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{{Lie groups |Other}}


In [[mathematics]], a '''diffeomorphism''' is an [[isomorphism]] of [[smooth manifold]]s. It is an [[invertible function]] that [[map (mathematics)|maps]] one [[differentiable manifold]] to another, such that both the function and its inverse are [[smooth function|smooth]].  
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[[Image:Diffeomorphism of a square.svg|right|thumb|The image of a rectangular grid on a square under a diffeomorphism from the square onto itself.]]


== Definition ==
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Given two [[manifolds]] ''M'' and ''N'', a [[differentiable]] map ''f'' : ''M'' → ''N'' is called a '''diffeomorphism''' if it is a [[bijection]] and its inverse ''f''<sup>−1</sup> : ''N'' →  ''M'' is differentiable as well. If these functions are ''r'' times continuously differentiable, ''f'' is called a '''''C<sup>r</sup>''-diffeomorphism''').


Two manifolds ''M'' and ''N'' are '''diffeomorphic''' (symbol usually being ≃) if there is a diffeomorphism ''f'' from ''M'' to ''N''. They are '''''C<sup>r</sup>'' diffeomorphic''' if there is an ''r'' times continuously differentiable bijective map between them whose inverse is also ''r'' times continuously differentiable.
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== Diffeomorphisms of subsets of manifolds ==
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Given a subset ''X'' of a manifold ''M'' and a subset ''Y'' of a manifold ''N'', a function ''f'' : ''X'' → ''Y'' is said to be smooth if for all ''p'' in ''X'' there is a neighborhood ''U'' ⊂ ''M'' of ''p'' and a smooth function ''g'' : ''U'' → ''N'' such that the restrictions agree <math>g_{|U \cap X} = f_{|U \cap X}</math> (note that ''g'' is an extension of ''f''). We say that ''f'' is a diffeomorphism if it is bijective, smooth and its inverse is smooth.


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'''Model Example.''' If ''U'', ''V'' are connected open subsets of '''R'''<sup>''n''</sup> such that ''V'' is [[simply connected]], a [[derivative|differentiable]] map ''f'' : ''U'' → ''V'' is a '''diffeomorphism''', if it is [[proper map|proper]] and if the [[Pushforward (differential)|differential]] ''Df<sub>x</sub>'' : '''R'''<sup>''n''</sup> → '''R'''<sup>''n''</sup> is [[bijection|bijective]] at each point ''x'' in ''U''.
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<blockquote>'''Remark 1.''' It is essential for ''U'' to be [[simply connected]] for the function ''f'' to be globally invertible (under the sole condition that its derivative is a bijective map at each point). For example, consider the "realification" of the complex square function
:<math>\begin{cases}
f : \mathbf{R}^2 \setminus \{(0,0)\} \to \mathbf{R}^2 \setminus \{(0,0)\} \\
(x,y)\mapsto(x^2-y^2,2xy)
\end{cases}</math>
Then ''f'' is surjective and its satisfies
:<math>\det Df_x=4(x^2+y^2)\neq0</math>
thus ''Df<sub>x</sub>'' is bijective at each point yet ''f'' is not invertible, because it fails to be injective, e.g., ''f''(1,0) = (1,0) = ''f''(−1,0).</blockquote>
 
<blockquote>'''Remark 2.''' Since the differential at a point (for a differentiable function)
:<math>Df_x : T_xU \to T_{f(x)}V</math>
is a [[linear map]] it has a well defined inverse if, and only if, ''Df<sub>x</sub>'' is a bijection. The matrix representation of ''Df<sub>x</sub>'' is the ''n'' × ''n'' matrix of first order partial derivatives whose entry in the ''i''-th row and ''j''-th column is <math>\partial f_i / \partial x_j</math>. We often use this so-called [[Jacobian matrix]] for explicit computations.</blockquote>
 
