Volume 2018, Issue 1 5360857
Research Article
Open Access

Estimates on the Bergman Kernels in a Tangential Direction on Pseudoconvex Domains in

Sanghyun Cho

Corresponding Author

Sanghyun Cho

Department of Mathematics, Sogang University, Seoul 04107, Republic of Korea sogang.ac.kr

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First published: 18 July 2018
Citations: 1
Academic Editor: Milan Pokorny

Abstract

Let Ω be a smoothly bounded pseudoconvex domain in and assume that where z0bΩ, the boundary of Ω. Then we get optimal estimates of the Bergman kernel function along some “almost tangential curve” Cb(z0, δ0) ⊂ Ω ∪ {z0}.

1. Introduction

Let Ω be a bounded domain in . A natural operator on Ω is the orthogonal projection
(1)
where H(Ω) denotes the holomorphic functions on Ω. There is a corresponding kernel function KΩ(z, w), called the Bergman kernel function on Ω. The nature of the singularity of KΩ(z, w) tells us much about the holomorphic function theory of the domain in question and has been studied extensively since Bergman’s original inquiries [1].

One of the methods for the estimates of the Bergman kernel is to construct maximal size of polydiscs in Ω where we have a plurisubharmonic function with maximal Hessian. For strongly pseudoconvex domains in , these polydiscs are of size δ > 0 in normal direction and of size δ1/2 in tangential directions. For weakly pseudoconvex domains, the size of the polydisc in tangential directions depends on the boundary geometry of Ω near z0bΩ, and hence we need complete analysis of the boundary geometry near z0.

However these analyses and hence the optimal estimates on the Bergman kernels are done only for special type of pseudoconvex domains of finite type in . These domains are, for example, pseudoconvex domains of finite type in [24], decoupled, convex, or uniformly extendable domains of finite type in [57], or pseudoconvex domains in with (n − 2) positive eigenvalues [8, 9]. For the estimates for weighted Bergman projections, one can also refer to [1012]. Nevertheless, the optimal estimates for general pseudoconvex domains of finite type in , n > 2, are not known, even for n = 3 case.

Assume that Ω is a smoothly bounded domain in with smooth defining function r with smooth boundary, bΩ. Regular finite 1-type at z0bΩ, denoted by , is the maximum order of vanishing of rγ for all one complex dimensional regular curve γ, γ(0) = z0, and γ(0) ≠ 0. Thus satisfies
(2)
where Δq(z0), 1 ≤ qn − 1, denotes finite q-type in the sense of D’Angelo [13]. Note that Δn−1(z0) = TBG(z0) where TBG(z0) is the type in the sense of Bloom-Graham.

Remark 1. Consider the domain Ω [13] in defined by

(3)
Then and Δ2(0) = 4 while Δ1(0) = as the complex analytic curve γ(t) = (t3, t2, 0) lies in the boundary. Note that γ(t) is not regular curve.

In the sequel, we let Ω be a smoothly bounded pseudoconvex domain in , and assume that where z0bΩ. Let Cb(z0, δ0) ⊂ Ω ∪ {z0} be the “almost tangential curve" connecting a point and z0bΩ as defined in (20). Note that dist(zδ, bΩ) ≈ δ for each zδCb(z0, δ0). Set τ1 = δ1/η, τ2 = τ(zδ, δ) where τ(zδ, δ) is defined in (51).

Theorem 2. Let Ω be a smoothly bounded pseudoconvex domain in and assume that where z0bΩ. Then KΩ(zδ, zδ), the Bergman kernel function of Ω at zδCb(z0, δ0), satisfies

(4)

Theorem 3. Let Ω and z0bΩ be as in Theorem 2. For each α = (α1, α2, α3), there is a constant Cα > 0, independent of δ > 0, such that

(5)
for zΩ and zδCb(z0, δ0).

