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On the topology of the Milnor boundary for real analytic singularities

R. Araújo dos Santos A. Menegon M. Ribeiro J. Seade  and  I. D. Santamaria Guarín
Abstract.

We study the topology of the boundaries of the Milnor fibers of real analytics map-germs f:(M,0)(K,0)f:(\mathbb{R}^{M},0)\to(\mathbb{R}^{K},0) and fI:=ΠIf:(M,0)(I,0)f_{I}:=\Pi_{I}\circ f:(\mathbb{R}^{M},0)\to(\mathbb{R}^{I},0) that admit Milnor’s tube fibrations, where ΠI:(K,0)(I,0)\Pi_{I}:({\mathbb{R}}^{K},0)\to({\mathbb{R}}^{I},0) is the canonical projection for 1I<K.1\leq I<K. For each II we prove that the Milnor boundary FI\partial F_{I} is given by the double of the Milnor tube fiber FI+1.F_{I+1}. We prove that if KI2K-I\geq 2, then the pair (FI,Ff)(\partial F_{I},\partial F_{f}) is a generalized (KI1)(K-I-1)-open-book decomposition with binding Ff\partial F_{f} and page FfFfF_{f}\setminus\partial F_{f} - the interior of the Milnor fibre FfF_{f} (see the definition below). This allows us to prove several new Euler characteristic formulae connecting the Milnor boundaries Ff,\partial F_{f}, FI,\partial F_{I}, with the respectives links f,I,\mathcal{L}_{f},\mathcal{L}_{I}, for each 1I<K,1\leq I<K, and a Lê-Greuel type formula for the Milnor boundary.

1. Introduction

One of the most active and challenging areas in singularity theory is the study of non-isolated singularities of complex spaces. For instance, if f:(n,0)(,0)f:(\mathbb{C}^{n},0)\to(\mathbb{C},0) is a holomorphic germ of function with non-isolated critical point, the degeneration process of the non-critical levels to the non-isolated singularity hypersurface defined by ff is still not well-understood, unlike the isolated singularity case.

One approach to this problem is to study such degeneration over a small sphere around the origin. In other words, one tries to understand the topology of the boundary of the Milnor fiber and how it degenerates to the link of ff. This problem has been attacked by several authors like Siersma [40, 41], Nemethi-Szilard [33], Michel-Pichon [29, 30, 31], Bobadilla-Menegon [16], Menegon-Seade [28] and Aguilar-Menegon-Seade [1].

The corresponding understanding for real analytic singularities is still very poor. Although one can define a Milnor fibration for many classes of real analytic germs of mapping f:(M,0)(K,0)f:(\mathbb{R}^{M},0)\to(\mathbb{R}^{K},0), not much is known about the topology of the corresponding Milnor fiber or the link of ff (see [34, 20, 28, 25, 21] for some results), and even less about the boundary of such objects.

The first part of this paper aims to introduce a new perspective to deal with such problem, inspired mainly by [14, 3, 27]. The idea is to relate the topology of the boundary of the Milnor fiber of ff, denoted by Ff\partial F_{f}, with the boundary of the Milnor fiber of the composition fIf_{I} of ff with some projection (K,0)(I,0)(\mathbb{R}^{K},0)\to(\mathbb{R}^{I},0), which we denote by FI\partial F_{I}. As a result, in Section 3 we prove that for KI2K-I\geq 2 there is a generalized open-book decomposition

fKIfKI:FIFfSKI1,\dfrac{f_{K-I}}{\|f_{K-I}\|}:\partial F_{I}\setminus\partial F_{f}\to S^{K-I-1}\,,

where fKIf_{K-I} is the composition of ff with the projection (K,0)(KI,0)(\mathbb{R}^{K},0)\to(\mathbb{R}^{K-I},0). The particular case 0KI10\leq K-I\leq 1 and the case of a complex ICIS (M+K,0)(K,0)({\mathbb{C}}^{M+K},0)\to({\mathbb{C}}^{K},0) are analyzed.

On the other hand, the understanding of the topology of the boundary of the Milnor fiber of the function-germ fIf_{I} also provides a tool to better understanding the topology of the Milnor fiber of the map-germ ff itself. In fact, in Section 4 we use the aforementioned open-book decomposition to obtain some formulae relating the Euler characteristics of FI\partial F_{I}, FfF_{f} and the link I\mathcal{L}_{I} of fIf_{I}, for I=1,,KI=1,\dots,K.

Finally, in the last section of the article we use those Euler characteristic formulae to get a hint on the possible topological behaviour of real analytic map-germs on an odd number of variables and how similar or different it can be when compared with the complex setting.

2. Notations and basics definitions

Let f:(M,0)(K,0),f=(f1,,fK)f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0),f=(f_{1},\ldots,f_{K}) be an analytic map germ and consider the following diagram

(1) (M,0){({\mathbb{R}}^{M},0)}(K,0){({\mathbb{R}}^{K},0)}(I,0){({\mathbb{R}}^{I},0)}(KI,0){({\mathbb{R}}^{K-I},0)}f\scriptstyle{f}fKI\scriptstyle{f_{K-I}}fI\scriptstyle{f_{I}}ΠKI\scriptstyle{\Pi_{K-I}}ΠI\scriptstyle{\Pi_{I}}

where the projections ΠI(y1,,yK)=(y1,,yI)\Pi_{I}(y_{1},\ldots,y_{K})=(y_{1},\ldots,y_{I}) and ΠKI(y1,,yK):=(yI+1,,yK),\Pi_{K-I}(y_{1},\ldots,y_{K}):=(y_{I+1},\ldots,y_{K}), fI=ΠIff_{I}=\Pi_{I}\circ f and fKI=ΠKIf.f_{K-I}=\Pi_{K-I}\circ f.

Basic notations and definitions:

The zero locus of ff is defined and denoted by V(f):={f=0},V(f):=\{f=0\}, respectively, V(fI)={fI=0}V(f_{I})=\{f_{I}=0\} and V(fKI)={fKI=0}.V(f_{K-I})=\{f_{K-I}=0\}. Hence,

V(fI)V(f)V(fKI).V(f_{I})\supseteq V(f)\subseteq V(f_{K-I}).

