This paper uses the reflection map to simplify nondegeneracy conditions for sphere maps and investigates the structure and bounds of their infinitesimal deformations, providing new characterizations.
Contribution
It introduces a new application of the reflection map to analyze infinitesimal deformations and bounds their dimension for nondegenerate sphere maps.
Findings
01
Bound on the dimension of infinitesimal deformations
02
Characterization of the homogeneous sphere map
03
Simplified nondegeneracy conditions
Abstract
The reflection map introduced by D'Angelo is applied to deduce simpler descriptions of nondegeneracy conditions for sphere maps and to the study of infinitesimal deformations of sphere maps. It is shown that the dimension of the space of infinitesimal deformations of a nondegenerate sphere map is bounded from above by the explicitly computed dimension of the space of infinitesimal deformations of the homogeneous sphere map. Moreover a characterization of the homogeneous sphere map in terms of infinitesimal deformations is provided.
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Full text
The reflection map and infinitesimal deformations of sphere mappings
The reflection map introduced by D’Angelo is applied to deduce simpler descriptions of nondegeneracy conditions for sphere maps and to the study of infinitesimal deformations of sphere maps. It is shown that the dimension of the space of infinitesimal deformations of a nondegenerate sphere map is bounded from above by the explicitly computed dimension of the space of infinitesimal deformations of the homogeneous sphere map. Moreover a characterization of the homogeneous sphere map in terms of infinitesimal deformations is provided.
2010 Mathematics Subject Classification:
32V40, 32V30
The author was supported by the Austrian Science Fund (FWF), project P28873-N35.
1. Introduction
The main motivation is the study of real-analytic CR maps of the unit sphereS2n−1 in Cn for n≥2, which is defined by
[TABLE]
For n=2 write z=z1,w=z2. A lot is known about mappings of spheres, see the survey by D’Angelo [DAngelo15] and the references therein. A prominent example of a sphere map is the homogeneous sphere map Hnd of degree d from S2n−1 into S2K−1 for some K=K(n,d)∈N, which consists of all lexicographically ordered monomials in z=(z1,…,zn)∈Cn of degree d and is given by
[TABLE]
The purpose of this article is to study the reflection map, which was introduced by D’Angelo [DAngelo03] in the case of sphere mappings and further investigated by the same author in [DAngelo07a] in the case of maps of hyperquadrics. The reflection map of a mapping H allows to effectively compute and deduce several properties of the X-variety associated to H. The X-variety was introduced and studied by Forstnerič in [Forstneric89] to extend CR maps satisfying certain smoothness assumptions. In the case of real-analytic CR maps of spheres it is shown that these maps are rational.
The homogeneous sphere map Hnd plays a crucial role in the classification of polynomial maps, see the works of D’Angelo [DAngelo88b, DAngelo91] and [DAngelo16] for rational sphere maps. The homogeneous sphere map appears in the definition of the reflection map CH for a rational sphere map H=P/Q:S2n−1→S2m−1 with Q=0 on S2n−1: Let VH:Cm→CK be a matrix with holomorphic entries, satisfying VH(X)⋅Hˉnd/Qˉ=X⋅Hˉ on S2n−1 for X∈Cm, where ⋅ denotes the euclidean inner product. The previous identity is achieved by the homogenization technique of D’Angelo [DAngelo88b]. VH is referred to as reflection matrix and CH(X):=VH(X)⋅Hˉnd/Qˉ for X∈Cm. See Section 2.4 below for more details.
In this article the reflection matrix will be applied in two ways. In the first case it is shown that nondegeneracy conditions of sphere maps can be rephrased in terms of rank conditions on the reflection matrix.
The nondegeneracy conditions considered here were introduced in [Lamel01] and [LM17] respectively. In the case of a sphere map H:S2n−1→S2m−1 they are defined as follows: If Γ denotes the set of real-analytic CR vector fields tangent to S2n−1, then H is called finitely nondegenerate at p∈S2n−1, if there is an integer ℓ∈N, such that,
[TABLE]
The map H is called holomorphically nondegenerate if there is no nontrivial holomorphic vector field tangent to S2m−1 along the image of H.
These notions of nondegeneracy were originally defined for submanifolds and introduced by [Stanton95] and [BHR96] respectively, see also the survey of Lamel [Lamel11].
For more details on nondegeneracy conditions for CR maps see also Section 2.2 below. Then the following theorem is shown:
Theorem 1**.**
Let H:S2n−1→S2m−1 be a rational map of degree d.
(a)
H* is finitely nondegenerate at p∈S2n−1 if and only if VH is of rank m at p∈S2n−1.*
(b)
H* is holomorphically nondegenerate if and only if VH is generically of rank m on S2n−1.*
This has immediate consequences to show sufficient and necessary conditions in terms of nondegeneracy conditions for the X-variety of H to be an affine bundle or that it agrees with the graph of the map, see Section 5 and Theorem 3 below for more details.
In the second case, applications of the reflection matrix to the study of infinitesimal deformations are provided. For M⊂CN and M′⊂CN′ real submanifolds consider the set H(M,M′) of all maps, which are holomorphic in a neighborhood of M and satisfying H(M)⊂M′. In [dSLR15a, dSLR15b, dSLR17, dSLR18] locally rigid maps were studied. They correspond to isolated points in the quotient space of H(M,M′) under automorphisms. A sufficient linear condition was provided for local rigidity of a given map, which is formulated in terms of infinitesimal deformations. An infinitesimal deformation of a map H:M→M′ is a holomorphic vector, defined in a neighborhood of M, whose real part is tangent to M′ along the image of H. The set of infinitesimal deformations of a map H is denoted by hol(H). Examples of infinitesimal deformations of a map H can be obtained from smooth curves of maps R∋t↦H(t), with H(0)=H, since dtdH(t)∣t=0∈hol(H).
The results involving infinitesimal deformations are summarized in the following theorem:
Theorem 2**.**
Let H:S2n−1→S2m−1 be a holomorphically nondegenerate rational map of degree d.
It holds that dimhol(H)≤dimhol(Hnd)=(d2d+n)K(n,d)2 and if H is assumed to be polynomial, then dimhol(H)=dimhol(Hnd) if and only if H is unitarily equivalent to Hnd.
This result contains an alternative characterization of the homogeneous sphere map to the one given in [Rudin84, DAngelo88b] or [DAngeloBook]*section 5.1.4, Theorem 3 and demonstrates a new method to compute infinitesimal deformations for sphere maps. While the article [dSLR15a] contains examples which required computer-assistance, it is shown in several examples in this article that the reflection matrix allows for explicit and effective computations of infinitesimal deformations of sphere maps.
2. Preliminaries
The purpose of this section is to introduce the necessary notions and notations needed throughout the article. These are only required for maps of spheres but without any effort and no loss of clarity the general case of maps of manifolds M and M′ is treated. To this end the following assumptions are made: Let M be a real-analytic generic submanifold of CN of codimension d. For a real-analytic CR submanifold M′⊂CN′ of codimension d′, let p′∈M′ and ρ′:V′×Vˉ′→Rd′,ρ′=(ρ1′,…,ρd′′), be a real-analytic mapping, such that M′∩V′={z′∈V′:ρ′(z′,zˉ′)=0}, where V′⊂CN′ is a neighborhood of p′∈M′ and the differentials dρ1′,…,dρd′′ are linearly independent in V′.
Denote Vˉ′={zˉ′∈CN′:z′∈V′}. The complex gradient ρj′z′ of ρj′ is given by ρj′z′=(∂z1′∂ρj′,…,∂zN′′∂ρj′). The following notation is used: v⋅w:=v1w1+⋯+vnwn for vectors v=(v1,…,vn)∈Cn and w=(w1,…,wn)∈Cn.
2.1. Infinitesimal deformations of CR maps
One of the main objects of this article are infinitesimal deformations of a CR map.