Remark 4. (1) In Theorems 2 and 3, we do not assume that Δ1(z0) < , but we assume only that (see Remark 1). With this weaker condition, we get optimal estimates for Bergman kernel function along special “almost tangential” direction, Cb(z0, δ0), but not normal or arbitrary direction.

(2) In [14], Herbort gives an example of a domain where the Bergman kernel grows logarithmically when zΩ approaches to z0bΩ in normal direction. Set

(6)
and for each small δ > 0, set zδ = (0,0, −δ). Thus zδ approaches to 0 ∈ bΩH in normal direction as δ → 0. In this case, Herbort shows that KΩ(zδ, zδ) ≈ δ−3(−log⁡δ) −1; that is, the kernel grows logarithmically. For the same domain ΩH in (6), we note that and hence τ1 = δ1/6, τ2 = δ1/3 in (4). Set Cb(z0, δ0)≔{(δ1/6/2, 0, −δ) : 0 ≤ δδ0}. Then zδ≔(δ1/6/2, 0, −δ) ∈ Cb(z0, δ0) approaches to 0 ∈ bΩ in “almost tangential direction”. In the Appendix of this paper, we will show that
(7)

In Section 2, we will construct special coordinates which reflect the regular finite type condition, , and then show that r(z) vanishes to order η in z1-direction. We then consider the slices of Ω by fixing z1. Then the domains become domains in , and hence we can handle them. Also, the condition Δ2(z0) < acts like the condition Δ1(z0) < on these slices.

For the estimates of K(z, w), Catlin [2, 15] constructed plurisubharmonic functions with maximal Hessian near each thin δ-strip of bΩ (Section 3 of [2]). In this paper, however, we will construct these functions only on nonisotropic polydiscs Qaδ(zδ)⊂⊂Ω for each zδCb(z0, δ0) (Proposition 23). This avoids complicated technical parts in Section 3 of [2]. To get estimates of KΩ(z, zδ), zΩ, zδCb(z0, δ0), we consider dilated domains Dδ for each δ > 0. Then the polydisc Qaδ(zδ)⊂⊂Ω becomes P(0,1)⊂⊂Dδ, independent of δ > 0, where P(0,1) is a polydisc of radius one with center at the origin. Therefore the uniform 1/2-subelliptic estimates for -equation hold on P(0,1), and the estimates for KΩ(z, zδ) follow.

Remark 5. Let Ω be a smoothly bounded pseudoconvex domain in , and assume that Δ1(z0) < , where z0bΩ. Then the conditions of Theorems 2 and 3 are satisfied. Near future, using the results of Theorems 2 and 3, we hope we can prove some function theories on Ω, for example, the existence of peak function for Ω that peaks at z0bΩ or necessary conditions for the Hölder estimates for -equation.

2. Special Coordinates

In the sequel, we let Ω be a smoothly bounded pseudoconvex domain in and assume that , z0bΩ. Note that m and η are positive integers. Without loss of generality, we may assume that z0 = 0. In the sequel, we let α = (α1, α2, α3) and β = (β1, β2, β3) be multi-indices and set α = (α1, α2) and z = (z1, z2), etc. In Theorem 3.1 in [16], You constructed special coordinates which represent the local geometry of bΩ near z0.

Theorem 6. Let Ω be a smoothly bounded pseudoconvex domain in with smooth defining function r and assume , 0 ∈ bΩ. Then there is a holomorphic coordinate system z = (z1, z2, z3) about 0 such that

(8)
where
(9)

(Idea of the proof) by the standard holomorphic coordinate changes, r(w) has the Taylor series expansion as in (8). Since , there is a regular curve which we may assume that satisfying |r(γ(t))| ≈ |t|η for all sufficiently small . Set z = (w1, w2 + γ2(w1), w3). Then, in z coordinates, r(z) has representation satisfying (8). Also (9) follows from the condition that m = Δ2(0).

Remark 7. (1) The second condition in (8) and property (9) say that r(z) vanishes to order η along z1 axis and order m along z2 axis.