The singular set of ff, denoted by Singf{\rm{Sing\hskip 2.0pt}}f, is defined to be the set of points x(M,0)x\in({\mathbb{R}}^{M},0) such that the rank of the Jacobian matrix df(x)df(x) is lower than KK. Analogously, we define the singular sets SingfI{\rm{Sing\hskip 2.0pt}}f_{I} and SingfKI{\rm{Sing\hskip 2.0pt}}f_{K-I} of FIF_{I} and FKIF_{K-I}, respectively. The discriminant set of ff is then defined by

Discf:=f(Singf).{\rm{Disc\hskip 2.0pt}}f:=f({\rm{Sing\hskip 2.0pt}}f)\,.

The polar set of ff relative to g(x):=x2g(x):=\|x\|^{2} is defined and denoted by Sing(f,g){\rm{Sing\hskip 2.0pt}}(f,g). Analogously, we define Sing(fI,g){\rm{Sing\hskip 2.0pt}}(f_{I},g) and Sing(fKI,g){\rm{Sing\hskip 2.0pt}}(f_{K-I},g).

The next diagram relates the singular and the polar sets:

(2) Sing(fI){{{\rm{Sing\hskip 2.0pt}}(f_{I})}}Sing(fI,g){{{\rm{Sing\hskip 2.0pt}}(f_{I},g)}}Sing(fIfI,g){{{\rm{Sing\hskip 2.0pt}}\left(\dfrac{f_{I}}{\|f_{I}\|},g\right)}}Sing(f){{{\rm{Sing\hskip 2.0pt}}(f)}}Sing(f,g){{{\rm{Sing\hskip 2.0pt}}(f,g)}}Sing(ff,g){{{\rm{Sing\hskip 2.0pt}}\left(\dfrac{f}{\|f\|},g\right)}}Sing(fkI){{{\rm{Sing\hskip 2.0pt}}(f_{k-I})}}Sing(fkI,g){{{\rm{Sing\hskip 2.0pt}}(f_{k-I},g)}}Sing(fkIfkI,g){{{\rm{Sing\hskip 2.0pt}}\left(\dfrac{f_{k-I}}{\|f_{k-I}\|},g\right)}}
Definition 2.1.

We say that a map germ f:(M,0)(K,0),f=(f1,,fK)f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0),f=(f_{1},\ldots,f_{K}) is tame, or satisfies the transversality condition at the origin if

Sing(f,g)V(f)¯Singf{0}\overline{{\rm{Sing\hskip 2.0pt}}(f,g)\setminus V(f)}\cap{\rm{Sing\hskip 2.0pt}}f\subseteq\{0\}

as a germ of set at the origin.

Lemma 2.2.

Let 1IK1.1\leq I\leq K-1. If ff is tame, then fIf_{I} and fKIf_{K-I} are tame as well.

It is well known that the tameness conditions for f,f, fIf_{I} and fKIf_{K-I} induce the following fibrations on the boundary of the closed ball SϵM1:=BϵMS_{\epsilon}^{M-1}:=\partial B_{\epsilon}^{M}:

(3) f|:SϵM1f1(Bη1K{0})Bη1K{0}f_{|}:S_{\epsilon}^{M-1}\cap f^{-1}(B_{\eta_{1}}^{K}\setminus\{0\})\to B_{\eta_{1}}^{K}\setminus\{0\}
(4) fI|:SϵM1fI1(Bη2I{0})Bη2I{0}{f_{I}}_{|}:S_{\epsilon}^{M-1}\cap f^{-1}_{I}(B_{\eta_{2}}^{I}\setminus\{0\})\to B_{\eta_{2}}^{I}\setminus\{0\}
(5) fKI|:SϵM1fKI1(Bη3KI{0})Bη3KI{0}{f_{K-I}}_{|}:S_{\epsilon}^{M-1}\cap f^{-1}_{K-I}(B_{\eta_{3}}^{K-I}\setminus\{0\})\to B_{\eta_{3}}^{K-I}\setminus\{0\}

Moreover, under the extra conditions Discf={0}{\rm{Disc\hskip 2.0pt}}f=\{0\} there also exists the Milnor tube’s fibration is the following sense: there exists ϵ0>0\epsilon_{0}>0 small enough such that for all 0<ϵϵ00<\epsilon\leq\epsilon_{0} there exists 0<η1ϵ0<\eta_{1}\ll\epsilon such that the restriction map

(6) f|:BϵMf1(Bη1K{0})Bη1K{0}f_{|}:B_{\epsilon}^{M}\cap f^{-1}(B_{\eta_{1}}^{K}\setminus\{0\})\to B_{\eta_{1}}^{K}\setminus\{0\}

is a locally trivial smooth fibration, where BϵM,B_{\epsilon}^{M}, respectively BϵK,B_{\epsilon}^{K}, stand for the closed ball in M{\mathbb{R}}^{M} with radius ϵ,\epsilon, centered at origin, respectively in K{\mathbb{R}}^{K} with radius η.\eta.

Hence, for the same reason, we conclude the existence of the Milnor tube fibrations for fIf_{I} and fKI:f_{K-I}:

(7) fI|:BϵMfI1(Bη2I{0})Bη2I{0}{f_{I}}_{|}:B_{\epsilon}^{M}\cap f^{-1}_{I}(B_{\eta_{2}}^{I}\setminus\{0\})\to B_{\eta_{2}}^{I}\setminus\{0\}
(8) fKI|:BϵMfKI1(Bη3KI{0})Bη3KI{0}{f_{K-I}}_{|}:B_{\epsilon}^{M}\cap f^{-1}_{K-I}(B_{\eta_{3}}^{K-I}\setminus\{0\})\to B_{\eta_{3}}^{K-I}\setminus\{0\}

From now on denote by FfF_{f}, FIF_{I} and FKIF_{K-I} the Milnor fibers of the fibrations (6), (7) and (8), respectively, by Ff\partial F_{f}, FI\partial F_{I} and FKI\partial F_{K-I} the fibers of (3), (4) and (5).

Consider the Milnor tube fibration fI|:BϵMfI1(Bη2I{0})Bη2I{0}{f_{I}}_{|}:B_{\epsilon}^{M}\cap f^{-1}_{I}(B_{\eta_{2}}^{I}\setminus\{0\})\to B_{\eta_{2}}^{I}\setminus\{0\} and zBη2I{0}.z\in B_{\eta_{2}}^{I}\setminus\{0\}. Thus the fiber FI=f1(ΠI1(z)).F_{I}=f^{-1}(\Pi_{I}^{-1}(z)).

