Submersion (mathematics)

In mathematics, a submersion is a differentiable map between differentiable manifolds whose differential is everywhere surjective. This is a basic concept in differential topology. The notion of a submersion is dual to the notion of an immersion.

Definition

Let M and N be differentiable manifolds and f : M → N be a differentiable map between them. The map f is a submersion at a point p ∈ M if its differential

Df_{p}:T_{p}M\to T_{{f(p)}}N\,

is a surjective linear map.^[1] In this case p is called a regular point of the map f, otherwise, p is a critical point. A point q ∈ N is a regular value of f if all points p in the pre-image f⁻¹(q) are regular points. A differentiable map f that is a submersion at each point p ∈ M is called a submersion. Equivalently, f is a submersion if its differential Df_p has constant rank equal to the dimension of N.

A word of warning: some authors use the term "critical point" to describe a point where the rank of the Jacobian matrix of f at p is not maximal.^[2] Indeed, this is the more useful notion in singularity theory. If the dimension of M is greater than or equal to the dimension of N then these two notions of critical point coincide. But if the dimension of M is less than the dimension of N, all points are critical according to the definition above (the differential cannot be surjective) but the rank of the Jacobian may still be maximal (if it is equal to dim M). The definition given above is more commonly used, e.g. in the formulation of Sard's theorem.

Submersion Theorem

Given a submersion between smooth manifolds $f:M\to N$ the fibers of $f$ , denoted $M_{x}=f^{-1}(\{p\})$ can be equipped with the structure of a smooth manifold. This theorem coupled with the Whitney embedding theorem implies that every smooth manifold can be described as the fiber of a smooth map $f:\mathbb {R} ^{n}\to \mathbb {R} ^{m}$ .

For example, consider

f:\mathbb {R} ^{3}\to \mathbb {R}

where

f(x,y,z)=x^{4}+y^{4}+z^{4}

The jacobian matrix is given by

{\begin{bmatrix}{\frac {\partial f}{\partial x}}&{\frac {\partial f}{\partial y}}&{\frac {\partial f}{\partial z}}\end{bmatrix}}={\begin{bmatrix}4x^{3}&4y^{3}&4z^{3}\end{bmatrix}}

This has maximal rank at every point except for $(0,0,0)$ . Also, the fibers

f^{-1}(\{t\})=\{(a,b,c)\in \mathbb {R} ^{3}:a^{4}+b^{4}+c^{4}=t\}

are empty for $t\leq 0$ . Hence we only have a smooth submersion

f:\mathbb {R} ^{3}\to \mathbb {R} _{>0}

and the subsets

M_{t}=\{(a,b,c)\in \mathbb {R} ^{3}:a^{4}+b^{4}+c^{4}=t\}

are smooth manifolds for $t>0$ .

Examples

Any projection $\pi :{\mathbb {R}}^{{m+n}}\rightarrow {\mathbb {R}}^{n}\subset {\mathbb {R}}^{{m+n}}$
Local diffeomorphisms
Riemannian submersions
The projection in a smooth vector bundle or a more general smooth fibration. The surjectivity of the differential is a necessary condition for the existence of a local trivialization.

Local normal form

If f: M → N is a submersion at p and f(p) = q ∈ N then there exist an open neighborhood U of p in M, an open neighborhood V of q in N, and local coordinates (x₁,…,x_m) at p and (x₁,…,x_n) at q such that f(U) = V and the map f in these local coordinates is the standard projection

f(x_{1},\ldots ,x_{n},x_{{n+1}},\ldots ,x_{m})=(x_{1},\ldots ,x_{n}).

It follows that the full pre-image f⁻¹(q) in M of a regular value q ∈ N under a differentiable map f: M → N is either empty or is a differentiable manifold of dimension dim M − dim N, possibly disconnected. This is the content of the regular value theorem (also known as the submersion theorem). In particular, the conclusion holds for all q ∈ N if the map f is a submersion.

Topological manifold submersions

Submersions are also well defined for general topological manifolds.^[3] A topological manifold submersion is a continuous surjection f : M → N such that for all p ∈ M, for some continuous charts ψ at p and φ at f(p), the map ψ⁻¹ ∘ f ∘ φ is equal to the projection map from R^m to Rⁿ, where m=dim(M) ≥ n=dim(N).

Notes

↑ Crampin & Pirani 1994, p. 243. do Carmo 1994, p. 185. Frankel 1997, p. 181. Gallot, Hulin & Lafontaine 2004, p. 12. Kosinski 2007, p. 27. Lang 1999, p. 27. Sternberg 2012, p. 378.
↑ Arnold, Gusein-Zade & Varchenko 1985.
↑ Lang 1999, p. 27.

References

Arnold, V. I.; Gusein-Zade, S. M.; Varchenko, A. N. (1985). Singularities of Differentiable Maps: Volume 1. Birkhäuser. ISBN 0-8176-3187-9.
Bruce, J. W.; Giblin, P. J. (1984), Curves and Singularities, Cambridge University Press, ISBN 0-521-42999-4
Crampin, Michael; Pirani, Felix Arnold Edward (1994). Applicable differential geometry. Cambridge, England: Cambridge University Press. ISBN 978-0-521-23190-9.
do Carmo, Manfredo Perdigao (1994). Riemannian Geometry. ISBN 978-0-8176-3490-2.
Frankel, Theodore (1997). The Geometry of Physics. Cambridge: Cambridge University Press. ISBN 0-521-38753-1.
Gallot, Sylvestre; Hulin, Dominique; Lafontaine, Jacques (2004). Riemannian Geometry (3rd ed.). Berlin, New York: Springer-Verlag. ISBN 978-3-540-20493-0.
Kosinski, Antoni Albert (2007) [1993]. Differential manifolds. Mineola, New York: Dover Publications. ISBN 978-0-486-46244-8.
Lang, Serge (1999). Fundamentals of Differential Geometry. Graduate Texts in Mathematics. New York: Springer. ISBN 978-0-387-98593-0.
Sternberg, Shlomo Zvi (2012). Curvature in Mathematics and Physics. Mineola, New York: Dover Publications. ISBN 978-0-486-47855-5.

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[1] Crampin & Pirani 1994, p. 243. do Carmo 1994, p. 185. Frankel 1997, p. 181. Gallot, Hulin & Lafontaine 2004, p. 12. Kosinski 2007, p. 27. Lang 1999, p. 27. Sternberg 2012, p. 378.

[2] Arnold, Gusein-Zade & Varchenko 1985.

[3] Lang 1999, p. 27.