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arXiv:1702.06908v2 [math.CV] 15 Sep 2018 JET VANISHING ORDERS AND EFFECTIVITY OF KOHN’S ALGORITHM IN DIMENSION 3 Dedicated to Professor Ngaiming Mok on the occasion of his 60th birthday SUNG-YEON KIM* AND DMITRI ZAITSEV** Abstract. We propose a new class of geometric invariants called jet vanishing orders, and use them to establish a new selection algorithm in the Kohn’s construction of subelliptic multipliers for special domains in dimension 3, inspired by the work of Y.-T. Siu [S10]. In particular, we obtain effective termination of our selection algorithm with explicit bounds both for the steps of the algorithm and the order of subellipticity in the corresponding subelliptic estimates. Our procedure possesses additional features of certain stability under high order perturbations, due to deferring the step of taking radicals to the very end, see Remark 1.2 for more details. We further illustrate by examples the sharpness in our technical results (in Section 3) and demonstrate the complete procedure for arbitrary high order perturbations of the Catlin-D’Angelo example [CD10] in Section 5. Our techniques here may be of broader interest for more general PDE systems, in the light of the recent program initiated by the breakthrough paper of Y.-T. Siu [S17]. Contents 1. Introduction 2 1.1. Kohn’s algorithm for special domains and subelliptic estimates 3 1.2. Multipliers and effectivity 5 1.3. Applications and further directions 5 1.4. Main results 6 1.5. Overview of our procedure 7 2. Vanishing orders, contact orders and jets 8 2.1. Normalised vanishing order 8 2.2. Contact order and finite type 10 2.3. Contact order along subvarieties. 10 2.4. Jet vanishing orders 10 3. Control of jet vanishing orders for Jacobian determinants 11 1991 Mathematics Subject Classification. 32T25, 32T27, 32W05, 32S05, 32B10, 32V15, 32V35, 32V40. Key words and phrases. Finite type, Multiplier ideals, Jacobian, subelliptic estimates, jets, germs of holomorphic functions, order of contact, ¯ -Neumann problem. *This research was supported by Basic Science Research Program through the National Research Foun- dation of Korea (NRF) funded by the Ministry of Science, ICT and Future Planning (grant number NRF- 2015R1A2A2A11001367). 1

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JET VANISHING ORDERS AND EFFECTIVITY OF KOHN’S ALGORITHM

IN DIMENSION 3

Dedicated to Professor Ngaiming Mok on the occasion of his 60th birthday

SUNG-YEON KIM* AND DMITRI ZAITSEV**

Abstract. We propose a new class of geometric invariants called jet vanishing orders, and usethem to establish a new selection algorithm in the Kohn’s construction of subelliptic multipliers forspecial domains in dimension 3, inspired by the work of Y.-T. Siu [S10]. In particular, we obtaineffective termination of our selection algorithm with explicit bounds both for the steps of thealgorithm and the order of subellipticity in the corresponding subelliptic estimates. Our procedurepossesses additional features of certain stability under high order perturbations, due to deferringthe step of taking radicals to the very end, see Remark 1.2 for more details.

We further illustrate by examples the sharpness in our technical results (in Section 3) anddemonstrate the complete procedure for arbitrary high order perturbations of the Catlin-D’Angeloexample [CD10] in Section 5.

Our techniques here may be of broader interest for more general PDE systems, in the light ofthe recent program initiated by the breakthrough paper of Y.-T. Siu [S17].

Contents

1. Introduction 21.1. Kohn’s algorithm for special domains and subelliptic estimates 31.2. Multipliers and effectivity 51.3. Applications and further directions 51.4. Main results 61.5. Overview of our procedure 72. Vanishing orders, contact orders and jets 82.1. Normalised vanishing order 82.2. Contact order and finite type 102.3. Contact order along subvarieties. 102.4. Jet vanishing orders 103. Control of jet vanishing orders for Jacobian determinants 11

1991 Mathematics Subject Classification. 32T25, 32T27, 32W05, 32S05, 32B10, 32V15, 32V35, 32V40.Key words and phrases. Finite type, Multiplier ideals, Jacobian, subelliptic estimates, jets, germs of holomorphic

functions, order of contact, ∂-Neumann problem.*This research was supported by Basic Science Research Program through the National Research Foun-

dation of Korea (NRF) funded by the Ministry of Science, ICT and Future Planning (grant number NRF-2015R1A2A2A11001367).

1

2 S.-Y. KIM & D. ZAITSEV

4. Selection algorithm and Proof of Theorem 1.1 164.1. Step 1; selecting a multiplier with minimal vanishing order 164.2. Step 2; selecting a multiplier with effectively bounded order along a zero curve of

another multiplier 174.3. Step 3; selecting a pair of multpliers with effectively bounded multiplicity and taking

the radical 185. Perturbations of Heier’s and Catlin-D’Angelo’s examples 19References 21

1. Introduction

In his seminal paper [K79], J.J. Kohn invented a purely algebraic construction of ideals ofsubelliptic multipliers for the ∂-Neumann problem. The goal of this note is to propose a new classof geometric invariants, called jet vanishing orders, that permits us to obtain a fine-grained controlof the effectiveness in the Kohn’s construction procedure of subelliptic multipliers for the so-calledspecial domains of finite D’Angelo type [D79, D82] in C3.Since this paper is dedicated to Professor Ngaiming Mok, we would like to mention a striking

parallel between the Kohn’s subelliptic multipliers ideals and the varieties of minimal rational tan-gents (VMRT) pioneered by N. Mok and J.-M. Hwang [HM98]. Both theories connect global PDEor algebraic-geometric structures with local differential-geometric objects that can be treated bylocal geometric and analytic methods, subsequently leading to important consequences of globalnature. For more details on the VMRT, see the articles and lecture notes by Hwang and Mok[Mo08, H14]. Another important parallel is historical. The VMRT theory was developed to studydeformation rigidity problems originated from the celebrated Kodaira-Spencer’s work on deforma-tion of complex structures, with an important ingredient coming from D. Spencer’s program togeneralize the Hodge theory of harmonic integrals. And it was the same program that led Spencerto formulate the ∂-Neumann problem, for which Kohn invented his multiplier ideals approach totackle the problem of local regularity (see [K-etal04] for a more detailed account).Note that Kohn’s original procedure in [K79] gives no effective bound on the order of subellip-

ticity ε in subelliptic estimates, as illustrated by examples of G. Heier [He08] and D.W. Catlin andJ.P. D’Angelo [CD10], see §1.2 and §5 below. On the other hand, Y.-T. Siu [S10, S17] obtaineda new effective procedure for special domains and outlined an extension of the special domainapproach to general real-analytic and smooth cases. Also note that for the special domains of theso-called triangular form in Cn, a different effective procedure in Kohn’s algorithm was given byCatlin-D’Angelo [CD10, Section 5]. Triangular systems were first introduced by D’Angelo [D95]under the term regular coordinate domains, where also an effective procedure for obtaining subel-liptic estimates was provided. See also D.W. Catlin and J.-S. Cho [CC08] and T.V. Khanh andG. Zampieri [KhZa14] for subelliptic estimates for triangular systems by a different method, andA. Basyrov, A.C. Nicoara and the second author [BNZ17] for an approximation of general smoothpseudoconvex boundaries by triangular systems of sums of squares matching the Catlin multitype.We next mention that A.C. Nicoara [N14] proposed a construction for the termination of the Kohn