<blockquote>'''Remark 3.''' Diffeomorphisms are necessarily between manifolds of the same [[dimension]]. Imagine that ''f'' were going from dimension ''n'' to dimension ''k''. If ''n'' < ''k'' then ''Df<sub>x</sub>'' could never be surjective, and if ''n'' > ''k'' then ''Df<sub>x</sub>'' could never be injective. So in both cases ''Df<sub>x</sub>'' fails to be a bijection.</blockquote>
 
<blockquote>'''Remark 4.''' If ''Df<sub>x</sub>'' is a bijection at ''x'' then we say that ''f'' is a local diffeomorphism (since by continuity ''Df<sub>y</sub>'' will also be bijective for all ''y'' sufficiently close to ''x'').</blockquote>
 
<blockquote>'''Remark 5.''' Given a smooth map from dimension ''n'' to dimension ''k'', if ''Df'' (resp. ''Df<sub>x</sub>'') is surjective then we say that ''f'' is a [[Submersion (mathematics)|submersion]] (resp. local submersion), and if ''Df'' (resp. ''Df<sub>x</sub>'') is injective we say that ''f'' is an [[Immersion (mathematics)|immersion]] (resp. local immersion).</blockquote>
 
<blockquote>'''Remark 6.''' A differentiable bijection is ''not'' necessarily a diffeomorphism, e.g. ''f''(''x'') = ''x''<sup>3</sup> is not a diffeomorphism from '''R''' to itself because its derivative vanishes at 0 (and hence its inverse is not differentiable at 0). This is an example of a homeomorphism that is not a diffeomorphism.</blockquote>
 
<blockquote>'''Remark 7.''' ''f'' being a diffeomorphism is a stronger condition than ''f'' being a [[homeomorphism]] (when ''f'' is a map between ''differentiable'' manifolds). For a diffeomorphism we need ''f'' and its inverse to be [[differentiable]]. For a homeomorphism we only require that ''f'' and its inverse be [[continuous function|continuous]]. Thus every diffeomorphism is a homeomorphism, but the converse is false: not every homeomorphism is a diffeomorphism.</blockquote>
 
Now, ''f'' : ''M'' → ''N'' is called a '''diffeomorphism''' if in [[Manifold#Differentiable manifolds|coordinates charts]] it satisfies the definition above. More precisely, pick any cover of ''M'' by compatible [[Manifold#Differentiable manifolds|coordinate charts]], and do the same for ''N''. Let φ and ψ be charts on ''M'' and ''N'' respectively, with ''U'' being the image of φ and ''V'' the image of ψ. Then the conditions says that the map ψ''f''φ<sup>−1</sup> : ''U'' → ''V'' is a diffeomorphism as in the definition above (whenever it makes sense). One has to check that for every pair of charts φ, ψ of two given [[Manifold#Differentiable manifolds|atlases]], but once checked, it will be true for any other compatible chart. Again we see that dimensions have to agree.
 
== Examples ==
Since any manifold can be locally parametrised, we can consider some explicit maps from '''R'''<sup>2</sup> into '''R'''<sup>2</sup>.
 
* Let
::<math>f(x,y) = \left (x^2 + y^3, x^2 - y^3 \right ).</math>
:We can calculate the Jacobian matrix:
::<math> J_f = \begin{pmatrix} 2x & 3y^2 \\ 2x & -3y^2 \end{pmatrix} . </math>
:The Jacobian matrix has zero determinant if, and only if ''xy'' = 0. We see that ''f'' is a diffeomorphism away from the ''x''-axis and the ''y''-axis.
 