Definition 1**.**
Let H:M→M′ be a real-analytic CR map. A real-analytic CR map X:M→CN′ is called an infinitesimal deformation of H, if for every p∈M and every real-analytic mapping ρ′=(ρ1′,…,ρd′′) defined in a neighborhood of H(p) vanishing on M′, it holds that,
[TABLE]
for some open neighborhood U⊂CN of p.
The space of infinitesimal deformations of H is denoted by hol(H).
For a real manifold M the space hol(M) of infinitesimal automorphisms of M consists of holomorphic vectors whose real part is tangent to M.
For a map H:M→M′ the subspace aut(H):=hol(M′)∣H(M)+H∗(hol(M))⊂hol(H) is referred to as the space of trivial infinitesimal deformations of H. Its complement in hol(H) is called the space of nontrivial infinitesimal deformations of H.
A map H is called infinitesimally rigid if hol(H)=aut(H).
The infinitesimal stabilizer of H is given by (S,S′)∈hol(M)×hol(M′) such that H∗(S)=−S′∣H(M). An infinitesimal automorphism S∈hol(M) is said to belong to the infinitesimal stabilizer of H if there exists S′∈hol(M′) such that H∗(S)=−S′∣H(M).
In the case of sphere mappings, for a real-analytic CR map H:S2k−1→S2m−1, a holomorphic map X:U→Cn, where U⊂Ck is an open neighborhood of S2k−1, is an infinitesimal deformation of H if Re(X(z)⋅H(z))=0 for z∈S2k−1.
2.2. Nondegeneracy conditions for CR maps
The purpose of this section is to provide the definitions of finite and holomorphic nondegeneracy for CR maps introduced by Lamel [Lamel01] and Lamel–Mir [LM17] respectively, and study some of their properties.
Definition 2**.**
A real-analytic CR map H:M→M′ is called holomorphically degenerate if there exists a real-analytic CR map Y:M→CN′ satisfying Y≡0 and for every p∈M and every real-analytic mapping ρ′=(ρ1′,…,ρd′′) defined in a neighborhood of H(p) vanishing on M′, it holds that,
[TABLE]
for some open neighborhood U⊂CN of p.
If a map is not holomorphically degenerate it is called holomorphically nondegenerate.
Simple examples of holomorphically degenerate maps are the following:
Example 1**.**
Let F:S2n−1→S2m−1, then H=F⊕0, where 0∈Ck, is a holomorphically degenerate sphere map from S2n−1 into S2(n+k)−1, since X=0⊕G for 0∈Cn and G a holomorphic function from Cn into Ck satisfies X⋅Hˉ=0.
Finite nondegeneracy is defined as follows:
Definition 3**.**
Consider a real-analytic CR map H:M→M′. Let Lˉ1,…,Lˉn a basis of CR vector fields of M and for a multiindex α=(α1,…,αn)∈Nn denote Lˉα=Lˉ1α1⋯Lˉnαn. Let p∈M. For each k∈N define the following subspaces of CN′:
[TABLE]
for a real-analytic mapping ρ′=(ρ1′,…,ρd′′) defined in a neighborhood of H(p) and vanishing on M′.
Define s(p):=N′−maxkdimCEk′(p), which is called the degeneracy of H at p. The map H is of constant degeneracys(q) at q∈M if p↦s(p) is a constant function in a neighborhood of q. If s(p)=0, then H is called finitely nondegenerate at p. Considering the smallest integer k0 such that Eℓ′(p)=Ek0′(p) for all ℓ≥k0 one can say more precisely that H is (k0,s)-degenerate at p. If the map is finitely nondegenerate at p one says that it is k0-nondegenerate at p.
Note that if a map is finitely nondegenerate at p, then it is also finitely nondegenerate at points in a neighborhood of p. If M is connected, by [Lamel01]*Lemma 22 the set of points where the map H:M→M′ is of constant degeneracy s(H):=minp∈Ms(p) is an open and dense subset of M. The number s(H) is called generic degeneracy of H.
Constant degeneracy can be phrased in terms of vector fields as follows:
Let H:M→M′ be a real-analytic CR mapping of constant degeneracy s in a neighborhood of p∈M. Then it holds that
[TABLE]
These following statements are analogous to the corresponding statements for manifolds or infinitesimal automorphisms, see [BERbook]*Theorem 11.5.1 and [BERbook]*Proposition 12.5.1.
Proposition 2**.**
Let H:M→M′ be a real-analytic CR map. Then the following statements hold:
(a)
If H is holomorphically degenerate, then dimRhol(H)=∞.
(b)
If H is finitely nondegenerate at p∈M, then it is holomorphically nondegenerate.
(c)
If the space of holomorphic vector fields at p∈M tangent to M′ along the image of H is of complex dimension s, then, outside a proper real-analytic variety of a neighborhood of p, the map H is of constant degeneracy s.
Note that if s=0, then (c) says that if the map H is holomorphically nondegenerate then H is finitely nondegenerate outside a proper real-analytic variety.
Moreover, if M is assumed to be connected, (c) yields the following statement: If at any p∈M the space of holomorphic vector fields at p∈M tangent to M′ along the image of H is of complex dimension at least s, then the generic degeneracy of H is at least s.
To show (a) argue as in [BERbook]*Proposition 12.5.1: If H is holomorphically degenerate, there exists a nontrivial holomorphic map X tangent to M′ along H(M). Then for each k∈N also Yk:=z1kX is tangent to M′ along H(M) and these maps are complex-linearly independent. Since M is generic and the real part of a nontrivial holomorphic map X^, restricted to M, cannot vanish on M (the vanishing of Re(X^)∣M would imply that X^≡0), the vector fields Re(Yk) are real-linearly independent, hence dimRhol(H)=∞.
To prove (b) denote by X(H) the set of holomorphic vector fields tangent to M′ along the image of H. Consider X=∑jaj(Z)∂Zj∂∈X(H) which, by the finite nondegeneracy of H and Proposition 1, satisfies aj(p)=0 and ∑jaj(Z)ρk′Zj(H(Z),H(Z))=0 for Z∈M,k=1,…,d′ and a real-analytic mapping ρ′=(ρ1′,…,ρd′′) defined in a neighborhood of H(p) and vanishing on M′. Taking derivatives w.r.t. CR vector fields L of M one gets
[TABLE]
for multiindices βm∈Nn for m=1,…,N′. Use coordinates as given in e.g. [BERbook]*Proposition 1.3.6 for M in (1), i.e. Z=(z,u+iϕ(z,zˉ,u))∈Cn×Cd, where ϕ is defined near [math] in R2N+d with values in Rd satisfying ϕ(p)=0 and dϕ(p)=0. Taking derivatives w.r.t. z and u one gets:
[TABLE]
where the expression “l.o.t.” stands for terms vanishing at Z=p. Evaluating at Z=p one gets that ∑jajZr(p)Lβmρk′Zj(H(Z),H(Z))∣Z=p=0 for 1≤k≤d′. Thus, since H is finitely nondegenerate at p, there are multiindices γm∈Nn and integers km∈N with 1≤km≤d′, such that the matrix (Lγmρkm′Zj(H(Z),H(Z))∣Z=p)1≤j,m≤N′ is of full rank, which implies that ajZℓ(p)=0. Proceeding inductively shows that all derivatives of aj(Z) have to vanish at p. This means that the holomorphic vector field X vanishes in a neighborhood of p on the generic submanifold M, hence X≡0, which implies that H is holomorphically nondegenerate.
