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		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;External links: &lt;/span&gt; rm COI / refspam&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{redirect-distinguish|Fractional integration|Autoregressive fractionally integrated moving average}}&lt;br /&gt;
{{Calculus|expanded=Specialized calculi}}&lt;br /&gt;
&lt;br /&gt;
In [[fractional calculus]], an area of [[mathematical analysis]], the &amp;#039;&amp;#039;&amp;#039;differintegral&amp;#039;&amp;#039;&amp;#039; is a combined  [[Differential operator|differentiation]]/[[integral operator|integration]] operator. Applied to a [[function (mathematics)|function]] ƒ, the &amp;#039;&amp;#039;q&amp;#039;&amp;#039;-differintegral of &amp;#039;&amp;#039;f&amp;#039;&amp;#039;, here denoted by&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathbb{D}^q f&amp;lt;/math&amp;gt;&lt;br /&gt;
is the [[Fractional_calculus#Historical_notes|fractional derivative]] (if &amp;#039;&amp;#039;q&amp;#039;&amp;#039; &amp;gt; 0) or [[Fractional_calculus#Fractional_integrals|fractional integral]] (if &amp;#039;&amp;#039;q&amp;#039;&amp;#039; &amp;lt; 0).  If &amp;#039;&amp;#039;q&amp;#039;&amp;#039; = 0, then the &amp;#039;&amp;#039;q&amp;#039;&amp;#039;-th differintegral of a function is the function itself.  In the context of fractional integration and differentiation, there are several definitions of the differintegral.&lt;br /&gt;
&lt;br /&gt;
==Standard definitions==&lt;br /&gt;
&lt;br /&gt;
The four most common forms are:&lt;br /&gt;
&lt;br /&gt;
*The [[Riemann–Liouville differintegral]]{{pb}}This is the simplest and easiest to use, and consequently it is the most often used. It is a generalization of the [[Cauchy formula for repeated integration]] to arbitrary order. Here, &amp;lt;math&amp;gt;n = \lceil q \rceil&amp;lt;/math&amp;gt;. &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt; \begin{align}&lt;br /&gt;
{}^{RL}_a\mathbb{D}^q_tf(t) &amp;amp; = \frac{d^qf(t)}{d(t-a)^q} \\&lt;br /&gt;
&amp;amp; =\frac{1}{\Gamma(n-q)} \frac{d^n}{dt^n} \int_{a}^t (t-\tau)^{n-q-1}f(\tau)d\tau&lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
*The [[Grunwald–Letnikov differintegral]]{{pb}}The Grunwald–Letnikov differintegral is a direct generalization of the definition of a [[derivative]].  It is more difficult to use than the Riemann–Liouville differintegral, but can sometimes be used to solve problems that the Riemann–Liouville cannot. &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\begin{align}&lt;br /&gt;
{}^{GL}_a\mathbb{D}^q_tf(t) &amp;amp; = \frac{d^qf(t)}{d(t-a)^q} \\&lt;br /&gt;
&amp;amp; =\lim_{N \to \infty}\left[\frac{t-a}{N}\right]^{-q}\sum_{j=0}^{N-1}(-1)^j{q \choose j}f\left(t-j\left[\frac{t-a}{N}\right]\right)&lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
*The [[Weyl differintegral]]{{pb}} This is formally similar to the Riemann–Liouville differintegral, but applies to [[periodic function]]s, with integral zero over a period.&lt;br /&gt;
*The [[Caputo differintegral]]{{pb}}In opposite to the Riemann-Liouville differintegral, Caputo derivative of a constant &amp;lt;math&amp;gt;f(t)&amp;lt;/math&amp;gt; is equal to zero. Moreover, a form of the Laplace transform allows to simply evaluate the initial conditions by computing finite, integer-order derivatives at point &amp;lt;math&amp;gt;a&amp;lt;/math&amp;gt;. &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\begin{align}&lt;br /&gt;
