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Submersion (mathematics)

From Wikipedia, the free encyclopedia
Differential map between manifolds whose differential is everywhere surjective
"Regular point" redirects here. For "regular point of an algebraic variety", seeSingular point of an algebraic variety.

Inmathematics, asubmersion is adifferentiable map betweendifferentiable manifolds whosedifferential is everywheresurjective. It is a basic concept indifferential topology, dual to that of animmersion.

Definition

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LetM andN bedifferentiable manifolds, and letf:MN{\displaystyle f\colon M\to N} be adifferentiable map between them. The mapf is asubmersion at a pointpM{\displaystyle p\in M} if itsdifferential

Dfp:TpMTf(p)N{\displaystyle Df_{p}\colon T_{p}M\to T_{f(p)}N}

is asurjectivelinear map.[1] In this case,p is called aregular point of the mapf; otherwise,p is acritical point. A pointqN{\displaystyle q\in N} is aregular value off if all pointsp in thepreimagef1(q){\displaystyle f^{-1}(q)} are regular points. A differentiable mapf that is a submersion at each pointpM{\displaystyle p\in M} is called asubmersion. Equivalently,f is a submersion if its differentialDfp{\displaystyle Df_{p}} hasconstant rank equal to the dimension ofN.

Some authors use the termcritical point to describe a point where therank of theJacobian matrix off atp is not maximal.:[2] Indeed, this is the more useful notion insingularity theory. If the dimension ofM is greater than or equal to the dimension ofN, then these two notions of critical point coincide. However, if the dimension ofM is less than the dimension ofN, 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 dimM). The definition given above is the more commonly used one, e.g., in the formulation ofSard's theorem.

Submersion theorem

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Given a submersionf:MN{\displaystyle f\colon M\to N} between smooth manifolds of dimensionsm{\displaystyle m} andn{\displaystyle n}, for eachxM{\displaystyle x\in M} there existsurjectivechartsϕ:URm{\displaystyle \phi :U\to \mathbb {R} ^{m}} ofM{\displaystyle M} aroundx{\displaystyle x}, andψ:VRn{\displaystyle \psi :V\to \mathbb {R} ^{n}} ofN{\displaystyle N} aroundf(x){\displaystyle f(x)}, such thatf{\displaystyle f} restricts to a submersionf:UV{\displaystyle f\colon U\to V} which, when expressed in coordinates asψfϕ1:RmRn{\displaystyle \psi \circ f\circ \phi ^{-1}:\mathbb {R} ^{m}\to \mathbb {R} ^{n}}, becomes an ordinaryorthogonal projection. As an application, for eachpN{\displaystyle p\in N} the corresponding fiber off{\displaystyle f}, denotedMp=f1(p){\displaystyle M_{p}=f^{-1}({p})} can be equipped with the structure of a smooth submanifold ofM{\displaystyle M} whose dimension equals the difference of the dimensions ofN{\displaystyle N} andM{\displaystyle M}.

This theorem is a consequence of theinverse function theorem (seeInverse function theorem#Giving a manifold structure).

For example, considerf:R3R{\displaystyle f\colon \mathbb {R} ^{3}\to \mathbb {R} } given byf(x,y,z)=x4+y4+z4.{\displaystyle f(x,y,z)=x^{4}+y^{4}+z^{4}.}. The Jacobian matrix is

[fxfyfz]=[4x34y34z3].{\displaystyle {\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){\displaystyle (0,0,0)}. Also, the fibers

f1({t})={(a,b,c)R3:a4+b4+c4=t}{\displaystyle f^{-1}(\{t\})=\left\{(a,b,c)\in \mathbb {R} ^{3}:a^{4}+b^{4}+c^{4}=t\right\}}

areempty fort<0{\displaystyle t<0}, and equal to a point whent=0{\displaystyle t=0}. Hence, we only have a smooth submersionf:R3(0,0,0)R>0,{\displaystyle f\colon \mathbb {R} ^{3}\setminus {(0,0,0)}\to \mathbb {R} _{>0},} and the subsetsMt={(a,b,c)R3:a4+b4+c4=t}{\displaystyle M_{t}=\left\{(a,b,c)\in \mathbb {R} ^{3}:a^{4}+b^{4}+c^{4}=t\right\}} are two-dimensional smooth manifolds fort>0{\displaystyle t>0}.

