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	<title>A Mind for Madness &#187; cohomology</title>
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		<title>A Mind for Madness &#187; cohomology</title>
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		<title>Generalized HT90</title>
		<link>http://hilbertthm90.wordpress.com/2008/12/12/generalized-ht90/</link>
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		<pubDate>Fri, 12 Dec 2008 22:03:23 +0000</pubDate>
		<dc:creator>hilbertthm90</dc:creator>
				<category><![CDATA[algebra]]></category>
		<category><![CDATA[topology]]></category>
		<category><![CDATA[chain complex]]></category>
		<category><![CDATA[coboundary]]></category>
		<category><![CDATA[cocycle]]></category>
		<category><![CDATA[cohomology]]></category>
		<category><![CDATA[galois theory]]></category>
		<category><![CDATA[hilbert theorem 90]]></category>
		<category><![CDATA[module]]></category>

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		<description><![CDATA[I officially promise this is my last post on Hilbert&#8217;s Theorem 90, but because of that it is going to go really fast for those who have not seen group cohomology (it is really cool, so I couldn&#8217;t pass it up).
An abelian group is a G-module (G a group) if for all  and  [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=hilbertthm90.wordpress.com&blog=3601932&post=293&subd=hilbertthm90&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>I officially promise this is my last post on Hilbert&#8217;s Theorem 90, but because of that it is going to go really fast for those who have not seen group cohomology (it is really cool, so I couldn&#8217;t pass it up).</p>
<p>An abelian group is a G-module (G a group) if for all <img src='http://l.wordpress.com/latex.php?latex=%5Csigma%5Cin+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma\in G' title='\sigma\in G' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=a%5Cin+A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a\in A' title='a\in A' class='latex' /> there is a unique element <img src='http://l.wordpress.com/latex.php?latex=%5Csigma%28a%29%5Cin+A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma(a)\in A' title='\sigma(a)\in A' class='latex' /> satisfying two conditions: <img src='http://l.wordpress.com/latex.php?latex=%5Csigma%28a%2Bb%29%3D%5Csigma%28a%29%2B%5Csigma%28b%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma(a+b)=\sigma(a)+\sigma(b)' title='\sigma(a+b)=\sigma(a)+\sigma(b)' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=%28%5Csigma%5Ctau%29%28a%29%3D%5Csigma%28%5Ctau%28a%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(\sigma\tau)(a)=\sigma(\tau(a))' title='(\sigma\tau)(a)=\sigma(\tau(a))' class='latex' /> for all <img src='http://l.wordpress.com/latex.php?latex=%5Csigma%2C+%5Ctau%5Cin+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma, \tau\in G' title='\sigma, \tau\in G' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=a%2Cb%5Cin+A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a,b\in A' title='a,b\in A' class='latex' />.</p>
<p>Just check any algebra text or <a href="http://unapologetic.wordpress.com/2007/04/21/modules/" target="_blank">here</a> for more information on modules.</p>