Denote by DKI=ΠI1(z)(Bη1K{0})D^{K-I}=\Pi^{-1}_{I}(z)\cap(B_{\eta_{1}}^{K}\setminus\{0\}) the (KI)(K-I)-dimensional closed disc given by the intersection of the fiber of projection ΠI:KI\Pi_{I}:{\mathbb{R}}^{K}\to{\mathbb{R}}^{I} with the closed ball Bη1K{0}B_{\eta_{1}}^{K}\setminus\{0\} on the target space of fibration (6).

Thus FI=f1(DKI)F_{I}=f^{-1}(D^{K-I}) and one may consider the restriction map f:FIDKIf:F_{I}\to D^{K-I} which is a smooth surjective proper submersion, and hence a smooth trivial fibration.

Therefore, the following homeomorphism follows FIFf×DKI,F_{I}\approx F_{f}\times D^{K-I}, which is a diffeomorphism after smoothing the corners. On the boundary of the Milnor fiber the following diffeomorphism holds true:

(9) FI(Ff×DKI)(Ff×SKI1).\partial F_{I}\approx(\partial F_{f}\times D^{K-I})\cup(F_{f}\times S^{K-I-1}).

We remark that the next Proposition is in the same vein as [12, Corollary 4].

Proposition 2.3.

Let f:(M,0)(K,0),f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0), M>K2,M>K\geq 2, be a tame map germ with Discf={0}{\rm{Disc\hskip 2.0pt}}f=\{0\} and for 1I<K1\leq I<K consider the composition map fI=ΠIff_{I}=\Pi_{I}\circ f where ΠI:KI\Pi_{I}:{\mathbb{R}}^{K}\to{\mathbb{R}}^{I} is the projection map. Then the boundary FI\partial F_{I} of the Milnor fiber FIF_{I} is obtained (up to homeomorphism) by the gluing together two disjoint copies of the Milnor fiber FI+1F_{I+1} along the common boundary FI+1.\partial F_{I+1}.

Proof.

The proof follows from the composition

(M,0){({\mathbb{R}}^{M},0)}(I+1,0){({\mathbb{R}}^{I+1},0)}(I,0){({\mathbb{R}}^{I},0)}fI+1\scriptstyle{f_{I+1}}fI=Π^IfI+1\scriptstyle{f_{I}=\widehat{\Pi}_{I}\circ f_{I+1}}Π^I\scriptstyle{\widehat{\Pi}_{I}}

where Π^I(y1,,yI+1)=(y1,,yI)\widehat{\Pi}_{I}(y_{1},\ldots,y_{I+1})=(y_{1},\ldots,y_{I}) and the fact that ff being tame implies the same to fI+1f_{I+1} and fI.f_{I}. In the same manner Discf={0}{\rm{Disc\hskip 2.0pt}}f=\{0\} implies DiscfI+1={0}{\rm{Disc\hskip 2.0pt}}f_{I+1}=\{0\}, DiscfI={0}.{\rm{Disc\hskip 2.0pt}}f_{I}=\{0\}.

Hence, FIFI+1×[1,1]F_{I}\approx F_{I+1}\times[-1,1] and the boundary

(10) FI(FI+1×[1,1])(FI+1×{1,1})\partial F_{I}\approx(\partial F_{I+1}\times[-1,1])\cup(F_{I+1}\times\{-1,1\})
Refer to caption
Figure 1.

Now it is easy to see that the closed manifold FI\partial F_{I} is obtained by the gluing the two disjoint copies of FI+1F_{I+1} given by FI+1×{1}FI+1×{1}F_{I+1}\times\{-1\}\cup F_{I+1}\times\{1\} along the boundaries of the cylinder FI+1×[1,1].\partial F_{I+1}\times[-1,1]. See the Figure (1). Therefore the result follows. ∎

3. Fibration structure on the boundary of the Milnor fiber

From now on we will consider ff tame, Discf={0},{\rm{Disc\hskip 2.0pt}}f=\{0\}, and V(f){0}.V(f)\neq\{0\}. One may adjust the radii η1,\eta_{1}, η2\eta_{2} and η3\eta_{3} in the fibrations (3), (4) and (5) such that FISϵM1f1(Bη1K{0})\partial F_{I}\subset S_{\epsilon}^{M-1}\cap f^{-1}(B_{\eta_{1}}^{K}\setminus\{0\}) and the restriction map fKI:FIKIf_{K-I}:\partial F_{I}\to{\mathbb{R}}^{K-I} is well defined, for any 1I<K.1\leq I<K.

Lemma 3.1.

The restriction map fKI:FIKIf_{K-I}:\partial F_{I}\to{\mathbb{R}}^{K-I} is a smooth submersion.

Proof.

For yBη2I{0}y\in B_{\eta_{2}}^{I}\setminus\{0\} consider FI=SϵM1fI1(y)\partial F_{I}=S_{\epsilon}^{M-1}\cap f_{I}^{-1}(y) and the matrix

A(x):=[dfI(x)dfKI(x)dg(x)].A(x):=\left[\begin{array}[]{c}{\rm{d}}f_{I}(x)\\ {\rm{d}}f_{K-I}(x)\\ {\rm{d}}g(x)\end{array}\right].

By the tameness of ff we have that for all xFIx\in\partial F_{I} the rank of A(x)A(x) is maximal. Hence fKIf_{K-I} is a smooth submersion. ∎

Now since 0KI0\in{\mathbb{R}}^{K-I} is a regular value of fKI:FIKIf_{K-I}:\partial F_{I}\to{\mathbb{R}}^{K-I} by the compactness of FI\partial F_{I} one may choose τ>0\tau>0 small enough and a closed disc DτKIKID^{K-I}_{\tau}\subset{\mathbb{R}}^{K-I} centered at the origin 0KI,0\in{\mathbb{R}}^{K-I}, such that all yDτKIy\in D^{K-I}_{\tau} is a regular value of the restriction map fKI.f_{K-I}.

Hence the restriction map fKI:FIfKI1(DτKI)DτKIf_{K-I}:\partial F_{I}\cap f^{-1}_{K-I}(D^{K-I}_{\tau})\to D^{K-I}_{\tau} is a smooth onto submersion, then a trivial fibration with the fiber diffeomorphic to Ff=FIfKI1(0).\partial F_{f}=\partial F_{I}\cap f_{K-I}^{-1}(0). Therefore,

(11) FIfKI1(DτKI)Ff×DτKI.\partial F_{I}\cap f^{-1}_{K-I}(D^{K-I}_{\tau})\approx\partial F_{f}\times D_{\tau}^{K-I}.

