On the connectedness of the boundary of π‘ž-complete domains (2024)

Rafael B. AndristFaculty of Mathematics and Physics,University of Ljubljana, Ljubljana, Sloveniarafael-benedikt.andrist@fmf.uni-lj.si

Abstract.

The boundary of every relatively compact Stein domain in a complex manifold of dimension at least two is connected. No assumptions on the boundary regularity are necessary. The same proofs hold also for qπ‘žqitalic_q-complete domains, and in the context of almost complex manifolds as well.

Key words and phrases:

pseudoconvex domain, ends of manifolds, Morse theory, almost complex manifolds

1991 Mathematics Subject Classification:

Primary 32F27, Secondary 32F10, 32Q60

1. Introduction

It seems to have been well-known to the experts in the 1980s that every bounded strictly pseudoconvex domain with π’ž2superscriptπ’ž2\mathcal{C}^{2}caligraphic_C start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT-smooth boundary in β„‚n,nβ‰₯2,superscriptℂ𝑛𝑛2\mathbb{C}^{n},n\geq 2,blackboard_C start_POSTSUPERSCRIPT italic_n end_POSTSUPERSCRIPT , italic_n β‰₯ 2 , has connected boundary. In fact, already in 1953 Serre pointed out that every Stein manifold of dimension at least 2222 has only one end (see Section 3). For a relatively compact Stein domain that admits a collar, this would already imply connectedness of the boundary.However, to the best knowledge of the author, the earliest publication mentioning that every bounded strictly pseudoconvex domain with π’ž2superscriptπ’ž2\mathcal{C}^{2}caligraphic_C start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT-smooth boundary in β„‚n,nβ‰₯2,superscriptℂ𝑛𝑛2\mathbb{C}^{n},n\geq 2,blackboard_C start_POSTSUPERSCRIPT italic_n end_POSTSUPERSCRIPT , italic_n β‰₯ 2 , has connected boundary, is due Rosay and Stout [MR0964461]*Corollary, p.1018 in 1989 where they actually prove a stronger result. Again, the connectedness of the boundary was noted by Balogh and Bonk [MR1793800]*p.513 under the same assumptions.In the monograph of Stout [MR2305474]*Corollary 2.4.7 it was established that every relatively compact, strictly pseudoconvex domain with π’ž2superscriptπ’ž2\mathcal{C}^{2}caligraphic_C start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT-smooth boundary in a Stein manifold of dimension at least two has connected boundary. The proof given there follows from a theorem of Forstnerič [MR1278436] about complements of Runge domains.

The almost complex case, but with a π’žβˆžsuperscriptπ’ž\mathcal{C}^{\infty}caligraphic_C start_POSTSUPERSCRIPT ∞ end_POSTSUPERSCRIPT-smooth defining J𝐽Jitalic_J-plurisubharmonic function on a neighborhood of the closure of the relatively compact domain is treated by Bertrand and Gaussier [MR3359581].

For the special case of bounded pseudoconvex domains in β„‚nsuperscriptℂ𝑛\mathbb{C}^{n}blackboard_C start_POSTSUPERSCRIPT italic_n end_POSTSUPERSCRIPT, a proof without any assumptions on the boundary regularity can be found in the second edition of the textbook of Jarnicki and Pflug [MR4201928]*Corollary 2.6.10. It relies mainly on a topological argument that was provided by Czarnecki, Kulczycki and Lubawski [MR2855300] with an elementary proof: For a bounded domain in ℝnsuperscriptℝ𝑛\mathbb{R}^{n}blackboard_R start_POSTSUPERSCRIPT italic_n end_POSTSUPERSCRIPT the connectedness of its complement is equivalent to the connectedness of its boundary. A very similar proof is given by Izzo [Izzo] who uses an elegant hom*ology argument that relies only on H1⁒(ℝn,β„€)=0subscript𝐻1superscriptℝ𝑛℀0H_{1}(\mathbb{R}^{n},\mathbb{Z})=0italic_H start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ( blackboard_R start_POSTSUPERSCRIPT italic_n end_POSTSUPERSCRIPT , blackboard_Z ) = 0 to obtain the above-mentioned topological fact.

We will prove the natural generalization of these results without any assumption on boundary regularity and on the ambient space.

Definition 1 ([MR3700709]*Definition 3.1.3).