JET VANISHING ORDERS 3

algorithm in the real-analytic case with an indication of the ingredients needed for the effectivity.We further refer to [K79, K84, D95, DK99, S01, S02, K04, S05, S09, CD10, S10, S17] for moreprofound and extensive discussion of subelliptic multipliers (see also [Ch06] for an algebraic ap-proach), as well as surveys [Si91, BSt99, FS01, M03, St06, MV15] and books [Mr66, FK72, Tr80,Ho90, D93, CS01, O02, Za08, St10, Ta11, Ha14, O15] for the ∂-Neumann problem in broadercontext.In relation to Kohn’s foundational work on the subelliptic multipliers, we would like to mention

a remarkable new development in the field due to Siu [S17] providing new techniques of generatingmultipliers for general systems of partial differential equations, including, as a special case, a newprocedure even for the case of the ∂-Neumann problem.Finally we mention the related important Nadel’s multiplier ideal sheaves [Na90] that were

originally motivated by the ones defined by Kohn [K79] and are in some sense dual to them. See[S01, §4], [S09, 1.4.6] for more detailed discussions of the relation between both types of multipliers,and the expository articles and books [S01, S02, De01, L04, S05, S09] for further information.

1.1. Kohn’s algorithm for special domains and subelliptic estimates. We shall considerso-called special domains as introduced by Kohn in [K79], defined locally near the origin byholomorphic functions in the first n variables:

(1.1) Ω := Re (zn+1) +

m∑

j=1

|Fj(z1, . . . , zn)|2 < 0 ⊂ Cn+1,

where F1, . . . , Fm is any collection of holomorphic functions vanishing at the origin in Cn (anddefined in its neighborhood).Understanding Kohn’s multipliers for the special domains is important, on the one hand, due

to their link with local analytic and algebraic geometry, and on the other hand, through theirconnection with more general cases via D’Angelo’s construction of associated families of holomor-phic ideals [D93, Chapter 3] and Siu’s program relating special domains approach with generalreal-analytic and smooth cases [S10, II.3, II. 4].Next recall the Kohn’s algorithm or, more precisely, its holomorphic variant for special domains

(1.1) (corresponding to q = 1 in the notation of [K79] and to algebraic geometric formulation in[S17, 2.9.4]). For any set S of germs of holomorphic functions at 0 in Cn, consider the ideal J(S)generated by all function germs g satisfying

df1 ∧ . . . ∧ dfn = g dz1 ∧ . . . ∧ dzn, f1, . . . , fn ∈ S,

i.e. by all Jacobian determinants

(1.2) g =∂(f1, . . . , fn)

∂(z1, . . . , zn)= det

(∂fi∂zj

).

Then the Kohn’s 0th multiplier ideal for (1.1) is defined as the radical

(1.3) I0 :=√J(S), S := F1, . . . , Fm,

4 S.-Y. KIM & D. ZAITSEV

and for any k > 0, the Kohn’s kth multiplier ideal is defined inductively by

(1.4) Ik :=√J(S ∪ Ik−1).

The obtained increasing sequence of ideals I0 ⊂ I1 ⊂ ... is said to terminate at k if Ik contains theunit 1.Kohn proved in [K79] that the necessary and sufficient condition for the ideal termination for

special domains (in fact, for his more general algorithm applied to domains with real-analyticboundaries) is the finiteness of the D’Angelo type of ∂Ω at 0. Note that Kohn’s algorithm isactually defined for domains with arbitrary smooth boundaries, in which generality, however, thecorresponding termination remains a major open problem. For a special domain (1.1), the typeequals 2τ(S), where S is given by (1.3) and

(1.5) τ(S) := supγ

inff∈S

ν(f γ)ν(γ)

is the type of the set S of holomorphic function germs, where the supremum is taken over allnonconstant germs of holomorphic curves γ : (C, 0) → (Cn, 0), and ν(g) denotes the vanishingorder of a smooth vector function g at 0, given by the lowest order of its nonvanishing partialderivative at 0. We refer to [D82, D93] for more detailed discussions of finite type and [M92b,BSt92, FIK96, D17, MM17, Z17] for equivalent characterizations in various particular cases, seealso [FLZ14].It follows from Kohn’s work [K79] that ideal termination at a boundary point p ∈ ∂Ω leads to

a subelliptic estimate of some order of subellipticity ε > 0 at that point, namely

(1.6) ‖u‖2ε ≤ C(‖∂u‖2 + ‖∂∗u‖2 + ‖u‖2),where ‖ · ‖ε and ‖ · ‖ are respectively the tangential Sobolev norm of the (fractional) order ε andthe standard L2 norm on Ω, u is any (0, 1) form in the domain of the adjoint operator ∂∗ (withrespect to the standard L2 product on Ω), smooth up to the boundary and with compact supportin a fixed neighborhood U of p in the closure Ω, such that both U and the real constant C > 0 areindependent of u, see [K79, Definition 1.11] for more details. (Note that Kohn obtained his resultsfor (p, q) forms with arbitrary p, q.) We mention that, even though the estimate (1.6) depends onthe choice of local coordinates (or the metric used in the L2 product), the subellipticity property(i.e. the existence of an estimate (1.6) for given ε) is invariant [Sw72, Ce08, CeSt09].In the same paper, Kohn further proved that his algorithm does terminate for pseudoconvex do-

mains with real-analytic boundaries of finite type, leading to subelliptic estimates, based on a resultof K. Diederich and J.E. Fornæss [DiF78] (see also E. Bedford and J.E. Fornæss [BF81], Siu [S10,Part IV] and Kohn [K10]). For pseudoconvex domains with smooth boundaries of D’Angelo finitetype, subelliptic estimates are due to D.W. Catlin [C87] by a different method, whereas the ter-mination of Kohn’s algorithm in that generality remains a major open problem (see e.g. the firstproblem in [DK99, Section 14]). Note that the finite type condition is also necessary for subellipticestimates due to the work of P. Greiner [Gr74] in C2 and D.W. Catlin [C83] in Cn.It is crucial to point out the particularly remarkable feature of Kohn’s procedure that allows

us to study functional-analytic estimates such as (1.6) with purely geometric methods applied to

JET VANISHING ORDERS 5

ideals of holomorphic functions. Consequently, our approach here is accessible to any geometerwithout familiarity with the functional-analytic aspect of the problem.

