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In [[mathematics]], a real or complex-valued function ''f'' on ''d''-dimensional [[Euclidean space]] satisfies a '''Hölder condition''', or is '''Hölder continuous''', when there are nonnegative real constants ''C'', α, such that
 
: <math> | f(x) - f(y) | \leq C|x - y|^{\alpha} </math>
 
for all ''x'' and ''y'' in the domain of ''f''.  More generally, the condition can be formulated for functions between any two [[metric space]]s. The number α is called the ''exponent'' of the Hölder condition.  If α = 1, then the function satisfies a [[Lipschitz condition]]. If α = 0, then the function simply is [[bounded function|bounded]]. The condition is named after [[Otto Hölder]].
 
==Hölder spaces==
Hölder spaces consisting of functions satisfying a Hölder condition are basic in areas of [[functional analysis]] relevant to solving [[partial differential equations]], and in [[dynamical system]]s. The Hölder space ''C''<sup>''k'',α</sup>(Ω), where Ω is an open subset of some Euclidean space and ''k'' ≥ 0 an integer, consists of those functions on Ω having continuous [[derivative]]s up to order ''k'' and such that the ''k''th partial derivatives are Hölder continuous with exponent α, where 0 < α ≤ 1. This is a locally convex [[topological vector space]]. If the Hölder coefficient
 
:<math> | f |_{C^{0,\alpha}} = \sup_{x \neq y \in \Omega} \frac{| f(x) - f(y) |}{|x-y|^\alpha}, </math>
 
is finite, then the function ''f'' is said to be ''(uniformly) Hölder continuous with exponent α in Ω.'' In this case, the Hölder coefficient serves as a [[seminorm]]. If the Hölder coefficient is merely bounded on [[compact set|compact]] subsets of Ω, then the function ''f'' is said to be ''locally Hölder continuous with exponent α in Ω.''
 
If the function ''f'' and its derivatives up to order ''k'' are bounded on the closure of Ω, then the Hölder space <math>C^{k,\alpha}(\overline{\Omega})</math> can be assigned the norm
 
:<math> \| f \|_{C^{k, \alpha}} = \|f\|_{C^k}+\max_{| \beta | = k} \left | D^\beta f  \right |_{C^{0,\alpha}}</math>
 
where β ranges over [[multi-index notation|multi-indices]] and
 
:<math>\|f\|_{C^k} = \max_{| \beta | \leq k} \sup_{x\in\Omega} \left |D^\beta f (x) \right |.</math>
 
These norms and seminorms are often denoted simply <math>| f |_{0,\alpha}</math> and <math>\| f \|_{k,\alpha}</math> or also <math>| f |_{0, \alpha,\Omega}\;</math> and <math>\| f \|_{k, \alpha,\Omega}</math> in order to stress the dependence on the domain of ''f''.  If Ω is open and bounded, then <math> C^{k,\alpha}(\overline{\Omega}) </math> is a [[Banach space]] with respect to the norm <math> \|\cdot\|_{C^{k, \alpha}} </math>.
 
==Compact embedding of Hölder spaces==
Let Ω be a bounded subset of some Euclidean space (or more generally, any totally bounded metric space) and let 0 < α < β ≤ 1 two Hölder exponents. Then, there is an obvious inclusion of the corresponding Hölder spaces:
 
:<math>C^{0,\beta}(\Omega)\to C^{0,\alpha}(\Omega),</math>
 
which is continuous since, by definition of the Hölder norms, the inequality
 
:<math>| f |_{0,\alpha,\Omega}\le \mathrm{diam}(\Omega)^{\beta-\alpha} | f |_{0,\beta,\Omega}</math>
 
holds for all ''f'' in ''C''<sup>0,β</sup>(Ω). Moreover, this inclusion is compact, meaning that bounded sets in the ‖ · ‖<sub>0,β</sub> norm are relatively compact in the ‖ · ‖<sub>0,α</sub> norm. This is a direct consequence of the [[Ascoli-Arzelà theorem]]. Indeed, let (''u<sub>n</sub>'') be a bounded sequence in ''C''<sup>0,β</sup>(Ω). Thanks to the Ascoli-Arzelà theorem we can assume without loss of generality that ''u<sub>n</sub>'' → ''u'' uniformly, and we can also assume ''u'' = 0. Then
:<math>|u_n-u|_{0,\alpha}=|u_n|_{0,\alpha}\to 0,</math>
because of
:<math>\frac{|u_n(x)-u_n(y)|}{|x-y|^\alpha}=\left(\frac{|u_n(x)-u_n(y)|}{|x-y|^\beta}\right)^{\frac{\alpha}{\beta}}|u_n(x)-u_n(y)|^{1-\frac{\alpha}{\beta}}</math>
 
