Abstract Generated abstract
This paper studies when a smooth closed simply connected manifold can be embedded in Euclidean space of dimension \(2n-1\), extending Whitney’s methods for embeddings in \(E^{2n}\) using ideas related to Pontryagin’s work on homotopy groups of spheres. The argument analyzes regular and completely regular maps, their double point submanifolds, normal bundle properties, and invariants of singular pairs, then uses Whitney-type deformations to eliminate singular pairs under suitable conditions. The main result proves that every simply connected odd-dimensional smooth closed manifold of dimension \(n>6\) admits a smooth embedding in \(E^{2n-1}\). A related conditional result is also obtained for even-dimensional simply connected manifolds, characterizing such embeddings in terms of the existence of an immersion into \(E^{2n-2}\).
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Reports of the Academy of Sciences of the USSR
- Volume 138, No. 4
MATHEMATICS
S. P. NOVIKOV
ON THE EMBEDDING OF SIMPLY CONNECTED MANIFOLDS IN EUCLIDEAN SPACE
(Presented by Academician P. S. Aleksandrov on 23 I 1961)
We shall consider smooth closed manifolds and their smooth mappings. As usual, we shall call a mapping \(f: M^n \to W^m\) regular if its Jacobian matrix has rank \(n\) at every point, and completely regular if the preimage of any point \(f^{-1}(w)\), where \(w \in W^m\), contains no more than two points. Our aim is to investigate the possibility of a smooth embedding \(M^n \subset E^{2n-1}\). The method generalizes the method of Whitney’s work \((^2)\), devoted to embeddings \(M^n \subset E^{2n}\), on the basis of ideas of L. S. Pontryagin concerning the homotopy groups of spheres \((^1)\).
Theorem 1. Every simply connected odd-dimensional manifold \(M^n\) with \(n > 6\) can be smoothly embedded in Euclidean space \(E^{2n-1}\).
The proof of this theorem is based on a series of lemmas devoted to the study of regular mappings as a whole. With the help of well-known techniques (developed by Whitney) it is easily proved:
Lemma 1*. For every regular mapping \(f: M^n \to E^{2n-k}\) with \(k < \left[\dfrac{n}{2}\right]\), there exists a \(C^1\)-close regular mapping \(g: M^n \to E^{2n-k}\) such that:
1) the equation \(g(x)=g(y)\) defines a closed submanifold \(\widetilde M_g^k \subset M^n \times M^n \setminus \Delta(M^n)\), where \(\Delta\) is the diagonal mapping;
2) the projection \(p: M^n \times M^n \to M^n\), considered on the submanifold \(\widetilde M_g^k\), is a smooth homeomorphism;
3) the mapping \(g\) is completely regular; on the special submanifold \(M_g^k = p(\widetilde M_g^k) \subset M^n\) it is a two-sheeted covering.
It follows from the lemma that the special manifold \(M_g^k\) decomposes into some number \(s\) of special pairs of mutually homeomorphic connected components
\[
\bigcup_{i=1}^{s} \left(M_{g,1}^{k,i} \cup M_{g,2}^{k,i}\right)
\]
such that \(g\left(M_{g,1}^{k,i}\right)=g\left(M_{g,2}^{k,i}\right)\), and some number \(t\) of connected manifolds
\[
\bigcup_{j=1}^{t} M_g^{k,j},
\]
on which the mapping \(g\) is a nontrivial 2-covering. Thus,
\[
M_g^k =
\left(\bigcup_{j=1}^{t} M_g^{k,j}\right)
\cup
\left(\bigcup_{i=1}^{t} \left(M_{g,1}^{k,i} \cup M_{g,2}^{k,i}\right)\right).
\]
Definition. We shall call a manifold \(M^n\) \(k\)-parallelizable if the \(\varepsilon\)-neighborhood \(U_\varepsilon^{(k)}\) of the \(k\)-dimensional skeleton of a smooth triangulation of the manifold \(M^n\) is parallelizable for sufficiently small \(\varepsilon\).
* For \(k=1\) this lemma is contained in Whitney’s works; see, for example, \((^3)\).
Obviously, for \(n>2k+2\) our definition does not depend on the triangulation, and a \(k\)-connected manifold is \(k\)-parallelizable. For \(k=1\) this definition means simply orientability. We also note that a \(k\)-parallelizable manifold is \((k-1)\)-parallelizable. In what follows we assume that \(n\geqslant 2k+3\).
Lemma 2. If the manifold \(M^n\) is \(k\)-parallelizable, then the singular submanifold \(M_g^k\subset M^n\) has a trivial normal bundle in the manifold \(M^n\) and is a \(\pi\)-manifold (i.e., the normal bundle under the embedding \(M_g^k\subset E^m\) is trivial for \(m\geqslant 2k+3\)).
The proof of this lemma is based on the fact that the manifold
\(M^n\times M^n\setminus \Delta(M^n)\) is also \(k\)-parallelizable and that the normal bundle of a manifold of dimension at most \(k\) in a \(k\)-parallelizable manifold of large dimension is arranged in the same way as in a Euclidean space of the same dimension.