To show (c) let {X1,…,Xs} be a basis of the space of holomorphic vector fields at p∈M tangent to M′ along the image of H and take X∈spanC{X1,…,Xs}. Consider the following equation for 1≤k≤d′:
[TABLE]
Take derivatives w.r.t. L and since X is holomorphic, it holds that,
[TABLE]
for any multiindex β∈Nn. This implies that for any sequence β1,…,βN′∈Nn of multiindices and integers km∈N with 1≤km≤d′ the vector field X belongs to the kernel of the matrix (Lβmρkm′Z(H(Z),H(Z)))1≤m≤N′. Hence outside a proper real-analytic variety Y of a neighborhood of p it holds that for any ℓ∈N one has dimCEℓ′(q)=N′−s for q∈Y, such that the degeneracy of H is equal to s for all q∈Y.
∎
2.3. Infinitesimal automorphisms of the unit sphere
In the following the well-known infinitesimal automorphisms of S2n−1,n≥2 are listed for later reference. For A=(A1,…,An)∈hol(S2n−1) the j-th component is given as follows:
[TABLE]
where αm,βmℓ∈C and sm∈R and dimRhol(S2n−1)=n(n+2). The following notation is required:
[TABLE]
For a map H:S2k−1→S2m−1 any T∈aut(H) can be written as T=T1+…+T4, such that the Tj are given as follows:
[TABLE]
where α′=(α1′,…,αm′)∈Cm, V′∈Cm×Cm is a matrix satisfying V′+\prescripttVˉ′=0, α=(α1,…,αk)∈Ck and z=(z1,…,zk)∈Ck.
2.4. The reflection matrix
The following definition is a summary of [DAngelo03]*Definition 2.1, 2.2 introducing the homogenization and reflection map (which appears in the study of the X-variety, see also [DAngelo07a] for the case of hyperquadric maps): Denote by H(n,d) the complex vector space of homogeneous polynomials of degree d in n holomorphic variables z=(z1,…,zn). Write Hˉ(n,d) for the complex vector space with basis consisting of homogeneous polynomials of degree d in n anti-holomorphic variables zˉ=(zˉ1,…,zˉn).
Definition 4**.**
Let H=QP:U⊂Cn→Cm be a rational map of degree d (not necessarily a sphere map), where P=(P1,…,Pm) and Q:Cn→C with Q=0 on U. Write H=Q1∑k=0dPk, where Pk is homogeneous of order k.
Define the reflection mapCH:Cm→Hˉ(n,d) of H by
[TABLE]
Since CH is linear and CH(X)∈Hˉ(n,d) there exists a matrix VH:Cm→CK(n,d) with holomorphic entries, such that
[TABLE]
and denote V:=QVH. The matrix V is referred to as reflection matrix of H.
Several properties of the reflection matrix and examples involving V are given in [DAngelo03].
3. Examples and constructions for sphere maps
In this section some particular examples of sphere maps and constructions of sphere maps are presented and their relation to the above nondegeneracy conditions are discussed.
3.1. The homogeneous sphere maps
The purpose of this section is to show some properties of the homogeneous sphere maps defined as follows:
Definition 5**.**
For d≥1 and n≥2 define K(n,d)=(dn+d−1) and I(n,d) as the set of all multiindices α∈Nn of length d equipped with the lexicographic order. Define the homogeneous sphere map Hnd in n variables of degree d as
[TABLE]
A direct computation or [DX17]*Theorem 4.2 shows that the infinitesimal stabilizer of Hnd is given by Sn2 and Sn3.
One can show that Hnd is holomorphically nondegenerate by using the Fourier coefficient technique as in [DAngelo88b]*Lemma 16. Instead of showing this, it is proved that Hnd is finitely nondegenerate on S2n−1. Before giving a proof of this fact some preparations are needed:
For n≥3 we define CR vector fields of S2n−1 by Lˉij=zi∂zˉj∂−zj∂zˉi∂ for 1≤i=j≤n. For n=2 the CR vector field of S3 is given by Lˉ=z∂wˉ∂−w∂zˉ∂.
Let {Xij:1≤i,j≤n} be a collection of vector fields. In order to denote powers of such vector fields the following notation is used: Define the set J:={α=(α1,…,αn)∈N3n:αj=(αj1,αj2,αj3)∈N3} and for α∈J write Xα:=Xα11α12α13⋯Xαn1αn2αn3. Define ∣α∣=∑j=1nαj3 for n≥3.
For two vector fields X and Y, their Lie bracket is denoted by [X,Y]:=X(Y)−Y(X).
In the following lemma some basic facts about CR vector fields and their commutators are given. The proofs consist of straight forward calculations and are omitted.
Lemma 1**.**
Assume n≥3. In the following for 1≤i,j,k,ℓ≤n assume i=j and k,ℓ∈{i,j}. Define the following vector fields for S2n−1:
[TABLE]
Then Tjk=−Tˉkj and Sij=Sji and the following commutator relations hold:
The map Hnd:S2n−1→S2K(n,d)−1 is d-nondegenerate at each point of S2n−1.
Proof.
Set H:=Hnd, fix 1≤m≤n and define the following set of multiindices
[TABLE]
where the index set J from the beginning of Section 3.1 is used.
It will be shown that the K(n,d)×K(n,d)-matrix
[TABLE]
is of full rank if zm=0. This implies that H is d-nondegenerate at each point of S2n−1. The proof consists of two steps:
(A)
It is proved that
[TABLE]
on S2n−1, for all multiindices α,β∈Jm with ∣α∣<∣β∣ and all γ∈J,δ∈Jm, where J is defined in the beginning of Section 3.1.
(B)
It is shown that for each 0≤k≤d the set Dmk:={LαH∣S2n−1:α∈Jm,∣α∣=k} consists of linearly independent vectors in CK(n,d) if zm=0.
Observe that the number of elements in Dmk is equal to K(n−1,k), such that ∑k=0dK(n−1,k)=K(n,d).
Thus, the two steps together imply that the matrix Am consists of linearly independent rows if zm=0.
In order to show (A) one proceeds by induction on the length of α in (3): For ∣α∣=0 one needs to argue as follows. Since H⋅Hˉ=1 on S2n−1, it follows that pH,β:=H⋅LˉβHˉ=0 on S2n−1 for all β∈Jm. This means that pH,β is a homogeneous polynomial vanishing on S2n−1, hence pH,β vanishes in Cn, see [DAngelo91]*section II or [DAngeloBook]*section 5.1.4. Applying zˉkzˉj∂ to pH,β≡0, implies that H⋅LˉβTγSδHˉ=0 for all γ∈J and δ∈Jm.
Assume that (3) holds for ∣α∣=k and ∣α∣+1<∣β∣. If one applies Lmj to (3) one obtains:
[TABLE]
on S2n−1. If one can show that
[TABLE]
the induction is completed and (A) is proved. In order to show (4), use the identities from Lemma 1, which imply that the expression of the left-hand side of (4) can be rewritten as a sum of terms of the form LαH⋅Lˉβ′Tγ′Sδ′LmjHˉ and LαH⋅Lˉβ′Tγ′Sδ′Hˉ, where ∣β′∣≥∣β∣−1,γ′∈J and δ′∈Jm. Hence using the induction hypothesis proves (4).
To prove (B) fix 0≤k≤d and assume that the set Dmk consists of vectors which are not linearly independent. By setting K:={α∈Jm:∣α∣=k}, the linear dependence says that there are cα∈C, not all of them are zero, such that
[TABLE]
on S2n−1. Since the left-hand side is a homogeneous polynomial, (5) holds in Cn. For α∈K define the multiindex
[TABLE]
such that zr(α):=z1k1…zm−1km−1zm+1km+1⋯znkn. Note that Lα=zˉmk∂zr(α)∂k+…, where … stands for derivatives of order k with coefficients being monomials of degree k containing zˉmℓ for ℓ<k. Define Rα:=∂zˉmk∂kLα.