* Let
::<math>g(x,y) = \left (a_0 + a_{1,0}x + a_{0,1}y + \cdots, \ b_0 + b_{1,0}x + b_{0,1}y + \cdots \right )</math>
:where the <math>a_{i,j}</math> and <math>b_{i,j}</math> are arbitrary real numbers, and the omitted terms are of degree at least two in ''x'' and ''y''. We can calculate the Jacobian matrix at '''0''':
::<math> J_g(0,0) = \begin{pmatrix} a_{1,0} & a_{0,1} \\ b_{1,0} & b_{0,1} \end{pmatrix}. </math>
:We see that ''g'' is a local diffeomorphism at '''0''' if, and only if,
::<math>a_{1,0}b_{0,1} - a_{0,1}b_{1,0} \neq 0,</math>
:i.e. the linear terms in the components of ''g'' are linearly independent as polynomials.
 
* Let
::<math>h(x,y) = \left (\sin(x^2 + y^2), \cos(x^2 + y^2) \right ).</math>
:We can calculate the Jacobian matrix:
::<math> J_h = \begin{pmatrix} 2x\cos(x^2 + y^2) & 2y\cos(x^2 + y^2) \\ -2x\sin(x^2+y^2) & -2y\sin(x^2 + y^2) \end{pmatrix} . </math>
:The Jacobian matrix has zero determinant everywhere! In fact we see that the image of ''h'' is the unit circle.
 
== Diffeomorphism group ==
Let ''M'' be a differentiable manifold that is [[second-countable]] and Hausdorff. The '''diffeomorphism group''' of ''M'' is the group of all ''C<sup>r</sup>'' diffeomorphisms of ''M'' to itself, and is denoted by Diff<sup>''r''</sup>(''M'') or Diff(''M'') when ''r'' is understood. This is a 'large' group, in the sense that it is not locally compact (provided ''M'' is not zero-dimensional).
 
===Topology===
The diffeomorphism group has two natural topologies, called the ''weak'' and ''strong'' topology {{harv|Hirsch|1997}}.  When the manifold is compact, these two topologies agree.  The weak topology is always metrizable.  When the manifold is not compact, the strong topology captures the behavior of functions "at infinity", and is not metrizable.  It is, however, still [[Baire space|Baire]].
 
Fixing a [[Riemannian metric]] on ''M'', the weak topology is the topology induced by the family of metrics
:<math>d_K(f,g) = \sup\nolimits_{x\in K} d(f(x),g(x)) + \sum\nolimits_{1\le p\le r} \sup\nolimits_{x\in K} \left \|D^pf(x) - D^pg(x) \right \|</math>
as ''K'' varies over compact subsets of ''M''.  Indeed, since ''M'' is σ-compact, there is a sequence of compact subsets ''K''<sub>''n''</sub> whose union is ''M''.  Then, define
:<math>d(f,g) = \sum\nolimits_n 2^{-n}\frac{d_{K_n}(f,g)}{1+d_{K_n}(f,g)}.</math>
 
The diffeomorphism group equipped with its weak topology is locally homeomorphic to the space of ''C<sup>r</sup>'' vector fields {{harv|Leslie|1967}}.  Over a compact subset of ''M'', this follows by fixing a Riemannian metric on ''M'' and using the [[exponential map]] for that metric. If ''r'' is finite and the manifold is compact, the space of vector fields is a [[Banach space]]. Moreover, the transition maps from one chart of this atlas to another are smooth, making the diffeomorphism group into a [[Banach manifold]].  If ''r''&nbsp;=&nbsp;∞ or if the manifold is σ-compact, the space of vector fields is a [[Fréchet space]].  Moreover, the transition maps are smooth, making the diffeomorphism group into a [[Fréchet manifold]].
 
===Lie algebra===
In particular, the [[Lie algebra]] of the diffeomorphism group of ''M'' consists of all [[vector field]]s on ''M'', equipped with the [[Lie bracket of vector fields]].  Somewhat formally, this is seen by making a small change to the coordinate x at each point in space:
: <math>x^{\mu} \to x^{\mu} + \varepsilon h^{\mu}(x)</math>
so the infinitesimal generators are the vector fields
 
:<math> L_{h} = h^{\mu}(x)\frac{\partial}{\partial x_\mu}.</math>
 
===Examples===
* When ''M''&nbsp;=&nbsp;''G'' is a [[Lie group]], there is a natural inclusion of ''G'' in its own diffeomorphism group via left-translation.  Let Diff(''G'') denote the diffeomorphism group of ''G'', then there is a splitting {{nowrap|Diff(''G'') ≃ ''G'' × Diff(''G'', ''e'')}} where Diff(''G'', ''e'') is the subgroup of Diff(''G'') that fixes the identity element of the group.
 
