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{{Short description|Partial converse of Taylor's theorem}}&lt;br /&gt;
In [[mathematics]], in particular in [[mathematical analysis]], the '''Whitney extension theorem''' is a partial converse to [[Taylor's theorem]].  Roughly speaking, the theorem asserts that if ''A'' is a closed subset of a Euclidean space, then it is possible to extend a given function of ''A'' in such a way as to have prescribed derivatives at the points of ''A''. It is a result of [[Hassler Whitney]].&lt;br /&gt;
&lt;br /&gt;
== Statement ==&lt;br /&gt;
A precise statement of the theorem requires careful consideration of what it means to prescribe the derivative of a function on a closed set.  One difficulty, for instance, is that closed subsets of Euclidean space in general lack a differentiable structure.  The starting point, then, is an examination of the statement of Taylor's theorem.&lt;br /&gt;
&lt;br /&gt;
Given a real-valued ''C''&amp;lt;sup&amp;gt;''m''&amp;lt;/sup&amp;gt; function ''f''('''x''') on '''R'''&amp;lt;sup&amp;gt;''n''&amp;lt;/sup&amp;gt;, Taylor's theorem asserts that for each '''a''', '''x''', '''y''' ∈ '''R'''&amp;lt;sup&amp;gt;''n''&amp;lt;/sup&amp;gt;, there is a function ''R''&amp;lt;sub&amp;gt;''α''&amp;lt;/sub&amp;gt;('''x''','''y''') approaching 0 uniformly as '''x''','''y''' → '''a''' such that&lt;br /&gt;
{{NumBlk|::|&amp;lt;math&amp;gt;f({\mathbf x}) = \sum_{|\alpha|\le m} \frac{D^\alpha f({\mathbf y})}{\alpha!}\cdot ({\mathbf x}-{\mathbf y})^{\alpha}+\sum_{|\alpha|=m} R_\alpha({\mathbf x},{\mathbf y})\frac{({\mathbf x}-{\mathbf y})^\alpha}{\alpha!}&amp;lt;/math&amp;gt;|{{EquationRef|1}}}}&lt;br /&gt;
where the sum is over [[multi-index|multi-indices]]&amp;amp;nbsp;''α''.&lt;br /&gt;
&lt;br /&gt;
Let ''f''&amp;lt;sub&amp;gt;''α''&amp;lt;/sub&amp;gt; = ''D''&amp;lt;sup&amp;gt;''α''&amp;lt;/sup&amp;gt;''f'' for each multi-index ''α''.  Differentiating (1) with respect to '''x''', and possibly replacing ''R'' as needed, yields&lt;br /&gt;
{{NumBlk|::|&amp;lt;math&amp;gt;f_\alpha({\mathbf x})=\sum_{|\beta|\le m-|\alpha|}\frac{f_{\alpha+\beta}({\mathbf y})}{\beta!}({\mathbf x}-{\mathbf y})^{\beta}+R_\alpha({\mathbf x},{\mathbf y})&amp;lt;/math&amp;gt;|{{EquationRef|2}}}}&lt;br /&gt;
where ''R''&amp;lt;sub&amp;gt;''α''&amp;lt;/sub&amp;gt; is ''o''(|'''x'''&amp;amp;nbsp;&amp;amp;minus;&amp;amp;nbsp;'''y'''|&amp;lt;sup&amp;gt;''m''&amp;amp;minus;|''α''|&amp;lt;/sup&amp;gt;) uniformly as '''x''','''y''' → '''a'''.&lt;br /&gt;
&lt;br /&gt;
Note that ({{EquationNote|2}}) may be regarded as purely a compatibility condition between the functions ''f''&amp;lt;sub&amp;gt;α&amp;lt;/sub&amp;gt; which must be satisfied in order for these functions to be the coefficients of the Taylor series of the function ''f''.  It is this insight which facilitates the following statement:&lt;br /&gt;
&lt;br /&gt;
'''Theorem.'''  Suppose that ''f''&amp;lt;sub&amp;gt;''α''&amp;lt;/sub&amp;gt; are a collection of functions on a closed subset ''A'' of '''R'''&amp;lt;sup&amp;gt;''n''&amp;lt;/sup&amp;gt; for all multi-indices α with &amp;lt;math&amp;gt;|\alpha|\le m&amp;lt;/math&amp;gt; satisfying the compatibility condition ({{EquationNote|2}}) at all points ''x'', ''y'', and ''a'' of ''A''.  Then there exists a function ''F''('''x''') of class ''C''&amp;lt;sup&amp;gt;''m''&amp;lt;/sup&amp;gt; such that:&lt;br /&gt;
# ''F'' = ''f''&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; on ''A''.&lt;br /&gt;
# ''D''&amp;lt;sup&amp;gt;''α''&amp;lt;/sup&amp;gt;''F'' = ''f''&amp;lt;sub&amp;gt;''α''&amp;lt;/sub&amp;gt; on ''A''.&lt;br /&gt;
# ''F'' is real-analytic at every point of '''R'''&amp;lt;sup&amp;gt;''n''&amp;lt;/sup&amp;gt;&amp;amp;nbsp;&amp;amp;minus;&amp;amp;nbsp;''A''.&lt;br /&gt;
&lt;br /&gt;