we have:
:<math>|u_n(x)-u_n(y)|^{1-\frac{\alpha}{\beta}}\le \left(2\|u_n\|_\infty\right)^{1-\frac{\alpha}{\beta}}=o(1).</math>
 
==Examples==
* If 0 < α ≤ β ≤ 1 then all <math>C^{0,\beta}(\overline{\Omega})</math> Hölder continuous functions on a ''bounded set'' Ω are also <math>C^{0,\alpha}(\overline{\Omega})</math> Hölder continuous. This also includes β = 1 and therefore all [[Lipschitz continuity|Lipschitz continuous]] functions on a bounded set are also ''C''<sup>0,α</sup> Hölder continuous.
 
* The function <math>f(x)=\sqrt{x}</math> defined on [0, 1] is '''not''' Lipschitz continuous, but is ''C''<sup>0,α</sup> Hölder continuous for α ≤ 1/2.
 
* In the same manner, the function ''f''(''x'') = ''x''<sup>β</sup> (with β ≤ 1) defined on [0, 1] serves as a prototypical example of a function that is ''C''<sup>0,α</sup> Hölder continuous for 0 < α ≤ β, but not for α > β.
 
* There are examples of uniformly continuous functions that are not ''α''&ndash;Hölder continuous for any α. For instance, the function defined on [0, 1/2] by ''f''(0) = 0 and by ''f''(''x'') = 1/log(''x'') otherwise is continuous, and therefore uniformly continuous by the [[Heine-Cantor theorem]].  It does not satisfy a Hölder condition of any order, however.
 
* For α > 1, any α&ndash;Hölder continuous function on [0, 1] is a constant.
 
* The [[Cantor function]] is Hölder continuous for any exponent α ≤ log(2)/log(3), and for no larger one. In the former case, the inequality of the definition holds with the constant ''C'' := 2.
 
* [[Peano curve]]s from [0, 1] onto the square [0, 1]<sup>2</sup> can be constructed to be 1/2&ndash;Hölder continuous. It can be proved that when α > 1/2, the image of a α&ndash;Hölder continuous function from the unit interval to the square cannot fill the square.
 
*A closed additive subgroup of an infinite dimensional Hilbert space ''H'', connected by α&ndash;Hölder continuous arcs with α > 1/2, is a linear subspace. There are closed additive subgroups of ''H'', not linear subspaces, connected by 1/2&ndash;Hölder continuous arcs. An example is the additive subgroup ''L''<sup>2</sup>('''R''', '''Z''') of the Hilbert space ''L''<sup>2</sup>('''R''', '''R''').
 
*Any α&ndash;Hölder continuous function ''f'' on a metric space ''X'' admits a [[modulus of continuity#Concave moduli, and Lipschitz approximation|Lipschitz approximation]] by means of a sequence of functions (''f<sub>k</sub>'') such that ''f<sub>k</sub>'' is ''k''-Lipschitz and
::<math>\|f-f_k\|_{\infty,X}=O \left (k^{-\frac{\alpha}{1-\alpha}} \right ).</math>
:Conversely, any such sequence (''f<sub>k</sub>'') of Lipschitz functions converges to an α&ndash;Hölder continuous uniform limit ''f''.
 