Let \(n\) be even, \(k=1\), and let the manifold \(M^n\) be orientable.
Lemma 3. The singular submanifold \(M_g^1\subset M^n\) consists only of singular pairs of circles.
Suppose, to the contrary, that the manifold \(M_g^1\) contains a circle \(S_g^1\subset M_g^1\) on which the mapping \(g\) is a connected 2-fold covering. Obviously, \(g(S_g^1)=S^1\subset E^{2n-1}\). Choose a system \((W_1,\ldots,W_{n-1})\) of independent vector fields, transversal to \(S_g^1\subset M^n\) and tangent to the manifold \(M^n\).
Then, roughly speaking, there is defined a decomposition of the normal bundle of \(g(S_g^1)\subset E^{2n-1}\) into the sum of plane bundles \(\mu_i^{(2)}\), \(i=1,\ldots,n-1\), generated by the vectors \(W_i\). Each plane bundle \(\mu_i^{(2)}\) is transversal to the circle \(g(S_g^1)\) and has the monodromy matrix
\(A_i=\begin{pmatrix}0&1\\[2pt]1&0\end{pmatrix}\), i.e., each bundle \(\mu_i^{(2)}\) is nonorientable. The Whitney sum of an odd number of such bundles is also nonorientable and, consequently, nontrivial. Since \(n-1\) is odd, whereas the normal bundle to a circle in Euclidean space must be trivial, we arrive at a contradiction. The lemma is proved.
For the general case, when \(k=1\), we have:
Lemma 4. The number \(t(g)\) of connected singular coverings is always even. The mapping \(g\) is regularly homotopic to a mapping \(g_1\) that has no singular nontrivial 2-fold coverings.
The proof of this lemma is of a somewhat different nature and is based on the study of the projection
\[ M^n \xrightarrow{\ \tilde g\ } E^{2n} \xrightarrow{\ \pi\ } E^{2n-1}, \]
where \(g=\pi\circ \tilde g\), and the mapping \(\tilde g\) is completely regular (one can always easily reduce it to this form by a small \(C^1\)-perturbation of the mapping in the space \(E^{2n}\), projecting a small perturbation into \(E^{2n-1}\), which, obviously, preserves the properties of Lemma 1).
The behavior of the projection is described more fully by the following trivial lemmas:
Lemma 4a. If the mapping \(\tilde g:M^n\to E^{2n}\) and \(\pi\tilde g:M^n\to E^{2n-1}\) are regular, then the mapping \(\tilde g\) is regularly homotopic to an embedding and has an even number of pairs of singular points.
Lemma 4b. A connected singular covering of the mapping \(g\) can arise under projection only from an odd number of pairs of singular points of the mapping \(\tilde g\).
A singular pair can arise under projection only from an even number of pairs of singular points of the mapping \(\tilde g\).
Lemma 4c. There exists a regular homotopy \(\widetilde{g}_t\) of the map \(\widetilde{g}=\widetilde{g}_0\) such that:
1) the maps \(\widetilde{g}_t\) and \(\pi \widetilde{g}_t\) are regular for \(t\leqslant 1\) and are completely regular for \(t=1\); the map \(\pi \widetilde{g}_1\) satisfies Lemma 1;
2) under the projection \(\pi\), from one pair of singular points there arise double points, and from nothing—singular pairs of circles of the map \(\pi \widetilde{g}_1\).
In what follows we shall consider only such maps
\[
g:M^n\to E^{2n-1}
\]
that have no linked singular double points. We shall also assume that \(\pi_1(M^n)=0\). Following Pontryagin \((^1)\), we shall define the invariant of a singular pair and the invariant of a map \(g\).
Definition of the invariant of a singular pair. Let \(S_1^1\) and \(S_2^1\subset M^n\), \(g(S_1^1)=g(S_2^1)\). Consider a pair of disks \(\sigma_1^2,\sigma_2^2\subset M^n\) such that \(\sigma_1^2\cap\sigma_2^2=\varnothing\) and \(\partial\sigma_1^2=S_1^1,\ \partial\sigma_2^2=S_2^1\). Choose a system of vector fields \(W_j^{(i)}\), \(i=1,2;\ j=1,\ldots,n-2\), tangent to \(M^n\) and orthogonal to \(\sigma_i^2\). Put \(W_{n-1}^{(i)}=\partial\sigma_i^2/\partial t\), where \(t\) are the radii of the films (i.e., transverse to \(S_i^1\) and to \(W_j^{(i)}\), \(j\leqslant n-2\)). Obviously, the vectors \(g(W_j^{(i)})=V_{j+(i-1)i}\), transverse to \(g(S_i^1)\), are defined and independent. They determine an element
\[
\alpha\in \pi_1(GL(2n-2))=Z_2 .
\]
Lemma 5. If the generating element of the group \(H^n(M^n,Z_2)\) has the form \(Sq^2(x)\), \(x\in H^{n-2}(M^n,Z_2)\), then the disks \(\sigma_i^2\) and the fields \(W_j^{(i)}\) can be chosen so that \(\alpha=0\).