Let X𝑋Xitalic_X be a complex manifold. We say that a domain Ξ©βŠ‚XΩ𝑋\Omega\subset Xroman_Ξ© βŠ‚ italic_X is qπ‘žqitalic_q-complete, if there exists a π’ž2superscriptπ’ž2\mathcal{C}^{2}caligraphic_C start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT-smooth exhaustion function Ο†:Ξ©β†’[0,+∞):πœ‘β†’Ξ©0\varphi\colon\Omega\to[0,+\infty)italic_Ο† : roman_Ξ© β†’ [ 0 , + ∞ ) that is qπ‘žqitalic_q-convex, i.e.if its Levi form has at most qβˆ’1π‘ž1q-1italic_q - 1 negative or zero eigenvalues at each point of ΩΩ\Omegaroman_Ξ©.

Theorem 2.

Let X𝑋Xitalic_X be a complex manifold with dimβ„‚X=nsubscriptdimensionℂ𝑋𝑛\dim_{\mathbb{C}}X=nroman_dim start_POSTSUBSCRIPT blackboard_C end_POSTSUBSCRIPT italic_X = italic_n and let Ξ©βŠ‚XΩ𝑋\Omega\subset Xroman_Ξ© βŠ‚ italic_X be a relatively compact qπ‘žqitalic_q-complete domain with n>qπ‘›π‘žn>qitalic_n > italic_q. Then the boundary βˆ‚Ξ©Ξ©\partial\Omegaβˆ‚ roman_Ξ© is connected.

By a result of Grauert [MR0098847] ΩΩ\Omegaroman_Ω is Stein if and only if it is 1111-complete, and thus we obtain the following corollary.

Corollary 3.

Let X𝑋Xitalic_X be a complex manifold with dimβ„‚X=n>1subscriptdimensionℂ𝑋𝑛1\dim_{\mathbb{C}}X=n>1roman_dim start_POSTSUBSCRIPT blackboard_C end_POSTSUBSCRIPT italic_X = italic_n > 1 and let Ξ©βŠ‚XΩ𝑋\Omega\subset Xroman_Ξ© βŠ‚ italic_X be a relatively compact Stein domain. Then the boundary βˆ‚Ξ©Ξ©\partial\Omegaβˆ‚ roman_Ξ© is connected.

Since a domain Ξ©βŠ‚XΩ𝑋\Omega\subset Xroman_Ξ© βŠ‚ italic_X in a Stein manifold X𝑋Xitalic_X is a domain of holomorphy if and only if it is pseudoconvex, we also arrive at the next corollary.

Corollary 4.

Let X𝑋Xitalic_X be a Stein manifold with dimβ„‚X=n>1subscriptdimensionℂ𝑋𝑛1\dim_{\mathbb{C}}X=n>1roman_dim start_POSTSUBSCRIPT blackboard_C end_POSTSUBSCRIPT italic_X = italic_n > 1 and let Ξ©βŠ‚XΩ𝑋\Omega\subset Xroman_Ξ© βŠ‚ italic_X be a relatively compact domain of holomorphy. Then the boundary βˆ‚Ξ©Ξ©\partial\Omegaβˆ‚ roman_Ξ© is connected.

The proof also extends to the almost complex situation.

Theorem 5.

Let (X,J)𝑋𝐽(X,J)( italic_X , italic_J ) be an almost complex manifold with dimℝXβ‰₯4subscriptdimensionℝ𝑋4\dim_{\mathbb{R}}X\geq 4roman_dim start_POSTSUBSCRIPT blackboard_R end_POSTSUBSCRIPT italic_X β‰₯ 4, and let Ξ©βŠ‚XΩ𝑋\Omega\subset Xroman_Ξ© βŠ‚ italic_X be a relatively compact domain with a π’ž2superscriptπ’ž2\mathcal{C}^{2}caligraphic_C start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT-smooth strictly J𝐽Jitalic_J-plurisubharmonic exhaustion function. Then the boundary βˆ‚Ξ©Ξ©\partial\Omegaβˆ‚ roman_Ξ© is connected.

Remark 6.

The result is sharp in the following sense:

  1. (1)

    In one dimension, every bounded domain of β„‚β„‚\mathbb{C}blackboard_C is pseudoconvex β€” and in fact a domain of holomorphy, but obviously does not need to have connected boundary. If we assume in addition that the domain is simply connected, its boundary will be connected, but in general not path-connected.

  2. (2)

    Unbounded domains, even when simply connected, do not need to have a connected complement, e.g.an infinite strip in β„‚β„‚\mathbb{C}blackboard_C. By taking direct products, this yields also counterexamples in higher dimensions.

Remark 7.