(2) There are much more terms (mixed with z1, z2 and their conjugates), compared to the h-extensible domain cases, in the summation part of (8).

In conjunction with multitype , we need to consider the dominating terms (in size) among the mixed terms in z1 and z2 variables in the summation part of (8). Using the notations of Section 3.2 in [16], set
(10)
Then there are (pν, qν) ∈ S for ν = 0,1, …, N and ην, λν > 0 for ν = 1, …, N, such that
(11)

Remark 8. (1) Here, pν’s and qν’s are the exponents of z1 and z2, respectively, in the dominating terms in the summation part of (8).

(2) If Δ1(z0) < , then the expression in (8) will be similar to that of case in [2], and hence we need not consider the above complicated pairs.

Set t0 = η. If 1 ≤ km, then qν−1 < kqν for some ν = 1, …, N. In this case, set
(12)
Then (pν−1, qν−1), (tl, l), and (pν, qν) are colinear points in the first quadrant of the plane, and λν (resp., ην) is the intercept of q-axis (resp., p-axis) of this line. Let Lν be the line segment from (pν−1, qν−1) to (pν, qν) for ν = 1, …, N, set L = L1L2 ∪ …∪LN, ΓL = {(α, β) ∈ Γ; (α1 + β1, α2 + β2) ∈ L}, and set
(13)
As in Corollary 3.8 and Remark 3.9 in [16], we can rewrite (8) so that
(14)
where is a nontrivial homogeneous polynomial of degree pν given by
(15)
and there are a small constant a0 > 0, and such that
(16)
for all α2 + β2 = qν with all ν = 1, …, N − 1. Property (16) means that there is (α, β) with terms mixed in z2 and variables for |z1d| < a0. Let |d| = 1 be the constant (direction) in (16) and we will fix d in the rest of this paper. In the sequel, we set equal to zl or , l = 1,2, 3.

Remark 9. (a) {tk} defined in (12) is strictly decreasing on k.

(b) Each of the summation parts of (14) contains the terms of the form where (tk, k)’s are the pairs, defined in (12), on the polyline L.

(c) Each term of the first summation part in (14) is pure in z2 or variables.

(d) Each term of the second summation part in (14) has terms mixed in z2 and , and it corresponds to the pair of integers (pν, qν), the vertices of the polyline L.

Lemma 10. Let d0(z1)≔r(z1, 0,0) be the term containing only z1 or variables in the first sum of (14). Then

(17)

Proof. From (8) and (14), we see that . On the other hand, since the regular 1-type at 0 ∈ bΩ is equal to , there is such that .

In the sequel, we let V be a small neighborhood of z0 = 0 ∈ bΩ where r(z) has expression as in (14). Since (r/z3)(0) ≠ 0, we may assume that |(r/z3)(z)| ≥ c0 for all zV for a uniform constant c0 > 0 by shrinking V if necessary. For each fixed δ > 0 and for each z = (z1, z2, z3) ∈ V satisfying |z1dδ1/η| < γδ1/η, for a sufficiently small γ > 0 to be chosen, we set , where π(z) is the composition of the projection onto z1z3 plane and then the projection onto bΩ along the Re⁡z3 direction. Using the Taylor series method in z3 variable about eδ, we see that
(18)
Since |eδ| ≪ 1 and on V, it follows from (17) that
(19)
for z1 near 0.
Now for each small δ > 0, set z(δ)≔(dδ1/η, 0,0) and set . For a small constant b > 0 to be chosen, set zδ = (dδ1/η, 0, eδbδ) ∈ Ω, and for a fixed small δ0 > 0 satisfying , set
(20)
connecting and z0 = 0 ∈ bΩ.

Following the same arguments as in the proof of Proposition 1.2 in [2], for each fixed , we can construct special coordinates about so that, in terms of new coordinates, there is no pure terms in z2 or variables in the first summation part of r(z) in (14). We will fix z1 variable and consider the coordinate changes only on z = (z2, z3) variables.