Proofs are given in the original paper of {{harvtxt|Whitney|1934}}, and in {{harvtxt|Malgrange|1967}}, {{harvtxt|Bierstone|1980}} and {{harvtxt|Hörmander|1990}}.&lt;br /&gt;
&lt;br /&gt;
==Extension in a half space==&lt;br /&gt;
{{harvtxt|Seeley|1964}} proved a sharpening of the Whitney extension theorem in the special case of a half space. A smooth function on a half space '''R'''&amp;lt;sup&amp;gt;''n'',+&amp;lt;/sup&amp;gt; of points where ''x''&amp;lt;sub&amp;gt;''n''&amp;lt;/sub&amp;gt; ≥ 0 is a smooth function ''f'' on the interior ''x''&amp;lt;sub&amp;gt;''n''&amp;lt;/sub&amp;gt; for which the derivatives ∂&amp;lt;suP&amp;gt;α&amp;lt;/sup&amp;gt; ''f'' [[Continuous extension|extend to continuous functions]] on the half space. On the boundary ''x''&amp;lt;sub&amp;gt;''n''&amp;lt;/sub&amp;gt; = 0, ''f'' restricts to smooth function. By [[Borel's lemma]], ''f'' can be extended to a  &lt;br /&gt;
smooth function on the whole of '''R'''&amp;lt;sup&amp;gt;''n''&amp;lt;/sup&amp;gt;. Since Borel's lemma is local in nature, the same argument shows that if &amp;lt;math&amp;gt;\Omega&amp;lt;/math&amp;gt; is a (bounded or unbounded) domain in '''R'''&amp;lt;sup&amp;gt;''n''&amp;lt;/sup&amp;gt; with smooth boundary, then any smooth function on the closure of &amp;lt;math&amp;gt;\Omega&amp;lt;/math&amp;gt; can be extended to a smooth function on '''R'''&amp;lt;sup&amp;gt;''n''&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Seeley's result for a half line gives a uniform extension map&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\displaystyle{E:C^\infty(\mathbf{R}^+)\rightarrow C^\infty(\mathbf{R}),}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
which is linear, continuous (for the topology of uniform convergence of functions and their derivatives on compacta) and takes functions supported in [0,''R''] into functions supported in [−''R'',''R'']&lt;br /&gt;
&lt;br /&gt;
To define &amp;lt;math&amp;gt;E,&amp;lt;/math&amp;gt; set&amp;lt;ref&amp;gt;{{harvnb|Bierstone|1980|p=143}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\displaystyle{E(f)(x)=\sum_{m=1}^\infty a_m f(-b_mx)\varphi(-b_mx) \,\,\, (x &amp;lt; 0),}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where φ is a smooth function of compact support on ''R'' equal to 1 near 0 and the sequences (''a''&amp;lt;sub&amp;gt;''m''&amp;lt;/sub&amp;gt;), (''b''&amp;lt;sub&amp;gt;''m''&amp;lt;/sub&amp;gt;) satisfy:&lt;br /&gt;
&lt;br /&gt;
* &amp;lt;math&amp;gt;b_m &amp;gt; 0&amp;lt;/math&amp;gt; tends to &amp;lt;math&amp;gt;\infty&amp;lt;/math&amp;gt;;&lt;br /&gt;
* &amp;lt;math&amp;gt;\sum a_m b_m^j = (-1)^j&amp;lt;/math&amp;gt; for &amp;lt;math&amp;gt;j \geq 0&amp;lt;/math&amp;gt; with the sum absolutely convergent.&lt;br /&gt;
&lt;br /&gt;
A solution to this system of equations can be obtained by taking &amp;lt;math&amp;gt;b_n = 2^n&amp;lt;/math&amp;gt; and seeking an [[entire function]]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;g(z)=\sum_{m=1}^\infty a_m z^m&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
such that &amp;lt;math&amp;gt;g\left(2^j\right) = (-1)^j.&amp;lt;/math&amp;gt; That such a function can be constructed follows from the [[Weierstrass factorization theorem|Weierstrass theorem]] and [[Mittag-Leffler theorem]].&amp;lt;ref&amp;gt;{{harvnb|Ponnusamy|Silverman|2006|pp=442–443}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It can be seen directly by setting&amp;lt;ref&amp;gt;{{harvnb|Chazarain|Piriou|1982}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;W(z)=\prod_{j \ge 1} (1-z/2^j),&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
an entire function with simple zeros at &amp;lt;math&amp;gt;2^j.&amp;lt;/math&amp;gt; The derivatives ''W'' '(2&amp;lt;sup&amp;gt;''j''&amp;lt;/sup&amp;gt;) are bounded above and below. Similarly the function&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;M(z)=\sum_{j \ge 1} {(-1)^j\over W^\prime(2^j) (z-2^j)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