* The diffeomorphism group of Euclidean space '''R'''<sup>''n''</sup> consists of two components, consisting of the orientation preserving and orientation reversing diffeomorphisms.  In fact, the [[general linear group]] is a [[deformation retract]] of subgroup Diff('''R'''<sup>''n''</sup>, 0) of diffeomorphisms fixing the origin under the map {{nowrap|''f''(''x'') {{mapsto}} ''f''(''tx'')/''t''}}, ''t''&nbsp;∈&nbsp;(0,1].  Hence, in particular, the general linear group is also a deformation retract of the full diffeomorphism group as well.
 
* For a finite set of points, the diffeomorphism group is simply the symmetric group.  Similarly, if ''M'' is any manifold there is a group extension {{nowrap|0 → Diff<sub>0</sub>(''M'') → Diff(''M'') → Σ(π<sub>0</sub>(''M''))}}.  Here Diff<sub>0</sub>(''M'')is the subgroup of Diff(''M'') that preserves all the components of ''M'', and Σ(π<sub>0</sub>(''M'')) is the permutation group of the set π<sub>0</sub>(''M'') (the components of ''M'').  Moreover, the image of the map {{nowrap|Diff(''M'') → Σ(π<sub>0</sub>(''M''))}} is the bijections of π<sub>0</sub>(''M'') that preserve diffeomorphism classes.
 
===Transitivity===
For a connected manifold ''M'' the diffeomorphism group acts transitively on ''M''. More generally, the diffeomorphism group acts transitively on the [[configuration space]] ''C<sub>k</sub>M''.  If the dimension of ''M'' is at least two the diffeomorphism group acts transitively on the [[configuration space]] ''F<sub>k</sub>M'': the action on ''M'' is [[Group action#Types of actions|multiply transitive]] {{harv|Banyaga|1997|p=29}}.
 
===Extensions of diffeomorphisms===
In 1926, [[Tibor Radó]] asked whether the [[Poisson integral|harmonic extension]] of any homeomorphism (or diffeomorphism) of the [[unit circle]] to the [[unit disc]] yields a diffeomorphism on the open disc. An elegant proof was provided shortly afterwards by [[Hellmuth Kneser]] and a completely different proof was discovered in 1945 by [[Gustave Choquet]], apparently unaware that the theorem was already known.
 
The (orientation-preserving) diffeomorphism group of the circle is pathwise connected. This can be seen by noting that any such diffeomorphism can be lifted to a diffeomorphism ''f'' of the reals satisfying {{nowrap|1=''f''(''x''+1) = ''f''(''x'') + 1}}; this space is convex and hence path connected. A smooth eventually constant path to the identity gives a second more elementary way of extending a diffeomorphism from the circle to the open unit disc (this is a special case of the [[Alexander trick]]). Moreover, the diffeomorphism group of the circle has the homotopy-type of the [[orthogonal group]] O(2).
 
The corresponding extension problem for diffeomorphisms of higher dimensional spheres '''S'''<sup>''n''−1</sup> was much studied in the 1950s and 1960s, with notable contributions from [[René Thom]], [[John Milnor]] and [[Stephen Smale]]. An obstruction to such extensions is given by the [[Abelian group|finite Abelian group]] Γ<sub>''n''</sub>, the "[[Exotic sphere#Twisted spheres|group of twisted spheres]]", defined as the [[quotient group|quotient]] of the Abelian [[component group]] of the diffeomorphism group by the subgroup of classes extending to diffeomorphisms of the ball ''B''<sup>''n''</sup>.
 