Assume zm=0. Expanding (5) as a power series in zˉ with vector-valued coefficients, the coefficient of zˉmk is given by
[TABLE]
Note that in the vector RαH∈CK(n,d) each monomial of Hd−k appears in exactly one component and it is of the following form:
[TABLE]
where 1≤j1(α)≤K(n,d) and mt(α),j1(α)1=ct(α)zt(α)=0 such that t(α)∈Nn with ∣t(α)∣=K(n,d−k).
Consider the minimal α0∈K w.r.t. the lexicographic order. If m=1, then α0=(2,…,2), and otherwise α0=(1,…,1). This implies that j1(α)≥j1(α0) for all α>α0.
Moreover t(α)>t(α0) for all α>α0, which can be seen as follows:
Denote the monomial in Hnd at the k-th position by hs(k),k=akzs(k), where s(k)∈Nn with ∣s(k)∣=K(n,d).
Note that s(j1(α))=α+t(α) and for α>α0 if j1(α0)≤j1(α), then s(j1(α0))≤s(j1(α)). Hence
[TABLE]
which implies that t(α0)<t(α). Thus, in (6), considering the coefficient of zt(α0) shows that cα0=0.
Proceed inductively and assume cα=0 for all α<α1,α∈K. Define K1=K∖{α∈K:α<α1}. Argue as above, since α1 is the minimal index in K1 it holds that j1(α)≥j1(α1) for all α>α1 and the same argument as above shows that t(α)>t(α1). Thus cα1=0, which proves (B) and completes the proof.
∎
3.2. The group invariant sphere maps
Another important class of sphere maps are the following, first introduced in [DAngelo88b]:
Definition 6**.**
Define Gℓ:S3→S2ℓ+3 for ℓ≥0 by
[TABLE]
where ckℓ≥0 for 1≤k≤ℓ+2 is given in [DAngelo88b] or [DAngeloBook]*section 5.2.2, Theorem 9.
The infinitesimal stabilizer of Gℓ consists of the vector field S23.
The maps Gℓ are invariant under a fixed-point-free finite unitary group and appear in [DKR03] as so-called sharp polynomials in the study of degree bounds for monomial maps.
3.3. The tensor product for infinitesimal deformations
Similar to the case of sphere maps ([DAngelo88b], [DAngelo91]*Definition 4) one can introduce a tensor operation for infinitesimal deformations.
Let A⊆Cn be a linear subspace such that Cn=A⊕A⊥ is an orthogonal decomposition. For v∈Cn write v=vA⊕vA⊥∈A⊕A⊥. Similarly one can decompose the image of a map F:S2n−1→S2m−1 w.r.t. A and write F=FA⊕FA⊥∈A⊕A⊥.
For vectors v=(v1,…,vn)∈Cn and w=(w1,…,wm)∈Cm the usual tensor product of v and w is denoted by
[TABLE]
Definition 7**.**
Let H:S2n−1→S2m−1 and G:S2n−1→S2ℓ−1 be CR maps, X∈hol(H) and A⊆Cm be a linear subspace, then
[TABLE]
is called the tensor product of X by G on A.
We recall that the tensor product of mappings of spheres was introduced in [DAngelo88b] and [DAngelo91]*Definition 4: For f:S2n−1→S2m−1 and g:S2n−1→S2ℓ−1 CR maps and A⊆Cm a linear subspace the tensor product of f by g on A given by E(A,g)f=(fA⊗g)⊕fA⊥ is a mapping of spheres, see [DAngelo91]*Lemma 5. An analogous result holds for infinitesimal deformations:
Lemma 3**.**
Let H:S2n−1→S2m−1 and G:S2n−1→S2ℓ−1 be CR maps, X∈hol(H) and A⊆Cm be a linear subspace. Then T(A,G)X∈hol(E(A,G)H).
Proof.
Set Y=T(A,G)X and F=E(A,G)H. By orthogonality it holds that on S2n−1,
[TABLE]
since ∥G∥2=1 on S2n−1, hence Y∈hol(F).
∎
The next result shows that holomorphic degeneracy is preserved by tensoring.
Lemma 4**.**
Let H:S2n−1→S2m−1 be a CR map, A⊆Cm a linear subspace and G:S2n−1→S2ℓ−1 a CR map. If H is holomorphically degenerate then E(A,G)H is holomorphically degenerate.
Proof.
Since H is holomorphically degenerate there exists a nontrivial holomorphic map W:Cn→Cm such that W⋅Hˉ=0 on S2n−1. Write H′=E(A,G)H and consider W′=T(A,G)W, which is a nontrivial holomorphic vector. Then the same computation (without taking the real part) as in the proof of Lemma 3 shows that W′⋅Hˉ′=0 on S2n−1, i.e. H′ is holomorphically degenerate.
∎
Example 2**.**
The converse of Lemma 4 is not true in general: Consider the holomorphically nondegenerate maps H:S3→S7,H(z,w)=(z,zw,z2w,w3) and G:S3→S5,G(z,w)=(z,zw,w2). Tensoring H at the first component with G one obtains the holomorphically degenerate map F′(z,w)=(z2,z2w,zw2,zw,z2w,w3). Moreover, if one applies a unitary change of coordinates and a projection C6→C5 to F′, one obtains F(z,w)=(z2,zw,2z2w,zw2,w3), which still is holomorphically degenerate: the holomorphic vector X=(0,−1,z/2,w,0) satisfies X⋅Fˉ=0 on S3.
Example 3**.**
For a sphere map H its trivial infinitesimal deformations may give rise to nontrivial infinitesimal deformations of tensors of H: Let H be the map
[TABLE]
and A be the complex subspace spanned by (1,0…,0)∈C4. Write H=(H1,…,H4) and define X=(a,0,…,0)−(aˉH1)H∈aut(H),a∈C∖{0}. Then it is straightforward to show that T(A,H1)X∈aut(E(A,H1)H).
Example 4**.**
Following [DL16]*Prop. 2.4 one can combine two sphere maps to construct a new sphere map into a higher dimensional sphere: For H:S2n−1→S2m−1 and G:S2n−1→S2ℓ−1 real-analytic CR maps define the juxtaposition of H and G with parameter t∈[0,1] as the map jt(H,G):S2n−1→S2(m+ℓ)−1 given by
[TABLE]
Note that jt(H,G) is holomorphically degenerate: The holomorphic vector field X=−tH⊕1−t2G satisfies X⋅Hˉ=0.
4. Nondegeneracy conditions for sphere maps
In this section it is shown that holomorphic and finite degeneracy can be expressed in terms of rank conditions of the reflection matrix.
Holomorphic nondegeneracy of a sphere map is equivalent to a generic rank condition of V:
Proposition 3**.**
Let H:S2n−1→S2m−1 be a rational map of degree d.
Then the following statements are equivalent:
(a)
H* is holomorphically nondegenerate.*
(b)
There is no nontrivial holomorphic map Y:U→Cm, where U is a neighborhood of S2n−1, such that VY=0 on S2n−1.
(c)
The matrix V is generically of rank m on S2n−1.
Proof.
For a map H=QP the following equation holds on S2n−1:
[TABLE]
for any vector X∈Cm. Let Y:U→Cm, where U is a neighborhood of S2n−1, be a nontrivial holomorphic map such that Y⋅Hˉ=0 on S2n−1. By (7), this is equivalent to VY⋅Hˉnd=0 on S2n−1. Since Hnd is holomorphically nondegenerate on S2n−1, the last equation is equivalent to VY=0 on S2n−1. From this consideration the equivalence of (a) and (b) follows.
The equivalence of (b) and (c) holds, since (b) is equivalent to the fact that V is injective on an open, dense subset of S2n−1, which is equivalent to (c). ∎
The following proposition shows that finite nondegeneracy of a map H is equivalent to a pointwise rank condition of VH:
Proposition 4**.**
Let H:S2n−1→S2m−1 be a rational map of degree d.