{}^{C}_a\mathbb{D}^q_tf(t) &amp;amp; = \frac{d^qf(t)}{d(t-a)^q} \\&lt;br /&gt;
&amp;amp; =\frac{1}{\Gamma(n-q)} \int_{a}^t \frac{f^{(n)}(\tau)}{(t-\tau)^{q-n+1}}d\tau&lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Definitions via transforms==&lt;br /&gt;
&lt;br /&gt;
The definitions of fractional derivatives given by Liouville, Fourier, and Grunwald and Letnikov coincide.&amp;lt;ref&amp;gt;{{cite book |url=https://books.google.com/books?id=mPXzp1f7ycMC&amp;amp;pg=PA11 |first=Richard |last=Herrmann|title=Fractional Calculus: An Introduction for Physicists |year=2011 |isbn=9789814551076 }}&amp;lt;/ref&amp;gt; They can be represented via Laplace, Fourier transforms or via Newton series expansion.&lt;br /&gt;
&lt;br /&gt;
Recall the [[continuous Fourier transform]], here denoted &amp;lt;math&amp;gt; \mathcal{F}&amp;lt;/math&amp;gt;:&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt; F(\omega) =  \mathcal{F}\{f(t)\} = \frac{1}{\sqrt{2\pi}}\int_{-\infty}^\infty f(t) e^{- i\omega t}\,dt &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Using the continuous Fourier transform, in Fourier space, differentiation transforms into a multiplication:&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\mathcal{F}\left[\frac{df(t)}{dt}\right] = i \omega \mathcal{F}[f(t)]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So,&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\frac{d^nf(t)}{dt^n} = \mathcal{F}^{-1}\left\{(i \omega)^n\mathcal{F}[f(t)]\right\}&amp;lt;/math&amp;gt;&lt;br /&gt;
which generalizes to&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\mathbb{D}^qf(t) = \mathcal{F}^{-1}\left\{(i \omega)^q\mathcal{F}[f(t)]\right\}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Under the [[bilateral Laplace transform]], here denoted by &amp;lt;math&amp;gt; \mathcal{L}&amp;lt;/math&amp;gt; and defined as &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt; \mathcal{L}[f(t)] =\int_{-\infty}^\infty e^{-st} f(t)\, dt&amp;lt;/math&amp;gt;, differentiation transforms into a multiplication&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\mathcal{L}\left[\frac{df(t)}{dt}\right] = s\mathcal{L}[f(t)].&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Generalizing to arbitrary order and solving for &amp;lt;math&amp;gt; \mathbb{D}^qf(t)&amp;lt;/math&amp;gt;, one obtains&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\mathbb{D}^qf(t)=\mathcal{L}^{-1}\left\{s^q\mathcal{L}[f(t)]\right\}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Representation via Newton series is the Newton interpolation over consecutive integer orders:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\mathbb{D}^qf(t) =\sum_{m=0}^{\infty} \binom {q}m \sum_{k=0}^m\binom mk(-1)^{m-k}f^{(k)}(x).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For fractional derivative definitions described in this section, the following identities hold:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathbb{D}^q(t^n)=\frac{\Gamma(n+1)}{\Gamma(n+1-q)}t^{n-q}&amp;lt;/math&amp;gt;&lt;br /&gt;
	&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathbb{D}^q(\sin(t))=\sin \left( t+\frac{q\pi}{2} \right) &amp;lt;/math&amp;gt;&lt;br /&gt;
	&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathbb{D}^q(e^{at})=a^q e^{at}&amp;lt;/math&amp;gt;&amp;lt;ref&amp;gt;See {{cite book |page=16 |url=https://books.google.com/books?id=mPXzp1f7ycMC&amp;amp;pg=PA11 |first=Richard |last=Herrmann|title=Fractional Calculus: An Introduction for Physicists | year=2011 |isbn=9789814551076 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Basic formal properties==&lt;br /&gt;