Denote by Tτ(Ff):=Ff×DτKIT_{\tau}(\partial F_{f}):=\partial F_{f}\times D_{\tau}^{K-I} the closed tubular neighbourhood of the embedded submanifold Ff\longhookrightarrowFI.\partial F_{f}\longhookrightarrow\partial F_{I}. See the Figure (2).

Refer to caption
Figure 2.

Then, by (9) it follows that the complement

(12) FIint(Tτ(Ff))Ff×SKI1\partial F_{I}\setminus int(T_{\tau}(\partial F_{f}))\approx F_{f}\times S^{K-I-1}

In this section we will prove that the embedded submanifold Ff\longhookrightarrowFI\partial F_{f}\longhookrightarrow\partial F_{I} yields on the boundary FI\partial F_{I} an interesting structure. For that, let f:(M,0)(K,0),M>K2f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0),M>K\geq 2 and take 1IK21\leq I\leq K-2 as in the beginning of section 2.

We are now ready to introduce the main result of this section. Before that, we introduce an appropriate definition which fits with the type of fibration structure we are able to prove on the boundary of the Milnor fibration.

Following H. Winkelnkemper in [42], A. Ranicki [39]111including the appendix ”The history and applications of open books”, by H. E. Winkelnkemper, E. Looijenga [18], see also [15] and [4, section 3], given MM a smooth manifold MM and NMN\subset M a submanifold of codimension k2k\geq 2 in M,M, suppose that for some trivialization t:T(N)N×Bkt:T(N)\to N\times B^{k} of a tubular neighbourhood T(N)T(N) of NN in M,M, the fiber bundle defined by the composition πt\pi\circ t in the diagram below

T(N)N{T(N)\setminus N}N×(Bk{0}){N\times(B^{k}\setminus\{0\})}Sk1{S^{k-1}}t\scriptstyle{t}πt\scriptstyle{\pi\circ t}π\scriptstyle{\pi}

where π(x,y):=yy,\pi(x,y):=\dfrac{y}{\|y\|}, extends to a smooth locally trivial fiber bundle p:MNSk1;p:M\setminus N\to S^{k-1}; e.i., p|T(N)N=πt.p_{|_{T(N)\setminus N}}=\pi\circ t.

In such a case the pair (M,N)(M,N) above will be called a generalized (k1)(k-1)-open-book decomposition on MM with binding NN and page the fiber p1(y),ySk1.p^{-1}(y),y\in S^{k-1}.

The main result of this section is:

Theorem 3.2.

Let f:(M,0)(K,0),f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0), M>K2,M>K\geq 2, be a tame map germ with Discf={0}.{\rm{Disc\hskip 2.0pt}}f=\{0\}. Then, for each 1I<K1\leq I<K such that KI2,K-I\geq 2, the pair (FI,Ff)(\partial F_{I},\partial F_{f}) is a generalized (KI1)(K-I-1)-open-book decomposition, with binding Ff\partial F_{f} and page FfFfF_{f}\setminus\partial F_{f}- the interior of the Milnor fiber Ff.F_{f}.

Proof.

Consider the restriction map fKI:FIKI.f_{K-I}:\partial F_{I}\to{\mathbb{R}}^{K-I}. It follows by Lemma 3.1 that we may adjust the radii of the fibrations (3), (4) and (5) such that for a small enough radius τ\tau in the diagram below

(13) FIfKI1(DτKI{0}){\partial F_{I}\cap f^{-1}_{K-I}(D^{K-I}_{\tau}-\{0\})}DτKI{0}{D^{K-I}_{\tau}-\{0\}}SKI1{S^{K-I-1}}fKI\scriptstyle{f_{K-I}}fKIfKI\scriptstyle{\dfrac{f_{K-I}}{\|f_{K-I}\|}}ΠR(z)=zz\scriptstyle{\Pi_{R}(z)=\frac{z}{\|z\|}}

the projection fKIfKI\dfrac{f_{K-I}}{\|f_{K-I}\|} is a (trivial) locally fiber bundle, where ΠR\Pi_{R} is the radial projection.

It induces the trivial fibration on the diagonal projection

(14) FIfKI1(SτKI1){\partial F_{I}\cap f^{-1}_{K-I}(S^{K-I-1}_{\tau})}SτKI1{S^{K-I-1}_{\tau}}SKI1{S^{K-I-1}}fKI\scriptstyle{f_{K-I}}fKIfKI\scriptstyle{\dfrac{f_{K-I}}{\|f_{K-I}\|}}ΠR(z)=zz\scriptstyle{\Pi_{R}(z)=\frac{z}{\|z\|}}

Applying again the Lemma 3.1 in the diagram below we get that the horizontal map is a locally trivial fibration over its image; and thus, the diagonal projection is again a locally trivial smooth fibration.

(15) FIfKI1(int(DτKI)){\partial F_{I}\setminus f^{-1}_{K-I}(int(D^{K-I}_{\tau}))}KI{0}{{\mathbb{R}}^{K-I}\setminus\{0\}}SKI1{S^{K-I-1}}fKI\scriptstyle{f_{K-I}}fKIfKI\scriptstyle{\dfrac{f_{K-I}}{\|f_{K-I}\|}}ΠR(z)=zz\scriptstyle{\Pi_{R}(z)=\frac{z}{\|z\|}}

Now we may glue the fibrations (13) and (15) along the fibration (14) to get a smooth projection of a locally trivial fiber bundle

(16) fKIfKI:FIFfSKI1.\dfrac{f_{K-I}}{\|f_{K-I}\|}:\partial F_{I}\setminus\partial F_{f}\to S^{K-I-1}.

Now see that the diffeomorphism of (11) says that the trivialization in the horizontal map of the diagram (9) is given by

FIfKI1(DτKI{0})Ff×(SτKI1×(0,τ]).\partial F_{I}\cap f^{-1}_{K-I}(D^{K-I}_{\tau}-\{0\})\approx\partial F_{f}\times(S_{\tau}^{K-I-1}\times(0,\tau]).

