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	<entry>
		<id>https://michaelnielsen.org/polymath/index.php?title=Thue-Morse-Hedlund_Sequence&amp;diff=3513</id>
		<title>Thue-Morse-Hedlund Sequence</title>
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		<updated>2010-08-13T08:04:21Z</updated>

		<summary type="html">&lt;p&gt;Jennie: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Set &amp;lt;math&amp;gt;t_n=1&amp;lt;/math&amp;gt; or &amp;lt;math&amp;gt;t_n=-1&amp;lt;/math&amp;gt; according to whether the binary expansion of &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; has an even or an odd number of `1&#039;s. The sequence &amp;lt;math&amp;gt;(t_n)&amp;lt;/math&amp;gt; is known as the Thue-Morse-Hedlund sequence. The purpose of this website is to show that &amp;lt;math&amp;gt;\delta(N,t)\gg N^{\log_4(3)}&amp;lt;/math&amp;gt;. The proof is lifted from Newman (1969). See the discussion following [http://gowers.wordpress.com/2010/01/06/erdss-discrepancy-problem-as-a-forthcoming-polymath-project/#comment-4775 this comment] and the next one for an easy proof of &amp;lt;math&amp;gt;\gg N^{1/2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We have the generating function identity&lt;br /&gt;
&lt;br /&gt;
[http://www.casino-virtuelle.com/ casino en ligne]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_{n=0}^{2^k-1} t_n x^n = \prod_{v=0}^{k-1} (1-x^{2^v}).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Set &amp;lt;math&amp;gt;N=2^{2m}-1&amp;lt;/math&amp;gt;, which is a multiple of 3. We have&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;(1-x^3)^{-1} \prod_{v=0}^{2m-1} (1-x^{2^v}) = \left(\sum_{j=0}^{N/3} t_{3j}\right) x^N + \text{other terms}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We have&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_{j=0}^{N/3} t_{3j} = \frac{1}{2\pi i} \int_{|x|=1/2} \frac{\prod_v (1-x^{2^v})}{1-x^3} \frac{dx}{x^{N+1}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The integrand has poles at 0, &amp;lt;math&amp;gt;\omega=\exp(2\pi i/3), \omega^2&amp;lt;/math&amp;gt; (the factor &amp;lt;math&amp;gt;1-x&amp;lt;/math&amp;gt; cancels). We can push the contour to a circle of radius &amp;lt;math&amp;gt;R&amp;lt;/math&amp;gt;, and let &amp;lt;math&amp;gt;R\to\infty&amp;lt;/math&amp;gt;. As the integrand is &amp;lt;math&amp;gt;O(R^{-4})&amp;lt;/math&amp;gt;, the limit is 0. In other words,&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;0=Res[f,0]+Res[f,\omega]+Res[f,\omega^2]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
with &amp;lt;math&amp;gt;f=\frac{\prod_{v=1}^{2m-1}(1-x^{2^v})}{(x-\omega)(x-\omega^2)x^{N+1}}&amp;lt;/math&amp;gt;. We get&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;Res[f,\omega]=\lim_{x\to\omega} \frac{\prod_{v=1}^{2m-1}(1-x^{2^v})}{(x-\omega^2)x^{N+1}} = \frac{(1-\omega)^{m-1}(1-\omega^2)^m}{(\omega-\omega^2)\omega^{N+1}}=-3^{m-1}&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;Res[f,\omega^2] = - 3^{m-1}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
whence&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sum_{j=0}^{N/3} t_{3j} = Res[f,0] = 2 \cdot 3^{m-1}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and &amp;lt;math&amp;gt;\delta(N,t) = 2 \cdot 3^{m-1} = \frac23 \cdot (N+1)^{\log_4(3)}.&amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Jennie</name></author>
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