<p>Now define an n-cochain of G over A to be a a function of n variables from G into A. If <img src='http://l.wordpress.com/latex.php?latex=n%3D0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n=0' title='n=0' class='latex' /> it is just an element of A. <img src='http://l.wordpress.com/latex.php?latex=C%5En%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C^n(G, A)' title='C^n(G, A)' class='latex' /> is the set of all n-cochains, and can be made into a group by the operation <img src='http://l.wordpress.com/latex.php?latex=%28f%2Bg%29%28%5Csigma_1%2C+%5Cldots%2C+%5Csigma_n%29%3Df%28%5Csigma_1%2C+%5Cldots%2C+%5Csigma_n%29%2Bg%28%5Csigma_1%2C+%5Cldots%2C+%5Csigma_n%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(f+g)(\sigma_1, \ldots, \sigma_n)=f(\sigma_1, \ldots, \sigma_n)+g(\sigma_1, \ldots, \sigma_n)' title='(f+g)(\sigma_1, \ldots, \sigma_n)=f(\sigma_1, \ldots, \sigma_n)+g(\sigma_1, \ldots, \sigma_n)' class='latex' />.</p>
<p>We can also get from <img src='http://l.wordpress.com/latex.php?latex=C%5En%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C^n(G, A)' title='C^n(G, A)' class='latex' /> to <img src='http://l.wordpress.com/latex.php?latex=C%5E%7Bn%2B1%7D%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C^{n+1}(G, A)' title='C^{n+1}(G, A)' class='latex' /> (which is what people who know about cohomology were hoping for), by the function <img src='http://l.wordpress.com/latex.php?latex=%5Cdelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\delta' title='\delta' class='latex' />:</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%28%5Cdelta+f%29%28%5Csigma_1%2C+%5Cldots%2C+%5Csigma_%7Bn%2B1%7D%29%3D%5Csigma_1%28f%28%5Csigma_2%2C+%5Cldots%2C+%5Csigma_%7Bn%2B1%7D%29%29%2B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(\delta f)(\sigma_1, \ldots, \sigma_{n+1})=\sigma_1(f(\sigma_2, \ldots, \sigma_{n+1}))+' title='(\delta f)(\sigma_1, \ldots, \sigma_{n+1})=\sigma_1(f(\sigma_2, \ldots, \sigma_{n+1}))+' class='latex' /></p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Csum_%7Bi%3D1%7D%5En%28-1%29%5Ei+f%28%5Csigma_1%2C+%5Cldots%2C+%5Csigma_i%5Csigma_%7Bi%2B1%7D%2C+%5Cldots%2C+%5Csigma_%7Bn%2B1%7D%29%2B%28-1%29%5E%7Bn%2B1%7Df%28%5Csigma_1%2C+%5Cldots%2C+%5Csigma_n%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sum_{i=1}^n(-1)^i f(\sigma_1, \ldots, \sigma_i\sigma_{i+1}, \ldots, \sigma_{n+1})+(-1)^{n+1}f(\sigma_1, \ldots, \sigma_n)' title='\sum_{i=1}^n(-1)^i f(\sigma_1, \ldots, \sigma_i\sigma_{i+1}, \ldots, \sigma_{n+1})+(-1)^{n+1}f(\sigma_1, \ldots, \sigma_n)' class='latex' />.</p>
<p>OK. That looks bad, but really in some sense it is the natural choice. I&#8217;ll leave it to you to check that this is both a homomorphism and that <img src='http://l.wordpress.com/latex.php?latex=%5Cdelta%5Cdelta+f%3D0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\delta\delta f=0' title='\delta\delta f=0' class='latex' /> (i.e. we have a chain complex).</p>
<p>Now if we label them <img src='http://l.wordpress.com/latex.php?latex=%5Cdelta_0%3A+A%5Cto+C%5E1%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\delta_0: A\to C^1(G, A)' title='\delta_0: A\to C^1(G, A)' class='latex' /></p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdelta_1%3A+C%5E1%28G%2C+A%29%5Cto+C%5E2%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\delta_1: C^1(G, A)\to C^2(G, A)' title='\delta_1: C^1(G, A)\to C^2(G, A)' class='latex' /> and</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdelta_n%3A+C%5En%28G%2C+A%29%5Cto+C%5E%7Bn%2B1%7D%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\delta_n: C^n(G, A)\to C^{n+1}(G, A)' title='\delta_n: C^n(G, A)\to C^{n+1}(G, A)' class='latex' />. Then we form <img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+H%5En%28G%2C+A%29%3D%5Cfrac%7B%5Cker%5Cdelta_n%7D%7Bim%5Cdelta_%7Bn-1%7D%7D%3D%5Cfrac%7BZ%5En%28G%2C+A%29%7D%7BB%5En%28G%2C+A%29%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle H^n(G, A)=\frac{\ker\delta_n}{im\delta_{n-1}}=\frac{Z^n(G, A)}{B^n(G, A)}' title='\displaystyle H^n(G, A)=\frac{\ker\delta_n}{im\delta_{n-1}}=\frac{Z^n(G, A)}{B^n(G, A)}' class='latex' />. We call the elements of <img src='http://l.wordpress.com/latex.php?latex=Z%5En%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Z^n(G, A)' title='Z^n(G, A)' class='latex' /> the n-cocycles and the elements of <img src='http://l.wordpress.com/latex.php?latex=B%5En%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B^n(G, A)' title='B^n(G, A)' class='latex' /> the n-coboundaries.</p>
<p>So if you don&#8217;t like that, we can scratch it now, since in HT90 we only care about <img src='http://l.wordpress.com/latex.php?latex=H%5E1%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H^1(G, A)' title='H^1(G, A)' class='latex' />, so let&#8217;s take a closer look at that. We can completely classify what the elements of <img src='http://l.wordpress.com/latex.php?latex=Z%5E1%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Z^1(G, A)' title='Z^1(G, A)' class='latex' /> look like. For any <img src='http://l.wordpress.com/latex.php?latex=f%5Cin+Z%5E1%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f\in Z^1(G, A)' title='f\in Z^1(G, A)' class='latex' /> and any <img src='http://l.wordpress.com/latex.php?latex=%5Csigma%2C+%5Ctau%5Cin+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma, \tau\in G' title='\sigma, \tau\in G' class='latex' /> we need <img src='http://l.wordpress.com/latex.php?latex=%28%5Cdelta+f%29%28%5Csigma%2C+%5Ctau%29%3D%5Csigma%28f%28%5Ctau%29%29-f%28%5Csigma%5Ctau%29%2Bf%28%5Csigma%29%3D0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(\delta f)(\sigma, \tau)=\sigma(f(\tau))-f(\sigma\tau)+f(\sigma)=0' title='(\delta f)(\sigma, \tau)=\sigma(f(\tau))-f(\sigma\tau)+f(\sigma)=0' class='latex' />. Which is to say that <img src='http://l.wordpress.com/latex.php?latex=f%28%5Csigma%5Ctau%29%3D%5Csigma%28f%28%5Ctau%29%29%2Bf%28%5Csigma%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f(\sigma\tau)=\sigma(f(\tau))+f(\sigma)' title='f(\sigma\tau)=\sigma(f(\tau))+f(\sigma)' class='latex' />.</p>
<p>Now let&#8217;s classify what <img src='http://l.wordpress.com/latex.php?latex=B%5E1%28G%2CA%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B^1(G,A)' title='B^1(G,A)' class='latex' /> looks like. Well, if <img src='http://l.wordpress.com/latex.php?latex=g%5Cin+B%5E1%28G%2C+A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g\in B^1(G, A)' title='g\in B^1(G, A)' class='latex' />, then <img src='http://l.wordpress.com/latex.php?latex=g%3D%5Cdelta+h&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g=\delta h' title='g=\delta h' class='latex' /> for some <img src='http://l.wordpress.com/latex.php?latex=h%5Cin+A%3DC%5E0%28G%2CA%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h\in A=C^0(G,A)' title='h\in A=C^0(G,A)' class='latex' />. So <img src='http://l.wordpress.com/latex.php?latex=g%28%5Csigma%29%3D%28%5Cdelta+h%29%28%5Csigma%29%3D%5Csigma%28a%29-a&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g(\sigma)=(\delta h)(\sigma)=\sigma(a)-a' title='g(\sigma)=(\delta h)(\sigma)=\sigma(a)-a' class='latex' /> for some <img src='http://l.wordpress.com/latex.php?latex=a%5Cin+A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a\in A' title='a\in A' class='latex' />. Well, I think you might be able to see the previous formulation of the theorem coming from unravelling these definitions.</p>