Then the following statements are equivalent:
(a)
H* is of degeneracy s at p∈S2n−1.*
(b)
The kernel of the matrix V is of dimension s at p∈S2n−1.
In particular, the map H is finitely nondegenerate at p∈S2n−1 if and only if the matrix V is of rank m at p∈S2n−1.
Since X⋅Hˉ=VHX⋅Hˉnd/Qˉ on S2n−1 for any X∈Cm and V is holomorphic, it follows that
[TABLE]
on S2n−1. For any sequence of multiindices α=(α1,…,αℓ),αj∈Nn and a sphere map F:S2n−1→S2k−1 define the ℓ×k-matrix Aqα(Fˉ):=(LˉαjFˉ∣q)1≤j≤ℓ for q∈S2n−1. Then it holds that
[TABLE]
for any p∈S2n−1, any sequence of multiindices β=(β1,…,βr),βj∈Nn and r∈N.
Observe that rkApγ(Hˉnd/Qˉ)=rkApγ(Hˉnd), for multiindices γ=(γ1,…,γK(n,d)),γj∈Nn, chosen according to the finite nondegeneracy of Hnd given in the proof of Lemma 2, which can be seen as follows: One has that
[TABLE]
where cεγj∈C involves some constants, derivatives of Qˉ and terms of the form Qˉ−mγj,ε for some mγj,ε∈N. Since the first row of Apγ(Hˉnd/Qˉ) consists of Hˉnd/Qˉ, using elementary row operations one can see that the rank of Apγ(Hˉnd/Qˉ) agrees with the rank of Apγ(Hˉnd).
Now it is possible to prove the equivalence of (a) and (b). Assume (a), then there is k0∈N, such that H is (k0,s)-degenerate at p. This means that dimCEk0′(p)=N′−s and hence, for any β=(β1,…,βr),βj∈Nn and r∈N, the kernel of the matrix Apβ(Hˉ) is at least of dimension s.
Consider γ=(γ1,…,γK(n,d)),γj∈Nn according to the finite nondegeneracy of Hnd given in the proof of Lemma 2. Let Xj for 1≤j≤s be linearly independent vectors in the kernel of Apγ(Hˉ).
By taking β=γ in (8), it follows that V(p)Xj∈kerApγ(Hˉnd/Qˉ). Since Hnd is finitely nondegenerate in S2n−1 and by the fact that rkApγ(Hˉnd/Qˉ)=rkApγ(Hˉnd), it follows that Xj∈kerV(p). Hence dimkerV(p)≥s.
Assume that dimkerV(p)=s′>s, i.e. there are linearly independent vectors Yj∈kerV for 1≤j≤s′. Since H is of degeneracy s there exists a sequence of multiindices δ=(δ1,…,δq),δj∈Nn and q∈N, such that the kernel of Apδ(Hˉ) is precisely of dimension s. Then Apδ(Hˉnd/Qˉ)V(p)Yj=0 and using (8) with β=δ, it follows that Apδ(Hˉ)Yj=0, i.e. Yj∈kerApδ(Hˉ) for 1≤j≤s′, which is a contradiction to dimkerApδ(Hˉ)=s.
For the other direction, assume (b) and argue similarly: If dimkerV(p)=s, consider any sequence of multiindices ϵ=(ϵ1,…,ϵt) for ϵj∈Nn and t∈N. Let Xj for 1≤j≤s be linearly independent vectors belonging to kerV(p). By (8) it follows that Xj∈kerApϵ(Hˉ). Thus, the degeneracy of H is at least s.
Assume the degeneracy of H is equal to s′>s. Argue as in the proof of the sufficient direction to conclude that dimkerV(p)≥s, which is a contradiction.
The last statement follows immediately from the above shown equivalence.
∎
Example 5**.**
For each ℓ≥0 the map Gℓ is finitely nondegenerate at p∈S3: In this case the reflection matrix V is the following (2ℓ+2)×(ℓ+2)-matrix:
[TABLE]
where \prescripttH~k=(zk,(1k)zk−1w,…,wk)∈Ck+1, blank spaces are filled up with zeros, D1 is the (2ℓ+2)×(2ℓ+2)-diagonal matrix whose nonzero entries are the reciprocals of the coefficients of H2ℓ+2 and D2 is the (ℓ+2)×(ℓ+2)-diagonal matrix which consists of the coefficients of Gℓ on the diagonal. It follows that V is of full rank on S3.
Example 6**.**
The map H(z,w)=(z4,z3w,3zw,w3), which sends S3 into S7, is listed in [DAngelo88b]. The reflection matrix is given by
[TABLE]
which is of full rank if and only if w=0 and if w=0 the kernel is of dimension 1, hence by Proposition 4 the map is finitely nondegenerate for w=0 and of degeneracy 1 when w=0. A direct computation (as in Definition 3) shows that the map is 3-nondegenerate at points {z=0,w=0}∩S3 and 4-nondegenerate when {z=0,∣w∣=1}. If w=0 and ∣z∣=1, the map is (3,1)-degenerate.
The following example gives a map, for which the set of points in S3 where the map is 2-degenerate consists of one isolated point.
Example 7**.**
The map H(z,w)=\bigl{(}(az-bzw)z,(az-bzw)w,\bar{b}z+\bar{a}zw,w^{2}\bigr{)}, for a,b∈C satisfying ∣a∣2+∣b∣2=1, sends S3 into S7. The matrix V is given by
[TABLE]
where D is the 4×4-diagonal matrix whose nonzero entries are the reciprocals of the coefficients of H3. Assuming a=b=21, it holds that V is of full rank if Y1:={z=0,w=0}∩S3 and the complex dimension of the kernel is 1 if Y_{2}\coloneqq\bigl{\{}\{z=0,w\neq 1\}\cup\{z\neq 0,w=0\}\bigr{\}}\cap S^{3}. The kernel of V is of complex dimension 2 at p0:=(0,1)∈S3. It can be shown by a direct computation (as in Definition 3) that H is 3-nondegenerate in Y1, (2,1)-degenerate in Y2 and (1,2)-degenerate at p0.
The following result gives conditions to guarantee that a sphere map is finitely degenerate:
Corollary 1**.**
If a rational sphere map H:S2n−1→S2m−1 of degree d satisfies K(n,d)<m, then H is finitely degenerate at any p∈S2n−1. In particular the map is holomorphically degenerate.
Proof.
The K(n,d)×m-matrix V satisfies rkV≤min(K(n,d),m)=K(n,d) on S2n−1.
If H would be finitely nondegenerate at p∈S2n−1, by Proposition 4, V would be injective at p, hence rkV=m at p, a contradiction. By Proposition 3 it follows that H is holomorphically degenerate. ∎
Example 8**.**
The map H(z,w)=(z,cos(t)w,sin(t)zw,sin(t)w2),t∈[0,2π), sends S3 to S7 and is holomorphically degenerate by Corollary 1. The reflection matrix V is given as follows:
[TABLE]
If sin(t)=0, then X(z,w)=(0,1,−cot(t)z,−cot(t)w) is a holomorphic vector field tangent to S7 along the image of H.
One can check that if cos(t),sin(t)=0 the map is of degeneracy 1 for z=0 and of degeneracy 2 if z=0. If cos(t)=0 and sin(t)=0 the map is of degeneracy 2 and when cos(t)=0 the map is 1-degenerate.
The set of points where the map is finitely degenerate can be described by using Proposition 4:
Corollary 2**.**
Let H:S2k−1→S2m−1 be of generic degeneracy s in S2k−1. The set of points in S2k−1, where H is of degeneracy s′>s is contained in a complex algebraic variety intersecting S2k−1.
Proof.