Hence the fiber of the diagonal fibration in the diagram (13) should be diffeomorphiuc to Ff×(0,τ].\partial F_{f}\times(0,\tau].

Refer to caption
Figure 3.

On the other hand, the diffeomorphism (12) assures that the fiber in the diagonal projection of the diagram (15) should be diffeomorphic to Ff.F_{f}. The fiber of the boundary trivial fibration (14) is clearly diffeomorphic to Ff.\partial F_{f}. Therefore, we conclude that the fiber of fibration (16) must be diffeomorphic to the gluing (using the identity diffeomorphism on the boundary) FfFf(Ff×(0,τ])=FfFf.F_{f}\cup_{\partial F_{f}}(\partial F_{f}\times(0,\tau])=F_{f}\setminus\partial F_{f}. See Figure (3) and the proof is finished for KI11,K-I-1\geq 1, i.e., KI2.K-I\geq 2.

Remark 3.3.

Notice that for KI=2K-I=2, a generalized open-book decomposition is an open-book in the usual sense. We also remark that in Theorem 3.2 we assumed KI2;K-I\geq 2; If we consider the case K=IK=I then by convention fKI:=f00f_{K-I}:=f_{0}\equiv 0 and 0={0},{\mathbb{R}}^{0}=\{0\}, so there is nothing to be said. For I=K1,I=K-1, then the study of the restriction function fKI:FIf_{K-I}:\partial F_{I}\to\mathbb{R} reduces to that of Proposition 2.3 and the construction above leads to a "fibration" over S0={1,1}.S^{0}=\{-1,1\}.

3.1. The case of ICIS holomorphic map germ

Let us consider now a holomorphic map germ f=(f1,,fK):(M+K,0)(K,0),K2.f=(f_{1},\ldots,f_{K}):({\mathbb{C}}^{M+K},0)\to({\mathbb{C}}^{K},0),K\geq 2. For 1I<K1\leq I<K consider the complex projections ΠI:(K,0)(I,0),ΠI(z1,,zK)=(z1,,zI),\Pi_{I}:({\mathbb{C}}^{K},0)\to({\mathbb{C}}^{I},0),\Pi_{I}(z_{1},\ldots,z_{K})=(z_{1},\ldots,z_{I}), and ΠKI:(K,0)(KI,0),ΠKI(z1,,zK)=(zI+1,,zK).\Pi_{K-I}:({\mathbb{C}}^{K},0)\to({\mathbb{C}}^{K-I},0),\Pi_{K-I}(z_{1},\ldots,z_{K})=(z_{I+1},\ldots,z_{K}). Thus, the compositions as in the diagram (1) becomes fI:=ΠIf=(f1,,fI)f_{I}:=\Pi_{I}\circ f=(f_{1},\ldots,f_{I}) and fKI:=ΠKIf=(fI+1,,fK).f_{K-I}:=\Pi_{K-I}\circ f=(f_{I+1},\ldots,f_{K}).

If we assume further that ff is ICIS, it is known that Discf:=f(Singf){\rm{Disc\hskip 2.0pt}}f:=f({\rm{Sing\hskip 2.0pt}}f) is a complex hypersurface in K,0{\mathbb{C}}^{K},0 and then for all δ>0\delta>0 small enough the space Bδ2KDiscf,B_{\delta}^{2K}\setminus{\rm{Disc\hskip 2.0pt}}f, where Bδ2KB_{\delta}^{2K} stand for the open ball in K2K.{\mathbb{C}}^{K}\equiv{\mathbb{R}}^{2K}. Then, the space Bδ2KDiscfB_{\delta}^{2K}\setminus{\rm{Disc\hskip 2.0pt}}f is a connected space.

In fact, it was proved by H. Hamm, Lê D. Tràng and by E. Looijenga in [17] that there exists ϵ0>0\epsilon_{0}>0 small enough such that for each 0<ϵϵ00<\epsilon\leq\epsilon_{0} there exists 0<δϵ0<\delta\ll\epsilon such that the projection map

f:B¯ϵ2M+2Kf1(Discf)Bδ2KDiscff:\overline{B}_{\epsilon}^{2M+2K}\setminus f^{-1}({\rm{Disc\hskip 2.0pt}}f)\to B_{\delta}^{2K}\setminus{\rm{Disc\hskip 2.0pt}}f

is a smooth locally trivial fibration. Thus, by the connectedness property of the base space the Milnor fiber FfF_{f} is uniquely defined, up to diffeomorphism.

In addition to that, the ICIS condition is equivalent to the condition SingfVf={0}.{\rm{Sing\hskip 2.0pt}}f\cap V_{f}=\{0\}. Hence, ff is tame according to the Definition 2.1. We may also use the argument of Looijenga in [17] for a "good representative" to guarantee that, up to a linear coordinate change in K,{\mathbb{C}}^{K}, it follows that either map germ fIf_{I} and fKIf_{K-I} are ICIS as well.

The following result is an interesting application of our Theorem 3.2 and also it provides an extension of [7, Proposition 3.2, p. 481]. See also [33, Chapter 3] and compare with [7, Proposition 3.2, p. 481].

Proposition 3.4.

Let f:(M+K,0)(K,0),K>I1,f:(\mathbb{C}^{M+K},0)\to({\mathbb{C}}^{K},0),K>I\geq 1, be a germ of ICIS such that fIf_{I} and fKIf_{K-I} are ICIS as well. Then, the Milnor projection fKIfKI:FIFfS2K2I1\dfrac{f_{K-I}}{\|f_{K-I}\|}:\partial F_{I}\setminus\partial F_{f}\to S^{2K-2I-1} induces a generalized (2K2I1)(2K-2I-1)-open-book decomposition on the boundary FI\partial F_{I} with binding Ff.\partial F_{f}.

Proof.

Since K>IK>I then KI1K-I\geq 1 and the dimension of the sphere on the target space is 2(KI)11.2(K-I)-1\geq 1. Hence, the same ideas in the proof of Theorem 3.2 work in this case. ∎

Remark 3.5.
  1. (1)

    We recall that if one has an isolated complex hypersurface singularity germ, then its link has a canonical contact structure which is Stein fillable (see for instance [35]). These statements extend naturally to the setting we envisage in Proposition 3.4.