Examples

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Maps between spheres

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A large class of examples of submersions are submersions between spheres of higher dimension, such as

f:Sn+kSk{\displaystyle f:S^{n+k}\to S^{k}}

whose fibers have dimensionn{\displaystyle n}. This is because the fibers (inverse images of elementspinSk{\displaystyle pinS^{k}}) are smooth manifolds of dimensionn{\displaystyle n}. Then, if we take a path

γ:ISk{\displaystyle \gamma :I\to S^{k}}

and take thepullback

MISn+kfIxγSk{\displaystyle {\begin{matrix}M_{I}&\to &S^{n+k}\\\downarrow &&\downarrow f\\I&x\rightarrow {\gamma }&S^{k}\end{matrix}}}

we get an example of a special kind ofbordism, called aframed bordism. In fact, the framed cobordism groupsΩnfr{\displaystyle \Omega _{n}^{fr}} are intimately related to thestable homotopy groups.

Families of algebraic varieties

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Another large class of submersions is given by families ofalgebraic varietiesπ:XS{\displaystyle \pi :{\mathfrak {X}}\to S} whose fibers are smooth algebraic varieties. If we consider the underlying manifolds of these varieties, we get smooth manifolds. For example, the Weierstrass familyπ:WtoA1{\displaystyle \pi :{\mathcal {W}}to\mathbb {A} ^{1}} ofelliptic curves is a widely studied submersion because it includes many technical complexities used to demonstrate more complex theory, such asintersection homology andperverse sheaves. This family is given by

W={(t,x,y)A1×A2:y2=x(x1)(xt)}{\displaystyle {\mathcal {W}}=\left\{(t,x,y)\in \mathbb {A} ^{1}\times \mathbb {A} ^{2}:y^{2}=x(x-1)(x-t)\right\}}

whereA1{\displaystyle \mathbb {A} ^{1}} is the affine line andA2{\displaystyle \mathbb {A} ^{2}} is the affine plane. Since we are considering complex varieties, these are equivalently the spacesC,C2{\displaystyle \mathbb {C} ,\mathbb {C} ^{2}} of the complex line and the complex plane. Note that we should actually remove the pointst=0,1{\displaystyle t=0,1} because there are singularities (since there is a double root).

Local normal form

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Iff:MN is a submersion atp andf(p) =qN, then there exists anopen neighborhoodU ofp inM, an open neighborhoodV ofq inN, and local coordinates(x1, …,xm) atp and(x1, …,xn) atq such thatf(U) =V, and the mapf in these local coordinates is the standard projection

f(x1,,xn,xn+1,,xm)=(x1,,xn).{\displaystyle f(x_{1},\ldots ,x_{n},x_{n+1},\ldots ,x_{m})=(x_{1},\ldots ,x_{n}).}

It follows that the full preimagef−1(q) inM of a regular valueq inN under a differentiable mapf:MN is either empty or a differentiable manifold of dimensiondimM − dimN, possiblydisconnected. This is the content of theregular value theorem (also known as thesubmersion theorem). In particular, the conclusion holds for allq inN if the mapf is a submersion.

Topological manifold submersions

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Submersions are also well-defined for generaltopological manifolds.[3] A topological manifold submersion is acontinuous surjectionf :MN such that for allp inM, for some continuous chartsψ atp andφ atf(p), the mapψ−1 ∘ f ∘ φ is equal to theprojection map fromRm toRn, wherem = dim(M) ≥n = dim(N).

See also

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Notes

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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.

References

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Further reading

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Basic concepts
Main results(list)
Maps
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