The set D of points where H is of degeneracy s′>s is the complement Y of the set where H is of generic degeneracy s, which is given by the union of the zero sets of any minor of V of size strictly less than rkV. Since V consists of holomorphic polynomial entries, Y is a complex algebraic variety and, by Proposition 4, agrees with D.
∎
Note that Proposition 4 shows that Corollary 1 and Corollary 2 are equivalent to [DAngelo03]*Corollary 4.4 and [DAngelo03]*Corollary 4.2 respectively.
5. The X-variety of a sphere map
In this section sufficient and necessary conditions in terms of nondegeneracy conditions are provided to guarantee that the X-variety of a sphere map satisfies certain properties, such as agreeing with the graph of the map or being an affine bundle.
First, the general definition of the X-variety of a map is repeated for the reader’s convenience, see [Forstneric89] and [DAngelo03]:
Definition 8**.**
Let M⊂CN and M′⊂CN′ be real-analytic hypersurfaces and H:M→M′ be a real-analytic CR map. Let p∈M and p′=H(p). Assume M∩U={Z∈U:ρ(Z,Zˉ)=0} and M′∩U′={Z′∈U′:ρ′(Z′,Zˉ′)=0}, where U⊂CN and U′⊂CN′ are neighborhoods of p and p′ and ρ and ρ′ are real-analytic defining functions for M and M′ defined in U and U′ respectively. Define the following set
[TABLE]
which is called the X-variety of H near p∈M.
Since H maps M into M′ it follows that (Z,H(Z))∈XH, i.e. the graph of H is contained in XH. In [DAngelo03]*Theorem 4.1 it is shown in the case when M⊂Cn and M′⊂Cm are unit spheres that for any z=0 it holds that (z,z′)∈XH if and only if z′−H(z)∈kerV(z). XH has an exceptional fiber at p∈S2n−1 if the dimension of the fiber {p′∈CN′:(p,p′)∈XH} exceeds its generic value. In [DAngelo03]*Corollary 4.2 it is argued that the set of points over which XH has an exceptional fiber agrees with the set of points p∈S2n−1 where the rank of V(p) drops.
Moreover, in [DAngelo03]*Theorem 4.1 the following properties of XH are proved:
(a)
XH is an affine bundle over Cn∖{0} if and only if the rank of V(z) is constant for each z=0 in the domain of H.
(b)
XH equals the graph of H if and only if, for each z=0 in the domain of H, the null space of V(z) is trivial.
Using the facts from Section 4, relating nondegeneracy conditions and rank conditions of the reflection matrix, the following characterizations hold:
Theorem 3**.**
Let H:S2n−1→S2m−1 be a real-analytic CR map. Then the following statements hold:
(a)
XH* is an affine bundle over Cn∖{0} if and only if H is of finite degeneracy s at any point of S2n−1.*
(b)
XH* equals the graph of H if and only if H is finitely nondegenerate at any point of S2n−1.*
(c)
XH* has an exceptional fiber at p∈S2n−1 if and only if H is not of generic degeneracy s(H) at p∈S2n−1.*
Proof.
The proofs of (a) and (b) follow from Proposition 4 and the characterizations from [DAngelo03]*Theorem 4.1 stated above. Since the rank conditions involved are constant on S2n−1, they also hold in a neighborhood of S2n−1, to which H extends.
For (c) note that the points where H is of generic degeneracy s(H) (see the remark after Definition 3) form an open dense subset S of S2n−1. Hence in the complement of S the degeneracy of H is strictly bigger and by Proposition 4 the rank of the reflection matrix is strictly smaller. Thus, the complement of S is precisely the set where XH possesses an exceptional fiber.
∎
6. Infinitesimal deformations of sphere maps
In this section infinitesimal deformations of rational sphere maps are studied. It turns out that similarly as in the case of sphere maps, where each sphere map is related to the homogeneous sphere map by tensoring, infinitesimal deformations of a sphere map are related to infinitesimal deformations of the homogeneous sphere map by the reflection matrix.
Lemma 5**.**
Let H=QP:U→S2m−1 be a holomorphically nondegenerate rational sphere map of degree d, where U is a neighborhood of S2k−1. Then each X∈hol(H) is of the form X=QX′, where X′ is a holomorphic polynomial of degree at most 2d satisfying Re(X′⋅Pˉ)=0 on S2k−1.
Proof.
Let H be given as in the assumption of the lemma, where P=(P1,…,Pm) and Q:U→C with Q=0 on U, a neighborhood of S2k−1. Then ∣Q∣2Re(X⋅Hˉ)=Re(QX⋅Pˉ). Set X′:=QX. Considering homogeneous expansions of X′=∑ℓ≥0X′ℓ and P=∑j=0dPj one obtains the following equation:
[TABLE]
After setting Z↦Zeit for t∈R collect the Fourier coefficient of degree d+ℓ0 for ℓ0≥1 to get:
[TABLE]
By the holomorphic nondegeneracy of H this implies that X′ℓ≡0 for ℓ≥2d+1, i.e. degX′≤2d.
∎
Denote by Pd(k,m) the space of complex polynomial maps from Ck to Cm of degree d with dimRPd(k,m)=2m∑ℓ=0d(ℓℓ+k−1). The following definition is justified by the previous Lemma 5 and in fact hol(H) can be identified with a space of polynomial maps.
Definition 9**.**
Let H=QP:U→S2m−1 be a holomorphically nondegenerate rational sphere map of degree d, where U is a neighborhood of S2k−1. Define dimhol(H):=dimR{X′∈P2d(k,m):QX′∈hol(H)}.
In [DAngelo91] and [DAngeloBook]*section 5.1.4, Theorem 4 it is shown that for any polynomial sphere map of degree d if one applies finitely many tensoring operations to it one obtains the homogeneous sphere map of degree d. Moreover in [DAngeloBook]*section 5.1.4, Theorem 3 it is shown that the homogeneous sphere map is up to a unitary transformation unique among all polynomial and homogeneous sphere maps. The following theorem gives the corresponding results in terms of infinitesimal deformations.
Theorem 4**.**
*Let H:S2n−1→S2m−1 be a holomorphically nondegenerate rational map of degree d, then dimhol(H)≤dimhol(Hnd).
If H:S2n−1→S2m−1 is a polynomial map of degree d, it holds that dimhol(H)=dimhol(Hnd) if and only if H is unitarily equivalent to Hnd.*
Proof.
Let H=QP:S2n−1→S2m−1 be a rational map with Q=0 on S2n−1.
Consider as in Definition 4 the matrix V:Cm→CK(n,d) whose entries are holomorphic polynomials in z∈Cn. Then it holds on S2n−1 that ∣Q∣2X⋅Hˉ=VX⋅Hˉnd for X∈Cm as in (7). Thus on S2n−1 one obtains,
[TABLE]
By Lemma 5 there are polynomials X1′,…,Xk′∈P2d(n,m) such that {Xj=QXj′:1≤j≤k} is a basis of hol(H). From Proposition 3 it follows that {VXj:1≤j≤k} is a set of linearly independent polynomials in hol(Hnd) which implies k≤dimhol(Hnd).
To show the nontrivial implication of the second claim, assume that H=P is polynomial of degree d and dimhol(P)=dimhol(Hnd).
By Proposition 3, since the reflection matrix V is injective on a dense, open subset S of S2n−1 as a map from hol(P) to hol(Hnd), it follows by the rank theorem that dimV(hol(P))=dimhol(P). Using the assumption dimhol(P)=dimhol(Hnd) this implies that V is invertible as a map from hol(P) to hol(Hnd), for z∈S. Thus, for any Y∈hol(Hnd) there exists X∈hol(P) with VX=Y, such that on S, the following equation holds:
[TABLE]
Choosing Y=iHnd∈aut(Hnd)⊂hol(Hnd) in the previous equation, it becomes after using Hnd⋅Hˉnd=1 on S2n−1:
[TABLE]
Note that the matrix B:=V−1 depends holomorphically on z∈U, where U is an open set in Cn, such that U∩S2n−1=S. Consider the homogeneous expansion of B=∑k≥0Bk and P=∑ℓ=0dPℓ. Take z↦eitz in (10), and collect Fourier coefficients. Looking at the constant Fourier coefficient we see that
[TABLE]
on S. This equation can be rewritten as in the proof of [DAngeloBook]*section 5.1.4, Theorem 3 as follows,
[TABLE]
such that the holomorphic nondegeneracy of Hnd implies that Hnd=\prescripttBˉ0Pd.
