤an1−Lηn,

a4n

Puwudu≤exp−C2

Pwx

L1Lan/n≤|x|≤an1−Lηn

≤exp−C2nαnTan 1/2

an P wxL1Lan/n≤|x|≤an1−Lηn.

(13)

Therefore,

a4n

PuwuQudu≤exp−C2nαP wxL∞Lan/n≤|x|≤an1−Lηn

exp−C2nαnTan 1/2

an P wxL1Lan/n≤|x|≤an1−Lηn.

2.40

Consequently we have

Tan an

j

wa4naβ4n

a4n<u

PuwuQudu

Tan an

j

exp−C2nαp2nwρ2L∞La

n/n≤|x|≤an1−Lηn

Tan

an

j

nTan1/2

an exp−C2n αp2

nwρ2L

1Lan/n≤|x|≤an1−Lηn

Oend3 Tan

an

j

Tan an

j Anx

an .

2.41

Lemma 2.7. If Qx/Qx is quasi-increasing on c1,or if 1x is nondecreasing on c1,, then one has

xQνu

xu

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

1 Tan

an

ν−1 n

a2

n

, 0≤uc1, c1≤xan2 ,

1 Tan

an

ν−1

n a2n

, c1≤u≤2c1, 0≤xc1,

Tan an

ν−1

n a2

n

, 2c1 ≤uan3 , 0≤xc1,

Tan an

ν−1

n a2n

, c1≤uan

3 , c1≤x

an

2 .

2.42

Proof. Casea-1. 0≤uc1andc1≤xan/2. Let

uQνx

ux

uQνc1

uc1

c1Qνx

c1−x

(14)

Then we haveQ1u1 from2.30. Then ifQx/Qxis quasi-increasing onc1,∞, there exists a pointξc1, xsuch that by1.13

Q2x Q

ν1ξ

Q

xQc1 xc1

ν−1 Q

an/2−Qc1 an/2−c1

Qan/2

Qan/2 ν−1

Q

an/2

an

Tan an

ν−1

n a2

n .

2.44

If1xis nondecreasing onc1,∞, there exists a pointξc1, xsuch that by2.28and 1.13

Q2xQ

νan/2Qνc1

an/2−c1

Qνan/2 Qan/2

Qan/2−Qc1 an/2−c1

Qan/2

Qan/2 ν−1

Q

an/2

an

Tan an

ν−1 n

a2

n .

2.45

Casea-2. Forc1 ≤u≤2c1and 0≤xc1, we have similarly to Casea-1,

Q2x1, Q1u Tan

an

ν−1

n a2

n

. 2.46

Caseb. 2c1≤uan/3 and 0≤xc1. Using the method of Casea-1, and similarly to Casea-2,

QνuQνx

ux

QνuQνc1

uc1

Tan an

ν−1

n a2n

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Casec.c1 ≤uan/3 andc1≤xan/2. We can prove similarly toQ1uandQ2x of Casea-1. IfQx/Qxis quasi-increasing onc1,∞, there exists a pointξc1, xsuch that by1.13

xQνu

xu

Q

ν1ξ

Q

xQu xu

Qan/2

Qan/2 ν−1

Q an/2 an

Tan an

ν−1

n a2

n .

2.48

If1xis nondecreasing onc

1,∞, there exists a pointξc1, xsuch that by1.13

QνxQνu

xu

Qνan/2−Qνu an/2−u

|Qan/2|

Qan/2 ν−1

Q an/2 an

Tan an

ν−1 n

a2

n .

2.49

Lemma 2.8. One has

xQνu

xu

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩ 1

uδ, 0≤uc1, 0≤xc1,

Tan an

ν−1

Qx, u, 0≤ua4n, an

2 ≤xan

1ηn,

Tan an

ν−1

Qx, u an

3 ≤ua4n, 0≤x

an

2 .

2.50

Proof. Casea. 0≤uc1and 0≤xc1. From2.30and1.14

uQνx

uxC

1

u

δ

. 2.51

Caseb-1. 0 ≤ uan/3 andan/2 ≤ xan1ηn. Since by1, page 64, Lemma 3.2a

Qan/2

Qan/3 ≥ 3 2

Λ1

(16)

we have

QxQuQx

1−Q

an/3

Qan/2

Qx

1− 2

3 Λ−1

. 2.53

Therefore, since for this case

QxQuQx, 2.54

we have

xQνu

xu

xQνu

QxQu Qx, u

Qνx Qx

Qx, u

Tan an

ν−1

Qx, u.

