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		<title>141.244.95.193: /* See also */</title>
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		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;See also&lt;/span&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;The &amp;#039;&amp;#039;&amp;#039;Hasse–Davenport relations&amp;#039;&amp;#039;&amp;#039;, introduced by {{harvs|txt|author2-link=Helmut Hasse|last2=Hasse|author1-link=Harold Davenport|last1=Davenport|year=1935}}, are two related identities for Gauss sums, one called the &amp;#039;&amp;#039;&amp;#039;Hasse–Davenport lifting relation&amp;#039;&amp;#039;&amp;#039;, and the other called the &amp;#039;&amp;#039;&amp;#039;Hasse–Davenport product relation&amp;#039;&amp;#039;&amp;#039;. The Hasse–Davenport lifting relation is an equality in [[number theory]] relating [[Gauss sum]]s over different fields. {{harvtxt|Weil|1949}} used it to calculate the zeta function of a  [[Fermat hypersurface]] over a finite field, which motivated the [[Weil conjectures]].&lt;br /&gt;
&lt;br /&gt;
Gauss sums are analogues of the [[gamma function]] over finite fields, and the Hasse–Davenport product relation is the analogue of Gauss&amp;#039;s multiplication formula&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\Gamma(z) \; \Gamma\left(z + \frac{1}{k}\right) \; \Gamma\left(z + \frac{2}{k}\right) \cdots&lt;br /&gt;
\Gamma\left(z + \frac{k-1}{k}\right) =&lt;br /&gt;
(2 \pi)^{ \frac{k-1}{2}} \; k^{1/2 - kz} \; \Gamma(kz). \,\!&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
In fact the Hasse–Davenport product relation follows from the analogous multiplication formula for &amp;#039;&amp;#039;p&amp;#039;&amp;#039;-adic gamma functions together with the [[Gross–Koblitz formula]]  of {{harvtxt|Gross|Koblitz|1979}}.&lt;br /&gt;
&lt;br /&gt;
== Hasse–Davenport lifting relation ==&lt;br /&gt;
Let &amp;#039;&amp;#039;F&amp;#039;&amp;#039; be a finite field with &amp;#039;&amp;#039;q&amp;#039;&amp;#039; elements, and &amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt; be the field such that [&amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt;:&amp;#039;&amp;#039;F&amp;#039;&amp;#039;] = &amp;#039;&amp;#039;s&amp;#039;&amp;#039;, that is, &amp;#039;&amp;#039;s&amp;#039;&amp;#039; is the [[Dimension (vector space)|dimension]] of the vector space &amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt; over &amp;#039;&amp;#039;F&amp;#039;&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;\alpha&amp;lt;/math&amp;gt; be an element of &amp;lt;math&amp;gt;F_s&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;\chi&amp;lt;/math&amp;gt; be a [[Multiplicative function|multiplicative]] [[Character (mathematics)|character]] from &amp;#039;&amp;#039;F&amp;#039;&amp;#039; to the complex numbers.&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;N_{F_s/F}(\alpha)&amp;lt;/math&amp;gt; be the norm from &amp;lt;math&amp;gt;F_s&amp;lt;/math&amp;gt; to &amp;lt;math&amp;gt;F&amp;lt;/math&amp;gt; defined by&lt;br /&gt;
:&amp;lt;math&amp;gt;N_{F_s/F}(\alpha):=\alpha\cdot\alpha^q\cdots\alpha^{q^{s-1}}.\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Let &lt;br /&gt;
&amp;lt;math&amp;gt;\chi&amp;#039;&amp;lt;/math&amp;gt; be the multiplicative character on &amp;lt;math&amp;gt;F_s&amp;lt;/math&amp;gt; which is the composition of &amp;lt;math&amp;gt;\chi&amp;lt;/math&amp;gt; with the [[Norm (mathematics)|norm]] from &amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt; to &amp;#039;&amp;#039;F&amp;#039;&amp;#039;, that is&lt;br /&gt;
:&amp;lt;math&amp;gt;\chi&amp;#039;(\alpha):=\chi(N_{F_s/F}(\alpha))&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Let ψ be some nontrivial additive character of &amp;#039;&amp;#039;F&amp;#039;&amp;#039;, and let &lt;br /&gt;