  2. (2)

    Still the complex ICIS above, the generalized open-book decomposition also extends with the same proof for the pair links (I,f),(\mathcal{L}_{I},\mathcal{L}_{f}), where I:=fI1(0)SϵM1\mathcal{L}_{I}:=f_{I}^{-1}(0)\cap S_{\epsilon}^{M-1} and f:=f1(0)SϵM1,\mathcal{L}_{f}:=f^{-1}(0)\cap S_{\epsilon}^{M-1}, for all ϵ>0\epsilon>0 smal enough.

4. The Euler characteristic formulae

Let f:(M,0)(K,0),f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0), M>K2,M>K\geq 2, be an analytic map-germ. We will assume along the section that ff is tame and Discf={0}.{\rm{Disc\hskip 2.0pt}}f=\{0\}. Thus, dimFf=MK\dim F_{f}=M-K and dimFf=MK1.\dim\partial F_{f}=M-K-1.

Denote by Ff^=FfFfFf\widehat{F_{f}}=F_{f}\cup_{\partial F_{f}}F_{f} the closed manifold built by gluing two copies of FfF_{f} along the boundary Ff\partial F_{f} using the identity diffeomorphism on Ff.\partial F_{f}. By the additive property of the Euler characteristic we have that χ(Ff^)=2χ(Ff)χ(Ff).\chi(\widehat{F_{f}})=2\chi(F_{f})-\chi(\partial F_{f}). Hence

(17) χ(Ff)={0,if M-K is even.2χ(Ff),if M-K is odd.\chi(\partial F_{f})=\begin{cases}0,&\quad\text{if M-K is even}.\\ 2\chi(F_{f}),&\quad\text{if M-K is odd}.\end{cases}

Applying again the additive Euler characteristic to the diffeomorphism (9) we get

χ(FI)=χ(Ff×DKI)+χ(Ff×SKI1)χ(Ff×SKI1)=\chi(\partial F_{I})=\chi(\partial F_{f}\times D^{K-I})+\chi(F_{f}\times S^{K-I-1})-\chi(\partial F_{f}\times S^{K-I-1})=
=χ(Ff)+χ(Ff).χ(SKI1)χ(Ff).χ(SKI1).=\chi(\partial F_{f})+\chi(F_{f}).\chi(S^{K-I-1})-\chi(\partial F_{f}).\chi(S^{K-I-1}).

Thus, together with (17) it reduces to

(18) χ(FI)={χ(Ff).χ(SKI1),if M-K is even.χ(Ff).χ(SKI),if M-K is odd.\chi(\partial F_{I})=\begin{cases}\chi(F_{f}).\chi(S^{K-I-1}),&\text{if M-K is even}.\\ \chi(F_{f}).\chi(S^{K-I}),&\text{if M-K is odd}.\end{cases}

We may consider the convention χ(S1)=χ()=0\chi(S^{-1})=\chi(\emptyset)=0 and the fact that for the 00-dimensional sphere χ(S0)=χ({1,1})=2.\chi(S^{0})=\chi(\{-1,1\})=2. Then all the above discussion, including the special cases of I=1I=1 and I=KI=K may be summarized as below. By convention, for I=1I=1 we denote F1:=Ff.F_{1}:=F_{f}.

Theorem 4.1.

Let f:(M,0)(K,0),f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0), M>K2,M>K\geq 2, be an analytic map-germ, tame with Discf={0}.{\rm{Disc\hskip 2.0pt}}f=\{0\}. Then:

  1. 1)1)

    χ(FI)=χ(Ff).χ(SMI1),\chi(\partial F_{I})=\chi(F_{f}).\chi(S^{M-I-1}), for any 1IK.1\leq I\leq K.

  2. 2)2)

    Lê-Greuel’s type formula: χ(FI+1)χ(FI)=2(1)MIχ(Ff),\chi(\partial F_{I+1})-\chi(\partial F_{I})=2(-1)^{M-I}\chi(F_{f}), for any 1I<K.1\leq I<K.

  3. 3)3)

    χ(FI)=χ(FI+2),\chi(\partial F_{I})=\chi(\partial F_{I+2}), for any 1I<K1.1\leq I<K-1.

Proof.

The item 1)1) follows from the identity (18). To prove the item 2)2) just exchange II by I+1I+1 in the item 1)1) and take the difference. The item 3)3) is immediate from item 1).1).

4.1. Relating the Euler characteristic of the links

Consider again f:(M,0)(K,0),f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0), M>K2,M>K\geq 2, a tame polynomial map-germ with Discf={0}.{\rm{Disc\hskip 2.0pt}}f=\{0\}. For each 1<IK1<I\leq K the map fI:(M,0)(I,0)f_{I}:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{I},0) admits the Milnor tube fibrations (4) and by restriction it induces the fibrations fI:BϵMfI1(SηI1)SηI1f_{I}:B^{M}_{\epsilon}\cap f_{I}^{-1}(S_{\eta}^{I-1})\to S_{\eta}^{I-1} with Milnor fibers FIF_{I} and the fibration fI:SϵM1fI1(SηI1)SηI1f_{I}:S^{M-1}_{\epsilon}\cap f_{I}^{-1}(S_{\eta}^{I-1})\to S_{\eta}^{I-1} with fiber FI.\partial F_{I}.

Denote by Tη(FI):=BϵMfI1(SηI)T_{\eta}(F_{I}):=B^{M}_{\epsilon}\cap f_{I}^{-1}(S_{\eta}^{I}) the Milnor tube of fIf_{I} and by I:=fI1(0)SϵM1\mathcal{L}_{I}:=f_{I}^{-1}(0)\cap S_{\epsilon}^{M-1} the respective link.

We may consider η\eta small enough such that the sphere SϵM1S_{\epsilon}^{M-1} is homeomorphic to the gluing Tη(fI)Tη(fI)Nη(fI),T_{\eta}(f_{I})\cup_{\partial T_{\eta}(f_{I})}N_{\eta}(f_{I}), where INη(fI):=fI1(BηI)\mathcal{L}_{I}\subset N_{\eta}(f_{I}):=f_{I}^{-1}(B^{I}_{\eta}) is a semi-algebraic neighbourhood that retract to the link I,\mathcal{L}_{I}, as proved by A. Durfee in [13].