1.2. Multipliers and effectivity. Recall [K79] that a germ at p ∈ ∂Ω of a smooth function onthe closure Ω is a subelliptic multiplier with order of subellipticity ε if, for some representativef of the germ, the estimate similar to (1.6) with ‖u‖2ε replaced by ‖fu‖2ε holds under the sameassumptions, namely

(1.7) ‖fu‖2ε ≤ C(‖∂u‖2 + ‖∂∗u‖2 + ‖u‖2),where both U and C may depend on f . It follows from Kohn’s work [K79, Section 4 and 7] thatthe ideals Ik as defined in (1.4) consist of subelliptic multipliers, i.e. satisfy (1.7) with some orderof subellipticity ε that may depend on the actual multipliers. More precisely, Kohn showed thattaking a Jacobian determinant in (1.2) reduces the order of subellipticity by 1/2, whereas takinga root of order s in the radical reduces it by 1/s. It is the last step where an effective control ofε may get lost, as it is a priori not clear what root order is required in order to obtain the fullradical. In fact, examples of Heier [He08, Section 1.1] and Catlin-D’Angelo [CD10, Proposition 4.4]illustrate precisely that, i.e. the lack of control of ε as the parameter K in the example goes toinfinity, whereas the type remains bounded (see Section 5 below). See also Siu [S17, 4.1] fora more elaborate and detailed explanation of this important phenomenon. A perturbation ofCatlin-D’Angelo’s example is treated in Section 5 below.In order to regain the effectiveness, one needs to restrict the the number of steps and the root

orders allowed in the radicals in terms of only the type and dimension, leading to an effectiveKohn algorithm in the terminology of Siu [S17, 2.6]). In addition, it is desired to have algorithmicselection rules for constructing sequences of the actual multipliers ending with 1. Our goal hereis to obtain a fine effectiveness control in terms of our new invariants (that are in turn controlledby the type) and a new selection procedure for the multipliers leading to an effective termination.In particular, we are going to the extreme to avoid taking radicals until the very last step, seeRemark 1.2 below for details.

1.3. Applications and further directions. Among notable applications of subelliptic estimates(1.6), J.J. Kohn and L. Nirenberg [KN65] proved that the latter imply local boundary regularityof the Kohn’s solution of the ∂-Neumann problem ∂u = f , i.e. the solution u is smooth atthose boundary points where f is. See [K72, DK99] and the references therein for more detaileddiscussions of this and many other applications.Another important application of subelliptic estimates, specifically demonstrating the impor-

tance of the effectivity, is a lower bound on the Bergman metric directly related to the order ofsubellipticity, due to J.D. McNeal [M92a]. The effective control in subelliptic estimates also playsimportant role in the construction of peak functions by J.E. Fornæss and J.D. McNeal [FM94]and in other results.It should be noted that applications of Kohn’s algorithm and its effectiveness are not limited to

subelliptic estimates. In their remarkable paper [DiF79], K. Diederich and J.E. Fornæss discovereda direct way of using Kohn’s multipliers to construct so-called plurisubharmonic “bumping” func-tions for arbitrary domains with real-analytic boundaries of finite type. The bumping functions are

6 S.-Y. KIM & D. ZAITSEV

subsequently applied in the same paper for Kobayashi metric estimates and Holder regularity ofproper holomorphic maps. However, the exponents in the crucial estimates could not be effectivelycontroled (in terms of the type and dimension) due to some steps involving Lojasiewicz inequal-ity. Here effective procedures for generating multipliers would allow for more explicit quantitativeconclusions.In a more recent work, Kohn [K00, K02, K04] has demonstrated some new use of subelliptic

multipliers by relating them to certain new microlocal subelliptic multipliers on real hypersurfaces,and establishing hypoellipticity of the b and the ∂-Neumann operator. In [K05] Kohn introducedan analogue of his theory of subelliptic multipliers for new classes of differential operators. Seealso L. Baracco [Ba15] and L. Baracco, S. Pinton and G. Zampieri [BaPZa15] for recent relatedresults.Inspired by Kohn’s original subelliptic multipliers, analogous notion of multiplier ideals for

the compactness estimate were studied by M. Celik [Ce08], E.J. Straube [St08], in their jointwork [CeSt09] and by M. Celik and Y.E. Zeytuncu [CeZ17]. Finally, we mention results byD. Chakrabarti and M.-C. Shaw [ChS11] connecting properties of the Kohn’s solution for in-dividual domains with corresponding properties for to their products, with some of their resultsrecently used by X.-X. Chen and S.K. Donaldson [ChD13] to study rigidity properties of complexstructures.

1.4. Main results. Our main new tool is the following invariant number associated to a set Sof germs of holomorphic functions at 0 in Cn, a germ of analytic subvariety (V, 0) in Cn and aninteger k:

(1.8) τkV (S) := supγ

inff∈S

ν(jkf γ)ν(γ)

, k ≥ 0,

where jkf = (∂αf)|α|≤k is the vector of all partial derivatives up to order k, and the supremumis taken over the set of all nonconstant germs of holomorphic maps γ : (C, 0) → (V, 0), and thevanishing order ν is as above. We call τkV the k-jet type of S along V . In particular, for k = 0, weobtain the D’Angelo type (1.5). It is easy to see that the k-jet types form a non-increasing sequencefor k = 0, 1, . . ., and become equal to 0 whenever k is greater or equal the minimum vanishingorder of a germ in S. Note that, even though the space of curves in (1.8) is infinite-dimensional,the computation of the k-jet type in C2 can be reduced to certain finite number of curves by aresult of J.D. McNeal and A. Nemethi [MN05] (see also [He08, LT08] for further results in thisdirection).Since the effective termination is well-known if at least one function Fj has order 1 (see e.g.

[CD10]), we shall assume that all functions Fj vanish of order ≥ 2 at 0. The following is a simplifiedversion (with rougher bounds) of the main result of the paper:

Theorem 1.1. In the context of Kohn’s algorithm for special domains (1.1) in C3 of D’Angelo

finite type ≤ 2T at 0, there is an effective algorithmic construction of a sequence of multipliers

(1.9) f1, . . . , fl, l ≤ T (T − 1) + 4,

JET VANISHING ORDERS 7

with fl = 1, based on the invariants (1.8). Every fj is obtained by taking a Jacobian determinantof a linear combination of elements in the set

(1.10) F1, . . . , Fm, f1, . . . , fj−1,except the two multipliers fl−2 = z1, fl−1 = z2 that are in the radical of the ideal I := (f1, . . . , fl−3)with a root order s ≤ T 2(T − 1)3, i.e. zs1, z

s2 ∈ I.

Remark 1.2. We would like to point out the following particular features in our multiplier con-struction in comparison to other known procedures. From the three different procedures in Kohn’sconstruction, namely (1) taking Jacobian determinants, (2) forming ideals and (3) taking the rad-icals, only the first one is used in our process to obtain a pair of multipliers generating an ideal offinite (effectively controlled) multiplicity. Only then the ideal is formed and the radical is takento obtain the linear multipliers, leading to the termination.In particular, our procedure possesses certain stability under high order perturbations, as illus-

trated in §5. Such stability is generally not available in procedures based on taking radicals. Forinstance, in the ring of germs of holomorphic functions at 0 in C2

z,w, f = w is in the radical of the

ideal generated by f 2 = w2, but any perturbation g = f 2 + zm = w2 + zm with m odd generatesan ideal Im having no other germs in its radical, i.e.