2.55

Caseb-2.an/3≤ua4nandan/2≤xan1ηn. There exists a pointξbetweenx

andusuch that by1.13

xQνu

xu

xQνu QxQu Qx, u

1ξ

Qx, u

ξ

ν−1

Qx, u

Tan an

ν−1

Qx, u.

2.56

Casec.an/3≤ua4nand 0≤xan/4. By the same method as Caseb, we have

xQνu

xu

Tan an

ν−1

Qx, u. 2.57

Lemma 2.9. Letan/2≤xan1ηn. Then

0≤ua4n

pnwρ2u d ν−1

dxν−1Qx, udu

Tan an

ν−1Anx

an . 2.58

(17)

Lemma 2.10. Let0≤xan/2.

aIf0≤xc1, then

0≤uc1

pnwρ2u d ν−1

dxν−1Qx, udu 1

an. 2.59

Moreover, one knows that

1

an

Tan an

ν−1Anx

an . 2.60

bIfQx/Qxis quasi-increasing onc1,, or ifQν1xis nondecreasing onc1,,

then

0≤ua4n

pnwρ2u d ν−1

dxν−1Qx, udu

Tan an

ν−1

Anx

an . 2.61

cIf there exists a constant0 ≤δ < 1such thatQν1xC1/xδon0,, then one has2.61.

Proof. aFor 0≤xc1we have from Lemmas2.8,2.1a, and2.2

0≤uc1

pnwρ2u d ν−1

dxν−1Qx, udu

0≤uc1

pnwρ2uuδdu

⎧ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎩

1

an, ρ≥0,

1

an n an

2ρ

0≤uc1

u2ρδ 1 an

n an

2ρ

, ρ <0

1 an,

2.62

because 12ρδ≥0 forρ <0. On the other hand, from1.19we see

nnν/1νδn, and

from1.22we seeAnxn/anfor 0≤xc1. So we have

1

an

n aνn1

n a2

n

Tan an

ν−1

Anx an

Tan an

ν−1

(18)

bFor 0≤xc1, we have froma, Lemmas2.7, and2.8

0≤ua4n

pnwρ2u d ν−1

dxν−1Qx, udu

0≤uc1

c1≤u≤2c1

2c1≤uan/3

an/3≤ua4n

Tan an

ν−1Anx

an .

2.64

Similarly, forc1≤xan/2 we have from Lemmas2.7and2.8

0≤ua4n

pnwρ2u d ν−1

dxν−1Qx, udu

0≤uc1

c1≤uan/3

an/3≤ua4n

Anx an

Tan an

ν−1

.

2.65

cThen by2.26andLemma 2.1a

0≤ua4n

pnwρ2u d ν−1

dxν−1Qx, udu

0≤ua4n

pnwρ2uuδdu

0≤ua4n

u2ρδ

uan/n2ρ

u2a2

n du

0<u<an/n

an/nuan/2

an/2≤ua4n

1

n

n a2n

1

an

ν−1

Anx an

Tan an

ν−1

.

2.66

Here, we use the fact 1/aδ

n< n/aνn1from1.19for the last inequality.

Lemma 2.11. Let0≤xan1ηn. Then for1≤jν−2,

0≤ua4n

pnwρ2u d j

dxjQx, udu Anx

an

Tan an

j

. 2.67

(19)

To prove1.21we need some lemmas.

Lemma 2.12. Let0< ε <1and|x| ≤εan.

aFor someC >0one has

Qεan QεanC

εΛ−1

Qεan n

an. 2.68

bFor any0< ε <1, there existsε1ε, n>0such that for2εanu

dj

dxjQx, uε1ε, n Anx

an n an

j

Qx, u

εanj , 2.69

andε1ε, n → 0asn → ∞.

Proof. aIt follows fromLemma 2.3b.bBy2.25,Lemma 2.3b, anda, we have

dj

dxjQx, uC j−1

k0

Qj1−kx

εank1

Qx, u

εanj

C j−1

k0

Qεan

εank1

εΛ−1

Qεan n an

jk

Qx, u εanj

C j−1

k0

εΛ−1 εank1

n an

εΛ−1

Qεan n an

jk

Qx, u εanj

Cn a2

n n an

j j−1

k0

εΛ−k−2

εΛ−1

Qεan

jk

1

n

k

Qx, u εanj

ε1ε, nAnx an

n an

j

Qx, u εanj ,

2.70

where we let

ε1ε, n:C j−1

k0

εΛ−k−2

εΛ−1

Qεan

jk

1

n

k

−→0 2.71

asn → ∞. Therefore, this lemma is proved.

