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		<summary type="html">&lt;p&gt;ChadwicBlunt: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The [[mathematical notation]] of &#039;&#039;&#039;multi-indices&#039;&#039;&#039; simplifies formulae used in [[multivariable calculus]], [[partial differential equation]]s and the theory of [[distribution (mathematics)|distribution]]s, by generalising the concept of an integer [[index notation|index]] to an ordered [[tuple]]  of indices. &lt;br /&gt;
&lt;br /&gt;
==Multi-index notation==&lt;br /&gt;
An &#039;&#039;n&#039;&#039;-dimensional &#039;&#039;&#039;multi-index&#039;&#039;&#039; is an &#039;&#039;n&#039;&#039;-[[tuple]]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\alpha = (\alpha_1, \alpha_2,\ldots,\alpha_n)&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
of [[natural number|non-negative integers]] (i.e. an element of the &#039;&#039;n&#039;&#039;-[[dimension]]al [[set]] of [[natural number]]s, denoted &amp;lt;math&amp;gt;\mathbb{N}^n_0&amp;lt;/math&amp;gt;). For multi-indices &amp;lt;math&amp;gt;\alpha, \beta \in \mathbb{N}^n_0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;x = (x_1, x_2, \ldots, x_n) \in \mathbb{R}^n&amp;lt;/math&amp;gt; one defines:&lt;br /&gt;
&lt;br /&gt;
;Componentwise sum and difference&lt;br /&gt;
:&amp;lt;math&amp;gt;\alpha \pm \beta= (\alpha_1 \pm \beta_1,\,\alpha_2 \pm \beta_2, \ldots, \,\alpha_n \pm \beta_n)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;[[Partial order]]&lt;br /&gt;
:&amp;lt;math&amp;gt;\alpha \le \beta \quad \Leftrightarrow \quad \alpha_i \le \beta_i \quad \forall\,i\in\{1,\ldots,n\}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;Sum of components (absolute value) &lt;br /&gt;
:&amp;lt;math&amp;gt;| \alpha | = \alpha_1 + \alpha_2 + \cdots + \alpha_n&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;[[Factorial]]&lt;br /&gt;
:&amp;lt;math&amp;gt;\alpha ! = \alpha_1! \cdot \alpha_2! \cdots \alpha_n!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;[[Binomial coefficient]]&lt;br /&gt;
:&amp;lt;math&amp;gt;\binom{\alpha}{\beta} = \binom{\alpha_1}{\beta_1}\binom{\alpha_2}{\beta_2}\cdots\binom{\alpha_n}{\beta_n} = \frac{\alpha!}{\beta!(\alpha-\beta)!}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;[[Multinomial coefficient]]&lt;br /&gt;
:&amp;lt;math&amp;gt;\binom{k}{\alpha} = \frac{k!}{\alpha_1! \alpha_2! \cdots \alpha_n! } = \frac{k!}{\alpha!} &amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;|\alpha|=k\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;[[Power (mathematics)|Power]]&lt;br /&gt;
:&amp;lt;math&amp;gt;x^\alpha = x_1^{\alpha_1} x_2^{\alpha_2} \ldots x_n^{\alpha_n}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
;Higher-order [[partial derivative]]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\partial^\alpha = \partial_1^{\alpha_1} \partial_2^{\alpha_2} \ldots \partial_n^{\alpha_n}&amp;lt;/math&amp;gt;   &lt;br /&gt;
where &amp;lt;math&amp;gt;\partial_i^{\alpha_i}:=\part^{\alpha_i} / \part x_i^{\alpha_i}&amp;lt;/math&amp;gt; (see also [[4-gradient]]).&lt;br /&gt;
&lt;br /&gt;
==Some applications==&lt;br /&gt;
The multi-index notation allows the extension of many formulae from elementary calculus to the corresponding multi-variable case. Below are some examples. In all the following, &amp;lt;math&amp;gt;x,y,h\in\mathbb{C}^n&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;\mathbb{R}^n&amp;lt;/math&amp;gt;), &amp;lt;math&amp;gt;\alpha,\nu\in\mathbb{N}_0^n&amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt;f,a_\alpha\colon\mathbb{C}^n\to\mathbb{C}&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;\mathbb{R}^n\to\mathbb{R}&amp;lt;/math&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