&lt;br /&gt;
*&amp;#039;&amp;#039;[[Linear operator|Linearity]] rules&amp;#039;&amp;#039; &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\mathbb{D}^q(f+g) = \mathbb{D}^q(f)+\mathbb{D}^q(g)&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\mathbb{D}^q(af) = a\mathbb{D}^q(f)&amp;lt;/math&amp;gt;&lt;br /&gt;
*&amp;#039;&amp;#039;Zero rule&amp;#039;&amp;#039; &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\mathbb{D}^0 f = f &amp;lt;/math&amp;gt;&lt;br /&gt;
*&amp;#039;&amp;#039;Product rule&amp;#039;&amp;#039; &amp;lt;math display=&amp;quot;block&amp;quot;&amp;gt;\mathbb{D}^q_t(fg) = \sum_{j=0}^{\infty} {q \choose j}\mathbb{D}^j_t(f)\mathbb{D}^{q-j}_t(g)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In general, &amp;#039;&amp;#039;composition (or [[semigroup]]) rule&amp;#039;&amp;#039; is a desirable property, but is hard to achieve mathematically and hence is &amp;#039;&amp;#039;&amp;#039;not always completely satisfied&amp;#039;&amp;#039;&amp;#039; by each proposed operator;&amp;lt;ref&amp;gt;See {{cite book |page=75 |chapter=2. Fractional Integrals and Fractional Derivatives §2.1 Property 2.4 |chapter-url=https://books.google.com/books?id=uxANOU0H8IUC&amp;amp;pg=PA75 |first1=A. A. |last1=Kilbas |first2=H. M. |last2=Srivastava |first3=J. J. |last3=Trujillo |title=Theory and Applications of Fractional Differential Equations |publisher=Elsevier |year=2006 |isbn=9780444518323 }}&amp;lt;/ref&amp;gt; this forms part of the decision making process on which one to choose:&lt;br /&gt;
&lt;br /&gt;
* &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\mathbb{D}^a\mathbb{D}^{b}f = \mathbb{D}^{a+b}f&amp;lt;/math&amp;gt; (ideally)&lt;br /&gt;
* &amp;lt;math display=&amp;quot;inline&amp;quot;&amp;gt;\mathbb{D}^a\mathbb{D}^{b}f \neq \mathbb{D}^{a+b}f&amp;lt;/math&amp;gt; (in practice)&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Fractional-order integrator]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{Reflist}}&lt;br /&gt;
{{refbegin}}&lt;br /&gt;
*{{cite book |first=Kenneth S. |last=Miller |editor-first=Bertram |editor-last=Ross |title=An Introduction to the Fractional Calculus and Fractional Differential Equations |publisher=Wiley |year=1993 |isbn=0-471-58884-9 }}&lt;br /&gt;
*{{cite book |first1=Keith B. |last1=Oldham |first2=Jerome |last2=Spanier |title=The Fractional Calculus; Theory and Applications of Differentiation and Integration to Arbitrary Order |publisher=Academic Press |series=Mathematics in Science and Engineering |volume=V |year=1974 |isbn=0-12-525550-0 }}&lt;br /&gt;
*{{cite book |first=Igor |last=Podlubny |title=Fractional Differential Equations. An Introduction to Fractional Derivatives, Fractional Differential Equations, Some Methods of Their Solution and Some of Their Applications |publisher=Academic Press  |series=Mathematics in Science and Engineering |volume=198 |year=1998 |isbn=0-12-558840-2 }}&lt;br /&gt;
*{{cite book |editor-first=A. |editor-last=Carpinteri |editor2-first=F. |editor2-last=Mainardi |title=Fractals and Fractional Calculus in Continuum Mechanics |publisher=Springer-Verlag |year=1998 |isbn=3-211-82913-X }}&lt;br /&gt;