<p>Theorem statement: If <img src='http://l.wordpress.com/latex.php?latex=K%2FF&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K/F' title='K/F' class='latex' /> is a finite Galois extension and <img src='http://l.wordpress.com/latex.php?latex=G%3DGal%28K%2FF%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G=Gal(K/F)' title='G=Gal(K/F)' class='latex' />, then <img src='http://l.wordpress.com/latex.php?latex=H%5E1%28G%2C+K%5E%5Ctimes%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H^1(G, K^\times)' title='H^1(G, K^\times)' class='latex' /> is trivial.</p>
<p>Proof: Let a be a cocycle. Then let <img src='http://l.wordpress.com/latex.php?latex=%5Calpha%3A+K%5Cto+K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha: K\to K' title='\alpha: K\to K' class='latex' /> by <img src='http://l.wordpress.com/latex.php?latex=c%5Cmapsto+%5Csum_%7B%5Csigma%5Cin+G%7Da%28%5Csigma%29%5Csigma%28c%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c\mapsto \sum_{\sigma\in G}a(\sigma)\sigma(c)' title='c\mapsto \sum_{\sigma\in G}a(\sigma)\sigma(c)' class='latex' />. As in the last post, <img src='http://l.wordpress.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha' title='\alpha' class='latex' /> is not 0 by linear independence. So let <img src='http://l.wordpress.com/latex.php?latex=c%5Cin+K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c\in K' title='c\in K' class='latex' /> such that <img src='http://l.wordpress.com/latex.php?latex=%5Calpha%28c%29%5Cneq+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha(c)\neq 0' title='\alpha(c)\neq 0' class='latex' /> and set <img src='http://l.wordpress.com/latex.php?latex=b%3D%5Calpha%28c%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='b=\alpha(c)' title='b=\alpha(c)' class='latex' />.</p>
<p>Then for any <img src='http://l.wordpress.com/latex.php?latex=%5Ctau%5Cin+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tau\in G' title='\tau\in G' class='latex' /> we have</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle%5Ctau%28b%29%3D%5Csum_%7B%5Csigma%5Cin+G%7D%5Ctau%28a%28%5Csigma%29%5Csigma%28c%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle\tau(b)=\sum_{\sigma\in G}\tau(a(\sigma)\sigma(c))' title='\displaystyle\tau(b)=\sum_{\sigma\in G}\tau(a(\sigma)\sigma(c))' class='latex' /></p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%3D%5Csum_%7B%5Csigma%5Cin+G%7D%5Ctau%28a%5Csigma%29%28%5Ctau%5Csigma%29%28c%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle =\sum_{\sigma\in G}\tau(a\sigma)(\tau\sigma)(c)' title='\displaystyle =\sum_{\sigma\in G}\tau(a\sigma)(\tau\sigma)(c)' class='latex' /></p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%3D%5Csum_%7B%5Csigma%5Cin+G%7Da%28%5Ctau%29%5E%7B-1%7Da%28%5Ctau%5Csigma%29%28%5Ctau%5Csigma%29%28c%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle =\sum_{\sigma\in G}a(\tau)^{-1}a(\tau\sigma)(\tau\sigma)(c)' title='\displaystyle =\sum_{\sigma\in G}a(\tau)^{-1}a(\tau\sigma)(\tau\sigma)(c)' class='latex' />. Now we use that <img src='http://l.wordpress.com/latex.php?latex=a&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a' title='a' class='latex' /> is a cocycle (in the kernel) to continue the equality as</p>
<p><img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%3D+a%28%5Ctau%29%5E%7B-1%7D%5Csum_%7B%5Csigma%5Cin+G%7Da%28%5Ctau%5Csigma%29%28%5Ctau%5Csigma%29%28c%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle = a(\tau)^{-1}\sum_{\sigma\in G}a(\tau\sigma)(\tau\sigma)(c)' title='\displaystyle = a(\tau)^{-1}\sum_{\sigma\in G}a(\tau\sigma)(\tau\sigma)(c)' class='latex' /></p>