;[[Multinomial theorem]]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \biggl( \sum_{i=1}^n x_i\biggr)^k = \sum_{|\alpha|=k} \binom{k}{\alpha} \, x^\alpha&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;[[Multi-binomial theorem]]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; (x+y)^\alpha = \sum_{\nu \le \alpha} \binom{\alpha}{\nu} \, x^\nu y^{\alpha - \nu}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;[[Leibniz rule (generalized product rule)|Leibniz formula]]&lt;br /&gt;
For smooth functions &#039;&#039;f&#039;&#039; and &#039;&#039;g&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\partial^\alpha(fg) = \sum_{\nu \le \alpha} \binom{\alpha}{\nu} \, \partial^{\nu}f\,\partial^{\alpha-\nu}g.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;[[Taylor series]]&lt;br /&gt;
For an [[analytic function]] &#039;&#039;f&#039;&#039; in &#039;&#039;n&#039;&#039; variables one has&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;f(x+h) = \sum_{\alpha\in\mathbb{N}^n_0}^{}{\frac{\partial^{\alpha}f(x)}{\alpha !}h^\alpha}.&amp;lt;/math&amp;gt;&lt;br /&gt;
In fact, for a smooth enough function, we have the similar &#039;&#039;&#039;Taylor expansion&#039;&#039;&#039;&lt;br /&gt;
:&amp;lt;math&amp;gt;f(x+h) = \sum_{|\alpha| \le n}{\frac{\partial^{\alpha}f(x)}{\alpha !}h^\alpha}+R_{n}(x,h),&amp;lt;/math&amp;gt;&lt;br /&gt;
where the last term (the remainder) depends on the exact version of Taylor&#039;s formula. For instance, for the Cauchy formula (with integral remainder), one gets &lt;br /&gt;
:&amp;lt;math&amp;gt;R_n(x,h)= (n+1) \sum_{|\alpha| =n+1}\frac{h^\alpha}{\alpha !}\int_0^1(1-t)^n\partial^\alpha f(x+th)\,dt.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;General [[partial differential operator]]&lt;br /&gt;
A formal &#039;&#039;N&#039;&#039;-th order partial differential operator in &#039;&#039;n&#039;&#039; variables is written as&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;P(\partial) = \sum_{|\alpha| \le N}{}{a_{\alpha}(x)\partial^{\alpha}}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
;[[Integration by parts]]&lt;br /&gt;
For smooth functions with [[compact support]] in a bounded domain &amp;lt;math&amp;gt;\Omega \subset \mathbb{R}^n&amp;lt;/math&amp;gt; one has &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\int_{\Omega}{}{u(\partial^{\alpha}v)}\,dx = (-1)^{|\alpha|}\int_{\Omega}^{}{(\partial^{\alpha}u)v\,dx}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This formula is used for the definition of [[Distribution (mathematics)|distribution]]s and [[weak derivative]]s.&lt;br /&gt;
&lt;br /&gt;
==An example theorem==&lt;br /&gt;
If &amp;lt;math&amp;gt;\alpha,\beta\in\mathbb{N}^n_0&amp;lt;/math&amp;gt; are multi-indices and &amp;lt;math&amp;gt;x=(x_1,\ldots, x_n)&amp;lt;/math&amp;gt;, then&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \part^\alpha x^\beta = &lt;br /&gt;
\begin{cases} &lt;br /&gt;
\frac{\beta!}{(\beta-\alpha)!} x^{\beta-\alpha} &amp;amp; \hbox{if}\,\, \alpha\le\beta,\\ &lt;br /&gt;
 0 &amp;amp; \hbox{otherwise.} \end{cases}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Proof===&lt;br /&gt;