*{{cite book |first=F. |last=Mainardi |title=Fractional Calculus and Waves in Linear Viscoelasticity: An Introduction to Mathematical Models |publisher=Imperial College Press |year=2010 |isbn=978-1-84816-329-4 |url=http://www.worldscibooks.com/mathematics/p614.html |archive-url=https://web.archive.org/web/20120519174508/http://www.worldscibooks.com/mathematics/p614.html |url-status=dead |archive-date=2012-05-19 }}&lt;br /&gt;
*{{cite book |first=V.E. |last=Tarasov |title=Fractional Dynamics: Applications of Fractional Calculus to Dynamics of Particles, Fields and Media |publisher=Springer |year=2010 |isbn=978-3-642-14003-7 |url=https://www.springer.com/physics/complexity/book/978-3-642-14003-7|series=Nonlinear Physical Science }}&lt;br /&gt;
*{{cite book |first=V.V. |last=Uchaikin |title=Fractional Derivatives for Physicists and Engineers |publisher=Springer |year=2012 |isbn=978-3-642-33910-3 |url=https://www.springer.com/physics/theoretical,+mathematical+%26+computational+physics/book/978-3-642-33910-3|series=Nonlinear Physical Science |bibcode=2013fdpe.book.....U }}&lt;br /&gt;
*{{cite book |first1=Bruce J. |last1=West |first2=Mauro |last2=Bologna |first3=Paolo |last3=Grigolini |title=Physics of Fractal Operators |publisher=Springer Verlag |year=2003 |isbn=0-387-95554-2 |url=https://books.google.com/books?id=EgyTpQZOga0C&amp;amp;pg=PR7}}&lt;br /&gt;
{{refend}}&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
* [http://mathworld.wolfram.com/FractionalCalculus.html MathWorld – Fractional calculus]&lt;br /&gt;
*[http://mathworld.wolfram.com/FractionalDerivative.html MathWorld – Fractional derivative]&lt;br /&gt;
*Specialized journal: [http://www.diogenes.bg/fcaa/ Fractional Calculus and Applied Analysis (1998-2014)] and [http://www.degruyter.com/view/j/fca Fractional Calculus and Applied Analysis (from 2015)]&lt;br /&gt;
*Specialized journal: [https://archive.today/20120712033445/http://fde.ele-math.com/ Fractional Differential Equations (FDE)]&lt;br /&gt;
*Specialized journal: [https://web.archive.org/web/20180421124535/http://www.nonlinearscience.com/journal_2218-3892.php Communications in Fractional Calculus] ({{issn|2218-3892}})&lt;br /&gt;
* Specialized journal: [http://fcag-egypt.com/Journals/JFCA/ Journal of Fractional Calculus and Applications (JFCA)]&lt;br /&gt;
*{{cite web |first1=Carl F. |last1=Lorenzo |first2=Tom T. |last2=Hartley |title=Initialized Fractional Calculus |date=2002 |work=Information Technology |publisher=Tech Briefs Media Group |url=https://www.techbriefs.com/component/content/article/tb/techbriefs/information-sciences/2264}}&lt;br /&gt;
* https://web.archive.org/web/20040502170831/http://unr.edu/homepage/mcubed/FRG.html&lt;br /&gt;
* [http://www.tuke.sk/podlubny/fc_resources.html Igor Podlubny&amp;#039;s collection of related books, articles, links, software, etc. ]&lt;br /&gt;
*{{cite journal |first=I. |last=Podlubny |title=Geometric and physical interpretation of fractional integration and fractional differentiation |journal=Fractional Calculus and Applied Analysis |volume=5 |issue=4 |pages=367–386 |year=2002 |url=http://www.tuke.sk/podlubny/pspdf/pifcaa_r.pdf |arxiv=math.CA/0110241 |bibcode=2001math.....10241P |access-date=2004-05-18 |archive-date=2006-04-07 |archive-url=https://web.archive.org/web/20060407100616/http://www.tuke.sk/podlubny/pspdf/pifcaa_r.pdf |url-status=dead }}&lt;br /&gt;
&lt;br /&gt;
[[Category:Fractional calculus]]&lt;br /&gt;
[[Category:Generalizations of the derivative]]&lt;br /&gt;
[[Category:Linear operators in calculus]]&lt;/div&gt;</summary>
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