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	<title>F_un mathematics &#187; lievenlb</title>
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	<link>http://matrix.cmi.ua.ac.be/fun</link>
	<description>ceci n'est pas un corps</description>
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		<title>Anyone interested?</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/anyone-interested.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/anyone-interested.html#comments</comments>
		<pubDate>Thu, 21 Jan 2010 13:39:05 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[media]]></category>
		<category><![CDATA[news]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=527</guid>
		<description><![CDATA[I&#8217;m about to write a series of posts on Borger&#8217;s notion of geometry over the field with one element using lambda-rings. Problem remains : where should I post them? Here, or elsewhere? In other words, are there any humans left here (or are the 50 to 60 daily hits robot-performed), and, more importantly, are any [...]]]></description>
			<content:encoded><![CDATA[<p>I&#8217;m about to write a series of posts on Borger&#8217;s notion of geometry over the field with one element using lambda-rings. Problem remains : where should I post them? Here, or elsewhere? In other words, are there any humans left here (or are the 50 to 60 daily hits robot-performed), and, more importantly, are any of those humans interested in reviving and revamping this site together?</p>

<p>Since the last activity here, there have been some interesting new Fun-developments, Connes and Consani posted at least two papers, Marcolli at least one, Manin put a new version of his cyclotomy paper online and there was even a &#8216;survey&#8217;-paper relating all different notions of Fun-geometry. So, imho, there&#8217;s plenty of new material to cover to keep the site going for a while. Interested in helping out?</p>
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		<slash:comments>6</slash:comments>
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		<item>
		<title>un dessin d&#8217;enfance</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/un-dessin-denfance.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/un-dessin-denfance.html#comments</comments>
		<pubDate>Mon, 01 Dec 2008 10:44:55 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[Manin2008]]></category>
		<category><![CDATA[news]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=504</guid>
		<description><![CDATA[Slides are available of a talk given last week in Reims on Manin's analytic F_un-geometry.]]></description>
			<content:encoded><![CDATA[<p>Last week I gave a talk at the <a href="http://loic.foissy.free.fr/colloque/programme.html">60th birthday conference for Jacques Alev</a>. If you are interested in the slides, <a href="http://matrix.cmi.ua.ac.be/fun/DATA/Alev60.pdf">here they are</a>.
The official title was supposed to be &#8220;dessins d&#8217;enfants&#8221; with this summary</p>

<blockquote>I will try to convince you that Grothendieck&#8217;s &#8216;dessins d&#8217;enfant&#8217; form an example of a noncommutative manifold over the mythical field with one element (in the sense of Soule and Connes-Consani).</blockquote>

<p>However, dessins only appear at the final slide. The main part of the talk consisted in explaining one sentence in <a href="http://matrix.cmi.ua.ac.be/fun/index.php/manin2008.html">Manin&#8217;s recent paper</a> (page 4, line 3):</p>

<blockquote>Soule&#8217;s definition of an <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-scheme <img src='/FUN/latexrender/pictures/02129bb861061d1a052c592e2dc6b383.gif' title='X' alt='X' align=absmiddle> involves besides <img src='/FUN/latexrender/pictures/ca479ec4b2acfe58ac12cca248ffc52c.gif' title='X_{\mathbb{PZ}}' alt='X_{\mathbb{PZ}}' align=absmiddle>, a <img src='/FUN/latexrender/pictures/ee77cd72573eec25fba471d91befc2d2.gif' title='\C' alt='\C' align=absmiddle>-algebra <img src='/FUN/latexrender/pictures/05eccbc64430711564758bae30372094.gif' title='\mathcal{A}_X' alt='\mathcal{A}_X' align=absmiddle>, and each cyclotomic point of <img src='/FUN/latexrender/pictures/7a8920a243e0bd71e80354f222a45475.gif' title='X_{\mathbb{Z}}' alt='X_{\mathbb{Z}}' align=absmiddle> coming from <img src='/FUN/latexrender/pictures/02129bb861061d1a052c592e2dc6b383.gif' title='X' alt='X' align=absmiddle> must assign &#8216;values&#8217; to the elements of <img src='/FUN/latexrender/pictures/05eccbc64430711564758bae30372094.gif' title='\mathcal{A}_X' alt='\mathcal{A}_X' align=absmiddle>. His choice of <img src='/FUN/latexrender/pictures/05eccbc64430711564758bae30372094.gif' title='\mathcal{A}_X' alt='\mathcal{A}_X' align=absmiddle> for the multiplicative group <img src='/FUN/latexrender/pictures/1b92a923714d2c7b5f0437ba234d6370.gif' title='\mathbb{G}_m' alt='\mathbb{G}_m' align=absmiddle> is that of continuous functions on the unit circle in <img src='/FUN/latexrender/pictures/ee77cd72573eec25fba471d91befc2d2.gif' title='\C' alt='\C' align=absmiddle>&#8230;
<strong>We suggest to consider the ring of Habiro&#8217;s analytic functions&#8230;</strong></blockquote>

<p>I promised Jacques to do a proper write-up of the talk (and include some more details on the final slide) so I might as well do a couple of posts on it, later.</p>
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		</item>
		<item>
		<title>Halloween-talk : prep-notes</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/halloween-talk-prep-notes.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/halloween-talk-prep-notes.html#comments</comments>
		<pubDate>Fri, 31 Oct 2008 12:05:51 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[KapranovSmirnov]]></category>
		<category><![CDATA[Kurokawa2005]]></category>
		<category><![CDATA[Manin1995]]></category>
		<category><![CDATA[Manin2006]]></category>
		<category><![CDATA[Manin2008]]></category>
		<category><![CDATA[news]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=481</guid>
		<description><![CDATA[The prep-notes for the halloween-talk on "F&#95;un and other ghost stories" at the <a href="http://www.math.ua.ac.be/algeo/?page_id=11">Arts</a> are available.]]></description>
			<content:encoded><![CDATA[<p>This afternoon I&#8217;ll give the first in a series of talks on F&#95;un-geometry in our <a href="http://www.math.ua.ac.be/algeo/?page_id=11">Art-seminar</a>. In the following sessions I will give a  detailed account of the construction of commutative and non-commutative algebraic geometry over <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>, but as it is <a href="http://en.wikipedia.org/wiki/Halloween">Halloween</a> today, I&#8217;ll start off with a couple of ghost-stories on conjectural applications of F&#95;un to other fields.</p>

<p>After a very brief historical intro, I&#8217;ll focus on this basic question : what geometric object is <img src='/FUN/latexrender/pictures/ff6a9905680b62d3d1694ab1e8fe6a6f.gif' title='\wis{spec}(\Z)' alt='\wis{spec}(\Z)' align=absmiddle> considered over the &#8216;absolute point&#8217; <img src='/FUN/latexrender/pictures/26b397fbe2b4e5fa6a2c293e54511339.gif' title='\wis{spec}(\mathbb{F}_1)' alt='\wis{spec}(\mathbb{F}_1)' align=absmiddle>? In particular, what is its &#8216;dimension&#8217; and what geometric object corresponds to prime numbers? I&#8217;ll follow the answers and motivations given by Yuri Manin in <a href="http://matrix.cmi.ua.ac.be/fun/index.php/manin2006.html">The notion of dimension in geometry and algebra</a>. There are (at least) three different answers to these questions :</p>

<p><strong>dim = 1</strong> : This is the classical approach we know from global field theory, <img src='/FUN/latexrender/pictures/ff6a9905680b62d3d1694ab1e8fe6a6f.gif' title='\wis{spec}(\Z)' alt='\wis{spec}(\Z)' align=absmiddle> is analogous to the affine line over a finite field, and, more generally prime ideals in number fields correspond to points on curves (over finite fields). Applications are to the Riemann hypothesis on zeta functions using the concept of &#8216;absolute motives&#8217; as in <a href="http://matrix.cmi.ua.ac.be/fun/index.php/manin1995.html">Manin&#8217;s 1995 paper</a> and recent work of <a href="http://matrix.cmi.ua.ac.be/fun/index.php/kurokawa2005.html">Kurokawa</a>.</p>

<p><strong>dim = 3</strong> : This is based on the Artin-Verdier-Mazur duality in etale topology suggesting that <img src='/FUN/latexrender/pictures/ff6a9905680b62d3d1694ab1e8fe6a6f.gif' title='\wis{spec}(\Z)' alt='\wis{spec}(\Z)' align=absmiddle> might be considered as the three-sphere <img src='/FUN/latexrender/pictures/903faf99a14b55b7ad3d1020786c49a8.gif' title='S^3' alt='S^3' align=absmiddle> with prime ideals corresponding to knots. Applications include the interpretation of power residue symbols and reciprocity laws as (higher) linking numbers as in the <a href="http://matrix.cmi.ua.ac.be/fun/index.php/kapranovsmirnov.html">Kapranov-Smirnov paper</a> and supported by recent work of Morishita.</p>