*Any α&ndash;Hölder function ''f'' on a subset ''X'' of a normed space ''E'' admits a [[modulus of continuity#Subadditive moduli, and extendibility|uniformly continuous extension]] to the whole space, which is Hölder continuous with the same constant ''C'' and the same exponent α. The larger such extension is:
::<math>f^*(x):=\inf_{y\in X}\left\{f(y)+C|x-y|^\alpha\right\}.</math>
 
*Functions in [[Sobolev space]] can be embedded into the appropriate Hölder space via [[Sobolev inequality#Morrey's inequality|Morrey's inequality]] if the spatial dimension is less than the exponent of the Sobolev space. To be precise, if ''n'' < ''p'' ≤ ∞ then there exists a constant ''C'', depending only on ''p'' and ''n'', such that
::<math>\|u\|_{C^{0,\gamma}(\mathbf{R}^n)}\leq C \|u\|_{W^{1,p}(\mathbf{R}^n)}</math>
:for all ''u'' ∈ ''C''<sup>1</sup>('''R'''<sup>''n''</sup>) ∩ ''L<sup>p</sup>''('''R'''<sup>''n''</sup>), where γ = 1 − (''n''/''p''). Thus if ''u'' ∈ ''W''<sup>1, ''p''</sup>('''R'''<sup>''n''</sup>), then ''u'' is in fact Hölder continuous of exponent γ, after possibly being redefined on a set of measure 0.
 
*Functions which are locally integrable and whose integrals satisfy an appropriate growth condition are also Hölder continuous. For example, if we let
::<math>u_{x,r} = \frac{1}{|B_r|} \int_{B_r(x)} u(y) dy</math>
:and ''u'' satisfies
::<math>\int_{B_r(x)} |u(y) - u_{x,r}|^2 dy \leq C r^{n+2\alpha},</math>
:then ''u'' is Hölder continuous with exponent α.<ref>See, for example, Han and Lin, Chapter 3, Section 1. This result was originally due to [[Sergio Campanato]].</ref>
 
*Functions whose ''oscillation'' decay at a fixed rate with respect to distance are Hölder continuous with an exponent that is determined by the rate of decay. For instance, if
::<math>w(u,x_0,r) = \sup_{B_r(x_0)} u - \inf_{B_r(x_0)} u</math>
:for some function ''u''(''x'') satisfies
::<math>w(u,x_0,\tfrac{r}{2}) \leq \lambda w(u,x_0,r)</math>
:for a fixed λ with 0 < λ < 1 and all sufficiently small values of ''r'', then ''u'' is Hölder continuous.
 
==Notes==
{{reflist}}
==References==
*{{cite book | author=[[Lawrence C. Evans]] | title=Partial Differential Equations | publisher=American Mathematical Society, Providence | year=1998 | isbn=0-8218-0772-2}}
*{{Cite book|first1=D.|last=Gilbarg|first2=Neil|last2=Trudinger|authorlink2=Neil Trudinger|title=Elliptic Partial Differential Equations of Second Order|publisher=Springer|publication-place=New York|year=1983|isbn=3-540-41160-7}}.
*{{Cite book|first1=Qing|last1=Han|first2=Fanghua|last2=Lin|authorlink2=Lin Fanghua|title=Elliptic Partial Differential Equations|publisher=[[Courant Institute of Mathematical Sciences]]|publication-place=New York|year=1997|isbn=0-9658703-0-8|oclc=38168365|postscript=<!-- Bot inserted parameter. Either remove it; or change its value to "." for the cite to end in a ".", as necessary. -->{{inconsistent citations}}}} {{MathSciNet|id=1669352}}
 
{{DEFAULTSORT:Holder Condition}}
[[Category:Functional analysis]]
[[Category:Lipschitz maps]]

Latest revision as of 10:49, 7 November 2013

In mathematics, a real or complex-valued function f on d-dimensional Euclidean space satisfies a Hölder condition, or is Hölder continuous, when there are nonnegative real constants C, α, such that

for all x and y in the domain of f. More generally, the condition can be formulated for functions between any two metric spaces. The number α is called the exponent of the Hölder condition. If α = 1, then the function satisfies a Lipschitz condition. If α = 0, then the function simply is bounded. The condition is named after Otto Hölder.

Hölder spaces

Hölder spaces consisting of functions satisfying a Hölder condition are basic in areas of functional analysis relevant to solving partial differential equations, and in dynamical systems. The Hölder space Ck(Ω), where Ω is an open subset of some Euclidean space and k ≥ 0 an integer, consists of those functions on Ω having continuous derivatives up to order k and such that the kth partial derivatives are Hölder continuous with exponent α, where 0 < α ≤ 1. This is a locally convex topological vector space. If the Hölder coefficient

is finite, then the function f is said to be (uniformly) Hölder continuous with exponent α in Ω. In this case, the Hölder coefficient serves as a seminorm. If the Hölder coefficient is merely bounded on compact subsets of Ω, then the function f is said to be locally Hölder continuous with exponent α in Ω.