meromorphic with simple poles and prescribed residues at &amp;lt;math&amp;gt;2^j.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
By construction&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\displaystyle{g(z)=W(z)M(z)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
is an entire function with the required properties.&lt;br /&gt;
&lt;br /&gt;
The definition for a half space in '''R'''&amp;lt;sup&amp;gt;''n''&amp;lt;/sup&amp;gt; by applying the operator ''R'' to the last variable ''x''&amp;lt;sub&amp;gt;''n''&amp;lt;/sub&amp;gt;. Similarly, using a smooth [[partition of unity]] and a local change of variables, the result for a half space implies the existence of an analogous extending map&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\displaystyle{C^\infty(\overline{\Omega}) \rightarrow C^\infty(\mathbf{R}^n)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
for any domain &amp;lt;math&amp;gt;\Omega&amp;lt;/math&amp;gt; in '''R'''&amp;lt;sup&amp;gt;''n''&amp;lt;/sup&amp;gt; with smooth boundary.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
* The [[Kirszbraun theorem]] gives extensions of Lipschitz functions.&lt;br /&gt;
* {{annotated link|Tietze extension theorem}}&lt;br /&gt;
* {{annotated link|Hahn–Banach theorem}}&lt;br /&gt;
&lt;br /&gt;
==Notes==&lt;br /&gt;
{{reflist|2}}&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*{{citation | title=Extension of range of functions | first=Edward James | last=McShane | journal=Bull. Amer. Math. Soc. | volume=40 | issue=12 | pages=837–842 | year=1934 | mr=1562984 | zbl=0010.34606 | doi=10.1090/s0002-9904-1934-05978-0| doi-access=free }}&lt;br /&gt;
*{{citation|title=Analytic extensions of differentiable functions defined in closed sets|first=Hassler|last=Whitney|authorlink=Hassler Whitney|journal=Transactions of the American Mathematical Society|year=1934|volume=36|pages=63–89|doi=10.2307/1989708|jstor=1989708|issue=1|publisher=American Mathematical Society|doi-access=free}}&lt;br /&gt;
*{{citation|journal=Bulletin of the Brazilian Mathematical Society|volume=11|issue=2|year=1980|pages= 139–189| &lt;br /&gt;
title=Differentiable functions|first=Edward|last= Bierstone|authorlink=Edward Bierstone|doi=10.1007/bf02584636}}&lt;br /&gt;
*{{citation|last=Malgrange|first= Bernard|title= Ideals of differentiable functions|series= Tata Institute of Fundamental Research Studies in Mathematics|volume=3| publisher=Oxford University Press|year=1967}}&lt;br /&gt;
*{{citation|last=Seeley|first= R. T.|title= Extension of C∞ functions defined in a half space|journal=Proc. Amer. Math. Soc. |volume=15|year= 1964 |pages=625–626|doi=10.1090/s0002-9939-1964-0165392-8|doi-access=free}}&lt;br /&gt;
*{{citation|last=Hörmander|first= Lars|title= The analysis of linear partial differential operators. I. Distribution theory and Fourier analysis|publisher= Springer-Verlag|year=1990|isbn=3-540-00662-1}}&lt;br /&gt;
*{{citation|title=Introduction to the Theory of Linear Partial Differential Equations|volume=14|series= Studies in Mathematics and Its Applications|first=Jacques|last= Chazarain|first2= Alain|last2= Piriou|publisher=Elsevier|year= 1982|isbn=0444864520}}&lt;br /&gt;
*{{citation|last=Ponnusamy|first= S.|last2= Silverman|first2= Herb|title= Complex variables with applications|publisher=Birkhäuser|year=2006|isbn= 0-8176-4457-1}}&lt;br /&gt;
*{{citation|last=Fefferman|first=Charles|authorlink=Charles Fefferman|title=A sharp form of Whitney's extension theorem|journal=[[Annals of Mathematics]]|year=2005|pages=509–577|doi=10.4007/annals.2005.161.509|mr=2150391|volume=161|issue=1|doi-access=free}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Theorems in analysis]]&lt;/div&gt;</summary>
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