For symplectic manifolds with contact type boundaries, the boundary does not need to be connected, see McDuff [MR1091622] and Geiges [MR1328705].

This short note is organized as follows:For completeness, in Section 2 we first give the proof for relatively compact, strictly pseudoconvex domains with π’ž2superscriptπ’ž2\mathcal{C}^{2}caligraphic_C start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT-smooth boundary in a Stein manifold. We could not find a reference for this proof which was communicated by Franc Forstnerič.

In Section 3 we provide the topological background for the theory of ends and of continua. In Section 4 we give the proofs for the general situation.

2. A Classical Proof for Smooth Boundary

The following proof for the situation where ΩΩ\Omegaroman_Ξ© is a relatively compact, strongly pseudoconvex domain with π’ž2superscriptπ’ž2\mathcal{C}^{2}caligraphic_C start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT-smooth boundary in a Stein manifold was communicated by Franc Forstnerič. This is likely the classical proof that was known at least since the 1980s:

Consider a relatively compact domain Ξ©={ρ<c}Ξ©πœŒπ‘\Omega=\{\rho<c\}roman_Ξ© = { italic_ρ < italic_c } in an n𝑛nitalic_n-dimensional Stein manifold X𝑋Xitalic_X, where n>1𝑛1n>1italic_n > 1 and ρ𝜌\rhoitalic_ρ is a strongly plurisubharmonic Morse function on a neighborhood of Ω¯¯Ω\overline{\Omega}overΒ― start_ARG roman_Ξ© end_ARG, with d⁒ρ≠0π‘‘πœŒ0d\rho\neq 0italic_d italic_ρ β‰  0 on βˆ‚Ξ©Ξ©\partial\Omegaβˆ‚ roman_Ξ©. Let Ξ©t={ρ≀t}subscriptΞ©π‘‘πœŒπ‘‘\Omega_{t}=\{\rho\leq t\}roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT = { italic_ρ ≀ italic_t } for t≀c𝑑𝑐t\leq citalic_t ≀ italic_c. The topology of Ξ©tsubscriptΩ𝑑\Omega_{t}roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT and βˆ‚Ξ©tsubscriptΩ𝑑\partial\Omega_{t}βˆ‚ roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT only changes when t𝑑titalic_t passes a critical level set of ρ𝜌\rhoitalic_ρ. (The local normal form of a strongly plurisubharmonic Morse function at an isolated critical point is known in principle since 1924 due to a result of Takagi [zbMATH02595788] which was recovered again by Schur [zbMATH03097391] and by Harvey and Wells [MR0330510].) When passing a local minimum, a new connected component of Ξ©tsubscriptΩ𝑑\Omega_{t}roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT appears, which is not a concern. The only other type of points which can change connectivity of Ξ©tsubscriptΩ𝑑\Omega_{t}roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT is a critical point of index 1111. At such a point, we add a 1111-handle to Ξ©tsubscriptΩ𝑑\Omega_{t}roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT. There are two possibilities – either this handle is attached with both ends to the same component of Ξ©tsubscriptΩ𝑑\Omega_{t}roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT, or it joins two distinct components. In both cases we see by inspection that the boundary of any connected component remains connected.

Handles of higher index up to 2⁒nβˆ’22𝑛22n-22 italic_n - 2 do not change connectivity of the domain or its boundary:The core of the handle of index kπ‘˜kitalic_k is a kπ‘˜kitalic_k-disc which is attached with its boundary (kβˆ’1)π‘˜1(k-1)( italic_k - 1 )-sphere to βˆ‚Ξ©tsubscriptΩ𝑑\partial\Omega_{t}βˆ‚ roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT. Removing a submanifold of real codimension β‰₯2absent2\geq 2β‰₯ 2 from a manifold does not disconnect the manifold: In our case, we apply this argument to the boundary sphere of the kπ‘˜kitalic_k-disc as a submanifold of βˆ‚Ξ©tsubscriptΩ𝑑\partial\Omega_{t}βˆ‚ roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT.

The connectivity of βˆ‚Ξ©tsubscriptΩ𝑑\partial\Omega_{t}βˆ‚ roman_Ξ© start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT would change by attaching a handle of index 2⁒nβˆ’12𝑛12n-12 italic_n - 1 (i.e.of real codimension 1111), but such is not allowed since ρ𝜌\rhoitalic_ρ is plurisubharmonic and nβ‰₯2𝑛2n\geq 2italic_n β‰₯ 2.