If the function f and its derivatives up to order k are bounded on the closure of Ω, then the Hölder space can be assigned the norm

where β ranges over multi-indices and

These norms and seminorms are often denoted simply and or also and in order to stress the dependence on the domain of f. If Ω is open and bounded, then is a Banach space with respect to the norm .

Compact embedding of Hölder spaces

Let Ω be a bounded subset of some Euclidean space (or more generally, any totally bounded metric space) and let 0 < α < β ≤ 1 two Hölder exponents. Then, there is an obvious inclusion of the corresponding Hölder spaces:

which is continuous since, by definition of the Hölder norms, the inequality

holds for all f in C0,β(Ω). Moreover, this inclusion is compact, meaning that bounded sets in the ‖ · ‖0,β norm are relatively compact in the ‖ · ‖0,α norm. This is a direct consequence of the Ascoli-Arzelà theorem. Indeed, let (un) be a bounded sequence in C0,β(Ω). Thanks to the Ascoli-Arzelà theorem we can assume without loss of generality that unu uniformly, and we can also assume u = 0. Then

because of

we have:

Examples

  • In the same manner, the function f(x) = xβ (with β ≤ 1) defined on [0, 1] serves as a prototypical example of a function that is C0,α Hölder continuous for 0 < α ≤ β, but not for α > β.
  • There are examples of uniformly continuous functions that are not α–Hölder continuous for any α. For instance, the function defined on [0, 1/2] by f(0) = 0 and by f(x) = 1/log(x) otherwise is continuous, and therefore uniformly continuous by the Heine-Cantor theorem. It does not satisfy a Hölder condition of any order, however.
  • For α > 1, any α–Hölder continuous function on [0, 1] is a constant.
  • The Cantor function is Hölder continuous for any exponent α ≤ log(2)/log(3), and for no larger one. In the former case, the inequality of the definition holds with the constant C := 2.
  • Peano curves from [0, 1] onto the square [0, 1]2 can be constructed to be 1/2–Hölder continuous. It can be proved that when α > 1/2, the image of a α–Hölder continuous function from the unit interval to the square cannot fill the square.
  • A closed additive subgroup of an infinite dimensional Hilbert space H, connected by α–Hölder continuous arcs with α > 1/2, is a linear subspace. There are closed additive subgroups of H, not linear subspaces, connected by 1/2–Hölder continuous arcs. An example is the additive subgroup L2(R, Z) of the Hilbert space L2(R, R).
  • Any α–Hölder continuous function f on a metric space X admits a Lipschitz approximation by means of a sequence of functions (fk) such that fk is k-Lipschitz and
Conversely, any such sequence (fk) of Lipschitz functions converges to an α–Hölder continuous uniform limit f.
  • Any α–Hölder function f on a subset X of a normed space E admits a uniformly continuous extension to the whole space, which is Hölder continuous with the same constant C and the same exponent α. The larger such extension is:
  • Functions in Sobolev space can be embedded into the appropriate Hölder space via Morrey's inequality if the spatial dimension is less than the exponent of the Sobolev space. To be precise, if n < p ≤ ∞ then there exists a constant C, depending only on p and n, such that
for all uC1(Rn) ∩ Lp(Rn), where γ = 1 − (n/p). Thus if uW1, p(Rn), then u is in fact Hölder continuous of exponent γ, after possibly being redefined on a set of measure 0.
  • Functions which are locally integrable and whose integrals satisfy an appropriate growth condition are also Hölder continuous. For example, if we let
and u satisfies
then u is Hölder continuous with exponent α.[1]
  • Functions whose oscillation decay at a fixed rate with respect to distance are Hölder continuous with an exponent that is determined by the rate of decay. For instance, if
for some function u(x) satisfies
for a fixed λ with 0 < λ < 1 and all sufficiently small values of r, then u is Hölder continuous.

Notes

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References

  1. See, for example, Han and Lin, Chapter 3, Section 1. This result was originally due to Sergio Campanato.