By some linear algebra this shows that Pd=UHnd, where U is a unitary matrix. Write P=UHnd+F, where F is a holomorphic polynomial of degree d−1.
Since P maps S2n−1 to S2K(n,d)−1 it holds on S2n−1 that,
[TABLE]
hence after setting F′=\prescripttUˉF, one obtains
[TABLE]
Consider z↦eitz and a homogeneous expansion of F′=∑j=0d−1Fj′ and collect the coefficient of eidt to get that Hnd⋅Fˉ0′=0, hence by the holomorphic nondegeneracy of Hnd one obtains F0′=0. Proceed inductively to show that Fk′=0 for k≤d−1. Assume that Fℓ′=0 for all 0≤ℓ≤k−1. Collect the coefficient of ei(d−k)t in (11) to obtain that,
[TABLE]
which, by using the induction hypothesis and the holomorphic nondegeneracy of Hnd, implies that Fk′=0. In total one obtains that P is unitarily equivalent to Hnd in S, hence they are equivalent everywhere on S2n−1. ∎
One has the following inequality for the dimension of the space of infinitesimal deformations, when the tensor product is involved.
Corollary 3**.**
Let A⊆Cm be a complex subspace, H:S2n−1→S2m−1 and G:S2n−1→S2ℓ−1 be non-constant real-analytic CR maps. Assume F=E(A,G)H. Then dimhol(H)≤dimhol(F) and if H is holomorphically nondegenerate and equality holds if and only if F=H.
Proof.
If F is holomorphically degenerate, by Proposition 2, the inequality is satisfied. Assume that F is holomorphically nondegenerate, then the same holds for H by Lemma 4.
Instead of using V as in the proof of Theorem 4, one considers V a linear map defined by V(X):=T(A,G)X. Then X⋅Hˉ=V(X)⋅Fˉ, i.e. X∈hol(H)⇔V(X)∈hol(F).
It holds that if there exists Y∈hol(H) with V(Y)=0 on S2n−1, then 0=V(Y)⋅Fˉ=Y⋅Hˉ on S2n−1, which implies, since H is holomorphically nondegenerate, that Y≡0.
From this it follows that the set {V(Xj):1≤j≤k}, for X1,…,Xk a basis of hol(H), is linearly independent in hol(F), which gives the claimed inequality.
For the equality, assume that dimhol(F)=dimhol(H)<∞. Then dimhol(H)=dimV(hol(H))≤dimhol(F)=dimhol(H), which implies, as in the proof of Theorem 4, that on S2n−1 the map V, as a map from hol(H) to hol(F), is invertible.
Using a similar argument as in the proof of Theorem 4 (replacing V by V~, Hnd by F and P by H and using X⋅Hˉ=V~(X)⋅Fˉ) it follows that H and F are unitarily equivalent, which can only happen, when the complex subspace A is trivial. This concludes the proof.
∎
The remainder of this section is a collection of lemmas concerning some properties of VH and its transpose and provide sufficient and necessary conditions for infinitesimal rigidity in terms of VH and its adjoint.
Proposition 5**.**
For any polynomial map H:S2n−1→S2m−1 of degree d one has VHH=Hnd and H=\prescripttVˉHHnd on S2n−1.
Proof.
Using the matrix VH from Definition 4 the following holds on S2n−1:
[TABLE]
for all X∈Cm. Taking X=H in the above equation and using H⋅Hˉ=1=Hnd⋅Hˉnd on S2n−1, it holds that,
[TABLE]
on S2n−1. Note that VHH has holomorphic components such that the holomorphic nondegeneracy of Hnd implies that VHH=Hnd.
For the other identity one has,
[TABLE]
for all X∈Cn, which concludes the proof.
∎
The following example shows that a similar relation as the second identity in Proposition 5 does not hold for infinitesimal deformations in general:
Example 9**.**
Let X be of the form as T1 in Section 2.3 with H being the map
[TABLE]
and α′=(0,0,0,a,0)∈C5. Then, on S3, one has:
[TABLE]
which does not extend holomorphically to a neighborhood of S3.
Lemma 6**.**
Let H:S2n−1→S2m−1 be a polynomial map of degree d.
(a)
It holds that X∈hol(H) if and only if X′:=\prescripttVˉHVHX satisfies Re(X′⋅Hˉ)=0 on S2n−1.
(b)
If Y∈hol(Hnd) has the property that \prescripttVˉHY is holomorphic, then Y∈VH(hol(H)).
In (b) the necessary direction need not be true as Example 9 shows.
which shows (a).
In (b) assume X:=\prescripttVˉHY is holomorphic. By Proposition 5 one has,
[TABLE]
on S2n−1 and taking the real part shows that X∈hol(H). Consider the above equation and note that one has X⋅Hˉ=VHX⋅Hˉnd, such that, since VHX is holomorphic, the holomorphic nondegeneracy of Hnd implies Y=VHX∈VH(hol(H)).
∎
Proposition 6**.**
Let H:S2n−1→S2m−1 be a polynomial map of degree d.
(a)
If the map H is infinitesimally rigid then \prescripttVˉHhol(Hnd)∩hol(H)=\prescripttVˉHVHaut(H)∩hol(H).
(b)
Assume that the map H is holomorphically nondegenerate. If \prescripttVˉHhol(Hnd)=\prescripttVˉHVHaut(H), then H is infinitesimally rigid.
Proof.
To prove (a), assume X∈\prescripttVˉHhol(Hnd)∩hol(H) such that there exists Y∈hol(Hnd) with X=\prescripttVˉHY. Thus, \prescripttVˉHY∈hol(H) (in particular \prescripttVˉHY is holomorphic) and by Lemma 6 (b) it holds that Y∈VHhol(H)=VHaut(H) by the infinitesimal rigidity of H. In total this shows that X∈\prescripttVˉHVHaut(H)∩hol(H).
For the other implication, note that if X∈\prescripttVˉHVHaut(H)∩hol(H), then, since VHaut(H)⊂hol(Hnd), it follows that X∈\prescripttVˉHhol(Hnd)∩hol(H).
For (b) let X∈hol(H), then VHX∈hol(Hnd) and hence \prescripttVˉHVHX∈\prescripttVˉHhol(Hnd)=\prescripttVˉHVHaut(H). Thus there exists T∈aut(H), such that AX=AT for A:=\prescripttVˉHVH. Since H is holomorphically nondegenerate it holds that the K(n,d)×m-matrix VH is injective on a dense open subset S of S2n−1 (see Proposition 3), hence one has rkVH=m in S. Since VH consists of holomorphic entries in z, this means that VH is of rank m in an open set U such that U∩S2n−1=S. It follows that the m×m-matrix A is of full rank m in U, and thus X=T in U. Since X and T are holomorphic they agree in Cn. This shows that X∈aut(H).
∎
7. Infinitesimal deformations of the homogeneous sphere map
In this section the dimension of the space of infinitesimal deformations of the homogeneous sphere map Hnd (see Definition 5) is computed.
Theorem 5**.**
The real dimension of the space of infinitesimal deformations of Hnd is given by (d2d+n)K(n,d)2.
Proof.