Lemma 2.13. Suppose that the one of the three conditions (a), (b), and (c) inTheorem 1.4is satisfied. Then for any0< ε <1/2, there existsε2ε, n>0such that for|x| ≤εanandj1, . . . , ν−1,

0≤ua4n

pnwρ2u d j

dxjQx, uduε2ε, n Anx

an n an

j

, 2.72

(20)

Proof. First, we consider the case of which cin Theorem 1.4is satisfied. Then the lemma follows from2.66withε2ε, n: 1/nν−1. Now, we consider the other cases. If we consider only for |x| ≤ εan and |u| ≤ 2εan in proving Lemmas 2.7and 2.8, then we know that for

|x| ≤εanandj1, . . . , ν−1

dj

dxjQx, u

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

1uδ Qεan Qεan

j

Qεan

εan , 0≤u≤2c1,

Qεan Qεan

j

Qεan

εan , 2c1 ≤u

ε

2an,

Qεan Qεan

jQεan

εan ,

ε

2anu≤2εan.

2.73

Then we have byLemma 2.12a

0≤u≤2εan

pnwρ2u d j

dxjQx, udu

0≤u≤2c1

2c1≤u≤2εan

1 aδn

Qεan Qεan

j

Qεan εan

⎛ ⎝a2njδ

n1j ε

Λ−2

εΛ−1

Qεan

j

Anx

an n an j , 2.74

and we can see that

ε3ε, n: a 2jδ n n1j ε

Λ−2

εΛ−1

Qεan

j

−→0 as n−→ ∞. 2.75

Finally, we estimate2εa

nua4n. ByLemma 2.12bwe have

2εanua4n

pnwρ2u d j

dxjQx, udu

2εanua4n

ε1ε, nAnx an

n an

j

1

εanjQx, u

pnwρ2udu

ε1ε, n 1

εnj

(21)

Therefore, if we letε2ε, n:ε3ε, n ε1ε, n 1/εnj,then

0≤ua4n

pnwρ2u d j

dxjQx, uduε2ε, n Anx

an n an

j

, 2.77

andε2ε, n → 0 asn → ∞by2.75and2.76.

From the proof ofLemma 2.6, we have the following. There existsε4n>0 satisfying

ε4n → 0 asn → ∞such that

ua4n

pnwρ2u d j

dxjQx, uduε4n Anx

an n an

j

. 2.78

Therefore, from Lemmas2.6,2.9,2.10, and2.11we obtain the estimate forAnjxin1.20,

and fromLemma 2.13and2.78we have the estimate for Anjxin1.21. Using

Cauchy-Schwarz Inequality we also have the estimate forBnjxin1.20and1.21. Consequently,

we provedTheorem 1.4, completely.

Proof ofTheorem 1.6. a 1.24follows from1,3.45easily.

bSuppose that1.23is satisfied on|x| ≥Dfor someD >0 large enough. Letx > D. From1.23we have for largex > D

ln

Qx QD

≤ln Qx

QD

λ

, 2.79

and we have for largex > D

Qx QD

Qx QD

λ

. 2.80

Caseλ >1. Then we can see by1, Lemma 3.43.18and2.80

Tat atQ

at Qat

QD

QDλatQat λ−1

Cat

t

Tat

λ−1

. 2.81

Therefore from the assumptionatC2we have for anyη >0

TatCλ, ηt2ηλ−11. 2.82

Case 0< λ≤1. Then we have by2.80

Tx xQ

x Qxx

QD QDλQx

λ−1

xQ

D

(22)

Therefore, from the assumptionatC2we have for anyη >0

TatCλ, ηtη. 2.84

Acknowledgments

The authors thank the referees for many kind suggestions and comments. The first author was supported by the Korea Research Foundation Grant funded by the Korean Government KRF-2008-C00017.

References

1 E. Levin and D. S. Lubinsky,Orthogonal Polynomials for Exponential Weights, vol. 4 ofCMS Books in Mathematics/Ouvrages de Math´ematiques de la SMC, Springer, New York, NY, USA, 2001.

2 H. S. Jung and R. Sakai, “Orthonormal polynomials with exponential-type weights,” Journal of Approximation Theory, vol. 152, no. 2, pp. 215–238, 2008.

3 Y. Kanjin and R. Sakai, “Pointwise convergence of Hermite-Fej´er interpolation of higher order for Freud weights,”Tohoku Mathematical Journal, vol. 46, no. 2, pp. 181–206, 1994.

4 P. V´ertesi, “Hermite-Fej´er interpolations of higher order. I,”Acta Mathematica Hungarica, vol. 54, no. 1-2, pp. 135–152, 1989.

5 H. S. Jung and R. Sakai, “Specific examples of exponential weights,” Communications of Korean Mathematical Society, vol. 24, no. 2, pp. 303–319, 2009.

References

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