<p><strong>dim = <img src='/FUN/latexrender/pictures/7ed9abff4dafd78d08e616c899412e92.gif' title='\infty' alt='\infty' align=absmiddle></strong> : This is supported by the fact that we are unable to realize <img src='/FUN/latexrender/pictures/ff6a9905680b62d3d1694ab1e8fe6a6f.gif' title='\wis{spec}(\Z)' alt='\wis{spec}(\Z)' align=absmiddle> as an affine <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-variety. Still, in his <a href="http://matrix.cmi.ua.ac.be/fun/index.php/manin2008.html">recent paper</a>, Manin suggests that a Soule-version of Witt vectors, by restricting the values of the &#8216;ghost variables&#8217; to cyclotomic numbers, might furnish a formal <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-approximation to the elusive arithmetic line. In this set-up, primes correspond to factors of these Witt-functors as exemplified by the decomposition <img src='/FUN/latexrender/pictures/90d314cb6a6f85a6c0b3f1589575dfc5.gif' title='\hat{\Z} = \prod_p \hat{\Z}_p' alt='\hat{\Z} = \prod_p \hat{\Z}_p' align=absmiddle> of the profinite numbers.</p>

<p>My prep-notes are far from ideal and are only meant to prevent me from getting too lost in these ghost-worlds. Anyway, <a class="wmp" rel="width:700,height:500" href="http://matrix.cmi.ua.ac.be/fun/DATA/halloweennotes.pdf">here they are</a>. Comments are very wellcome!</p>

<p>I hope to turn these notes into a series of more readable posts in the upcoming days and weeks&#8230;</p>
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		</item>
		<item>
		<title>Consani on F_un</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/consani-on-f_un.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/consani-on-f_un.html#comments</comments>
		<pubDate>Tue, 28 Oct 2008 20:13:16 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[Connes-C-M-2008]]></category>
		<category><![CDATA[webcasts]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=459</guid>
		<description><![CDATA[Katia Consani gave a talk "On the notion of geometry over F&#95;un" at <a href="http://www.fields.utoronto.ca/programs/scientific/08-09/arith_hypergeo/geometry/">the Fields institute</a>.]]></description>
			<content:encoded><![CDATA[<p>Katia Consani gave a talk &#8220;On the notion of geometry over <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>&#8221; at <a href="http://www.fields.utoronto.ca/programs/scientific/08-09/arith_hypergeo/geometry/">the Fields institute</a>.</p>

<p>It is a bit odd hearing a talk without seeing any slides or blackboard images, but then, here is the streaming audio (you need to have Real Player installed).</p>

<p><a class="wmp"  href="http://av.fields.utoronto.ca:8080/ramgen/08-09/geometry/consani.rm">Consani F_un talk at Fields Institute</a></p>
]]></content:encoded>
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		<item>
		<title>noncommutative F_un geometry (2)</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/noncommutative-f_un-geometry-2.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/noncommutative-f_un-geometry-2.html#comments</comments>
		<pubDate>Thu, 16 Oct 2008 18:40:34 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[research]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=412</guid>
		<description><![CDATA[Last time, we tried to generalize the Connes-Consani approach to the noncommutative world but didn't specify what we meant by noncommutative varieties or schemes and how they were related to Grothendieck's dessins d'enfants. That's what we will do today.]]></description>
			<content:encoded><![CDATA[<p><a href="http://matrix.cmi.ua.ac.be/fun/index.php/towards-noncommutative-f_un-geometry.html">Last time</a> we tried to generalize the <a href="http://matrix.cmi.ua.ac.be/fun/index.php/connes-consani-for-undergraduates-1.html">Connes-Consani</a> approach to commutative algebraic geometry over the field with one element <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle> to the noncommutative world by considering covariant functors</p>

<p><img src='/FUN/latexrender/pictures/220d06084d8271bede9c4882cffba9ef.gif' title='N~:~\wis{groups} \rightarrow \wis{sets}' alt='N~:~\wis{groups} \rightarrow \wis{sets}' align=absmiddle></p>

<p>which over <img src='/FUN/latexrender/pictures/ee77cd72573eec25fba471d91befc2d2.gif' title='\C' alt='\C' align=absmiddle> resp. <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle> become visible by a complex (resp. integral) algebra having suitable universal properties.</p>

<p>However, we didn&#8217;t specify what we meant by a complex noncommutative variety (resp. an integral noncommutative scheme). In particular, we claimed that the <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-&#8217;points&#8217; associated to the functor</p>

<p><img src='/FUN/latexrender/pictures/f96f7838d9f36dae0d48d0f59d6094ea.gif' title='D~:~\wis{groups} \rightarrow \wis{sets} \qquad G \mapsto G_2 \times G_3' alt='D~:~\wis{groups} \rightarrow \wis{sets} \qquad G \mapsto G_2 \times G_3' align=absmiddle> (here <img src='/FUN/latexrender/pictures/3c1f98133869e157b6522ec0c5995f42.gif' title='G_n' alt='G_n' align=absmiddle> denotes all elements of order <img src='/FUN/latexrender/pictures/7b8b965ad4bca0e41ab51de7b31363a1.gif' title='n' alt='n' align=absmiddle> of <img src='/FUN/latexrender/pictures/dfcf28d0734569a6a693bc8194de62bf.gif' title='G' alt='G' align=absmiddle>)</p>

<p>were precisely the modular dessins d&#8217;enfants of Grothendieck, but didn&#8217;t give details. We&#8217;ll try to do this now.</p>

<p>For algebras over a field we follow the definition, due to <a href="http://arxiv.org/abs/math/0606241">Kontsevich and Soibelman</a>, of so called &#8220;noncommutative <strong>thin</strong> schemes&#8221;. Actually, the <strong>thinness</strong>-condition is implicit in both Soule&#8217;s-approach as that of Connes and Consani : we do not consider R-points in general, but only those of rings R which are finite and flat over our basering (or field).</p>

<p>So, what is a <strong>noncommutative thin scheme</strong> anyway? Well, its a covariant functor (commuting with finite projective limits)</p>

<p><img src='/FUN/latexrender/pictures/3e2c9b94dcebdbacb517c0d90f25e761.gif' title='\mathbb{X}~:~\wis{Alg}^{fd}_k \rightarrow \wis{sets}' alt='\mathbb{X}~:~\wis{Alg}^{fd}_k \rightarrow \wis{sets}' align=absmiddle></p>

<p>from finite-dimensional (possibly noncommutative) <img src='/FUN/latexrender/pictures/8ce4b16b22b58894aa86c421e8759df3.gif' title='k' alt='k' align=absmiddle>-algebras to sets. Now, the usual dual-space operator gives an anti-equivalence of categories</p>

<p><img src='/FUN/latexrender/pictures/831a040b86cba7fe562ccd375a921eb7.gif' title='\wis{Alg}^{fd}_k \leftrightarrow \wis{Coalg}^{fd}_k \qquad A=C^* \leftrightarrow C=A^*' alt='\wis{Alg}^{fd}_k \leftrightarrow \wis{Coalg}^{fd}_k \qquad A=C^* \leftrightarrow C=A^*' align=absmiddle></p>

<p>so a thin scheme can also be viewed as a contra-variant functor (commuting with finite direct limits)</p>

<p><img src='/FUN/latexrender/pictures/a8b0945832ccabfc36d94d6ab7092209.gif' title='\mathbb{X}~:~\wis{Coalg}^{fd}_k \rightarrow \wis{Sets}' alt='\mathbb{X}~:~\wis{Coalg}^{fd}_k \rightarrow \wis{Sets}' align=absmiddle></p>

<p>In particular, we are interested to associated to any {tex]k[/tex]-algebra <img src='/FUN/latexrender/pictures/7fc56270e7a70fa81a5935b72eacbe29.gif' title='A' alt='A' align=absmiddle> its <strong>representation functor</strong> :</p>

<p><img src='/FUN/latexrender/pictures/973cb6a4150780b1a9418e9e3161c24c.gif' title='\wis{rep}(A)~:~\wis{Coalg}^{fd}_k \rightarrow \wis{Sets} \qquad C \mapsto Alg_k(A,C^*)' alt='\wis{rep}(A)~:~\wis{Coalg}^{fd}_k \rightarrow \wis{Sets} \qquad C \mapsto Alg_k(A,C^*)' align=absmiddle></p>

<p>This may look strange at first sight, but <img src='/FUN/latexrender/pictures/0f1a0bf001f82a76496bc5b40d6efaf7.gif' title='C^*' alt='C^*' align=absmiddle> is a finite dimensional algebra and any <img src='/FUN/latexrender/pictures/7b8b965ad4bca0e41ab51de7b31363a1.gif' title='n' alt='n' align=absmiddle>-dimensional representation of <img src='/FUN/latexrender/pictures/7fc56270e7a70fa81a5935b72eacbe29.gif' title='A' alt='A' align=absmiddle> is an algebra map <img src='/FUN/latexrender/pictures/12345e625eacc69d0c09771460bd0fb6.gif' title='A \rightarrow M_n(k)' alt='A \rightarrow M_n(k)' align=absmiddle> and we take <img src='/FUN/latexrender/pictures/0d61f8370cad1d412f80b84d143e1257.gif' title='C' alt='C' align=absmiddle> to be the dual coalgebra of this image.</p>

