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*[[Áreas temáticas|'''Áreas Temáticas''']]
 
*[[Áreas temáticas|'''Áreas Temáticas''']]
  
<!-- some LaTeX macros we want to use: -->
+
<math xmlns="http://www.w3.org/1998/Math/MathML">
$
+
   <mstyle displaystyle="true">
   \newcommand{\Re}{\mathrm{Re}\,}
+
    <mi>f</mi>
  \newcommand{\pFq}[5]{{}_{#1}\mathrm{F}_{#2} \left( \genfrac{}{}{0pt}{}{#3}{#4} \bigg| {#5} \right)}
+
    <mrow>
$
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      <mo>(</mo>
+
      <mi>a</mi>
We consider, for various values of $s$, the $n$-dimensional integral
+
      <mo>)</mo>
\begin{align}
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    </mrow>
  \label{def:Wns}
+
     <mo>=</mo>
  W_n (s)
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    <mfrac>
  &:=
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      <mn>1</mn>
  \int_{[0, 1]^n}
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      <mrow>
     \left| \sum_{k = 1}^n \mathrm{e}^{2 \pi \mathrm{i} \, x_k} \right|^s \mathrm{d}\boldsymbol{x}
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        <mn>2</mn>
\end{align}
+
        <mi>&#x3C0;</mi>
which occurs in the theory of uniform random walk integrals in the plane,
+
        <mi>i</mi>
where at each step a unit-step is taken in a random direction.  As such,
+
      </mrow>
the integral \eqref{def:Wns} expresses the $s$-th moment of the distance
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    </mfrac>
to the origin after $n$ steps.
+
    <msub>
+
      <mo>&#x222E;</mo>
By experimentation and some sketchy arguments we quickly conjectured and
+
      <mrow>
strongly believed that, for $k$ a nonnegative integer
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        <mi>&#x3B3;</mi>
\begin{align}
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      </mrow>
  \label{eq:W3k}
+
    </msub>
  W_3(k) &= \Re \, \pFq32{\frac12, -\frac k2, -\frac k2}{1, 1}{4}.
+
    <mfrac>
\end{align}
+
      <mrow>
Appropriately defined, \eqref{eq:W3k} also holds for negative odd integers.
+
        <mi>f</mi>
The reason for \eqref{eq:W3k} was  long a mystery, but it will be explained
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        <mo>(</mo>
at the end of the paper.
+
        <mi>z</mi>
 +
        <mo>)</mo>
 +
      </mrow>
 +
      <mrow>
 +
        <mi>z</mi>
 +
        <mo>&#x2212;</mo>
 +
        <mi>a</mi>
 +
      </mrow>
 +
    </mfrac>
 +
    <mi>d</mi>
 +
    <mi>z</mi>
 +
  </mstyle>
 +
</math>

Edição das 14h31min de 7 de maio de 2014

[math] \ltmstyle displaystyle="true"\gt \ltmi\gtf\lt/mi\gt \ltmrow\gt \ltmo\gt(\lt/mo\gt \ltmi\gta\lt/mi\gt \ltmo\gt)\lt/mo\gt \lt/mrow\gt \ltmo\gt=\lt/mo\gt \ltmfrac\gt \ltmn\gt1\lt/mn\gt \ltmrow\gt \ltmn\gt2\lt/mn\gt \ltmi\gtπ\lt/mi\gt \ltmi\gti\lt/mi\gt \lt/mrow\gt \lt/mfrac\gt \ltmsub\gt \ltmo\gt∮\lt/mo\gt \ltmrow\gt \ltmi\gtγ\lt/mi\gt \lt/mrow\gt \lt/msub\gt \ltmfrac\gt \ltmrow\gt \ltmi\gtf\lt/mi\gt \ltmo\gt(\lt/mo\gt \ltmi\gtz\lt/mi\gt \ltmo\gt)\lt/mo\gt \lt/mrow\gt \ltmrow\gt \ltmi\gtz\lt/mi\gt \ltmo\gt−\lt/mo\gt \ltmi\gta\lt/mi\gt \lt/mrow\gt \lt/mfrac\gt \ltmi\gtd\lt/mi\gt \ltmi\gtz\lt/mi\gt \lt/mstyle\gt [/math]