3. Ends of topological spaces

The definition of ends of a topological space goes back to Freudenthal [MR1545233] and has led to a well developed theory, see the textbook of Hughes and Ranicki [MR1410261].

Definition 8.
  1. (1)

    A neighborhood of an end in a non-compact topological space X𝑋Xitalic_X is a subspace UβŠ‚Xπ‘ˆπ‘‹U\subset Xitalic_U βŠ‚ italic_X which contains a component of Xβˆ–K𝑋𝐾X\setminus Kitalic_X βˆ– italic_K for a non-empty compact subspace KβŠ‚X𝐾𝑋K\subset Xitalic_K βŠ‚ italic_X.

  2. (2)

    An end e𝑒eitalic_e of X𝑋Xitalic_X is an equivalence class of sequences of connected open neighborhoods XβŠƒU1βŠƒU2βŠƒβ€¦superset-of𝑋subscriptπ‘ˆ1superset-ofsubscriptπ‘ˆ2superset-of…X\supset U_{1}\supset U_{2}\supset\dotsitalic_X βŠƒ italic_U start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT βŠƒ italic_U start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT βŠƒ … such that

    β‹‚i=1∞Ui=βˆ…superscriptsubscript𝑖1subscriptπ‘ˆπ‘–\bigcap_{i=1}^{\infty}U_{i}=\emptysetβ‹‚ start_POSTSUBSCRIPT italic_i = 1 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT ∞ end_POSTSUPERSCRIPT italic_U start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT = βˆ…

    subject to the equivalence relation

    (XβŠƒU1βŠƒU2βŠƒβ€¦)∼(XβŠƒV1βŠƒV2βŠƒβ€¦)similar-tosuperset-of𝑋subscriptπ‘ˆ1superset-ofsubscriptπ‘ˆ2superset-of…superset-of𝑋subscript𝑉1superset-ofsubscript𝑉2superset-of…(X\supset U_{1}\supset U_{2}\supset\dots)\sim(X\supset V_{1}\supset V_{2}%\supset\dots)( italic_X βŠƒ italic_U start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT βŠƒ italic_U start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT βŠƒ … ) ∼ ( italic_X βŠƒ italic_V start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT βŠƒ italic_V start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT βŠƒ … )

    if for each Uisubscriptπ‘ˆπ‘–U_{i}italic_U start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT there exists j𝑗jitalic_j with UiβŠ†Vjsubscriptπ‘ˆπ‘–subscript𝑉𝑗U_{i}\subseteq V_{j}italic_U start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT βŠ† italic_V start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT, and for each Vjsubscript𝑉𝑗V_{j}italic_V start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT there exists i𝑖iitalic_i with VjβŠ†Uisubscript𝑉𝑗subscriptπ‘ˆπ‘–V_{j}\subseteq U_{i}italic_V start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT βŠ† italic_U start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT.

Remark 9 ([MR1410261]*Example3(i)).

Let X𝑋Xitalic_X be a topological space with a proper map Ο†:Xβ†’[0,+∞):πœ‘β†’π‘‹0\varphi\colon X\to[0,+\infty)italic_Ο† : italic_X β†’ [ 0 , + ∞ ) which is onto, and such that the inverse images Ut=Ο†βˆ’1⁒(t,+∞)βŠ†Xsubscriptπ‘ˆπ‘‘superscriptπœ‘1𝑑𝑋U_{t}=\varphi^{-1}(t,+\infty)\subseteq Xitalic_U start_POSTSUBSCRIPT italic_t end_POSTSUBSCRIPT = italic_Ο† start_POSTSUPERSCRIPT - 1 end_POSTSUPERSCRIPT ( italic_t , + ∞ ) βŠ† italic_X, tβ‰₯1𝑑1t\geq 1italic_t β‰₯ 1 are connected. Then X𝑋Xitalic_X has one end.

Lemma 10.

Let X𝑋Xitalic_X be a locally compact Hausdorff space with a countable basis of topology. Then X𝑋Xitalic_X has one end if and only if there exists an exhaustion by compacts (Kj)jβˆˆβ„•subscriptsubscript𝐾𝑗𝑗ℕ(K_{j})_{j\in\mathbb{N}}( italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT ) start_POSTSUBSCRIPT italic_j ∈ blackboard_N end_POSTSUBSCRIPT of X𝑋Xitalic_X such that Xβˆ–Kj𝑋subscript𝐾𝑗X\setminus K_{j}italic_X βˆ– italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT is connected for every jβˆˆβ„•π‘—β„•j\in\mathbb{N}italic_j ∈ blackboard_N.