Proposition 11. For each fixed , there is a holomorphic coordinate system such that in the new coordinates ζ defined by

(21)
where
(22)
and where , l = 2,3, …, m, depends smoothly on , the function given by satisfies
(23)

Proof. For , define

(24)
where w = (w2, w3). Then we have
(25)

Assume that (22) and (23) hold for l ≥ 2. That is, we have defined so that can be written as

(26)
If we define Φl = Φl−1ϕl, where
(27)
then satisfies (26) for l replaced by l + 1. If we proceed up to l = m and set , then by setting , we see that (22) and (23) hold.

In the sequel, we will use the coordinate changes in Proposition 11 only at , (in particular at in Section 3). We want to study the dependence of about . For each , set , and we note that
(28)
where ρl is defined in the inductive step of the proof of Proposition 11. Set
(29)
and set ρ0 = r. Then and
(30)
To study the dependence of and hence dependence of about in (23), we thus need to study the dependence of on variable. For a convenience, set , i.e., remove tilde’s, and assume that satisfies
(31)
for a sufficiently small γ > 0 to be chosen. In view of (19), we see that satisfies (31). In following we let z be the given coordinates, and we let ζ be the coordinates obtained from holomorphic coordinates changes of z, as in l-th step of coordinate changes in the proof of Proposition 11. Also we let (resp., ), k = 1,2, 3, denote any partial derivative operator of order s with respect to zk and (resp., ζk and ) variables. According to the coordinate changes in Proposition 11, we note that .

Proposition 12. Assume that satisfies (31). Then for each i = 0,1, …, m + 1, we have

(32)
and for each α2, β2 > 0 with α2 + β2 = qν, for some qν in (14), we have
(33)

Proof. We will prove by induction on i. From (14), (17), and (31) one obtains

(34)
and hence (32) follows for i = 0. Since ρ1(z1, ζ) = r(z1, ζ2, z3 + e0ζ3), it follows, from (31) and chain rule, that
(35)
because we are evaluating at . This proves (32) for i = 1.

By induction, assume that (32) holds for i = 0,1, …, s. For the defined in (29), it follows, from (34) and induction hypothesis, that

(36)
for i = 1, …, s. Since we are evaluating at ζ2 = 0, it follows, for s ≥ 1, that
(37)
By (30), (36), and (37) and by induction, (32) holds for i = s + 1 because tkts if ks.

Now we prove (33). Assume α2 + β2 = qν with α2 > 0, β2 > 0 where (pν, qν) are the pairs corresponding to the second summation part of (14). Note that the first summation part of (14) will be annihilated by because it contains the pure terms of z2 or mixed with . Thus it follows from (14), (16), and (31) that

(38)
Since ρ1(z1, ζ) = r(z1, ζ2, z3 + e0ζ3), it follows from (31) and (38) that
(39)
Similarly, since ρ2(z1, ζ) = ρ1(z1, ζ2, ζ3 + e1ζ2), it follows from (36) that
(40)
because for qν ≥ 2. This proves (33) for i = 2.

By induction assume that (33) holds for i = 2, …, s. If k = qν = αν + βν with αν > 0 and βν > 0, that is, if has mixed derivatives of /ζ2 and , we note that (37) becomes

(41)
If k = qνs, (33) follows from (41) and induction hypothesis of (33). If qν > s, it follows, from (36), (41), and induction hypothesis of (33), that
(42)
because for qν > s. Therefore (33) is proved for i = s + 1.

Recall the expression of ρ = ρm+1 and coefficient functions in (23).

Corollary 13. Assume that satisfies (31). Then

(43)
and if j + k = qν for some qν in (14), then
(44)

Proof. From (23) we see that

(45)
where and j, k > 0. Hence it follows from (32) that
(46)
Assume qν = j + km for some qν. Thus j, k > 0 and it follows from (23), (33), and (41) that
(47)
because .