In the case when
\[
H^n(M^n,Z_2)/\operatorname{Im} Sq^2=Z_2,
\]
the invariant \(\alpha\) of a singular pair does not depend on the choice of the disks \(\sigma_i^2\). In this case we shall regard the sum of the invariants
\[
\sum_k \alpha_k
\]
over all singular pairs \(S_k=(S_{g,1}^{1,k}\cup S_{g,2}^{1,k})\) as the invariant of the map
\[
g:M^n\to E^{2n-1},
\]
if it has no linked singular double points.
Lemma 6. For a simply connected odd-dimensional manifold \(M^n\), \(n=4l+3\), the invariant
\[
\sum_k \alpha_k=0
\]
for any regular map
\[
g:M^n\to E^{2n-1},
\]
possessing all the properties of Lemma 1*.
This lemma is an important step, and its direct geometric proof is quite difficult. But from the recent works of Hirsch \((^4)\), devoted to regular maps, it is extracted more simply.
Let \(S_1\) and \(S_2\) be two singular pairs of the map
\[
g:M^n\to E^{2n-1}
\]
such that \(\alpha(S_1)=\alpha(S_2)\).
Lemma 7. There exists a regular homotopy \(g_t\) of the map \(g=g_0\) such that the map \(g_1\) satisfies Lemma 1 and has two fewer singular pairs than the map \(g=g_0\).
The proof generalizes the well-known proof of Whitney \((^2)\) for pairs of singular points. We glue into the manifold \(M^n\) the rings
\[
B_1=S_1^1\times I
\quad\text{and}\quad
B_2=S_2^1\times I
\]
so that \(S_i^1\times \varepsilon\) form the pair \(S_1\), and \(S_i^1\times(1-\varepsilon)\) form the pair \(S_2\). It is necessary that \(B_1\cap B_2=\varnothing\). On the rings we prescribe vector fields \(W_j^{(i)}\), \(i=1,2;\ j=1,\ldots,n-2\), extended from the disks \(\sigma_i^2\), determining the invariants \(\alpha(S_i)\). One can easily arrange that the frames
\[
(\tau_i,g(W_j^{(1)}),g(W_j^{(2)})),
\]
where \(\tau_i\) are vector fields tangent to \(g(S_i)\), determine opposite orientations for \(i=1,2\). Next we glue in a “Whitney cell”
\[
\psi:\sigma^2\times S^1\to E^{2n-1}
\]
such that
\[
\psi(\sigma^2\times S^1)\cap g(M^n)=g(B_1)\cup g(B_2).
\]
It is also necessary that on the boundaries
* If \(n=4l+1\), one can assert the existence of maps \(g:M^n\to E^{2n-1}\) with zero invariant, since there exists an immersion \(M^n\to E^{2n-2}\) \((^4)\).
the mapping \(\psi\) has certain compatibility properties. After this, by virtue of the coincidence of the invariants of the pairs \(S_1\) and \(S_2\), one can specify, in a small neighborhood \(U(\psi(\sigma^2\times S^1))\), a suitable coordinate system, one of whose coordinates is a point of the circle, two others are a standard 2-frame on \(\sigma^2\), and the remaining ones satisfy our boundary conditions and are independent of these. Having specified the coordinates, we perform in the neighborhood \(U(\psi(\sigma^2\times S^1))\) a Whitney deformation with the coordinate of the circle held fixed.
Iterating this construction and using Lemma 6, we arrive at a mapping
\[
g_S:M^n\to E^{2n-1},
\]
which has special pairs only with zero invariant.
After this, with the mapping \(g_S\) one can proceed in two ways: either, following (2), glue in additional pairs with zero invariants and apply Lemma 7, or else carry out the direct separation of a pair with zero invariant.* In either case we arrive at an embedding. Thus, the theorem follows from the preceding lemmas.
I note that the lemmas imply the following conditional
Theorem 2. Let \(n=2l\), \(n\geqslant 6\), and \(\pi_1(M^n)=0\). An embedding \(M^n\subset E^{2n-1}\) exists if and only if there exists an immersion \(M^n\to E^{2n-2}\) (see \((^4)\)).*
Mathematical Institute named after V. A. Steklov
Academy of Sciences of the USSR
Received
20 I 1961
REFERENCES CITED
- L. S. Pontryagin, Tr. Matem. inst. im. V. A. Steklova Akademii nauk SSSR, 45 (1955).
- H. Whitney, Ann. of Math., 37, No. 2 (1944).
- H. Whitney, Ann. of Math., 37, No. 3 (1944).
- M. Hirsh, Trans. Am. Math. Soc., 93, No. 2 (1959).
* The method of separating one special pair with zero invariant was suggested to me by D. B. Fuks, who kindly read the present work.
** A more precise investigation shows that, for \(n=4l+2\), the invariant \(\alpha\) defined above is a homotopy invariant of the manifold; it does not depend on the immersion
\[
g:M^n\to E^{2n-1}
\]
when \(n\not\equiv 1\pmod 4\).