√Im = Im (since the zero variety of Im is

locally irreducible at 0). This problem does not occur in our construction because we only takeradicals from ideals of finite codimension, where any germ vanishing at 0 is in the radical.

Corollary 1.3. For special domains (1.1) of finite type ≤ 2T at 0 in C3, a subelliptic estimate(1.6) at 0 holds with the order of subellipticity

ε ≥ 1

2l−1s≥ 1

2T (T−1)+3 T 2(T − 1)3,

where l is the number of multipliers in (1.9) and s is the radical root order in Theorem 1.1.

Proof. It follows from Kohn’s work [K79, Sections 4 and 7], that in the context of Theorem 1.1,a Jacobian determinant of the Fj has the order of subellipticity ≥ 1/4 (see [K79, (4.29, 4.64)]and [S17, 2.9.2]), and taking any further Jacobian determinant reduces the order of subellipticityby 1/2 (see [K79, (4.42, 4.64)]), whereas taking a root of order s reduces it by 1/s (see [K79,4.36]). Applying these calculations to the construction in Theorem 1.1, we obtain the desiredconclusion.

Note that we obtained more refined bounds than those given in Theorem 1.1 and Corollary 1.3in terms of our new invariants (1.8). Also we illustrate in Section 5 how our procedure can beapplied to the Catlin-D’Angelo’s example as well as its higher order perturbations.

1.5. Overview of our procedure. Following [S10, S17], we call the functions Fj in (1.1) pre-multipliers, to distinguish them from the multipliers obtained via the algorithm. It is importantto emphasize that the pre-multipliers are only used inside the Jacobian determinants (1.2) but arenever added to the ideals directly.On a large scale, there are 3 major steps, each reducing the dimension of the variety defined by

the multipliers (resembling Kohn’s original algorithm for real-analytic hypersurfaces [K79]).

8 S.-Y. KIM & D. ZAITSEV

The first step consists of constructing the first multiplier f1 as Jacobian determinant from thepre-multipliers with effectively bounded vanishing order at 0. Our method gives a bound of atmost ≤ T (T − 1). In fact, a finer bound is given in terms of the k-jet types (as defined by (1.8))of the pre-multipliers along their zero curves, see (4.1). Note that other bounds are known fromthe work of D’Angelo [D82, D93], Siu [S10, S17] and Nicoara [N12]. Any known effective bound dcan be used at this step to proceed with our construction.The second major step aims to reduce the dimension of the variety

V := f1 = 0from 1 to 0. Our method here is based on a sequence of minor steps constructing new multipliersthat gradually reduce the jet order k ≥ 0 for which the k-jet type along V can be effectivelybounded. The construction starts with k = d ≤ T (T −1) (the vanishing order of f1), and at everyminor step, the order k is reduced from kj to kj+1 < kj , where the new kj+1-jet type along V getsan effective bound equal to the previous bound for the kj-jet type plus at most (kj −kj+1)(T −1).In other words, lowering the jet order by a number N increases the type bound by N(T − 1). Infact, the method gives a finer bound with T replaced by the vanishing order of pre-multipliersonly along curves in V . Based on the configuration of the k-jet types, multiple possible choicesfor kj are available (see Section 3 for details), where fewer Jacobian determinant iterations can betraded for possibly higher vanishing order bound and vice versa. At the end of this major step, weobtain a multiplier fl−3 whose type (i.e. the (0-jet) type as defined for k = 0 in (1.8)) along V iseffectively bounded by an estimate no worse than d(T − 1) (where d ≤ T (T − 1) is the vanishingorder of f1). The proof is based on the core technical results in Section 3 with examples givenillustrating the sharpness of the assumptions.Finally, the third major step consists of taking the coordinate functions fl−2 := z1 and fl−1 := z2

in the radical of the finite type ideal I(f1, fl−3), and subsequently their Jacobian determinantfl = 1. The corresponding radical root order can be effectively bounded by

td ≤ d2(T − 1) ≤ T 2(T − 1)3

in terms of the vanishing order d of f1 and the type t ≤ d(T − 1) of fl−3 along V . See Lemma 4.3for the bound td.

2. Vanishing orders, contact orders and jets

2.1. Normalised vanishing order. We write f : (Cn, 0) → C for a germ at 0 of a holomorphicfunction in Cn (without specifying the value f(0)), and

ν(f) := min|α| : ∂αz f(0) 6= 0 ∈ N ∪ ∞, N = 0, 1, . . .for the vanishing order of f , also called multiplicity in the literature, (the minimum is ∞ if theset is empty), where

α = (α1, . . . , αn) ∈ Nn, |α| := α1 + . . .+ αn,

is a multiindex and

∂αz = ∂α1

z1. . . ∂αn

zn

JET VANISHING ORDERS 9

is the corresponding partial derivative with respect to chosen coordinates (z1, . . . , zn) ∈ Cn. Clearlyν(f) does not depend on the choice of local holomorphic coordinates.More generally, for any set S of germs of holomorphic maps (on the same Cn), define its vanishing

order to be the minimum vanishing order for its elements:

ν(S) := minν(f) : f ∈ S.It is clear that ν(S) = ν(I(S)), where I is the ideal generated by S. In particular, for anyholomorphic map germ

f = (f1, . . . , fm) : (Cn, 0) → C

m,

define its vanishing order to be the vanishing order of the set of its components, i.e.

ν(f) := minj=1,...,m

ν(fj).

It is again easy to see that ν(f) also does not depend on the choice of local holomorphic coordinatesin C

m in a neighborhood of f(0).Now following D’Angelo [D82, D93], for every germ of a holomorphic map

γ 6≡ 0: (Cm, 0) → (Cn, 0), f : (Cn, 0) → Cℓ,

define its normalized vanishing order of f along γ by

(2.1) νγ(f) :=ν(f γ)ν(γ)

.

In case m = 1 (considered here), the normalized vanishing order is invariant under singularparameter changes γ 7→ γ ϕ, where ϕ : (C, 0) → (C, 0) is any nonconstant germ of a holomorphicmap. Similarly, for a set S of holomorphic map germs, define its normalized vanishing order alongγ by

νγ(S) := minνγ(f) : f ∈ S,and again νγ(S) = νγ(I(S)) for the ideal I(S) generated by S.Note that in general, the normalized vanishing order may not be an integer, and, in fact, can

be any rational number p/q > 1 as the example

γ(t) := (tp, tq), f(z, w) := z, νγ(f) = p/q,

shows.It is easy to see that given f , one has νγ(f) = ν(f) for a generic linear map γ. In general, νγ(f)

can only become larger:

Lemma 2.1. The normalized vanishing order of f along any map γ is always greater or equalthan the vanishing order:

(2.2) νγ(f) ≥ ν(f).

Proof. Expanding into a power series f =∑fαz

α with |α| ≥ ν(f), and substituting γ, we concludeν(f γ) ≥ ν(f) ν(γ) as desired.

10 S.-Y. KIM & D. ZAITSEV

2.2. Contact order and finite type. Let S be a set of germs of holomorphic functionsf : (Cn, 0) → C. Then in view of Lemma 2.1 (and the remark before it), the vanishing ordersatisfies

ν(S) = minγνγ(S).