<p>Kontsevich and Soibelman proved that every noncommutative thin scheme <img src='/FUN/latexrender/pictures/87424079238ee3bbdef326eb500ba525.gif' title='\mathbb{X}' alt='\mathbb{X}' align=absmiddle> is representable by a <img src='/FUN/latexrender/pictures/8ce4b16b22b58894aa86c421e8759df3.gif' title='k' alt='k' align=absmiddle>-coalgebra. That is, there exists a unique coalgebra <img src='/FUN/latexrender/pictures/f17b53e909f83ed42346d115698b87b8.gif' title='C_{\mathbb{X}}' alt='C_{\mathbb{X}}' align=absmiddle> (which they call the coalgebra of &#8216;distributions&#8217; of <img src='/FUN/latexrender/pictures/87424079238ee3bbdef326eb500ba525.gif' title='\mathbb{X}' alt='\mathbb{X}' align=absmiddle>) such that for every finite dimensional <img src='/FUN/latexrender/pictures/8ce4b16b22b58894aa86c421e8759df3.gif' title='k' alt='k' align=absmiddle>-algebra <img src='/FUN/latexrender/pictures/9d5ed678fe57bcca610140957afab571.gif' title='B' alt='B' align=absmiddle> we have</p>

<p><img src='/FUN/latexrender/pictures/624766c1ffce952313ded3e7e14be547.gif' title='\mathbb{X}(B) = Coalg_k(B^*,C_{\mathbb{X}})' alt='\mathbb{X}(B) = Coalg_k(B^*,C_{\mathbb{X}})' align=absmiddle></p>

<p>In the case of interest to us, that is for the functor <img src='/FUN/latexrender/pictures/25c53c37be92839fb94efcf769aaa148.gif' title='\wis{rep}(A)' alt='\wis{rep}(A)' align=absmiddle> the coalgebra of distributions is <strong>Kostant&#8217;s dual coalgebra</strong> <img src='/FUN/latexrender/pictures/8ebf546239a6ad271da355b91d2d6102.gif' title='A^o' alt='A^o' align=absmiddle>. This is the not the full linear dual of <img src='/FUN/latexrender/pictures/7fc56270e7a70fa81a5935b72eacbe29.gif' title='A' alt='A' align=absmiddle> but contains only those linear functionals on <img src='/FUN/latexrender/pictures/7fc56270e7a70fa81a5935b72eacbe29.gif' title='A' alt='A' align=absmiddle> which factor through a finite dimensional quotient.</p>

<p>So? You&#8217;ve exchanged an algebra <img src='/FUN/latexrender/pictures/7fc56270e7a70fa81a5935b72eacbe29.gif' title='A' alt='A' align=absmiddle> for some coalgebra <img src='/FUN/latexrender/pictures/8ebf546239a6ad271da355b91d2d6102.gif' title='A^o' alt='A^o' align=absmiddle>, but where&#8217;s the geometry in all this? Well, let&#8217;s look at the commutative case. Suppose <img src='/FUN/latexrender/pictures/78327fcf330f26dda2775b6d0e296d9d.gif' title='A= \C[X]' alt='A= \C[X]' align=absmiddle> is the coordinate ring of a smooth affine variety <img src='/FUN/latexrender/pictures/02129bb861061d1a052c592e2dc6b383.gif' title='X' alt='X' align=absmiddle>, then its dual coalgebra looks like</p>

<p><img src='/FUN/latexrender/pictures/0a8bbcf65c24a37837f0568e82f1668d.gif' title='\C[X]^o = \oplus_{x \in X} U(T_x(X))' alt='\C[X]^o = \oplus_{x \in X} U(T_x(X))' align=absmiddle></p>

<p>the direct sum of all universal (co)algebras of tangent spaces at points <img src='/FUN/latexrender/pictures/4202025ca33a0244467654fcec511b07.gif' title='x \in X' alt='x \in X' align=absmiddle>. But how do we get the variety out of this? Well, any coalgebra has a <strong>coradical</strong> (being the sun of all simple subcoalgebras) and in the case just mentioned we have</p>

<p><img src='/FUN/latexrender/pictures/f1f529926096ef580112b00d56b1f99d.gif' title='corad(\C[X]^o) = \oplus_{x \in X} \C e_x' alt='corad(\C[X]^o) = \oplus_{x \in X} \C e_x' align=absmiddle></p>

<p>so every point corresponds to a unique simple component of the coradical. In the general case, the coradical of the dual coalgebra <img src='/FUN/latexrender/pictures/8ebf546239a6ad271da355b91d2d6102.gif' title='A^o' alt='A^o' align=absmiddle> is the direct sum of all simple finite dimensional representations of <img src='/FUN/latexrender/pictures/7fc56270e7a70fa81a5935b72eacbe29.gif' title='A' alt='A' align=absmiddle>. That is, the direct summands of the coalgebra give us a noncommutative variety whose points are the simple representations, and the remainder of the coalgebra of distributions accounts for infinitesimal information on these points (as do the tangent spaces in the commutative case).</p>

<p>In fact, it was a surprise to me that one can describe the dual coalgebra quite explicitly, and that <img src='/FUN/latexrender/pictures/7c58535e573e641f1bb587182dfa1fa8.gif' title='A_{\infty}' alt='A_{\infty}' align=absmiddle>-structures make their appearance quite naturally. See <a href="http://arxiv.org/abs/0805.2377">this paper</a> if you&#8217;re in for the details on this.</p>

<p>That settles the problem of what we mean by the noncommutative variety associated to a complex algebra. But what about the integral case? In the above, we used extensively the theory of Kostant-duality which works only for algebras over fields&#8230;</p>

<p>Well, not quite. In the case of <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle> (or more general, of Dedekind domains) one can repeat Kostant&#8217;s proof word for word provided one takes as the definition of the dual <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle>-coalgebra
of an algebra (which is <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle>-torsion free)</p>

<p><img src='/FUN/latexrender/pictures/46d0b426355e9d3ffd50f1348b17c491.gif' title='A^o = \{ f~:~A \rightarrow \Z~:~A/Ker(f)~\text{is finitely generated and torsion free}~\}' alt='A^o = \{ f~:~A \rightarrow \Z~:~A/Ker(f)~\text{is finitely generated and torsion free}~\}' align=absmiddle></p>

<p>(over general rings there may be also variants of this duality, as in <a href="http://books.google.com/books?hl=en&amp;id=u0slIpdBjYUC&amp;dq=Joyal+Street+Quantum+groups+current+algebra&amp;printsec=frontcover&amp;source=web&amp;ots=YnWkAV4k9k&amp;sig=p9DpIEr7Ya4ssfjXlWWFDI3GndE&amp;sa=X&amp;oi=book_result&amp;resnum=4&amp;ct=result">Street&#8217;s book an Quantum groups</a>). Probably lots of people have come up with this, but the only explicit reference I have is to the <a href="http://www.math.ua.ac.be/~lebruyn/LeBruyn1981a.pdf">first paper I&#8217;ve ever written</a>. So, also for algebras over <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle> we can define a suitable noncommutative integral scheme (the coradical approach accounts only for the maximal ideals rather than all primes, but somehow this is implicit in all approaches as we consider only <strong>thin</strong> schemes).</p>

<p>Fine! So, we can make sense of the noncommutative geometrical objects corresponding to the group-algebras <img src='/FUN/latexrender/pictures/9f67100ec869296bd12a399bcc1ec6e4.gif' title='\C \Gamma' alt='\C \Gamma' align=absmiddle> and <img src='/FUN/latexrender/pictures/441a5469f757839d24deb1839e39cd21.gif' title='\Z \Gamma' alt='\Z \Gamma' align=absmiddle> where <img src='/FUN/latexrender/pictures/dbb9fd360cf27517e29bb4aa18649d08.gif' title='\Gamma = PSL_2(\Z)' alt='\Gamma = PSL_2(\Z)' align=absmiddle> is the modular group (the algebras corresponding to the <img src='/FUN/latexrender/pictures/ea8bb0d19e7aed356dcc05e8d7bcde7e.gif' title='G \mapsto G_2 \times G_3' alt='G \mapsto G_2 \times G_3' align=absmiddle>-functor). But, what might be the points of the noncommutative scheme corresponding to <img src='/FUN/latexrender/pictures/1a8d90864748c26c2c4478bf7c4892f0.gif' title='\mathbb{F}_1 \Gamma' alt='\mathbb{F}_1 \Gamma' align=absmiddle>???</p>

<p>Well, let&#8217;s continue the path cut out before. &#8220;Points&#8221; should correspond to finite dimensional &#8220;simple representations&#8221;. Hence, what are the finite dimensional simple <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-representations of <img src='/FUN/latexrender/pictures/07710b5c43702a8bb7b9104eacc6ba71.gif' title='\Gamma' alt='\Gamma' align=absmiddle>? (Or, for that matter, of any group <img src='/FUN/latexrender/pictures/dfcf28d0734569a6a693bc8194de62bf.gif' title='G' alt='G' align=absmiddle>)</p>