Thus,

χ(SϵM1)=χ(Tη(fI))+χ(Nη(fI))χ(Tη(fI))=χ(FI)χ(SI1)+χ(I)χ(FI)χ(SI1).\chi(S_{\epsilon}^{M-1})=\chi(T_{\eta}(f_{I}))+\chi(N_{\eta}(f_{I}))-\chi(\partial T_{\eta}(f_{I}))=\chi(F_{I})\chi(S^{I-1})+\chi(\mathcal{L}_{I})-\chi(\partial F_{I})\chi(S^{I-1}).

Hence,

(19) χ(I)=χ(SM1)χ(Ff)χ(SI1)+χ(FI)χ(SI1)\chi(\mathcal{L}_{I})=\chi(S^{M-1})-\chi(F_{f})\chi(S^{I-1})+\chi(\partial F_{I})\chi(S^{I-1})
Lemma 4.2.

The following holds true:

χ(I)=χ(SM1)+(1)MI1χ(Ff)χ(SI1).\chi(\mathcal{L}_{I})=\chi(S^{M-1})+(-1)^{M-I-1}\chi(F_{f})\chi(S^{I-1}).
Proof.

The proof follows from Proposition 18 and equation (19). ∎

The next result provides in particular a second proof of [14, Proposition 7.1, p. 4861].

Proposition 4.3.

Let f:(M,0)(K,0),f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0), M>K2,M>K\geq 2, be a tame polynomial map-germ with Discf={0}.{\rm{Disc\hskip 2.0pt}}f=\{0\}. Then:

  1. 1)1)

    χ(I+1)χ(I)=2(1)MIχ(Ff),\chi(\mathcal{L}_{I+1})-\chi(\mathcal{L}_{I})=2(-1)^{M-I}\chi(F_{f}), for each 1I<K.1\leq I<K.

  2. 2)2)

    χ(I+2)=χ(I),\chi(\mathcal{L}_{I+2})=\chi(\mathcal{L}_{I}), for each 1I<K1.1\leq I<K-1.

Proof.

In the equation (19) just exchange II by I+1I+1 and take the difference. Then we have

χ(I+1)χ(I)=χ(Ff)χ(SI1)χ(FI)χ(SI1)χ(Ff)χ(SI)+χ(FI+1)χ(SI).\chi(\mathcal{L}_{I+1})-\chi(\mathcal{L}_{I})=\chi(F_{f})\chi(S^{I-1})-\chi(\partial F_{I})\chi(S^{I-1})-\chi(F_{f})\chi(S^{I})+\chi(\partial F_{I+1})\chi(S^{I}).

Now we may apply Proposition 4.1, item 1),1), to get

χ(I+1)χ(I)=(1)MIχ(Ff)χ(SI1)+(1)MIχ(Ff)χ(SI)=2(1)MIχ(Ff).\chi(\mathcal{L}_{I+1})-\chi(\mathcal{L}_{I})=(-1)^{M-I}\chi(F_{f})\chi(S^{I-1})+(-1)^{M-I}\chi(F_{f})\chi(S^{I})=2(-1)^{M-I}\chi(F_{f}).

This ends the proof of item 1).1). Item 2)2) is trivial. ∎

Remark 4.4.

We point out that the Lê-Greuel type formula obtained in the Theorem 4.1, item (2), is somehow similar to that obtained in [11, Theorem 1, p. 3], but with the difference that in [11] the authors worked with the Euler number of the Milnor fibers, instead of its boundary.

In view of the Proposition 4.1 and the Proposition 4.3, we can see that for all 1I<K1\leq I<K we have χ(FI+1)χ(FI)=χ(I+1)χ(I).\chi(\partial F_{I+1})-\chi(\partial F_{I})=\chi(\mathcal{L}_{I+1})-\chi(\mathcal{L}_{I}). Thus, χ(FI+1)χ(I+1)=χ(FI)χ(I)==χ(F2)χ(2)=χ(F1)χ(1).\chi(\partial F_{I+1})-\chi(\mathcal{L}_{I+1})=\chi(\partial F_{I})-\chi(\mathcal{L}_{I})=\cdots=\chi(\partial F_{2})-\chi(\mathcal{L}_{2})=\chi(\partial F_{1})-\chi(\mathcal{L}_{1}). Hence, it suggests the following definition.

Definition 4.5.

Let f:(M,0)(K,0),f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0), M>K2,M>K\geq 2, be a tame polynomial map-germ with Discf={0}{\rm{Disc\hskip 2.0pt}}f=\{0\}. The degree of degeneracy on the Milnor boundary of ff is defined as the number

DB(f):=χ(F1)χ(1).DB(f):=\chi(\partial F_{1})-\chi(\mathcal{L}_{1})\,.

Clearly, if ff has an isolated singularity at the origin one has that DB(f)=0DB(f)=0.

5. On the boundaries of the Milnor fibers and the links on each stage I.

In the real setting we do not expect to prove theorems regarding the degree of connectivity of the Milnor fibers, its boundaries nor the respective links of fI,f_{I}, on each stage II. Notwithstanding, in the case where the dimension MM of the source space is even, for all I,I, 1IK,1\leq I\leq K, we may write χ(FI)=χ(SI+1)χ(FI)\chi(\partial F_{I})=\chi(S^{I+1})\chi(F_{I}) and as an application of Lemma 4.2 we conclude that χ(FI)=χ(I),\chi(\partial F_{I})=\chi(\mathcal{L}_{I}), and hence DB(f)=0.DB(f)=0. However, if the source space MM is odd-dimensional some interesting relations between the boundaries of the Milnor fiber, the links of the singularities and the Milnor fibers on the Milnor tubes come up on each stage II, and it provides a way to distinguish between the homotopy type of the Milnor boundary and the link of the singularities fIf_{I} for each 1IK,1\leq I\leq K, as described below.

We first remind that for odd dimension M2M\geq 2 the equation (19) becomes

():χ(I)=2χ(Ff)χ(SI1)+χ(FI)χ(SI1).(*):~{}\chi(\mathcal{L}_{I})=2-\chi(F_{f})\chi(S^{I-1})+\chi(\partial F_{I})\chi(S^{I-1}).

This allows us to prove the below result whose proof we left as an exercise.

Lemma 5.1.