At the opposite end, define (as in [D82] and [D93, 2.3.2, Definition 9]) the contact order or thetype of S by

τ(S) := supγ

νγ(S) = supγ

minf∈S

νγ(f).

(Note that the minimum in the right-hand side is always achieved, since the denominator in (2.1)is fixed.) We say that the set S is of finite type T = τ(S) if the latter number is finite. Sinceνγ(S) = νγ(I(S)) for the ideal I(S) generated by S, we also have

ν(S) = ν(I(S)), τ(S) = τ(I(S)).

2.3. Contact order along subvarieties. Let f : (Cn, 0) → Cm be a germ of a holomorphic map

as before and V ⊂ Cn any complex-analytic subvariety passing through 0. Then the contact orderof f along V is defined by

(2.3) τV (f) := supγ

νγ(f)

where the supremum is taken over all non-constant germs of holomorphic maps γ : (C, 0) → (V, 0).In particular, if V is (a germ of) an irreducible curve at 0, the right-hand side in (2.3) is

independent of γ, since in this case, any two nonzero germs γ : (C, 0) → (V, 0) are related by asequence of singular reparametrizations. In general, the contact order along V is the maximumcontact order along the irreducible components of V at 0.

2.4. Jet vanishing orders. The main new tool in this paper is the following notion of jet van-ishing order.For every integer k ≥ 0, and a germ of a holomorphic map f : (Cn, 0) → Cm, consider its k-jet

jkf , which in local coordinates can be regarded as a germ of a holomorphic map

F = jkf = (∂αz f)|α|≤k : (Cn, 0) → C

N ,

(for suitable integer N dependent on n, m and k) given by all partial derivatives of the componentsof f up to order k. Then define the k-jet vanishing order of f by

(2.4) νk(f) := ν(jkf) = min|α|≤k

ν(∂αz f),

which is also equal to max(ν(f)− k, 0).Further, define the k-jet normalized vanishing order of f along a nonzero germ γ : (Cm, 0) →

(Cn, 0) by

νkγ (f) := νγ(jkf) = min

|α|≤kνγ(∂

αz f),

JET VANISHING ORDERS 11

(which are the minimum vanishing orders of the partial derivatives up to order k along γ), andthe k-jet contact order of f along a subvariety V by

(2.5) τkV (f) := τV (jkf) = sup

γ

νkγ (f),

where as in (2.3), the supremum is taken over all non-constant germs of holomorphic mapsγ : (C, 0) → (V, 0). Note that again, this definition is independent of holomorphic local coor-dinates, and we have the monotonicity:

(2.6) νk1(f) ≥ νk2(f), νk1γ (f) ≥ νk2γ (f), τk1V (f) ≥ τk2V (f), k1 ≤ k2.

As consequence of (2.4) and the definitions, we have the stabilisation property

(2.7) νk(f) = νkγ (f) = τkV (f) = 0, k ≥ ν(f),

for any γ and any V .Similarly, for any set S of germs of holomorphic maps f : (Cn, 0) → Cm, define the numbers

νk(S) := ν(jkS), νkγ (S) := νγ(jkS), τk(S) := τ(jkS), τkV (S) := τV (j

kS),

that, in fact, depend only on the ideal generated by S, where jkS denotes the set of all k-jets ofelements in S.

3. Control of jet vanishing orders for Jacobian determinants

This section is the technical core of the paper. Our goal is to obtain fine control of how the jetvanishing orders along curves change under taking Jacobian determinants. The main idea is to havea control of certain “good” terms in the multiplier expansion and to avoid possible cancellationswith other terms. This is achieved via certain technical conditions comparing jet vanishing ordersfor different jet orders. We also illustrate by examples that our technical conditions are sharp.For a holomorphic curve germ γ 6≡ 0: (C, 0) → (C2, 0), we can always change coordinates

(z, w) ∈ C2 to achieve

(3.1) γ = (α, β), ν(α) > ν(β) ≥ 1.

We first give a comparison condition between jet vanishing orders νk−1γ (F ) and νkγ (F ) of a

function germ F along γ to guarantee that the minimum vanishing order along γ among partialderivatives of F is achieved for its transversal derivatives.

Lemma 3.1. Given γ satisfying (3.1) and a germ of a holomorphic map

F : (C2, 0) → C,

assume that the jet vanishing orders of F along γ satisfy

(3.2) νk−1γ (F ) > νkγ (F ) + 1

for some k ≥ 1.Then

(3.3) νkγ (F ) = νγ(∂kzF ),

12 S.-Y. KIM & D. ZAITSEV

i.e. the minimum vanishing order among all partial derivatives of order k is achieved for the kthderivative transversal to (the image of) γ:

νγ(∂kzF ) = min

a+b≤kνγ(∂

az∂

bwF ).

Proof. Assume on the contrary that

νγ(∂az∂

bwF ) < νγ(∂

kzF )

for some a < k and b ≤ k − a. We can choose a and b such that the minimum vanishing order isachieved, i.e.

(3.4) νkγ (F ) = νγ(∂az∂

bwF ) < νγ(∂

kzF ).

In view of (3.2), we must have the top order a+ b = k here, in particular, b = k − a ≥ 1. Then

(3.5) ν(∂az∂bwF (γ)) ≤ ν(∂a+1

z ∂b−1w F (γ)) < ν

(∂a+1z ∂b−1

w F (γ)α′

β ′

),

as we have assumed ν(α) > ν(β). Differentiating in the parameter of γ, we obtain

(∂az∂

b−1w F (γ)

)′= β ′

(∂a+1z ∂b−1

w F (γ)α′

β ′+ ∂az∂

bwF (γ)

),

from which, using (3.5), we conclude

(3.6) ν((∂az∂

b−1w F (γ))′

)= ν(∂az∂

bwF (γ)) + ν(β)− 1.

Since our definition of the k-jet vanishing order implies

ν((∂az∂

b−1w F (γ))′

)≥ ν(β) νk−1

γ (F )− 1,

we have in view of (3.4) and (3.6),

(3.7) ν(β) νkγ (F ) = ν(∂az∂bwF (γ)) = ν

((∂az∂

b−1w F (γ))′

)− ν(β) + 1 ≥ ν(β) νk−1

γ (F )− ν(β).

On the other hand, by our assumption (3.2), we have

ν(β) νk−1γ (F )− ν(β) > ν(β) νkγ (F ),

which contradicts (3.7) completing the proof.

Example 3.2. For

γ(t) = (0, t), F (z, w) = w2 + zw2,

compute

ν0γ(F ) = νγ(F ) = 2, νγ(∂zF ) = 2, νγ(∂wF ) = 1, ν1γ(F ) = 1.

Hence (3.2) is violated and the conclusion of Lemma 3.1 fails. This shows the sharpness of ourassumption (3.2).

JET VANISHING ORDERS 13

The following is our main technical result. Again, we need to assume a comparison conditionbetween different jet vanishing orders to guarantee that the terms from lower order jets do notcancel with the terms providing the needed vanishing order control. Here we use different lettersF and ϕ for the function germs to emphasize their different roles. The role of F is to provide thejet vanishing orders νkγ (F ), whereas for ϕ, only the usual vanishing order νγ(ϕ) is used.