<p>Here we come back to <a href="http://matrix.cmi.ua.ac.be/fun/index.php/f_un-and-group-representations.html">Javier&#8217;s post on this</a> : a finite dimensional <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-vectorspace is a finite set. A <img src='/FUN/latexrender/pictures/07710b5c43702a8bb7b9104eacc6ba71.gif' title='\Gamma' alt='\Gamma' align=absmiddle>-representation on this set (of n-elements) is a group-morphism</p>

<p><img src='/FUN/latexrender/pictures/5d823e15cbcec066ba69a18a42700ce1.gif' title='\Gamma \rightarrow GL_n(\mathbb{F}_1) = S_n' alt='\Gamma \rightarrow GL_n(\mathbb{F}_1) = S_n' align=absmiddle></p>

<p>hence it gives a permutation representation of <img src='/FUN/latexrender/pictures/07710b5c43702a8bb7b9104eacc6ba71.gif' title='\Gamma' alt='\Gamma' align=absmiddle> on this set. But then, if finite dimensional <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-representations of <img src='/FUN/latexrender/pictures/07710b5c43702a8bb7b9104eacc6ba71.gif' title='\Gamma' alt='\Gamma' align=absmiddle> are the finite permutation representations, then the <strong>simple</strong> ones are the <strong>transitive</strong> permutation representations. That is, the points of the noncommutative scheme corresponding to <img src='/FUN/latexrender/pictures/1a8d90864748c26c2c4478bf7c4892f0.gif' title='\mathbb{F}_1 \Gamma' alt='\mathbb{F}_1 \Gamma' align=absmiddle> are the conjugacy classes of subgroups <img src='/FUN/latexrender/pictures/401dcae919a95fc9f2be807022f0c396.gif' title='H \subset \Gamma' alt='H \subset \Gamma' align=absmiddle> such that <img src='/FUN/latexrender/pictures/5e00c1fc9fa757c015857630bae4c6b1.gif' title='\Gamma/H' alt='\Gamma/H' align=absmiddle> is finite. But these are exactly the modular dessins d&#8217;enfants introduced by Grothendieck as I explained a while back elsewhere (see for example <a href="http://www.neverendingbooks.org/index.php/modular-quilts-and-cuboid-tree-diagrams.html">this post</a> and others in the same series).</p>
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		<title>Kapranov-Smirnov on F_un</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/kapranov-smirnov-on-f_un.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/kapranov-smirnov-on-f_un.html#comments</comments>
		<pubDate>Wed, 15 Oct 2008 19:29:08 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[quotes]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=402</guid>
		<description><![CDATA["One can postulate, of course, that spec(F&#95;un) is the absolute point, but the real problem is to develop non-trivial consequences of this point of view."]]></description>
			<content:encoded><![CDATA[<p>One of the true treasures of our <a href="http://matrix.cmi.ua.ac.be/fun/index.php/category/media/library">F_un library</a> is the unpublished paper by M. Kapranov and A. Smirnov <a href="http://matrix.cmi.ua.ac.be/fun/index.php/kapranovsmirnov.html">&#8220;Cohomology determinants and reciprocity laws: number field case&#8221;</a>.</p>

<p>It is far from easy to read (at least for me), but I&#8217;ve found every effort trying to make sense of even a single paragraph time well invested. Here are the opening lines :</p>

<p>&#8220;Analogies between number fields and function fields have been a long-time source of inspiration in arithmetic. However, one of the most intruiging problems in this approach, namely the problem of the absolute point, is still far from being satisfactorily understood.<br /></p>

<p>The scheme <img src='/FUN/latexrender/pictures/ff6a9905680b62d3d1694ab1e8fe6a6f.gif' title='\wis{spec}(\Z)' alt='\wis{spec}(\Z)' align=absmiddle>, the final object in the category of schemes, has dimension 1 with respect to the Zariski topology and at least 3 with respect to the etale topology. <br /></p>

<p>This generated a long-standing desire to introduce a more mythical object <img src='/FUN/latexrender/pictures/44c29edb103a2872f519ad0c9a0fdaaa.gif' title='P' alt='P' align=absmiddle>, the &#8220;absolute point&#8221; with a natural morphism</p>

<p><img src='/FUN/latexrender/pictures/4b6fef2f3f65afa0dd201a7bd9927ed3.gif' title='\pi_X~:~X \rightarrow P' alt='\pi_X~:~X \rightarrow P' align=absmiddle></p>

<p>given for any arithmetic scheme <img src='/FUN/latexrender/pictures/02129bb861061d1a052c592e2dc6b383.gif' title='X' alt='X' align=absmiddle> so that global invariants of <img src='/FUN/latexrender/pictures/02129bb861061d1a052c592e2dc6b383.gif' title='X' alt='X' align=absmiddle> have an interpretation in terms of a version of direct image with respect to <img src='/FUN/latexrender/pictures/ccf4c3ddc587facea92c50d48b6bbac9.gif' title='\pi_X' alt='\pi_X' align=absmiddle>.&#8221;</p>

<p>And a few paragraphs further they issue a firm warning to all who think they can attack this problem without proper preparation.</p>

<p>&#8220;First of all, it is an old idea to interpret combinatorics of finite sets as the <img src='/FUN/latexrender/pictures/cc06bf9e271cb74cbbd556dab2096545.gif' title='q \rightarrow 1' alt='q \rightarrow 1' align=absmiddle> limit of linear algebra over the finite fields <img src='/FUN/latexrender/pictures/6d2b4c3c1671bd7647831bd61e2b9f68.gif' title='\mathbb{F}_q' alt='\mathbb{F}_q' align=absmiddle>. This had lead to frequent consideration of the folklore object <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>, the &#8220;field with one element&#8221;.<br /></p>

<p><strong>One can postulate, of course, that <img src='/FUN/latexrender/pictures/26b397fbe2b4e5fa6a2c293e54511339.gif' title='\wis{spec}(\mathbb{F}_1)' alt='\wis{spec}(\mathbb{F}_1)' align=absmiddle> is the absolute point, but the real problem is to develop non-trivial consequences from this point of view.</strong>&#8220;</p>

<p>Perhaps, the <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-idea might have led to a real breakthrough if it had landed around 1930 in Germany. Whether it will do the same today, remains to be seen&#8230;</p>
]]></content:encoded>
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		</item>
		<item>
		<title>noncommutative F_un geometry (1)</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/towards-noncommutative-f_un-geometry.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/towards-noncommutative-f_un-geometry.html#comments</comments>
		<pubDate>Mon, 13 Oct 2008 19:10:03 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[Connes-Consani2008]]></category>
		<category><![CDATA[research]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=344</guid>
		<description><![CDATA[It is perhaps surprising that Alain Connes and Katia Consani, two icons of noncommutative geometry, restrict themselves to define <strong>commutative</strong> algebraic geometry over the field with one element. Remains the fact that their approach screams for a noncommutative extension.]]></description>
			<content:encoded><![CDATA[<p>It is perhaps surprising that Alain Connes and Katia Consani, two icons of noncommutative geometry, restrict themselves to define <strong>commutative</strong> algebraic geometry over <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>, the field with one element.</p>

<p>My guess of why they stop there is as good as anyone&#8217;s. Perhaps they felt that there is already enough noncommutativity in Soule&#8217;s gadget-approach (the algebra <img src='/FUN/latexrender/pictures/05eccbc64430711564758bae30372094.gif' title='\mathcal{A}_X' alt='\mathcal{A}_X' align=absmiddle> as in <a href="http://matrix.cmi.ua.ac.be/fun/index.php/gadgets-a-la-soule.html">this post</a> may very well be noncommutative). Perhaps they were only interested in the Bost-Connes system which can be entirely encoded in their commutative <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-geometry. Perhaps they felt unsure as to what the noncommutative scheme of an affine noncommutative algebra might be. Perhaps &#8230;</p>

<p>Remains the fact that their approach screams for a noncommutative extension. Their basic object is a covariant functor</p>

<p><img src='/FUN/latexrender/pictures/556e076c38de8261dc7835f1fbecff3f.gif' title='N~:~\wis{abelian} \rightarrow \wis{sets} \qquad A \mapsto N(A)' alt='N~:~\wis{abelian} \rightarrow \wis{sets} \qquad A \mapsto N(A)' align=absmiddle></p>

<p>from finite abelian groups to sets, together with additional data to the effect that there is a unique minimal integral scheme associated to <img src='/FUN/latexrender/pictures/8d9c307cb7f3c4a32822a51922d1ceaa.gif' title='N' alt='N' align=absmiddle>. In a series of posts on the Connes-Consani paper (starting <a href="http://matrix.cmi.ua.ac.be/fun/index.php/connes-consani-for-undergraduates-1.html">here</a>) I took some care of getting rid of all scheme-lingo and rephrasing everything entirely into algebras. But then, this set-up can be extended verbatim to noncommuative <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-geometry, which should start from a covariant functor</p>

<p><img src='/FUN/latexrender/pictures/220d06084d8271bede9c4882cffba9ef.gif' title='N~:~\wis{groups} \rightarrow \wis{sets}' alt='N~:~\wis{groups} \rightarrow \wis{sets}' align=absmiddle></p>