Proof.

The β€œif” part is straightforward, see also Remark 9. We only need to provide a proof for the β€œonly if” part: Assume to get a contradiction that no exhaustion by compacts (Kj)jsubscriptsubscript𝐾𝑗𝑗(K_{j})_{j}( italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT ) start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT of X𝑋Xitalic_X exists such that Xβˆ–Kj𝑋subscript𝐾𝑗X\setminus K_{j}italic_X βˆ– italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT is connected for every jβˆˆβ„•π‘—β„•j\in\mathbb{N}italic_j ∈ blackboard_N, but that X𝑋Xitalic_X has only one end. We can always pass to a subsequence, and thus we may assume that Xβˆ–Kj𝑋subscript𝐾𝑗X\setminus K_{j}italic_X βˆ– italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT always has at least two connected components. Moreover, we can assume that none of these components is contained in a compact Kℓ⁒(j),β„“>j,subscript𝐾ℓ𝑗ℓ𝑗K_{\ell(j)},\ell>j,italic_K start_POSTSUBSCRIPT roman_β„“ ( italic_j ) end_POSTSUBSCRIPT , roman_β„“ > italic_j , for otherwise we could have included this component already in the compact Kjsubscript𝐾𝑗K_{j}italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT.Now we pick a connected component U1subscriptπ‘ˆ1U_{1}italic_U start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT of Xβˆ–K1𝑋subscript𝐾1X\setminus K_{1}italic_X βˆ– italic_K start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT. For every jβ‰₯2𝑗2j\geq 2italic_j β‰₯ 2 we a pick a connected component of Xβˆ–Kj𝑋subscript𝐾𝑗X\setminus K_{j}italic_X βˆ– italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT that is contained in Ujβˆ’1subscriptπ‘ˆπ‘—1U_{j-1}italic_U start_POSTSUBSCRIPT italic_j - 1 end_POSTSUBSCRIPT. This is always possible, since we eliminated superficial connected components by our choice of compacts Kjsubscript𝐾𝑗K_{j}italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT. This sequence of neighborhoods (Uj)jsubscriptsubscriptπ‘ˆπ‘—π‘—(U_{j})_{j}( italic_U start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT ) start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT defines an end of X𝑋Xitalic_X.Since Xβˆ–K1𝑋subscript𝐾1X\setminus K_{1}italic_X βˆ– italic_K start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT has at least two connected components, we choose another sequence of neighborhoods (Vj)jsubscriptsubscript𝑉𝑗𝑗(V_{j})_{j}( italic_V start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT ) start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT such that Ujsubscriptπ‘ˆπ‘—U_{j}italic_U start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT and Vjsubscript𝑉𝑗V_{j}italic_V start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT are different connected components of Xβˆ–Kj𝑋subscript𝐾𝑗X\setminus K_{j}italic_X βˆ– italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT for every jβˆˆβ„•π‘—β„•j\in\mathbb{N}italic_j ∈ blackboard_N, and hence define two different ends.∎

Definition 11.

A continuum is a non-empty, compact, connected metric space.

Lemma 12 ([MR1192552]*Theorem 1.8).

The intersection of a decreasing sequence of continua is a continuum.

Proposition 13.

Let X𝑋Xitalic_X be a manifold with countable basis of topology and let Ξ©βŠ‚XΩ𝑋\Omega\subset Xroman_Ξ© βŠ‚ italic_X be a relatively compact domain with one end. Then ΩΩ\Omegaroman_Ξ© has connected boundary.

Proof.

We apply Lemma 10 to obtain an exhaustion by compacts Kjsubscript𝐾𝑗K_{j}italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT such that Ξ©βˆ–KjΞ©subscript𝐾𝑗\Omega\setminus K_{j}roman_Ξ© βˆ– italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT is connected for every jβˆˆβ„•π‘—β„•j\in\mathbb{N}italic_j ∈ blackboard_N. Then Ξ©βˆ–(Kj)∘Ωsuperscriptsubscript𝐾𝑗\Omega\setminus(K_{j})^{\circ}roman_Ξ© βˆ– ( italic_K start_POSTSUBSCRIPT italic_j end_POSTSUBSCRIPT ) start_POSTSUPERSCRIPT ∘ end_POSTSUPERSCRIPT are a decreasing sequence of continua. Thus its limit, which is the boundary βˆ‚Ξ©Ξ©\partial\Omegaβˆ‚ roman_Ξ©, is also a continuum by Lemma 12.∎

Remark 14.