The proof follows from the [[power rule]] for the [[differential calculus|ordinary derivative]]; if &#039;&#039;&amp;amp;alpha;&#039;&#039; and &#039;&#039;&amp;amp;beta;&#039;&#039; are in {0,&amp;amp;nbsp;1,&amp;amp;nbsp;2,&amp;amp;nbsp;.&amp;amp;nbsp;.&amp;amp;nbsp;.}, then&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{d^\alpha}{dx^\alpha} x^\beta = \begin{cases} \frac{\beta!}{(\beta-\alpha)!} x^{\beta-\alpha} &amp;amp; \hbox{if}\,\, \alpha\le\beta, \\ 0 &amp;amp; \hbox{otherwise.} \end{cases}\qquad(1)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Suppose &amp;lt;math&amp;gt;\alpha=(\alpha_1,\ldots, \alpha_n)&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\beta=(\beta_1,\ldots, \beta_n)&amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt;x=(x_1,\ldots, x_n)&amp;lt;/math&amp;gt;. Then we have that&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\begin{align}\part^\alpha x^\beta&amp;amp;= \frac{\part^{\vert\alpha\vert}}{\part x_1^{\alpha_1} \cdots \part x_n^{\alpha_n}} x_1^{\beta_1} \cdots x_n^{\beta_n}\\&lt;br /&gt;
&amp;amp;= \frac{\part^{\alpha_1}}{\part x_1^{\alpha_1}} x_1^{\beta_1} \cdots&lt;br /&gt;
\frac{\part^{\alpha_n}}{\part x_n^{\alpha_n}} x_n^{\beta_n}.\end{align}&amp;lt;/math&amp;gt;	 &lt;br /&gt;
&lt;br /&gt;
For each &#039;&#039;i&#039;&#039; in {1,&amp;amp;nbsp;.&amp;amp;nbsp;.&amp;amp;nbsp;.,&amp;amp;nbsp;&#039;&#039;n&#039;&#039;}, the function &amp;lt;math&amp;gt;x_i^{\beta_i}&amp;lt;/math&amp;gt; only depends on &amp;lt;math&amp;gt;x_i&amp;lt;/math&amp;gt;. In the above, each partial differentiation &amp;lt;math&amp;gt;\part/\part x_i&amp;lt;/math&amp;gt; therefore reduces to the corresponding ordinary differentiation &amp;lt;math&amp;gt;d/dx_i&amp;lt;/math&amp;gt;. Hence, from equation (1), it follows that &amp;lt;math&amp;gt;\part^\alpha x^\beta&amp;lt;/math&amp;gt; vanishes if &#039;&#039;&amp;amp;alpha;&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039;&amp;amp;nbsp;&amp;gt;&amp;amp;nbsp;&#039;&#039;&amp;amp;beta;&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;&#039;&#039; for at least one &#039;&#039;i&#039;&#039; in {1,&amp;amp;nbsp;.&amp;amp;nbsp;.&amp;amp;nbsp;.,&amp;amp;nbsp;&#039;&#039;n&#039;&#039;}. If this is not the case, i.e., if &#039;&#039;&amp;amp;alpha;&#039;&#039;&amp;amp;nbsp;&amp;amp;le;&amp;amp;nbsp;&#039;&#039;&amp;amp;beta;&#039;&#039; as multi-indices, then&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{d^{\alpha_i}}{dx_i^{\alpha_i}} x_i^{\beta_i} = \frac{\beta_i!}{(\beta_i-\alpha_i)!} x_i^{\beta_i-\alpha_i}&amp;lt;/math&amp;gt;&lt;br /&gt;
for each &amp;lt;math&amp;gt;i&amp;lt;/math&amp;gt; and the theorem follows. &amp;lt;math&amp;gt;\Box&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
*[[Einstein notation]]&lt;br /&gt;
*[[Index notation]]&lt;br /&gt;
*[[Ricci calculus]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* Saint Raymond, Xavier (1991). &#039;&#039;Elementary Introduction to the Theory of Pseudodifferential Operators&#039;&#039;. Chap 1.1 . CRC Press. ISBN 0-8493-7158-9&lt;br /&gt;
&lt;br /&gt;
{{PlanetMath attribution|id=4376|title=multi-index derivative of a power}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Combinatorics]]&lt;br /&gt;
[[Category:Mathematical notation]]&lt;br /&gt;
[[Category:Articles containing proofs]]&lt;br /&gt;
&lt;br /&gt;
[[bg:Мултииндекс]]&lt;br /&gt;
[[de:Multiindex]]&lt;br /&gt;
[[fr:Multi-indice]]&lt;br /&gt;
[[it:Notazione multi-indice]]&lt;br /&gt;
[[pl:Notacja wielowskaźnikowa]]&lt;br /&gt;
[[pt:Índice múltiplo]]&lt;br /&gt;
[[ru:Мультииндекс]]&lt;br /&gt;
[[zh:多重指标]]&lt;/div&gt;</summary>
		<author><name>ChadwicBlunt</name></author>
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