<p>from all finite groups to sets. Let&#8217;s recall quickly what the additional info should be making this functor a noncommutative (affine) F&#95;un scheme :</p>

<p>There should be a finitely generated <img src='/FUN/latexrender/pictures/ee77cd72573eec25fba471d91befc2d2.gif' title='\C' alt='\C' align=absmiddle>-algebra <img src='/FUN/latexrender/pictures/e1e1d3d40573127e9ee0480caf1283d6.gif' title='R' alt='R' align=absmiddle> together with a natural transformation (the &#8216;evaluation&#8217;)</p>

<p><img src='/FUN/latexrender/pictures/8c3afdd5ca72e3f5dff988e805cb2697.gif' title='e~:~N \rightarrow \wis{maxi}(R) \qquad N(G) \mapsto Hom_{\C-alg}(R, \C G)' alt='e~:~N \rightarrow \wis{maxi}(R) \qquad N(G) \mapsto Hom_{\C-alg}(R, \C G)' align=absmiddle></p>

<p>(both <img src='/FUN/latexrender/pictures/e1e1d3d40573127e9ee0480caf1283d6.gif' title='R' alt='R' align=absmiddle> and the group-algebra <img src='/FUN/latexrender/pictures/2e4a76a99dfbdcc71eb1788004eadcb2.gif' title='\C G' alt='\C G' align=absmiddle> may be noncommutative). The pair <img src='/FUN/latexrender/pictures/c99201bf35e7e2936dc7c070f8a52d47.gif' title='(N, \wis{maxi}(R))' alt='(N, \wis{maxi}(R))' align=absmiddle> is then called a gadget and there is an obvious notion of &#8216;morphism&#8217; between gadgets.</p>

<p>The crucial extra ingredient is an affine <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle>-algebra (possibly noncommutative) <img src='/FUN/latexrender/pictures/5dbc98dcc983a70728bd082d1a47546e.gif' title='S' alt='S' align=absmiddle>
such that <img src='/FUN/latexrender/pictures/8d9c307cb7f3c4a32822a51922d1ceaa.gif' title='N' alt='N' align=absmiddle> is a subfunctor of <img src='/FUN/latexrender/pictures/f4e021d7d3608dd44bc4dff7abd5602b.gif' title='\wis{mini}(S)~:~G \mapsto Hom_{\Z-alg}(S,\Z G)' alt='\wis{mini}(S)~:~G \mapsto Hom_{\Z-alg}(S,\Z G)' align=absmiddle> together with the following universal property :</p>

<p>any affine <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle>-algebra <img src='/FUN/latexrender/pictures/b9ece18c950afbfa6b0fdbfa4ff731d3.gif' title='T' alt='T' align=absmiddle> having a gadget-morphism <img src='/FUN/latexrender/pictures/745c86514b4f4757196f905310f3ef89.gif' title='~(N,\wis{maxi}(R)) \rightarrow (\wis{mini}(T),\wis{maxi}(T \otimes_{\Z} \C))' alt='~(N,\wis{maxi}(R)) \rightarrow (\wis{mini}(T),\wis{maxi}(T \otimes_{\Z} \C))' align=absmiddle> comes from a <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle>-algebra morphism <img src='/FUN/latexrender/pictures/a757b668f0f1a122a8a95087a2214ed1.gif' title='T \rightarrow S' alt='T \rightarrow S' align=absmiddle>. (If this sounds too cryptic for you, please read the series on C-C mentioned before).</p>

<p>So, there is no problem in defining noncommutative affine F&#95;un-schemes. However, as with any generalization, this only makes sense provided (a) we get something new and (b) we have interesting examples, not covered by the restricted theory.</p>

<p>At first sight we do not get something new as in the only example we did in the C-C-series (the forgetful functor) it is easy to prove (using the same proof as given in <a href="http://matrix.cmi.ua.ac.be/fun/index.php/connes-consani-for-undergraduates-3.html">this post</a>) that the forgetful-functor <img src='/FUN/latexrender/pictures/f9e448bababa2ae7d05a093f55f5488a.gif' title='\wis{groups} \rightarrow \wis{sets}' alt='\wis{groups} \rightarrow \wis{sets}' align=absmiddle> still has as its integral form the integral torus <img src='/FUN/latexrender/pictures/e3d4bec6c9a471771dcfbd613a74510b.gif' title='\Z[x,x^{-1}]' alt='\Z[x,x^{-1}]' align=absmiddle>. However, both theories quickly diverge beyond this example.</p>

<p>For example, consider the functor</p>

<p><img src='/FUN/latexrender/pictures/e3d0a9205ba4caede128b720bab7123d.gif' title='\wis{groups} \rightarrow \wis{sets} \qquad G \mapsto G \times G' alt='\wis{groups} \rightarrow \wis{sets} \qquad G \mapsto G \times G' align=absmiddle></p>

<p>Then, if we restrict to abelian finite groups <img src='/FUN/latexrender/pictures/c3a4ef9ef1948b24315bd47983059e71.gif' title='\wis{abelian}' alt='\wis{abelian}' align=absmiddle> it is easy to see (again by a similar argument) that the two-dimensional integer torus <img src='/FUN/latexrender/pictures/14ea5c4e0623fb8f5d6028ea0b4baded.gif' title='\Z[x,y,x^{-1},y^{-1}]' alt='\Z[x,y,x^{-1},y^{-1}]' align=absmiddle> is the correct integral form. However, this algebra cannot be the correct form for the functor on the category of all finite groups as any <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle>-algebra map <img src='/FUN/latexrender/pictures/dd6942bd7d91bf502831f29b2a21407e.gif' title='\phi~:~\Z[x,y,x^{-1},y^{-1}] \rightarrow \Z G' alt='\phi~:~\Z[x,y,x^{-1},y^{-1}] \rightarrow \Z G' align=absmiddle> determines (and is determined by) a pair of <strong>commuting</strong> units in <img src='/FUN/latexrender/pictures/f11e6a65915746e47f0180ead7b480c8.gif' title='\Z G' alt='\Z G' align=absmiddle>, so the above functor can not be a subfunctor if we allow non-Abelian groups.</p>

<p>But then, perhaps there isn&#8217;t a minimal integral <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle>-form for this functor? Well, yes there is. Take the <strong>free group</strong> in two letters (that is, all words in noncommuting <img src='/FUN/latexrender/pictures/0eba98d3b1ffa6586336bc51a0ee7c2c.gif' title='x,y,x^{-1}' alt='x,y,x^{-1}' align=absmiddle> and <img src='/FUN/latexrender/pictures/7f3509943ed45dca6bc7253ad677e248.gif' title='y^{-1}' alt='y^{-1}' align=absmiddle> satisfying only the trivial cancellation laws between a letter and its inverse), then the corresponding integral group-algebra <img src='/FUN/latexrender/pictures/9153f883c612988f5505a1c9a54a5721.gif' title='\Z \mathcal{F}_2' alt='\Z \mathcal{F}_2' align=absmiddle> does the trick.</p>

<p>Again, the proof-strategy is the same. Given a gadget-morphism we have an algebra map <img src='/FUN/latexrender/pictures/e1f8a2aae2ee29c3380c002d58f10655.gif' title='f~:~T \mapsto \C \mathcal{F}_2' alt='f~:~T \mapsto \C \mathcal{F}_2' align=absmiddle> and we have to show, using the universal property that the image of <img src='/FUN/latexrender/pictures/b9ece18c950afbfa6b0fdbfa4ff731d3.gif' title='T' alt='T' align=absmiddle> is contained in the integral group-algebra <img src='/FUN/latexrender/pictures/9153f883c612988f5505a1c9a54a5721.gif' title='\Z \mathcal{F}_2' alt='\Z \mathcal{F}_2' align=absmiddle>. Take a generator
<img src='/FUN/latexrender/pictures/fbade9e36a3f36d3d676c1b808451dd7.gif' title='z' alt='z' align=absmiddle> of <img src='/FUN/latexrender/pictures/b9ece18c950afbfa6b0fdbfa4ff731d3.gif' title='T' alt='T' align=absmiddle> then the degree of the image <img src='/FUN/latexrender/pictures/b23d8bcdb490736c53d5b677455a8cd2.gif' title='f(z)' alt='f(z)' align=absmiddle> is bounded say by <img src='/FUN/latexrender/pictures/8277e0910d750195b448797616e091ad.gif' title='d' alt='d' align=absmiddle> and we can always find a subgroup <img src='/FUN/latexrender/pictures/ac474f7d1044009276b686fb6f12bf85.gif' title='H \subset \mathcal{F}_2' alt='H \subset \mathcal{F}_2' align=absmiddle> such that <img src='/FUN/latexrender/pictures/39528ae5dec855f8464042886118a250.gif' title='\mathcal{F}_2/H' alt='\mathcal{F}_2/H' align=absmiddle> is a fnite group and the quotient map <img src='/FUN/latexrender/pictures/c669dcf2af878fb987733ea982b5a882.gif' title='\C \mathcal{F}_2 \rightarrow \C \mathcal{F}_2/H' alt='\C \mathcal{F}_2 \rightarrow \C \mathcal{F}_2/H' align=absmiddle> is injective on the subspace spanned by all words of degree strictly less than <img src='/FUN/latexrender/pictures/765f09f9b6abc99f555c131a5475b9db.gif' title='d+1' alt='d+1' align=absmiddle>. Then, the usual diagram-chase finishes the proof.</p>