Remark 14. Suppose that qν−1 < lqν and pνtl < pν−1. Then (pν, qν), (tl, l), and (pν−1, qν−1) are colinear points. From the standard interpolation method, we have

(48)
for all sufficiently small a, b ≥ 0. Assume that j, k > 0 and l = j + kqν for any of ν = 1,2, …, N. Therefore it follows from (43) and (48) that
(49)
Therefore the terms of the form , with j + k = qν for some qν, in the summation part in (23), are the major terms which bounds the other summation terms from above.

In the sequel, we assume that satisfies (31). As in Section 1 in [2], for each , set
(50)
In view of Remark 14, we will consider Al(z1) only for l = qν, 0 ≤ νN − 1. From (9) and (44) we note that
(51)
because q0 = m. For each sufficiently small δ > 0, set
(52)
and set
(53)
From (51) and (52), we see that if δ < δ, then
(54)

Lemma 15. For each 0 < ϵ ≤ 1, .

Proof. Set and . Then

(55)
Therefore because 0 < ϵ ≤ 1.

Proposition 16. Assume satisfies (31). Then

(56)
where .

Proof. By (31), we note that |z1| ≈ δ1/η. Assume that . Then by (51). Therefore it follows, from (50) and (52), that

(57)
and hence it follows from (52) and (53) that
(58)
Thus follows. Similarly, one can show that .

Let 0 < σ < 1 be a small constant to be determined (in Remark 22). By Lemma 15, for each 0 < σ < 1, independent of δ > 0. Therefore there is a smallest integer , 0 ≤ sm − 1, such that
(59)
Then ts = qν(s) for some qν(s) by (53). In following, for the fixed integer in (59), set δs = σsδ, , and τ1 = δ1/η as usual. If we define , where Φ3(ζ) is defined in (22), we may regard that is a biholomorphism. For each , set . For each small γ > 0, define
(60)
and set and when s = 0.

Proposition 17. The function satisfies

(61)

Proof. Recall that ρ = ρm+1, and |z1| = δ1/η in (32). When k = 0, it follows from (12) (t0 = η) and (32) that

(62)
Assume 1 ≤ km. Then by (12), qν−1 < kqν for some ν, and hence it follows that pνtkpν−1. Therefore one obtains, from (48)–(52), that
(63)
From (32) and (63), it follows that
(64)

Using the z coordinates defined in (14), set
(65)
Then Lk, k = 1,2, are tangential holomorphic vector fields and |L3r| ≥ c0 > 0 on VΩ for a uniform constant c0 > 0. For any j, k with j, k > 0, define
(66)
In ζ-coordinates defined by , set , k = 1,2, 3 and set , k = 1,2. If we define
(67)
then by functoriality,
(68)

Lemma 18. There is a small constant c2 > 0 such that

(69)
provided γ > 0 is sufficiently small.

Proof. Since the level sets of ρ are pseudoconvex, it follows from (61) that

(70)
Recall that is the term which contains only z1 or variables in the first summation part of (14). Therefore it follows, from (17), (19), and (23), that
(71)
because |z1| = |dδ1/η| = τ1 = δ1/η. If , it follows from (61) and (71) and by using the Taylor series method that
(72)
provided γ > 0 is sufficiently small. Thus (69) follows from (68), (70), and (72).

In the sequel, we let c2 and C2 be the constants which may different from time to time but depend only on the derivatives of r or ρ up to order η. Recall that , k = 1,2. By using (61), and by using Taylor series method, one obtains that
(73)
provided γ > 0 is sufficiently small, where and . Note that we can write
(74)
where . By applying or successively to , we obtain that
(75)
where, by (73) and by using induction method, Rj+k−1 satisfies
(76)
Combining the estimate in (61), (75), and (76), one obtains that
(77)
Assume that (59) holds. Thus ts = qν(s) for some qν(s), and hence it follows from (53) that . Therefore it follows from (23) and (50) that there exist integers j, k > 0 with j + k = ts = qν(s), such that
(78)
For these j, k > 0, it follows from (61), (75), (76), and (78) and by using the Taylor series method that there are constants c2, C2 > 0 such that
(79)
provided γ > 0 is sufficiently small.