Lemma 3.3. Given germs of holomorphic maps

γ 6≡ 0: (C, 0) → (C2, 0), F, ϕ : (C2, 0) → C,

suppose that

(3.8) ν(ϕ) ≥ 2,

and for some k ≥ 1,

(3.9) νk−1γ (F ) > νkγ (F ) + νγ(ϕ)− 1,

where νkγ is the k-jet vanishing order along γ. Then the Jacobian determinant

G := det

(∂F∂ϕ

)

satisfiesνk−1γ (G) = νkγ (F ) + νγ(ϕ)− 1.

Proof. By definition, we haveG = ∂zF ∂wϕ− ∂wF ∂zϕ,

and hence

(3.10) ∂az∂bwG = ∂a+1

z ∂bwF ∂wϕ− ∂az∂b+1w F ∂zϕ+ error terms, a+ b = k − 1,

where the error terms are bilinear expressions in jk−1F and jkϕ.After a coordinate change if necessary, we may assume that the assumptions of Lemma 3.1 are

satisfied, in particularν(γ) = ν(β)

and β 6≡ 0.Next our assumption (3.9) implies that the (normalized) vanishing order of the error terms in

(3.10) along γ is strictly bigger than

νkγ (F ) + νγ(ϕ)− 1.

Therefore, to prove the lemma, it is enough to show that

(3.11) mina+b=k−1

(νγ(∂

a+1z ∂bwF ∂wϕ− ∂az∂

b+1w F ∂zϕ)

)= νkγ (F ) + νγ(ϕ)− 1.

Since (∂az∂

bwF (γ)

)′= ∂a+1

z ∂bwF (γ)α′ + ∂az∂

b+1w F (γ)β ′

and(ϕ(γ))′ = ∂zϕ(γ)α

′ + ∂wϕ(γ)β′,

14 S.-Y. KIM & D. ZAITSEV

substituting these into the first two terms in the right-hand side of (3.10), we obtain

(3.12) ∂a+1z ∂bwF (γ) ∂wϕ(γ)− ∂az∂

b+1w F (γ) ∂zϕ(γ) = ∂a+1

z ∂bwF (γ)(ϕ(γ))′

β ′−(∂az∂

bwF (γ)

)′

β ′∂zϕ(γ).

Since for a+ b = k − 1,

ν

((∂az∂

bwF (γ)

)′

β ′∂zϕ(γ)

)= ν((∂az∂

bwF (γ))

′)− ν(β ′) + ν(∂zϕ(γ))

= ν((∂az∂bwF (γ)))− 1− ν(β) + 1 + ν(∂zϕ(γ))

= ν(β)(νγ(∂

az∂

bwF )− 1 + νγ(∂zϕ)

)

≥ ν(β)(νk−1γ (F )− 1 + νγ(∂zϕ)

)

we obtain by (3.9), (3.8) and Lemma 2.1,

(3.13) ν

((∂az∂

bwF (γ)

)′

β ′∂zϕ(γ)

)> ν(β)(νkγ (F ) + νγ(ϕ)− 1), a+ b ≤ k − 1.

On the other hand, we have

ν

(∂a+1z ∂bwF (γ)

(ϕ(γ))′

β ′

)= ν(∂a+1

z ∂bwF (γ)) + ν((ϕ(γ))′)− ν(β ′)

= ν(∂a+1z ∂bwF (γ)) + ν(ϕ(γ))− ν(β)

= ν(β)(νγ(∂

a+1z ∂bwF ) + νγ(ϕ)− 1)

),

where in view of (3.3), the minimum of the vanishing order of the last expression for a+ b = k−1is achieved for (a, b) = (k − 1, 0) and equals to

(3.14) ν(β)(νkγ (F ) + νγ(ϕ)− 1

).

Together with (3.13), this implies that the minimum for a + b = k − 1 of the right-hand side in(3.12) equals (3.14). This gives the desired relation (3.11), completing the proof.

Example 3.4. Let

F (z, w) = zk + zk−1ws, ϕ(z, w) = wl + azw, γ(t) = (0, t), l ≥ 2.

Then

νk−1γ (F ) = s, νkγ (F ) = 0, νγ(ϕ) = l.

In particular, our comparison assumption (3.9) is violated if and only if s ≤ l − 1. Then for theJacobian determinant G as Lemma 3.3, we have

G = det

(kzk−1 + (k − 1)zk−2ws szk−1ws−1

aw lwl−1 + a(l − s)zw

)

JET VANISHING ORDERS 15

and hence for s = l − 1 and a = lk/s, the terms with zk−1wl−1 cancel and we obtain

νk−1γ (G) = min

(νk−1γ (zk−2ws+l−1), νk−1

γ (zk−1ws+1))= min(s+ l − 1, s+ 1) = l,

failing the conclusion (3.9) of Lemma 3.3. Hence our assumption (3.9) is sharp.

As first direct consequence in combination with Lemma 2.1, we obtain an estimate for the (total)vanishing order of the Jacobian determinant:

Corollary 3.5. Under the assumptions of Lemma 3.3,

ν(G) ≤ νkγ (F ) + νγ(ϕ) + k − 1.

As next immediate consequence of Lemma 3.3, we obtain:

Corollary 3.6. Given germs of holomorphic maps

γ 6≡ 0: (C, 0) → (C2, 0), F, ϕ : (C2, 0) → C,

suppose that

(3.15) ν(ϕ) ≥ 2.

Thenνk−1γ (G) ≤ νkγ (F ) + νγ(ϕ)− 1,

where either G = F or G = det

(∂F∂ϕ

).

Repeatedly applying Corollary 3.6, we obtain:

Corollary 3.7. Given germs of holomorphic maps

γ 6≡ 0: (C, 0) → (C2, 0), f, ϕ : (C2, 0) → C,

suppose that ν(ϕ) ≥ 2, and define fj+1 inductively by

f1 := f, fj+1 := det

(∂fj∂ϕ

), j = 1, 2, . . . .

Then for every k ∈ 0, . . . , ν(f), there exists j ∈ 1, . . . , ν(f)− k + 1 such that

νkγ (fj) ≤ (ν(f)− k)(νγ(ϕ)− 1).

In particular, for k = 0,νγ(fj) ≤ ν(f)(νγ(ϕ)− 1)

holds for some j ∈ 1, . . . , ν(f) + 1.Proof. Setting m := ν(f), we obtain from the definition of the m-jet vanishing order that

νmγ (f1) = νmγ (f) = 0.

Then Corollary 3.6 implies that there exist j ∈ 1, 2 such that

νm−1γ (fj) ≤ νγ(ϕ)− 1.

16 S.-Y. KIM & D. ZAITSEV

Next let k = m− 1 and repeat the argument for F = fj, to conclude that there exist j ∈ 1, 2, 3such that

νm−2γ (fj) ≤ 2(νγ(ϕ)− 1).