<p>What makes this work is that the free group <img src='/FUN/latexrender/pictures/0c61ec6c9b3500dcab0d1db1db88ecd8.gif' title='\mathcal{F}_2' alt='\mathcal{F}_2' align=absmiddle> has &#8216;enough&#8217; subgroups of finite index, a property it shares with many interesting discrete groups. Whence the blurb-message :</p>

<p><strong>if the integers <img src='/FUN/latexrender/pictures/1458a437b3c6456f9ebf61d46c9ed13e.gif' title='\Z' alt='\Z' align=absmiddle> see a discrete group <img src='/FUN/latexrender/pictures/07710b5c43702a8bb7b9104eacc6ba71.gif' title='\Gamma' alt='\Gamma' align=absmiddle>, then the field <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle> sees its profinite completion <img src='/FUN/latexrender/pictures/1ba3a9b99264a6e87528f70185abb016.gif' title='\hat{\Gamma} = \underset{\leftarrow}{lim}~\Gamma/ H' alt='\hat{\Gamma} = \underset{\leftarrow}{lim}~\Gamma/ H' align=absmiddle></strong></p>

<p><img src="http://matrix.cmi.ua.ac.be/fun/DATA/grothendieckserre.jpg" align=left > So, yes, we get something new by extending the Connes-Consani approach to the noncommutative world, but do we have interesting examples? As &#8220;interesting&#8221; is a subjective qualification, we&#8217;d better invoke the authority-argument.</p>

<p><a href="http://en.wikipedia.org/wiki/Alexander_Grothendieck">Alexander Grothendieck</a> (sitting on the right, manifestly <strong>not</strong> disputing a vacant chair with Jean-Pierre Serre, drinking on the left (a marvelous picture taken by F. Hirzebruch in 1958)) was pushing the idea that profinite completions of arithmetical groups were useful in the study of the absolute Galois group <img src='/FUN/latexrender/pictures/3aadea961997fae6a7cab08024f6bdd0.gif' title='Gal(\overline{\mathbb{Q}}/\mathbb{Q})' alt='Gal(\overline{\mathbb{Q}}/\mathbb{Q})' align=absmiddle>, via his theory of <a href="http://en.wikipedia.org/wiki/Dessin_d'enfant">dessins d&#8217;enfants</a> (children;s drawings).</p>

<p>In a previous life, I&#8217;ve written a <a href="http://www.neverendingbooks.org/index.php/the-best-rejected-proposal-ever.html">series of posts</a> on dessins d&#8217;enfants, so I&#8217;ll restrict here to the basics. A smooth projective <img src='/FUN/latexrender/pictures/72f8bff84956a57bc22ae12ebcc186e4.gif' title='\overline{\mathbb{Q}}' alt='\overline{\mathbb{Q}}' align=absmiddle>-curve <img src='/FUN/latexrender/pictures/02129bb861061d1a052c592e2dc6b383.gif' title='X' alt='X' align=absmiddle> has a Belyi-map <img src='/FUN/latexrender/pictures/787b7794a09a64ef0a5e0a9ce1cba8a8.gif' title='X \rightarrow \mathbb{P}^1_{\overline{\mathbb{Q}}}' alt='X \rightarrow \mathbb{P}^1_{\overline{\mathbb{Q}}}' align=absmiddle> ramified only in three points <img src='/FUN/latexrender/pictures/b1ac14b500ebd79fac7ec4feaffbedfd.gif' title='\{ 0,1,\infty \}' alt='\{ 0,1,\infty \}' align=absmiddle>. The &#8220;drawing&#8221; corresponding to <img src='/FUN/latexrender/pictures/02129bb861061d1a052c592e2dc6b383.gif' title='X' alt='X' align=absmiddle> is a bipartite graph, drawn on the Riemann surface <img src='/FUN/latexrender/pictures/d9929d78f8782355570c407fc2c7115b.gif' title='X_{\C}' alt='X_{\C}' align=absmiddle> obtained by lifting the unit interval <img src='/FUN/latexrender/pictures/ccfcd347d0bf65dc77afe01a3306a96b.gif' title='[0,1]' alt='[0,1]' align=absmiddle> to <img src='/FUN/latexrender/pictures/02129bb861061d1a052c592e2dc6b383.gif' title='X' alt='X' align=absmiddle>. As the absolute Galois group acts on all such curves (and hence on their corresponding drawings), the action of it on these dessins d&#8217;enfants may give us a way into the multiple mysteries of the absolute Galois group.</p>

<p>In his <a href="http://www.math.jussieu.fr/~leila/grothendieckcircle/EsquisseFr.pdf">&#8220;Esquisse d&#8217;un programme&#8221;</a> (<a href="http://www.math.jussieu.fr/~leila/grothendieckcircle/EsquisseEng.pdf">Sketch of a program</a> if you prefer to read it in English) he writes :</p>

<p>&#8220;C&#8217;est ainsi que mon attention s&#8217;est portÃ©e vers ce que j&#8217;ai appelÃ© depuis la <strong>&#8220;gÃ©omÃ©trie algÃªbrique anabÃ©lienne&#8221;</strong>, dont le point de dÃ©part est justement une Ã©tude (pour le moment limitÃ©e Ã  la caractÃ©ristique zÃ©ro) de l&#8217;action de groupe de Galois &#8220;absolus&#8221; (notamment les groupes <img src='/FUN/latexrender/pictures/ff18717c543f7d4dab0640196317e50e.gif' title='Gal(\overline{K}/K)' alt='Gal(\overline{K}/K)' align=absmiddle>, ou <img src='/FUN/latexrender/pictures/a5f3c6a11b03839d46af9fb43c97c188.gif' title='K' alt='K' align=absmiddle> est une extension de type fini du corps premier) sur des groupes fondamentaux gÃ©omÃ©triques (profinis) de variÃ©tÃ©s algÃ©briques (dÃ©finies sur <img src='/FUN/latexrender/pictures/a5f3c6a11b03839d46af9fb43c97c188.gif' title='K' alt='K' align=absmiddle>), et plus particuliÃ¨rement (rompant avec une tradition bien enracinÃ©e) des groupes fondamentaux qui sont trÃ©s Ã©loignÃ©s des groupes abÃ©liens (et que pour cette raison je nomme &#8220;anabÃ©liens&#8221;). Parmi ces groupes, et trÃ©s proche du groupe <img src='/FUN/latexrender/pictures/ff20d676c1bdcf4295f123e067e0e5cc.gif' title='\hat{\pi}_{0,3}' alt='\hat{\pi}_{0,3}' align=absmiddle>, il y a le compactifiÃ© profini du groupe modulaire <img src='/FUN/latexrender/pictures/c8a5c475ac3118e6f6f9239d51c55eec.gif' title='SL_2(\mathbb{Z})' alt='SL_2(\mathbb{Z})' align=absmiddle>, dont le quotient par le centre <img src='/FUN/latexrender/pictures/967ffa3ca82c4b8aad1075067fb3fec5.gif' title='\pm 1' alt='\pm 1' align=absmiddle> contient le prÃ©cÃ©dent comme sous-groupe de congruence mod 2, et peut s&#8217;interprÃ©ter d&#8217;ailleurs comme groupe &#8220;cartographique&#8221; orientÃ©, savoir celui qui classifie les cartes orientÃ©es triangulÃ©es (i.e. celles dont les faces des triangles ou des monogones).&#8221;</p>

<p>and a bit further, he writes :</p>

<p>&#8220;L&#8217;Ã©lÃ©ment de structure de <img src='/FUN/latexrender/pictures/c8a5c475ac3118e6f6f9239d51c55eec.gif' title='SL_2(\mathbb{Z})' alt='SL_2(\mathbb{Z})' align=absmiddle> qui me fascine avant tout, est bien sur l&#8217;action extÃ©rieure du groupe de Galois <img src='/FUN/latexrender/pictures/d571de1334315e15323218f6acb5e390.gif' title='Gal(\overline{\Q}/\Q)' alt='Gal(\overline{\Q}/\Q)' align=absmiddle> sur le compactifiÃ© profini. Par le thÃ©orÃ¨me de Bielyi, prenant les compactifiÃ©s profinis de sous-groupes d&#8217;indice fini de <img src='/FUN/latexrender/pictures/c8a5c475ac3118e6f6f9239d51c55eec.gif' title='SL_2(\mathbb{Z})' alt='SL_2(\mathbb{Z})' align=absmiddle>, et l&#8217;action extÃ©rieure induite (quitte Ã  passer Ã©galement Ã  un sous-groupe overt de <img src='/FUN/latexrender/pictures/a39e20800c1a029c811302b0630af1d4.gif' title='Gal(\overline{\Q},\Q)' alt='Gal(\overline{\Q},\Q)' align=absmiddle>),  on trouve essentiellement les groupes fondamentaux de toutes les courbes algÃ©briques dÃ©finis sur des corps de nombres <img src='/FUN/latexrender/pictures/a5f3c6a11b03839d46af9fb43c97c188.gif' title='K' alt='K' align=absmiddle>, et l&#8217;action extÃ©rieure de <img src='/FUN/latexrender/pictures/ff18717c543f7d4dab0640196317e50e.gif' title='Gal(\overline{K}/K)' alt='Gal(\overline{K}/K)' align=absmiddle> dessus.&#8221;</p>