Lemma 19. There is C2 > 0 such that

(80)

Proof. By functoriality, we have

(81)
From (23), we see that
(82)
and it follows from (61) that
(83)
Therefore (80) follows from (73), (81), and (83) and by using Taylor series method.

Note that , for some qν(s), and hence there exist j > 0, k > 0 with j + k = ts. In view of (79), we may assume that
(84)
is valid (when j = 1, we replace by ). Set
(85)
By using the estimates (73)–(76), one obtains that
(86)
and similarly,
(87)
for , where and .

Lemma 20. Assume that (59) holds. Then

(88)

Proof. Suppose . In view of (51)–(53), (56), and (59), we see that

(89)
and hence it follows that
(90)
This together with (73)–(78) implies the estimate (88).

In the sequel, we write
(91)

Lemma 21. There is a positive number σ > 0, independent of and δ, such that if and if (59) holds, then there are constants c2 > 0 and C2 > 0, independent of , δ and σ > 0, such that

(92)

Proof. Suppose . From (87) and (88), we note that

(93)
for j, k = 1,2 where and . Using (84)–(88) and (93) and by using small (large) constant method, one obtains that
(94)
for some c2 > 0 and C2 > 0 provided σ > 0 is sufficiently small.

Remark 22. From now on, we fix constants c2 > 0 and C2 > 0, which depend only on the derivatives of r or ρ of order up to η on V, satisfying (69), (73), (80), and (86)–(92), and set for a convenience. Now we choose and fix γ > 0 and then fix σ > 0 so that

(95)

3. Estimates on the Bergman Kernels

Recall that where z(δ) = (dδ1/η, 0, −δ) and where π is the projection defined before (19). Also note that where and where is the holomorphic coordinate function defined in Proposition 11 about . Also recall Cb(z0, δ0) defined in (20). In this section we estimate the Bergman kernel function KΩ(z, zδ), for zΩ and zδCb(z0, δ0).

To get optimal estimates of the Bergman kernel, we need to construct a plurisubharmonic function which has maximal Hessian near each thin neighborhood of bΩ as in [2, 15]. It contains complicated estimates depending on the type conditions of each boundary points. In this paper, however, we will construct such functions only at . This will make the estimates much simpler than those in [2, 15] but still contain many complicated estimates.

Note that σ > 0 and γ > 0 are fixed in Remark 22 and hence the type ts and the integer s defined in (59) depend only on . Recall that δs = σsδ, τ1 = δ1/η, , and . From (54) we have
(96)
Let us write L = a1L1 + a2L2 + a3L3.

Proposition 23. There exist a smooth plurisubharmonic function on that satisfies the following:

(i) , for , and is supported in .

(ii) There exist a small constant b > 0 such that if , then

(97)

(iii) If where Φ3 is defined in (22), then

(98)
holds for all where .

Proof. For each fixed , we note that the integers and ts, defined in (59), will be fixed. Set and . Note that provided δ > 0 is sufficiently small. Since δs = σsδ, it follows from (80) that

(99)
for . From now on, we fix and set λs = σ−2sλ.

We may assume that the level sets of r are pseudoconvex on V and on VΩ, where we may assume that . Also 4C2γ1/2c2/10 by (95). Therefore it follows from (69) and (99) that

(100)
for .

Let ψ(ζ) be defined by

(101)
where χ is a smooth function such that χ(t) = 1 for t < γ2/9 and χ(t) = 0 for tγ2, satisfying |Dkχ| ≤ Ckγ−2k. Set . Note that has similar expression as in (22). Thus it follows, from (22), (29), (30), and chain rule, that
(102)
Here α = (α1, α2, α3) and |α| = α1 + α2 + α3. Since , one obtains
(103)
where and .