We repeat this process to show inductively that for any positive integer ℓ ≤ m, there existsj ∈ 1, . . . , ℓ+ 1 such that

νℓγ(fj) ≤ (m− ℓ)(νγ(ϕ)− 1)

as desired.

4. Selection algorithm and Proof of Theorem 1.1

We shall write C for the set of nonzero germs of holomorphic maps (C, 0) → (C2, 0). Let S bea set of holomorphic function germs (C2, 0) → C with minimal vanishing order

m := ν(S) ≥ 2,

and the finite type

T := τ(S).

4.1. Step 1; selecting a multiplier with minimal vanishing order. Choose any f0 = f ∈ Swith minimal (total) vanishing order

ν(f) = ν(S) = m.

Then choose any γ ∈ C in the zero set of f (i.e. νγ(f) = ∞). Finally choose any ϕ ∈ S with

νγ(ϕ) ≤ T

and set

µ := mink − 1 + νkγ (f) : νk−1γ (f) > νkγ (f) + νγ(ϕ)− 1, 1 ≤ k ≤ m.

Since νγ(f) = ∞, it is easy to see that

µ ≤ k0 − 1 + νk0γ (f) ≤ k0 − 1 + (m− k0)(νγ(ϕ)− 1) ≤ (m− 1)(νγ(ϕ)− 1),

where

k0 := maxk : νk−1γ (f) > νkγ (f) + νγ(ϕ)− 1, 1 ≤ k ≤ m.

Then the multiplier

f1 := det

(∂f∂ϕ

).

satisfies for some k,

k + νkγ (f1) ≤ µ+ νγ(ϕ)− 1

in view of Lemma 3.3. In particular, it follows that the vanishing order

(4.1) ν(f1) ≤ µ+ νγ(ϕ)− 1 ≤ m(νγ(ϕ)− 1) ≤ m(T − 1).

Thus we have found a multiplier f1 ∈ J(S) (as defined in §1.1) whose vanishing order is boundedby any of the above estimates.

JET VANISHING ORDERS 17

Remark 4.1. The main outcome of this step is to construct a multiplier f1 with controlled vanishingorder. Our method gives an explicit estimate for this order. Note that the initial function (pre-multiplier) f0 ∈ S is only used in this step. Once a multiplier f1 is constructed, it will be used inthe sequel for the curve selection and the computation of jet vanishing orders.

4.2. Step 2; selecting a multiplier with effectively bounded order along a zero curve

of another multiplier. Now choose any multiplier f1 with vanishing order

ν(f1) ≤ d ≤ m(T − 1).

Note that Step 1 yields such f1, however, any other f1 with a sharper estimate d can be chosen.Let γi ∈ C be germs of curves parametrizing irreducible components of the zero set of f1. Chooseϕ ∈ span(S) with

νγi(ϕ) ≤ T,

which can be any generic linear combination of elements in S. Then Corollary 3.7 implies that

νm−1γi

(fj) ≤ T − 1,

where j ∈ 1, 2 depending on i, and

f2 := det

(∂f1∂ϕ

).

Lemma 4.2. Let Φ, S0 be two sets of germs of holomorphic maps (C2, 0) → C and define induc-tively

Sj+1 := Sj ∪det

(∂f∂ϕ

): f ∈ Sj ∪ Φ, ϕ ∈ Φ

, j ≥ 0.

Writed := ν(S0)

for the minimum vanishing order of functions in S0 and assume that the type

τ(Φ) := supγ

νγ(Φ) = supγ

minϕ∈Φ

νγ(ϕ)

is finite. Assume further thatν(Φ) ≥ 2.

Then for k < d, the k-jet type of Sj satisfies

τk(Sd−k) ≤ (d− k)(τ(Φ)− 1).

In particular, for k = 0, we obtain

τ(Sd) ≤ d(τ(Φ)− 1).

Proof. Choose f ∈ S0 withν(f) = d

and let γ parametrize a curve in C2. By the definition of type, there exists ϕ ∈ Φ with

νγ(ϕ) ≤ τ(Φ).

18 S.-Y. KIM & D. ZAITSEV

Then Corollary 3.7 implies that there exists a sequence Fk ∈ Sk such that

νd−kγ (Fk) ≤ (d− k)(νγ(ϕ)− 1),

which completes the proof.

4.3. Step 3; selecting a pair of multpliers with effectively bounded multiplicity and

taking the radical. Let Φ be the set of pre-multipliers and let

S0 :=

det

(∂f∂ϕ

): f, ϕ ∈ Φ

.

Then Step 2 implies that there exists an integer d ≤ m(T − 1) such that

τ(Sd) ≤ d(T − 1).

Choose F ∈ S0 such thatν(F ) = d.

Then by the definition of τ(Sd), for each irreducible component Cj of F = 0, there exists Fj ∈ Sd

such thatνCj

(Fj) ≤ d(T − 1).

Choose a generic linear combination F of Fj. Then F is a multiplier satisfying

(4.2) νCj(F ) ≤ d(T − 1) for all j.

Lemma 4.3. Let I = (F, F ) be the ideal generated by F and F . Let d := ν(F ) be the vanishing

order and t := τF=0(F ) the contact order of F along the zero curve of F (i.e. the maximalvanishing order along an irreducible component). Then the multiplicity

(4.3) D(I) := dim (Cz, w/I)satisfies D(I) ≤ dt.

Proof. The proof can be obtained by following the arguments of D’Angelo’s proof of Theorem 2.7in [D82], more precisely, by combining [D82, (2.12)] with [D82, Lemma 2.11].

Remark 4.4. A pair (F, F ) satisfying the assumptions of Lemma 4.3 can be an called an effectiveregular sequence. Recall that a regular sequence (see e.g. [D93, 2.2.3, Definition 6]) is any sequence(f1, . . . , fs) in a local ring R, if each fj+1 is a non-zero-divisor in the quotient R/(f1, . . . , fj) for anyj = 1, . . . , s (for j = 1, the quotient needs to be interpreted as R itself). In our case, the additionaleffectiveness of the regular sequence condition comes from the estimates of the two orders – thevanishing order of F and the contact order of F along the zero curve C of F . Note that for theconclusion of Lemma 4.3 to hold, we need to estimate the contact order (the maximum order over

irreducible components of C) for F rather than its vanishing order along C (the minimum orderover the irreducible components).

Corollary 4.5. Under the assumptions of Lemma 4.3, for a := dt, one has ha ∈ I for any germof holomorphic function h with h(0) = 0, i.e. I contains the a-th power of the maximal ideal.

JET VANISHING ORDERS 19

Proof. The statement follows directly from the inequality K(I) ≤ D(I) in [D82, Theorem 2.7],see also [D93, 2.1.6, Page 57], where K(I) is the minimal power of the maximal ideal containedin I and D(I) is the multiplicity.

Proof of Theorem 1.1. By Corollary 4.5, we have za, wa as multipliers, where

a = dt, d ≤ T (T − 1), t ≤ d(T − 1)

implying, in particular,a ≤ T 2(T − 1)3.