Define the map H^nd(z)=(zα)∣α∣=d∈CK(n,d) and write Y=DndX∈hol(Hnd), where Dnd is given as in the hypothesis. Then X has to satisfy the following equation on S2n−1,
[TABLE]
In the above equation consider the homogeneous expansion of X=∑k≥0Xk, where Xk∈CK(n,d) is a homogeneous polynomial in z of order k≥0. Change coordinates via z↦eiθz for θ∈R as in [DAngelo88b]*Lemma 16 to obtain after shifting indices, on S2n−1:
[TABLE]
This implies Xℓ≡0 for ℓ≥2d+1, such that −d≤s,t≤d. Collect Fourier coefficients of eirθ for −d≤r≤d in (12) such that for X∈hol(Hnd) it is enough to study the solutions of the following equations:
[TABLE]
on S2n−1. For r=0 the equation is real and will be treated below. Fix 1≤r≤d and homogenize (13) as in [DAngelo91]*section II by multiplying the second term with ∥z∥2r, such that the following equation holds for all z∈Cn:
[TABLE]
Write Xd−r=Bnd,rH^nd−r, where Bnd,r is a K(n,d)×K(n,d−r)-matrix and write zαH^nd=Cnd,αH^nd+r, where Cnd,α is a K(n,d)×K(n,d+r)-matrix whose entries consist of [math]’s or 1’s. Rewrite the second term of (14) as
[TABLE]
Write zαH^nd−r=Dnd,αH^nd−r, where Dnd,α is a K(n,d)×K(n,d−r)-matrix whose entries consist of [math]’s or 1’s, such that using the holomorphic nondegeneracy of Hnd, one obtains
[TABLE]
Setting Xd+r=And,rH^nd+r, where And,r is an K(n,d)×K(n,d+r)-matrix, (15) gives:
[TABLE]
This implies that the solutions of (13) depend on the entries of Bnd,r for 1≤r≤d. The number of real entries in Bnd,r for 1≤r≤d is given by
which is a homogeneous equation and hence holds on Cn. Writing Xd=Bnd,0H^nd, where Bnd,0 is a K(n,d)×K(n,d)-matrix, in (17) shows that \prescripttBnd,0+Bˉnd,0=0. Hence Bnd,0 depends on K(n,d)2 real parameters. Moreover the stabilizer of Hnd consists of Sn2 and Sn3 and the remaining elements of aut(Hnd) coming from hol(S2n−1) appear in (13) for r=1 and have been taken into account in (16).
In total, adding (16) and the number of real solutions of (13) for r=0 gives the claimed dimension of hol(Hnd), which finishes the proof.
∎
For n=2 write H2d(z,w)=(a1dzd,a2dzd−1w,…,ad+1dwd), where (akd)2=(k−1d) for 1≤k≤d+1, such that dimRhol(H2d)=(d+1)3 and any X∈hol(H2d) is a real linear combination of infinitesimal deformations Nd,rm,k of the following form:
[TABLE]
where 0≤r≤d, Dd+1 is the (d+1)×(d+1)-diagonal matrix with entries 1/akd for 1≤k≤d+1, Cd,rm,k=(cij) is a (d+1)×(d+1−r)-matrix with cmk∈{1,i} for 1≤m≤d+1 and 1≤k≤d+1−r and all other entries are [math] and 0j denotes the zero-vector in Cj. To illustrate which nontrivial infinitesimal deformations for H2d appear, a list for d=2,3 is given. Note that if N is a nontrivial infinitesimal deformation of H2d, then N~=ϕ′∘N∘ϕ is again a nontrivial infinitesimal deformation of H2d different from N, where ϕ(z,w)=(w,z) and
[TABLE]
Below half of all nontrivial infinitesimal deformations of H2d are listed as rows of the matrix Y2d. The remaining nontrivial elements of hol(H2d) can be deduced by applying ϕ and ϕ′ to each row of Y2d.
[TABLE]
where a,b∈C, which are also listed in [dSLR17]*Example 1.
[TABLE]
where a,b,c,d,e,f,g,j,k∈C.
Using the fact that for a sphere map H and any X∈hol(H) one has VHX∈hol(Hnd) (see (9) in the proof of Theorem 4) it is possible to compute hol(H) from a description of hol(Hnd): By considering each element of hol(Hnd) one needs to check if it can be written as VHY, where Y is a holomorphic vector field, such that Y∈hol(H). The vector fields obtained in this way span hol(H).
Example 11**.**
The map H(z,w)=(z,zw,w2) from S3 to S5 is of finite degeneracy 1 in S3∩{z=0} and 2-nondegenerate otherwise. Its infinitesimal stabilizer consists of S23.
It can be checked that H is infinitesimally rigid.
Example 12**.**
For the family of sphere maps Gℓ for ℓ≥1 there are infinitesimal rigid maps and some maps which admit nontrivial infinitesimal deformations:
One can compute that for G1:S3→S5 the space hol(G1) only consists of trivial infinitesimal deformations, see also [DAngelo03]. The map G4:S3→S11 given by
[TABLE]
where c1=c4=3,c2=33 and c3=30 is not infinitesimally rigid, since the vector
[TABLE]
corresponds to a nontrivial infinitesimal deformation of G4. This can be verified by showing that X is not of the form as the trivial infinitesimal deformation given in Section 2.3.
Some of the nontrivial infinitesimal deformations of Hnd originate from curves passing through the map as the following example shows: In the following a family of finitely nondegenerate rational sphere maps is constructed, which contains the homogeneous sphere map Hnd for d odd. It is well-known that families of sphere maps exist, see the examples in [DAngelo88a] and [FHJZ10]*Examples 4.1, 4.2, which motivated the construction. See also [DL16] for a study of homotopies of sphere maps.
Theorem 6**.**
For k≥1 the map H22k+1:S3→S2k+2 is not locally rigid. More precisely, there exists a family Fsk:S3→S2k+2 of (2k+1)-nondegenerate rational maps, where s∈R is sufficiently close to [math], with F0k=H22k+1 and each Fsk is not equivalent to H22k+1 for s=0.
Proof.
Consider for s∈R the map Ts=(Ts1,Ts2):S3→S3 given by
[TABLE]
such that T0(z,w)=(z,w), which is an automorphism of S3 when s=1. Define cℓ:=(ℓ2k+1) and note that ck=ck+1. Set
[TABLE]
It holds for all s that Fsk maps S3 into S2k+2, since it originates from H22k+1 by applying the inverse of tensoring to the (k+1)-th and (k+2)-th component using the map (z,w)↦(z,w), and then tensoring the (k+1)-th component of the resulting map with Ts.
Furthermore F0k=H22k+1 and since F0k is (2k+1)-nondegenerate by Lemma 2, the same holds for each map Fsk for s sufficiently close to [math].
The remaining step is to show that for s sufficiently close to [math], when s=0 the map Fsk is not equivalent to a polynomial sphere map (in particular H22k+1). To see this apply the polynomiality criterion of Faran–Huang–Ji–Zhang [FHJZ10]*Remark 2.3 (A). More precisely, write Fsk=QP with P=(P1,…,P2k+2) and Q being the denominator of Ts, and d:=degFsk=max{degP,degQ}=2k+1. Consider the map
[TABLE]
where r1:=s(s−2) and r2:=r1+2. Write F^=(F^1,…,F^d,Q^), then Fsk is equivalent to a polynomial map if and only if there exist a1,a2,A1,…,Ad∈C and C∈C∖{0} such that
[TABLE]
The claim is that under the assumption s=0 the equation (18) has no solution. Comparing the coefficient of z2td−2 one obtains that a1=0. Then the coefficient of ztd−1 gives r1=0, which cannot be satisfied for 0=s<2. This finishes the proof.
∎
Note that for k=1 the vector dsd∣s=0Fs1 is a nontrivial infinitesimal deformation of H23 from Example 10, when the parameter k∈C used there is taken to be real.