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		<title>Financial models with long-tailed distributions and volatility clustering</title>
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		<summary type="html">&lt;p&gt;195.37.142.72: /* Infinitely divisible distributions */ missing power&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[linear algebra]], a &#039;&#039;&#039;Moore matrix&#039;&#039;&#039;, introduced by {{harvs|txt|authorlink=E. H. Moore|first=E. H.| last=Moore|year=1896}}, is a  [[matrix (math)|matrix]] defined over a [[finite field]]. When it is a square matrix its  [[determinant]] is called a &#039;&#039;&#039;Moore determinant&#039;&#039;&#039; (this is unrelated to the [[Moore determinant of a quaternionic Hermitian matrix]]). The Moore matrix has successive powers of the [[Frobenius automorphism]] applied to the first column, so it is an &#039;&#039;m&#039;&#039; &amp;amp;times; &#039;&#039;n&#039;&#039; matrix&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;M=\begin{bmatrix}&lt;br /&gt;
\alpha_1 &amp;amp; \alpha_1^q &amp;amp; \dots &amp;amp; \alpha_1^{q^{n-1}}\\&lt;br /&gt;
\alpha_2 &amp;amp; \alpha_2^q &amp;amp; \dots &amp;amp; \alpha_2^{q^{n-1}}\\&lt;br /&gt;
\alpha_3 &amp;amp; \alpha_3^q &amp;amp; \dots &amp;amp; \alpha_3^{q^{n-1}}\\&lt;br /&gt;
\vdots &amp;amp; \vdots &amp;amp; \ddots &amp;amp;\vdots \\&lt;br /&gt;
\alpha_m &amp;amp; \alpha_m^q &amp;amp; \dots &amp;amp; \alpha_m^{q^{n-1}}\\&lt;br /&gt;
\end{bmatrix}&amp;lt;/math&amp;gt;&lt;br /&gt;
or&lt;br /&gt;
:&amp;lt;math&amp;gt;M_{i,j} = \alpha_i^{q^{j-1}}&amp;lt;/math&amp;gt;&lt;br /&gt;
for all indices &#039;&#039;i&#039;&#039; and &#039;&#039;j&#039;&#039;. (Some authors use the [[transpose]] of the above matrix.)&lt;br /&gt;
&lt;br /&gt;
The Moore determinant of a square Moore matrix (so &#039;&#039;m&#039;&#039; = &#039;&#039;n&#039;&#039;) can be expressed as:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\det(V) = \prod_{\mathbf{c}} \left( c_1\alpha_1 + \cdots + c_n\alpha_n \right), &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;&#039;c&#039;&#039;&#039; runs over a complete set of direction vectors, made specific by having the last non-zero entry equal to 1, i.e.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\det(V) = \prod_{1 \le i \le n} \prod_{c_1, \dots, c_{i-1}} \left( c_1\alpha_1 + \cdots + c_{i-1}\alpha_{i-1} + \alpha_i \right). &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In particular the Moore determinant vanishes if and only if the elements in the left hand column are [[linearly dependent]] over the finite field of order &#039;&#039;q&#039;&#039;. So it is analogous to the [[Wronskian]] of several functions.&lt;br /&gt;
&lt;br /&gt;
Dickson used the Moore determinant in finding the [[modular invariant of a group|modular invariants]] of the [[general linear group]] over a finite field.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Alternant matrix]]&lt;br /&gt;
* [[Vandermonde determinant]]&lt;br /&gt;
* [[List of matrices]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
*{{Citation | last1=Dickson | first1=Leonard Eugene | author1-link=Leonard Eugene Dickson | editor1-last=Magnus | editor1-first=Wilhelm | editor1-link=Wilhelm Magnus | title=Linear groups: With an exposition of the Galois field theory | origyear=1901 | url=http://www.archive.org/details/lineargroupswith00dickuoft | publisher=[[Dover Publications]] | location=New York | series=Dover Phoenix editions | isbn=978-0-486-49548-4 | mr=0104735 | year=1958}}&lt;br /&gt;
* {{cite book | authorlink=David Goss | author=David Goss | title=Basic Structures of Function Field Arithmetic | year=1996 | publisher=[[Springer Verlag]] | isbn=3-540-63541-6}}  Chapter 1.&lt;br /&gt;
*{{Citation | last1=Moore | first1=E. H. | author1-link=E. H. Moore | title=A two-fold generalization of Fermat&#039;s theorem. | doi=10.1090/S0002-9904-1896-00337-2 | jfm=27.0139.05 | year=1896 | journal=American M. S. Bull. | volume=2 | pages=189–199}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Matrices]]&lt;br /&gt;
[[Category:Determinants]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{Linear-algebra-stub}}&lt;/div&gt;</summary>
		<author><name>195.37.142.72</name></author>
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