Taking the ath roots z, w of za, wa, and taking their Jacobian determinant, we obtain the lastmultiplier 1 leading to the algorithm termination. Furthermore, taking generic linear combinations

at each step, we obtain a single sequence f1, . . . , fl of multipliers with fl−3 = F satisfying (4.2),and hence satisfying the desired properties as in the statement of Theorem 1.1. This completesthe proof.

5. Perturbations of Heier’s and Catlin-D’Angelo’s examples

Heier [He08] and Catlin and D’Angelo [CD10] gave examples of special domains in C3, where the

original Kohn’s procedure [K79] of taking full radicals at every step does not lead to an effectiveestimate (in terms of the type and the dimension) for the order of subellipticity in subellipticestimate. The main reason is the lack of control of the root order in the radical. Heier’s exampleis

Re z3 + |z31 + z1zK2 |2 + |z2|2, K ≥ 2,

where the set of pre-multipliers is S = z31+z1zK2 , z2 and a calculation of Kohn’s multiplier idealsyields, in the notation of Section 1.1:

I0 =√J(S) = J(S) = (3z21 + zK2 ), J(S ∪ I0) = (z1, z

K2 ), I1 =

√J(S ∪ I0) = (z1, z2),

where the last radical requires taking elements of the root order K that can be arbitrarily high incomparison with the D’Angelo type 6. As consequence, the corresponding order of subellipticityε in the subelliptic estimate (1.6) obtained this way is not effectively controlled by the type. Notethat since z2 ∈ S, z1 ∈ J(S ∪ I0), it is easy to regain the effectivity by taking another Jacobiandeterminant instead of the radical to obtain

1 ∈ J(S ∪ J(S ∪ I0)),leading to an effective subelliptic estimate with ε = 1/8. In particular, the step of taking radicalsfor this example can be avoided completely, due to the presence of the linear pre-multiplier z2 ∈ S.A similar lack of effectivity phenomenon is exhibited in the Catlin-D’Angelo’s example as ex-

plained in [CD10, Section 4] and [S17, Section 4] (where, however, it is not possible to avoid takingradicals when there is no pre-multiplier of vanishing order 1). Furthermore, the same lack of con-trol with the same argument also applies to higher order perturbations of that example (that maynot be of a triangular form).More precisely, consider perturbations Ω ⊂ C3 of the Catlin-D’Angelo’s example given by

Re z3 + |F1(z1, z2)|2 + |F2(z1, z2)|2 < 0,

20 S.-Y. KIM & D. ZAITSEV

F1 = zM1 +O(L), F2 = zN2 + zK1 z2 +O(L), K > M ≥ 2, N ≥ 3,

where we use the notationO(L) = O(|(z1, z2)|L).

Then for L sufficiently large, the explicit calculations in [CD10, Proposition 4.4] and [S17, Section4.1] show that the root order required for the radical I1 of J1 := J(S∪I0) (in the notation of §1.1)is at least K, i.e. (I1)

K−1 6⊂ J1. As consequence, the order of subellipticity obtained this way isnot effectively controlled by the type.We now illustrate how our selection procedure modifying the original Kohn’s algorithm applies

to this case. For simplicity, we shall assume L sufficiently large but effectively bounded from belowby the type T = max(M,N) (i.e. L ≥ Φ(T ) for suitable function Φ that can be directly com-puted), and K being sufficiently large (when the above non-effectivity occurs). The first multipliergenerating J0 := J(S) is(5.1)

f1 := det

(∂F1

∂F2

)= det

(MzM−1

1 0KzK−1

1 z2 NzN−12 + zK1

)=MNzM−1

1 zN−12 +MzK+M−1

1 +O(L− 1),

where the perturbation error estimate L − 1 is only rough for the sake of simplicity. Then amonodromy argument implies that the zero set of f1 is the union of the (possibly reducible)curves

(5.2) zM−11 = O(L−N), NzN−1

2 + zK1 = O(L−M).

For any parametrisation γ of an irreducible component of the first curve, we take in our Step 2

ϕ = F2, νγ(ϕ) = N,

and compute

f2 = det

(∂f1∂ϕ

)∼ zM−2

1 z2(N−1)2 +O(L− 2) mod zK−1

1 ,

where we write ∼ for the equality up to a constant factor. The corresponding jet vanishing ordersof f1 are

ν0γ(f1), . . . , νM−2γ (f1) ≥

L−N

M − 1, νM−1

γ (f1) = N −1, νMγ (f1) = N −2, . . . , νM+N−2γ (f1) = 0.

Then our comparison condition (3.10) holds for k =M−1, and hence Lemma 3.3 gives the desiredcontrol of the next lower jet vanishing order

νM−2γ (f2) = 2(N − 1).

Next, continuing as in Step 2 in the previous section, we obtain the sequence of multipliers

fj = det

(∂fj−1

∂ϕ

)∼ zM−j

1 zj(N−1)2 +O(L− j) mod zK−j+1

1 , j = 1, 2, . . . ,M,

where the last multiplier

fM = zM(N−1)2 +O(L−M) mod zK−M+1

1

has the finite order M(N − 1) along γ.

JET VANISHING ORDERS 21

Similarly, for any curve γ in the variety defined by the second equation (5.2), we take in ourStep 1 the other pre-multiplier

ψ = F1 = zM1 +O(L), νγ(ψ) =M.

Then following our Step 2 procedure, we obtain the sequence of multipliers

g1 = f1, gj = det

(∂gj−1

∂ψ

)∼ z

j(M−1)1 zN−j

2 +O(L− j), j = 2, . . . , N,

where the last multiplier

gN = zN(M−1)1 +O(L−N)

has the finite order N(M − 1) along γ.Finally, in Step 3, we take

F = f1 =MNzM−11 zN−1

2 +MzK+M−11 +O(L− 1),

F = fM + gN = zM(N−1)2 + z

N(M−1)1 +O(L−max(M,N)) mod zK−M+1

1

such that

d = ν(F ) =M +N − 2, t = νF=0(F ) = max(N(M − 1),M(N − 1))

and the ideal generated by F and F has the multiplicity ≤ dt which bounds the root order inthe radical, to obtain the multipliers z1 and z2, and hence their Jacobian determinant, leading tothe desired termination. Furthermore, the number of steps and the root order when taking theradical, and hence the order of subellipticity in Corollary 1.3 are explicitly controlled in terms ofthe type 2T = 2max(M,N).

Acknowledgements. We would like to thank Professor Joseph J. Kohn for suggesting thetopic and encouragement, and Professor John P. D’Angelo for careful reading of the manuscriptand numerous helpful remarks as well as many inspiring discussions. We are also grateful to Pro-fessor Yum-Tong Siu for his interest and encouragement and for kindly sending us his paper [S17]containing the most recent account on the subject and setting future development perspectives.We finally would like to thank the anonymous referee for careful reading and numerous helpfulsuggestions.

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S.-Y. Kim: Center for Mathematical Challenges, Korea Institute for Advanced Study, 85

Hoegiro, Dongdaemun-gu, Seoul, Korea

E-mail address : [email protected]

D. Zaitsev: School of Mathematics, Trinity College Dublin, Dublin 2, Ireland

E-mail address : [email protected]