Suppose that z satisfies Ψ(z) ≥ 1/4. Using the fact that Lkr = 0, k = 1,2, and the fact that 84C2γ−9/2 = (c2/5)λ ≤ (c2/5)λs, it follows from (100)–(103) that

(104)
We note that the negative part in (104) contains γ1/2λ instead of γ1/2λs.

Let h be a smooth convex function such that h(t) = 0 for t ≤ 1/2 and h(t) > 0 for t > 1/2 and h(9/8) ≤ 1. Set and set . Suppose . Then s = 0, and hence (79) holds for δs = δ with j = k = 1; that is,

(105)
For those z with Ψ(z) ≥ 1/4, it follows from (104) (with λs = λ) and (105) that
(106)
If Ψ(z) ≤ 1/4, then and hence . Hence is a smooth plurisubharmonic function supported on , and .

Now assume and assume that (59) holds. Then (79) holds for some positive integers j, k with j + k = ts. Let G(z) be the function defined in (85). From (88) and (95), we see that

(107)
, because and tsm. Set
(108)
where ϕ(t) is a smooth function that satisfies ϕ(t) = t, for t ≤ 1/16, ϕ(t) = 0 for t ≥ 1, and ϕ(t) ≤ 1/8 for all t. Thus and because h(9/8) ≤ 1. By (107) we note that ϕ(z) = z on , and we also note that if , in particular, outside . From (92), we obtain that
(109)
for , because γ1/2C2c2/40.

Assuming that , we note that the negative coefficient part of of the Hessian of in (104) is controlled by the first term in the third line of (109), and the error terms of the coefficients of and in the third line of (109) are controlled by the corresponding coefficients of the Hessian of in (104). In either or cases, it follows from (104), (106), and (109) that

(110)
for .

Note that parameters, c2, C2, γ, σ, and λ, are fixed in Remark 22, independent of δ > 0. Therefore the upper bound of follows from (84)–(88), (96), (99), (102), and (103). Note that , if r(z)>−δ/4λs = −δσ2s/4λ, and this property holds on if we take b > 0 sufficiently small; say, 0 < 2b < σ2m/λ2. Also note that Ψ = 1 on . This fact together with (96) and (110) proves properties (i) and (ii). Property (iii) follows from (22), (30), (32), and (96).

For each zδ = (dδ1/η, 0, eδbδ) ∈ Cb(z0, δ0), set .

Proposition 24. There is a small constant a > 0 such that R2aδ(ζδ)⊂⊂Ω for all sufficiently small δ > 0.

Proof. From (22)–(29), we obtain that

(111)
for all sufficiently small δ > 0. Assume ζR2aδ(ζδ) and write
(112)
From (61), and by using Taylor series method, one obtains that
(113)
for a uniform constant C2 > 0. Similarly, we obtain |E2| ≤ 4aC2δ. Combining these estimates and (111) and if we set a = b/24C2, then we obtain that
(114)

Remark 25. (1) Set . Then, by functoriality, Proposition 23 holds, where is replaced by , and is replaced by .

For each fixed δ > 0, and for each fixed , set . Note that on V. Thus it follows, from transformation formula, that
(115)
In view of Propositions 23 and 24, there is a smooth plurisubharmonic weight function which has maximal Hessian on Qaδ(zδ)⊂⊂Ω. We also note that by (56). If we use these properties and (115), we get the following estimates for the Bergman kernel function KΩ(zδ, zδ) at zδCb(z0, δ0) as in Theorem 6.1 in [2]:
(116)
This proves Theorem 2.
Now we want to get derivative estimates of K(z, zδ) for zΩ and zδCb(z0, δ0). In view of (115), we will estimate where and . We will follow the methods in [3, 9] which use dilated coordinates. For each fixed δ > 0, we recall that τ1 = δ1/η, τ2 = τ(zδ, δ) and τ3 = δ. Define a dilation map Dδ given by
(117)
set
(118)
and set
(119)
where and where is defined in Proposition 23.
Set
(120)
and write . The properties of λδ(w), which follow from Propositions 23 and 24 and Remark 25, are summarized in the following proposition.