<p>So, is there a noncommutative affine variety over <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle> of which the unique minimal integral model is the integral group algebra of the modular group <img src='/FUN/latexrender/pictures/441a5469f757839d24deb1839e39cd21.gif' title='\Z \Gamma' alt='\Z \Gamma' align=absmiddle> (with <img src='/FUN/latexrender/pictures/dbb9fd360cf27517e29bb4aa18649d08.gif' title='\Gamma = PSL_2(\Z)' alt='\Gamma = PSL_2(\Z)' align=absmiddle>? Yes, here it is</p>

<p><img src='/FUN/latexrender/pictures/83f60da2e412964cb99464351ba17306.gif' title='N_{\Gamma}~:~\wis{groups} \rightarrow \wis{sets} \qquad G \mapsto G_2 \times G_3' alt='N_{\Gamma}~:~\wis{groups} \rightarrow \wis{sets} \qquad G \mapsto G_2 \times G_3' align=absmiddle></p>

<p>where <img src='/FUN/latexrender/pictures/3c1f98133869e157b6522ec0c5995f42.gif' title='G_n' alt='G_n' align=absmiddle> is the set of all elements of order <img src='/FUN/latexrender/pictures/7b8b965ad4bca0e41ab51de7b31363a1.gif' title='n' alt='n' align=absmiddle> in <img src='/FUN/latexrender/pictures/dfcf28d0734569a6a693bc8194de62bf.gif' title='G' alt='G' align=absmiddle>. The reason behind this is that the modular group is the free group product <img src='/FUN/latexrender/pictures/625446d319dcbcfc9925b05937f20d4c.gif' title='C_2 \ast C_3' alt='C_2 \ast C_3' align=absmiddle>.</p>

<p>Fine, you may say, but all this is just algebra. Where is the noncommutative complex variety or the noncommutative integral scheme in all this? Well, we can introduce them too but as this post is already 1300 words long, I&#8217;ll better leave this for <a href="http://matrix.cmi.ua.ac.be/fun/index.php/noncommutative-f_un-geometry-2.html">another time</a>. In case you cannot stop thinking about it, here&#8217;s the short answer.</p>

<p>The complex noncommutative variety has as its &#8216;points&#8217; all finite dimensional simple complex representations of the modular group, and the &#8216;points&#8217; of the noncommutative <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>-scheme are exactly the (modular) dessins d&#8217;enfants&#8230;</p>
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		<title>Andre Weil on the Riemann hypothesis</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/andre-weil-on-the-rh.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/andre-weil-on-the-rh.html#comments</comments>
		<pubDate>Sun, 12 Oct 2008 19:51:57 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[featured]]></category>
		<category><![CDATA[outreach]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=335</guid>
		<description><![CDATA[Don't be fooled by introductory remarks to the effect that 'the field with one element was conceived by Jacques Tits...' Let's have it out into the open : F_un mathematics' goal is no less than proving the Riemann Hypothesis.]]></description>
			<content:encoded><![CDATA[<p>Don&#8217;t be fooled by introductory remarks to the effect that &#8216;the field with one element was conceived by Jacques Tits half a century ago, etc. etc.&#8217;</p>

<p>While this is a historic fact, and, Jacques Tits cannot be given enough credit for bringing a touch of surrealism into mathematics, but this is not the main drive for people getting into F_un, today.</p>

<p>There is a much deeper and older motivation behind most papers published recently on  <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>. Few of the authors will be willing to let you in on the secret, though, because if they did, it would sound much too presumptuous&#8230;</p>

<p>So, let&#8217;s have it out into the open : <strong>F_un mathematics&#8217; goal is no less than proving the <a href="http://en.wikipedia.org/wiki/Riemann_hypothesis">Riemann Hypothesis</a></strong>.</p>

<p>And even then, authors hide behind a smoke screen. The &#8216;official&#8217; explanation being &#8220;we would like to copy Weil&#8217;s proof of the Riemann hypothesis in the case of function fields of curves over finite fields, by considering spec(Z) as a &#8216;curve&#8217; over an algebra &#8216;dessous&#8217; Z namely <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>&#8220;. Alas, at this moment, none of the geometric approaches over the field with one element can make this stick.</p>

<p>Believe me for once, the main <a href="http://planetmath.org/encyclopedia/KroneckersJugendtraum.html">Jugendtraum</a> of most authors is to get a grip on cyclotomy over <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>. It is no accident that Connes makes a dramatic pauze in his <a href="http://matrix.cmi.ua.ac.be/fun/index.php/connes-on-youtube.html">YouTubeVideo</a> to let the viewer see this equation on the backboard</p>

<p><img src='/FUN/latexrender/pictures/f7f6ec8b3668baad324e0d24e8cd31e4.gif' title='\mathbb{F}_{1^n} \otimes_{\mathbb{F}_1} \Z = \Z[x]/(x^n-1)' alt='\mathbb{F}_{1^n} \otimes_{\mathbb{F}_1} \Z = \Z[x]/(x^n-1)' align=absmiddle></p>

<p>But, what is the basis of all this childlike enthusiasm? A somewhat concealed clue is given in the introduction of the <a href="http://matrix.cmi.ua.ac.be/fun/index.php/kapranovsmirnov.html">Kapranov-Smirnov paper</a>. They write :</p>

<p>&#8220;In [?] the affine line over <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle> was considered; it consists formally of 0 and all the roots of unity. Put slightly differently, this leads to the consideration of &#8220;algebraic extensions&#8221; of <img src='/FUN/latexrender/pictures/8d70c57340e9aa1ea22100d150e22714.gif' title='\mathbb{F}_1' alt='\mathbb{F}_1' align=absmiddle>. By analogy with genuine finite fields we would like to think that there is exactly one such extension of any given degree n, denote it by <img src='/FUN/latexrender/pictures/2c6b29321e4cadc35730bf7f8bf5c372.gif' title='\mathbb{F}_{1^n}' alt='\mathbb{F}_{1^n}' align=absmiddle>.</p>

<p>Of course, <img src='/FUN/latexrender/pictures/2c6b29321e4cadc35730bf7f8bf5c372.gif' title='\mathbb{F}_{1^n}' alt='\mathbb{F}_{1^n}' align=absmiddle> does not exist in a rigorous sense, but we can think if a scheme <img src='/FUN/latexrender/pictures/02129bb861061d1a052c592e2dc6b383.gif' title='X' alt='X' align=absmiddle> contains n-th roots of unity, then it is defined over <img src='/FUN/latexrender/pictures/2c6b29321e4cadc35730bf7f8bf5c372.gif' title='\mathbb{F}_{1^n}' alt='\mathbb{F}_{1^n}' align=absmiddle>, so that there is a morphism</p>

<p><img src='/FUN/latexrender/pictures/3c2bf75f7900de279e26739fbab32f15.gif' title='p_X~:~X \rightarrow spec(\mathbb{F}_{1^n}' alt='p_X~:~X \rightarrow spec(\mathbb{F}_{1^n}' align=absmiddle></p>

<p><strong>The point of view that adjoining roots of unity is analogous to the extension of the base field goes back, at least to Weil (Lettre a Artin, Ouvres, vol 1) and Iwasawa&#8230;</strong>&#8220;</p>

<p>Okay, so rush down to your library, pick out the first of three volumes of Andre Weil&#8217;s collected works, look up his letter to Emil Artin written on July 10th 1942 (19 printed pages!), and head for the final section. Weil writes :</p>

<p><img src="http://matrix.cmi.ua.ac.be/fun/DATA/andreweil1.jpg" align=right> &#8220;Our proof of the Riemann hypothesis (in the function field case, red.) depended upon the extension of the function-fields by roots of unity, i.e. by constants; the way in which the Galois group of such extensions operates on the classes of divisors in the original field and its extensions gives a linear operator, the characteristic roots (i.e. the eigenvalues) of which are the roots of the zeta-function.</p>

<p>On a number field, the nearest we can get to this is by adjunction of <img src='/FUN/latexrender/pictures/ae131293bb0d8d0df32a71e52fc4078b.gif' title='l^n' alt='l^n' align=absmiddle>-th roots of unity, <img src='/FUN/latexrender/pictures/2db95e8e1a9267b7a1188556b2013b33.gif' title='l' alt='l' align=absmiddle> being fixed; the Galois group of this infinite extension is cyclic, and defines a linear operator on the projective limit of the (absolute) class groups of those successive finite extensions; <strong>this should have something to do with the roots of the zeta-function of the field</strong>. However, our extensions are ramified (but only at a finite number of places, viz. the prime divisors of <img src='/FUN/latexrender/pictures/2db95e8e1a9267b7a1188556b2013b33.gif' title='l' alt='l' align=absmiddle>). Thus a preliminary study of similar problems in function-fields might enable one to guess what will happen in number-fields.&#8221;</p>