If the boundary βˆ‚Ξ©Ξ©\partial\Omegaβˆ‚ roman_Ξ© of the relatively compact domain ΩΩ\Omegaroman_Ξ© admits a collar, then we have a one-by-one correspondence between ends and boundary components.

4. Proofs

It was already noted by Serre that a Stein manifold of complex dimension at least two has only one end [MR0064155]*p.59, see also [MR3185220]. His short cohom*ological argument for this fact is given with more details by Gilligan and Huckleberry [MR0616269]*p.186.

Another way of seeing this is to consider a strictly plurisubharmonic Morse exhaustion function which is the approach taken by Forstnerič [MR1278436].

Proof of Theorem 2.

Let dimβ„‚X=nsubscriptdimensionℂ𝑋𝑛\dim_{\mathbb{C}}X=nroman_dim start_POSTSUBSCRIPT blackboard_C end_POSTSUBSCRIPT italic_X = italic_n. Since ΩΩ\Omegaroman_Ξ© is relatively compact, by a small perturbation we may assume that the π’ž2superscriptπ’ž2\mathcal{C}^{2}caligraphic_C start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT-smooth exhaustion function Ο†:Ξ©β†’[0,+∞):πœ‘β†’Ξ©0\varphi\colon\Omega\to[0,+\infty)italic_Ο† : roman_Ξ© β†’ [ 0 , + ∞ ) is a Morse function and still qπ‘žqitalic_q-complete. The Morse index at a critical point is at most n+qβˆ’1π‘›π‘ž1n+q-1italic_n + italic_q - 1 (see the monograph of Forstnerič [MR3700709]*Sections 3.10 and 3.11 for more details). Note that 2⁒nβˆ’1>n+qβˆ’1⟺n>q⟺2𝑛1π‘›π‘ž1π‘›π‘ž2n-1>n+q-1\Longleftrightarrow n>q2 italic_n - 1 > italic_n + italic_q - 1 ⟺ italic_n > italic_q is satisfied by assumption. Since we glue only handles of dimension ≀n+qβˆ’1absentπ‘›π‘ž1\leq n+q-1≀ italic_n + italic_q - 1, and ΩΩ\Omegaroman_Ξ© has real dimension 2⁒n2𝑛2n2 italic_n, the complement of any sublevel set of Ο†πœ‘\varphiitalic_Ο† is connected. By Lemma 10 the domain ΩΩ\Omegaroman_Ξ© has only one end. Proposition 13 now gives the conclusion.∎

Proof of Theorem 5.

Let dimℝX=2⁒nsubscriptdimensionℝ𝑋2𝑛\dim_{\mathbb{R}}X=2nroman_dim start_POSTSUBSCRIPT blackboard_R end_POSTSUBSCRIPT italic_X = 2 italic_n. Let Ο†:Ω→ℝ:πœ‘β†’Ξ©β„\varphi\colon\Omega\to\mathbb{R}italic_Ο† : roman_Ξ© β†’ blackboard_R be a strictly J𝐽Jitalic_J-plurisubharmonic exhaustion function. Since the domain ΩΩ\Omegaroman_Ξ© is relatively compact, we may slightly disturb Ο†πœ‘\varphiitalic_Ο† if necessary to obtain a strictly J𝐽Jitalic_J-plurisubharmonic Morse exhaustion function. By [MR3012475]*Corollary 3.4 the Morse index of Ο†πœ‘\varphiitalic_Ο† at a critical point in an almost complex manifold is at most n𝑛nitalic_n. Now the conclusion is the same as in the proof of Theorem 2 above.∎

Remark 15.

The proofs of these two theorems can also be given without using the theory of ends, by instead considering the exhaustion functions and their connected superlevel sets, and applying Lemma 12 directly to them. However, conceptually, it seems more natural to use Proposition 13 which reflects that the β€œreason” comes from the fact that these relatively compact domains have one end.

Acknowledgments

The author would like to thank Matteo Fiacchi, Franc Forstnerič, Tobias Harz, Gerrit Hermann, Hendrik Hermann, Alexander Izzo, and Jaka Smrekar for interesting and helpful discussions and suggestions.

Funding

The first author was supported by the European Union (ERC Advanced grant HPDR, 101053085 to Franc Forstnerič) and grant N1-0237 from ARRS, Republic of Slovenia.

References

    On the connectedness of the boundary of π‘ž-complete domains (2024)
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