Let MM odd and II such that M>KI2.M>K\geq I\geq 2. Then, for each II the following conditions hold for the links I\mathcal{L}_{I} and the boundaries FI\partial F_{I} of the Milnor fibers FI:F_{I}:

  1. (1)

    if II is even then χ(I)=2,\chi(\mathcal{L}_{I})=2, by equation ().(*). Moreover, since dimFI=MI\dim F_{I}=M-I is odd then χ(FI)=2χ(FI)=2χ(Ff);\chi(\partial F_{I})=2\chi(F_{I})=2\chi(F_{f});

  2. (2)

    if II is odd then χ(I)=22χ(Ff),\chi(\mathcal{L}_{I})=2-2\chi(F_{f}), by equation ().(*). Moreover, since dimFI=MI1\dim\partial F_{I}=M-I-1 is odd then χ(FI)=0.\chi(\partial F_{I})=0.

Now we are ready to state the main result of this section.

Theorem 5.2.

Consider MM odd, M>KI2.M>K\geq I\geq 2. Let f:(M,0)(K,0)f:(\mathbb{R}^{M},0)\to(\mathbb{R}^{K},0) and fI:(M,0)(I,0)f_{I}:(\mathbb{R}^{M},0)\to(\mathbb{R}^{I},0) be real analytic map germs as in the diagram (1). Then, χ(Ff)=1\chi(F_{f})=1 if and only if χ(FI)=χ(I)\chi(\partial F_{I})=\chi(\mathcal{L}_{I}) in some stage I.I. Moreover, if the last equality holds true on any stage II it also will holds true on all stages I,I, 2IK<M.2\leq I\leq K<M.

Proof.

The proof follows from Lemma 5.1.

For the "if" case, we can see that χ(FI)=χ(Ff)=1\chi(F_{I})=\chi(F_{f})=1 implies that the two quantities χ(FI)=χ(I)\chi(\partial F_{I})=\chi(\mathcal{L}_{I}) in the either cases of Lemma 5.1. Moreover, the equality in some stage II clearly implies that on all I,I, 2IK<M.2\leq I\leq K<M.

For the "only if" case, if we suppose that in some stage (even or odd) II the equality χ(FI)=χ(I)\chi(\partial F_{I})=\chi(\mathcal{L}_{I}) holds true, then again by Lemma 5.1 we conclude that 2χ(FI)=2.2\chi(F_{I})=2. Therefore, χ(Ff)=1.\chi(F_{f})=1.

The next result provides a natural class of map germs where one of two conditions above holds true. Beside that, it also provides another proof of [3, Proposition 3, item ii), p. 71].

Corollary 5.3.

Let f:(M,0)(K,0)f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0), with M>K2M>K\geq 2 and MM odd, be a real analytic map-germ with an isolated critical point at the origin. Then, for each I,I, M>KI1,M>K\geq I\geq 1, we have that χ(FI)=1.\chi(F_{I})=1.

Proof.

The proof might be left as exercise, but we will screatch it below for the sake of convenience.

Since ff have an isolated singular point at the origin, one may apply the diagram (2) to get that Sing(fI){0}{\rm{Sing\hskip 2.0pt}}(f_{I})\subseteq\{0\} for each fixed I.I. It is enough to consider the case Sing(fI)={0},{\rm{Sing\hskip 2.0pt}}(f_{I})=\{0\}, because the case Sing(fI)={\rm{Sing\hskip 2.0pt}}(f_{I})=\emptyset the result follows as an easy application of the Inverse Function Theorem version for map germs.

Now, if we assume further that MM is odd then for each II the link I\mathcal{L}_{I} must be not empty, and it is in fact a smooth manifold diffeomorphic to FI\partial F_{I} and thus χ(FI)=χ(I).\chi(\partial F_{I})=\chi(\mathcal{L}_{I}). Therefore, one may apply the Theorem 5.2 and conclude that χ(FI)=1,\chi(F_{I})=1, for each 1IK<M.1\leq I\leq K<M.

Remark 5.4.

For the existence of map germ (M,0)(K,0),({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0), M odd, M>K2,M>K\geq 2, with isolated critical point at the origin, the reader may consult [4, section 5.2, p. 101].

Corollary 5.5.

Let M>KI1M>K\geq I\geq 1 and ff be as in Theorem 5.2. If χ(Ff)1\chi(F_{f})\neq 1 then at all stages I,I, the Milnor boundary FI\partial F_{I} and the respective link I\mathcal{L}_{I} of fIf_{I} cannot be homotopically equivalent.

Proof.

It is now trivial because χ(FI)=χ(Ff)1,\chi(F_{I})=\chi(F_{f})\neq 1, on each stage I.I. Therefore, by Theorem 5.2 the respectives Milnor boundary FI\partial F_{I} and the link I\mathcal{L}_{I} can not be homotopically equivalent. ∎

The next example shows that for odd-dimension MM it is easy to construct a family of map germ where the Euler characteristic of the Milnor fiber is not equal to one.

Example 5.6.

Let f:(M,0)(K,0)f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0) be an analytic map germ M>K2,M>K\geq 2, with Singf={0},{\rm{Sing\hskip 2.0pt}}f=\{0\}, and g:(K,0)(K,0)g:({\mathbb{R}}^{K},0)\to({\mathbb{R}}^{K},0) be an analytic ramified covering map branched along {0}\{0\} with t-sheets, t2.t\geq 2. Then, for all fixed z(K,0),z\in({\mathbb{R}}^{K},0), 0<z1,0<\|z\|\ll 1, and all xg1(z)x\in g^{-1}(z) the map gg is a local diffeomorphism and the fiber g1(z)g^{-1}(z) consists of a finite number of points, and we set t:=#g1(z).t:=\#g^{-1}(z). Thus, Singg={0}{\rm{Sing\hskip 2.0pt}}g=\{0\} and the composition map germ h=gf:(M,0)(K,0)h=g\circ f:({\mathbb{R}}^{M},0)\to({\mathbb{R}}^{K},0) safisfies that Singh=f1(0)Vh.{\rm{Sing\hskip 2.0pt}}h=f^{-1}(0)\subseteq V_{h}. Since ff is tame, it is not hard to see that hh is tame as well. Then the map hh admits a Milnor tube fibration with Milnor fiber Fh=i=1tFfF_{h}=\sqcup_{i=1}^{t}F_{f} (t-disjoint copies of FfF_{f}). Therefore we have that χ(Fh)=t.χ(Ff)=t2,\chi(F_{h})=t.\chi(F_{f})=t\geq 2, where we use that χ(Ff)=1\chi(F_{f})=1 by Corollary 5.3.

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