===Connectedness===
For manifolds the diffeomorphism group is usually not connected. Its component group is called the [[mapping class group]]. In dimension 2, i.e. for [[surface]]s, the mapping class group is a [[finitely presented group]], generated by [[Dehn twist]]s ([[Max Dehn|Dehn]], [[W. B. R. Lickorish|Lickorish]], [[Allen Hatcher|Hatcher]]).{{Citation needed|date=December 2009}} [[Max Dehn]] and [[Jakob Nielsen (mathematician)|Jakob Nielsen]] showed that it can be identified with the [[outer automorphism group]] of the [[fundamental group]] of the surface.
 
[[William Thurston]] refined this analysis by [[Nielsen-Thurston classification|classifying elements of the mapping class group]] into three types: those equivalent to a [[Periodic function#Periodic mapping|periodic]] diffeomorphism; those equivalent to a diffeomorphism leaving a simple  closed curve invariant; and those equivalent to [[Pseudo-Anosov map|pseudo-Anosov diffeomorphisms]]. In the case of the [[torus]] '''S'''<sup>1</sup> × '''S'''<sup>1</sup> = '''R'''<sup>2</sup>/'''Z'''<sup>2</sup>, the mapping class group is just the [[modular group]] SL(2, '''Z''') and the classification reduces to the classical one in terms of [[Möbius transformation#Elliptic transforms|elliptic]], [[Möbius transformation#Parabolic transforms|parabolic]] and [[Möbius transformation#Hyperbolic transforms|hyperbolic]] matrices. Thurston accomplished his classification by observing that the mapping class group acted naturally on a [[compactification (mathematics)|compactification]] of [[Teichmüller space]]; since this enlarged space was homeomorphic to a closed ball, the [[Brouwer fixed-point theorem]] became applicable.
 
If ''M'' is an oriented  smooth closed manifold, it was conjectured by Smale that the [[identity component]] of the group of orientation-preserving diffeomorphisms is simple. This had first been proved for a product of circles by [[Michel Herman]]; it was proved in full generality by Thurston.
 
===Homotopy types===
* The diffeomorphism group of '''S'''<sup>2</sup> has the homotopy-type of the subgroup O(3).  This was proven by Steve Smale.<ref>Smale,
Diffeomorphisms of the 2-sphere, Proc. Amer. Math. Soc. 10 (1959) 621–626.</ref>
 
* The diffeomorphism group of the torus has the homotopy-type of its linear automorphisms: '''S'''<sup>1</sup> × '''S'''<sup>1</sup> × GL(2, '''Z''').
 
* The diffeomorphism groups of orientable surfaces of genus ''g'' > 1 have the homotopy-type of their mapping class groups—i.e.: the components are contractible.
 
* The homotopy-type of the diffeomorphism groups of 3-manifolds are fairly well-understood via the work of Ivanov, Hatcher, Gabai and Rubinstein although there are a few outstanding open cases, primarily 3-manifolds with finite fundamental groups.
 
* The homotopy-type of diffeomorphism groups of ''n''-manifolds for ''n'' > 3 are poorly undersood. For example, it is an open problem whether or not Diff('''S'''<sup>4</sup>) has more than two components.  But via the work of Milnor, Kahn and Antonelli it's known that Diff('''S'''<sup>''n''</sup>) does not have the homotopy-type of a finite CW-complex provided ''n'' > 6.
 
== Homeomorphism and diffeomorphism ==
It is easy to find a homeomorphism that is not a diffeomorphism, but it is more difficult to find a pair of [[homeomorphic]] manifolds that are not diffeomorphic.  In dimensions 1, 2, 3, any pair of homeomorphic smooth manifolds are diffeomorphic. In dimension 4 or greater, examples of homeomorphic but not diffeomorphic pairs have been found. The first such example was constructed by [[John Milnor]] in dimension 7. He constructed a smooth 7-dimensional manifold (called now [[Milnor's sphere]]) that is homeomorphic to the standard 7-sphere but not diffeomorphic to it. There are in fact 28 oriented diffeomorphism classes of manifolds homeomorphic to the 7-sphere (each of them is the total space of a [[fiber bundle]] over the 4-sphere with the [[3-sphere]] as the fiber).
 