<p>A few years later, in 1947, he makes this a bit more explicit in his marvelous essay &#8220;L&#8217;avenir des mathematiques&#8221; (The future of mathematics). Weil is still in shell-shock after the events of the second WW, and writes in beautiful archaic French sentences lasting forever :</p>

<p>&#8220;L&#8217;hypothÃ¨se de Riemann, aprÃ¨s qu&#8217;on eut perdu l&#8217;espoir de la dÃ©montrer par les mÃ©thodes de la thÃ©orie des fonctions, nous apparaÃ®t aujourd&#8217;hui sous un jour nouveau, qui la montre insÃ©parable de la conjecture d&#8217;Artin sur les fonctions L, ces deux problÃ¨mes Ã©tant deux aspects d&#8217;une mÃªme question arithmÃ©tico-algÃ©brique, <strong>oÃ¹ l&#8217;Ã©tude simultanÃ©e de toutes les extensions cyclotomiques d&#8217;un corps de nombres donnÃ© jouera sans doute le rÃ´le dÃ©cisif</strong>.</p>

<p>L&#8217;arithmÃ©tique gaussienne gravitait autour de la loi de rÃ©ciprocitÃ© quadratique; nous savons maintenant que celle-ci n&#8217;est qu&#8217;un premier example, ou pour mieux dire le paradigme, des lois dites &#8220;du corps de classe&#8221;, qui gouvernent les extensions abÃ©liennes des corps de nobres algÃ©briques; nous savons formuler ces lois de maniÃ¨re Ã  leur donner l&#8217;aspect d&#8217;un ensemble cohÃ©rent; mais, si plaisante Ã  l&#8217;Å“il que soit cette faÃ§ade, nous ne savons si elle ne masque pas des symmÃ©tries plus cachÃ©es.</p>

<p>Les automorphismes induits sur les groupes de classes par les automorphismes du corps, les propriÃ©tÃ©s des restes de normes dans les cas non cycliques, le passage Ã  la limite (inductive ou projective) <strong>quand on remplace le corps de base par des extensions, par example cyclotomiques, de degrÃ© indÃ©finiment croissant, sont autant de questions sur lesquelles notre ignorance est Ã  peu prÃ¨s complÃ¨te, et dont l&#8217;Ã©tude contient peut-Ãªtre la clef de l&#8217;hypothese de Riemann</strong>; Ã©troitement liÃ©e Ã  celles-ci est l&#8217;Ã©tude du conducteur d&#8217;Artin, et en particulier, dans le cas local, la recherche de la reprÃ©sentation dont la trace s&#8217;exprime au moyen des caractÃ¨res simples avec des coefficients Ã©gaux aux exposants de leurs conducteurs.</p>

<p>Ce sont lÃ  quelques-unes des directions qu&#8217;on peut et qu&#8217;on doit songer Ã  suivre afin de pÃ©nÃ©trer dans le mystÃ¨re des extensions non abÃ©liennes; il n&#8217;est pas impossible que nous touchions lÃ  Ã  des principes d&#8217;une fÃ©conditÃ© extraordinaire, et que le premier pas dÃ©cisif une fois fait dans cette voie doive nous ouvrir l&#8217;accÃ¨s Ã  de vastes domaines dont nous soupÃ§onnons Ã  peine l&#8217;existence; car jusqu&#8217;ici, pour amples que soient nos gÃ©nÃ©ralisations des rÃ©sultats de Gauss, on ne peut dire que nous les ayons vraiment dÃ©passÃ©s.&#8221;</p>
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		<title>Fields Institute Workshop</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/fields-institute-workshop.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/fields-institute-workshop.html#comments</comments>
		<pubDate>Sun, 12 Oct 2008 08:31:07 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[news]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=337</guid>
		<description><![CDATA[The Fields Institute organizes a Workshop on Arithmetic Geometry with talks by Soule, Consani and Durov a.o. and topics including Arakelov geometry ('including the infinity-adic') and 'Generalized rings and schemes'.]]></description>
			<content:encoded><![CDATA[<p>From october 20-24 there will be a <a href="http://www.fields.utoronto.ca/programs/scientific/08-09/arith_hypergeo/geometry/index.html">Workshop on Arithmetic Geometry: Diophantine Approximation and Arakelov theory</a> at the <a href="http://www.fields.utoronto.ca/">Fields Institute</a> in Toronto, Canada.</p>

<p>Probably, the field with one element will appear in several talks with people such as Soule, Consani and Durov scheduled and topics such as Arakelov geometry (&#8216;including the infinity-adic&#8217;) and &#8216;Generalized rings and schemes&#8217; included.</p>

<p>Hopefully, more information will become available so that we can follow the workshop from a distant&#8230;</p>
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		<title>one week F_un blogging</title>
		<link>http://matrix.cmi.ua.ac.be/fun/index.php/one-week-f_un-blogging.html</link>
		<comments>http://matrix.cmi.ua.ac.be/fun/index.php/one-week-f_un-blogging.html#comments</comments>
		<pubDate>Fri, 10 Oct 2008 15:26:24 +0000</pubDate>
		<dc:creator>lievenlb</dc:creator>
				<category><![CDATA[news]]></category>

		<guid isPermaLink="false">http://matrix.cmi.ua.ac.be/fun/?p=322</guid>
		<description><![CDATA[Our highly paid IC-experts do not know that MPG also stand for the <a href="http://www.mpg.de/">Max Planck Gesellschaft</a> and that the string .mpg. is contained in all official email-addresses from MPI ... This almost prematurely killed this blog.]]></description>
			<content:encoded><![CDATA[<p>The email-spam filter of the university of antwerp is incredibly strong. It detects all sorts of dubious extensions, such as &#8220;mpg&#8221; for &#8216;moving picture experts group&#8217;, the standard video-format, saving us from unpleasant surprises in our inboxes.</p>

<p>Little do our highly paid IC-experts know of the fact that MPG may also stand for the <a href="http://www.mpg.de/">Max Planck Gesellschaft</a> and that the string .mpg. is contained in all official email-addresses coming from the <a href="http://www.mpim-bonn.mpg.de/">Max Planck Institute for Mathematics in Bonn</a>&#8230;</p>

<p>This almost prematurely killed this blog.</p>

<p>It all started with <a href="http://www.neverendingbooks.org/index.php/f_un-with-manin.html#comment-6004">Javier&#8217;s comment</a> telling that they were planning to run a F_un seminar at the MPI. I had already promised to give a couple of talks at our <a href="http://www.math.ua.ac.be/algeo/?page_id=11">ARTs seminar</a> and as the Manin and Connes-Consani papers hit the arXiv a few days before, I thought it might be fun (no pun intended) to talk about them (or better, starting from them).</p>

<p>I asked Javier whether they were interested in setting up a blog that could serve as a vehicle to have some interaction between the two seminars. But I&#8217;ve made <a href="http://www.neverendingbooks.org/index.php/the-future-of-this-blog-2.html">blog-proposals</a> before leading nowhere, so I set up a small test-blog to show what I had in mind.</p>

<p>I copy/pasted a few older F_un posts from neverendingbooks to the new blog and didn&#8217;t care to remove links to other blogs which resulted in a few unwanted trackbacks in the comments of the <a href="http://sbseminar.wordpress.com/2007/08/14/the-field-with-one-element/">Field with one element post</a> over at the Secret Blogging Seminar.</p>

<p>Suddenly, the test-site got several hits daily coming from the SBS, while I wasn&#8217;t getting any feedback from the MPI, so after a week I chmodded the entry page and forgot the whole project.</p>

<p>Last friday afternoon, Javier used his Granada-account to ask whether I did receive his emails on the blog-project (quod non, via &#8216;mpg&#8217;). As their seminar was scheduled to start the next tuesday we decided on the spot to resurrect the test-blog and make it publicly available (we didn&#8217;t even have an &#8216;about&#8217; page at the time&#8230;).</p>

<p>As math-blogging is a pretty small community, the F_un blog was inevitably discovered early on and thanks to generous links provided by <a href="http://golem.ph.utexas.edu/category/2008/10/the_blog_of_fun.html">David Corfield at the n-category cafe</a> and <a href="http://www.math.columbia.edu/%7Ewoit/wordpress/?p=971">Peter Woit at Not Even Wrong</a> more people are coming here than we ever anticipated. Below the stats at 5 pm Brussels-time, precisely 1 week after start-up (you can see the effect of David&#8217;s evening-post on october 5th and Peter&#8217;s evening(in Europe)-post on october 8th).</p>

<p><center>
<img src="http://matrix.cmi.ua.ac.be/fun/DATA/firstweek.jpg">
</center></p>

<p>Now that we&#8217;re pretty sure that everyone who might be interested in this blog knows of its existence, we &#8216;only&#8217; have to provide content. Speaking of which, we are still looking for people willing to join the project!</p>
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