Proposition 26. For each δ > 0 there is λδ(w), defined on Ωδ, such that

(1) λδ(w) is smooth plurisubharmonic in Ωδ, and |λδ| ≤ 1;

(2) , for some ;

(3) if wP(0,1);

(4) .

The weight function with the properties in Proposition 26 is the key ingredient for the derivative estimates of the Bergman kernel function off the diagonal. Set and let Nδ be the Neumann operator on Ωδ. Then we have the following L2 estimates of Nδ (Proposition 3.14 in [3]).

Proposition 27. Let hL2 be a (0,1) form and supp⁡hP. Then there is C > 0, independent of δ > 0, so that

(121)

Note that Dδ(ζδ) = 0. Set
(122)
From (117) and Proposition 24, we note that
(123)
independent of δ > 0. Let with ξ1 = 1 in a neighborhood of 0 and ξ2 = 1 on supp⁡ξ1. From (123), we see that supp⁡ξ2P(0,1)⊂⊂P(0,2)⊂⊂Ωδ, independent of δ > 0. Therefore we have the following elliptic estimates:
(124)
where □δ is the complex Laplacian on Ωδ.

Remark 28. The estimates in (124) are on the polydisc P(0,1)⊂⊂P(0,2)⊂⊂Ωδ, strictly inside of Ωδ, independent of δ > 0. Therefore we gain two derivatives in (124) and it is stable; that is, Cs is independent of δ > 0. Also we note that we do not require that Δ1(z0) < . Since where , we can also apply the estimate (121) on P(0,2).

Let , ∫ϕ = 1, and ϕ be polyradial. In terms of w-coordinates in (117), we have the following well known representation of Bergman kernel function on Ωδ.
(125)
Let χC(Ωδ) with χ = 1 outside P(0,1) and χ = 0 on supp⁡ϕ. Combining (121)–(125), we can prove the following lemma as in the proof of Theorem 4.2 in [3].

Lemma 29. For each s ≥ 0 there is Cs > 0 such that

(126)

Now, if we use the estimate (126) with s = |α| + 3, we can prove Theorem 3 as in the proof of Theorem 4.2 in [3].

Conflicts of Interest

The author declares that there are no conflicts of interest regarding the publication of this paper.

Acknowledgments

The author was partially supported by the Sogang University Research Fund.

    Appendix

    We recall Herbort’s example ΩH in (6). Therefore η = 6 = Δ1(0) and hence τ1 = δ1/6, τ2 = δ1/3, and τ3 = δ in our notations. For each fixed δ > 0, set zδ = (δ1/6/2, 0, −δ). Then zδΩH and approaches to 0 ∈ bΩH in “almost tangential direction” as the points do along Cb(z0, δ0). In this case, we will show that
    (A.1)
    which is exactly same result as Theorem 2.

    Proof of (A.1). Set

    (A.2)
    Then the polydisc Pδ(zδ) about zδ is contained in ΩH. Therefore the upper bound follows. Let us show lower bounds.

    Let Δ3 be the unit polydisc in . Since the localization lemma is valid for ΩH, we will estimate . Set

    (A.3)
    and set
    (A.4)
    Then ΩH = G1G2 and zδG1G2. Set fδ = 8δ11/6z1/(z3δ) 2. Then fδ(zδ) = 1. Note that
    (A.5)
    where we have used . Set and . Then
    (A.6)
    where we have used the polar coordinates: , k = 1,2 in the second line.

    Set and . Then

    (A.7)
    Write . Set δ−2/3x1/2 = x. Then
    (A.8)
    Also,
    (A.9)
    Combining (A.5)–(A.9), we obtain that . Therefore .

    Remark 30. Set f(z) = exp⁡(z3/(1 − z3)). Then f is a peak function that peaks at 0 ∈ bΩH for the domain ΩH.

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