&amp;lt;math&amp;gt;\psi&amp;#039;&amp;lt;/math&amp;gt; be the additive character on &amp;lt;math&amp;gt;F_s&amp;lt;/math&amp;gt; which is the composition of &amp;lt;math&amp;gt;\psi&amp;lt;/math&amp;gt; with the [[Trace (mathematics)|trace]] from &amp;#039;&amp;#039;F&amp;#039;&amp;#039;&amp;lt;sub&amp;gt;s&amp;lt;/sub&amp;gt; to &amp;#039;&amp;#039;F&amp;#039;&amp;#039;, that is&lt;br /&gt;
:&amp;lt;math&amp;gt;\psi&amp;#039;(\alpha):=\psi(Tr_{F_s/F}(\alpha))&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Let &lt;br /&gt;
:&amp;lt;math&amp;gt;\tau(\chi,\psi)=\sum_{x\in F}\chi(x)\psi(x)&amp;lt;/math&amp;gt; &lt;br /&gt;
be the [[Gauss sum]] over &amp;#039;&amp;#039;F&amp;#039;&amp;#039;, and let&lt;br /&gt;
&amp;lt;math&amp;gt;\tau(\chi&amp;#039;,\psi&amp;#039;)&amp;lt;/math&amp;gt; be the Gauss sum over &amp;lt;math&amp;gt;F_s&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Then the &amp;#039;&amp;#039;&amp;#039;Hasse–Davenport lifting relation&amp;#039;&amp;#039;&amp;#039; states that&lt;br /&gt;
:&amp;lt;math&amp;gt;(-1)^s\cdot \tau(\chi,\psi)^s=-\tau(\chi&amp;#039;,\psi&amp;#039;).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Hasse–Davenport product relation ==&lt;br /&gt;
The Hasse–Davenport product relation states that&lt;br /&gt;
:&amp;lt;math&amp;gt;\prod_{a\bmod m} \tau(\chi\rho^a,\psi) = -\chi^{-m}(m)\tau(\chi^m,\psi)\prod_{a\bmod m} \tau(\rho^a,\psi)&amp;lt;/math&amp;gt;&lt;br /&gt;
where ρ is a multiplicative character of exact order &amp;#039;&amp;#039;m&amp;#039;&amp;#039; dividing &amp;#039;&amp;#039;q&amp;#039;&amp;#039;–1 and χ is any multiplicative character and ψ is a non-trivial additive character.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
*{{Citation | last1=Davenport | first1=Harold | last2=Hasse | first2=Helmut | title=Die Nullstellen der Kongruenzzetafunktionen in gewissen zyklischen Fällen. (On the zeros of the congruence zeta-functions in some cyclic cases) | url=http://resolver.sub.uni-goettingen.de/purl?GDZPPN002173123 | language=German | id={{Zbl|0010.33803}} | year=1935 | journal=Journal für Reine und Angewandte Mathematik | issn=0075-4102 | volume=172 | pages=151–182}}&lt;br /&gt;
*{{Citation | last1=Gross | first1=Benedict H. | last2=Koblitz | first2=Neal | author2-link=Neal Koblitz | title=Gauss sums and the p-adic Γ-function | url=http://dx.doi.org/10.2307/1971226 | doi=10.2307/1971226 | id={{MR|534763}} | year=1979 | journal=[[Annals of Mathematics|Annals of Mathematics. Second Series]] | issn=0003-486X | volume=109 | issue=3 | pages=569–581}}&lt;br /&gt;
*{{cite book&lt;br /&gt;
  | last = Ireland&lt;br /&gt;
  | first = Kenneth&lt;br /&gt;
  | first2 = Michael |last2=Rosen&lt;br /&gt;
  | title = A Classical Introduction to Modern Number Theory&lt;br /&gt;
  | publisher = Springer&lt;br /&gt;
  | year = 1990&lt;br /&gt;
  | pages = 158–162&lt;br /&gt;
  | isbn = 0-387-97329-X}}&lt;br /&gt;
*{{Citation | last1=Weil | first1=André | author1-link=André Weil | title=Numbers of solutions of equations in finite fields | url=http://www.ams.org/bull/1949-55-05/S0002-9904-1949-09219-4/home.html | doi=10.1090/S0002-9904-1949-09219-4  | mr=0029393 | year=1949 | journal=[[Bulletin of the American Mathematical Society]] | issn=0002-9904 | volume=55 | pages=497–508 | issue=5}} Reprinted in Oeuvres Scientifiques/Collected Papers by André Weil ISBN 0-387-90330-5&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Hasse-Davenport Relation}}&lt;br /&gt;
[[Category:Cyclotomic fields]]&lt;/div&gt;</summary>
		<author><name>141.244.95.193</name></author>
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