Much more extreme phenomena occur for [[4-manifold]]s: in the early 1980s, a combination of results due to [[Simon Donaldson]] and [[Michael Freedman]] led to the discovery of [[exotic R4]]s:  there are uncountably many pairwise non-diffeomorphic open subsets of '''R'''<sup>4</sup> each of which is homeomorphic to '''R'''<sup>4</sup>, and also  there are  uncountably many pairwise non-diffeomorphic differentiable manifolds homeomorphic to '''R'''<sup>4</sup> that do not embed smoothly in '''R'''<sup>4</sup>.
 
== See also ==
* [[Étale morphism]]
* [[Large diffeomorphism]]
* [[Local diffeomorphism]]
* [[supermanifold|Superdiffeomorphism]]
 
== Notes ==
{{reflist}}
 
== References ==
Chaudhuri, Shyamoli, Hakuru Kawai and S.-H Henry Tye. "Path-integral formulation of closed strings," Phys. Rev. D, 36: 1148, 1987.
* {{citation
|authorlink= Augustin Banyaga
|last= Banyaga
|first= Augustin
|title= The structure of classical diffeomorphism groups
|series= Mathematics and its Applications, 400
|publisher= Kluwer Academic
|year= 1997
|isbn= 0-7923-4475-8
}}
 
* {{citation
|last= Duren
|first= Peter L.
|title= Harmonic Mappings in the Plane
|series= Cambridge Mathematical Tracts, 156
|publisher= Cambridge University Press
|year= 2004
|isbn= 0-521-64121-7
}}
 
* {{springer|title=Diffeomorphism|id=p/d031650}}
 
* {{Citation
|last1= Hirsch
|first1= Morris
|title= Differential Topology
|publisher= [[Springer-Verlag]]
|location= Berlin, New York
|isbn= 978-0-387-90148-0
|year= 1997
}}
 
* {{citation
|last= Kriegl |first= Andreas
|last2= Michor |first2= Peter
|title= The convenient setting of global analysis
|series= Mathematical Surveys and Monographs, 53
|publisher= American Mathematical Society
|year= 1997
|isbn= 0-8218-0780-3
}}
 
* {{Citation
|last1= Leslie
|first1= J. A.
|title= On a differential structure for the group of diffeomorphisms
|mr= 0210147
|year= 1967
|journal= [[Topology (journal)|Topology. an International Journal of Mathematics]]
|issn= 0040-9383
|volume= 6
|issue= 2
|pages= 263–271
|doi= 10.1016/0040-9383(67)90038-9
}}
 
* {{citation
  |authorlink= John Milnor |last= Milnor |first= John W.
  |title= Collected Works Vol. III, Differential Topology
  |publisher= American Mathematical Society
  |year= 2007
  |isbn= 0-8218-4230-7
}}
 
* {{citation
  |last=Omori |first=Hideki
  |title= Infinite-dimensional Lie groups
  |series = Translations of Mathematical Monographs, 158
  |publisher = American Mathematical Society
  |year = 1997
  |isbn = 0-8218-4575-6
}}
 
* {{citation
  |authorlink = Hellmuth Kneser |last=Kneser |first= Hellmuth
  |title= Lösung der Aufgabe 41.
  |journal = Jahresbericht der Deutschen Mathematiker-Vereinigung
  |volume = 35
  |issue = 2
  |pages = 123.
  |year = 1926
  |language = German
}}
 
[[Category:Diffeomorphisms| ]]
[[Category:Mathematical physics]]

Latest revision as of 01:44, 6 December 2014

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