<p><img src='http://l.wordpress.com/latex.php?latex=%3Da%28%5Ctau%29%5E%7B-1%7Db&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='=a(\tau)^{-1}b' title='=a(\tau)^{-1}b' class='latex' />.</p>
<p>Aha, so <img src='http://l.wordpress.com/latex.php?latex=a%28%5Ctau%29%3Db%5Ctau%28b%29%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a(\tau)=b\tau(b)^{-1}' title='a(\tau)=b\tau(b)^{-1}' class='latex' /> is a coboundary! Thus every cocycle is a coboundary, so the quotient is trivial.</p>
<p>Test your understanding by now trying to prove the other formulation as a corollary to this (remember you assume that G is cyclic in that version and have to relate it back to the norm).</p>
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		<title>Hilbert&#8217;s Theorem 90&#8230;the math</title>
		<link>http://hilbertthm90.wordpress.com/2008/12/11/hilberts-theorem-90the-math/</link>
		<comments>http://hilbertthm90.wordpress.com/2008/12/11/hilberts-theorem-90the-math/#comments</comments>
		<pubDate>Thu, 11 Dec 2008 22:33:35 +0000</pubDate>
		<dc:creator>hilbertthm90</dc:creator>
				<category><![CDATA[algebra]]></category>
		<category><![CDATA[cohomology]]></category>
		<category><![CDATA[cyclic galois group]]></category>
		<category><![CDATA[determinant]]></category>
		<category><![CDATA[galois theory]]></category>
		<category><![CDATA[hilbert satz 90]]></category>
		<category><![CDATA[hilbert's theorem 90]]></category>
		<category><![CDATA[linear algebra]]></category>
		<category><![CDATA[norm]]></category>
		<category><![CDATA[trace]]></category>

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		<description><![CDATA[So now that I&#8217;ve presented the origins of Hilbert&#8217;s Theorem 90, I thought it might be good to actually present it mathematically with a proof.
Statement: Suppose K is a finite Galois extension of F with  cyclic, say  of order n. If , then  if and only if  for some .
Let&#8217;s parse [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=hilbertthm90.wordpress.com&blog=3601932&post=288&subd=hilbertthm90&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>So now that I&#8217;ve presented the origins of Hilbert&#8217;s Theorem 90, I thought it might be good to actually present it mathematically with a proof.</p>
<p>Statement: Suppose K is a finite Galois extension of F with <img src='http://l.wordpress.com/latex.php?latex=G%3DGal%28K%2FF%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G=Gal(K/F)' title='G=Gal(K/F)' class='latex' /> cyclic, say <img src='http://l.wordpress.com/latex.php?latex=G%3D%3C%5Csigma+%3E&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G=&lt;\sigma &gt;' title='G=&lt;\sigma &gt;' class='latex' /> of order n. If <img src='http://l.wordpress.com/latex.php?latex=a%5Cin+K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a\in K' title='a\in K' class='latex' />, then <img src='http://l.wordpress.com/latex.php?latex=N_%7BK%2FF%7D%28a%29%3D1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='N_{K/F}(a)=1' title='N_{K/F}(a)=1' class='latex' /> if and only if <img src='http://l.wordpress.com/latex.php?latex=a%3Db%2F%5Csigma%28b%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a=b/\sigma(b)' title='a=b/\sigma(b)' class='latex' /> for some <img src='http://l.wordpress.com/latex.php?latex=b%5Cin+K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='b\in K' title='b\in K' class='latex' />.</p>
<p>Let&#8217;s parse this a little before the proof. First off let&#8217;s define the notation <img src='http://l.wordpress.com/latex.php?latex=N_%7BK%2FF%7D%28a%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='N_{K/F}(a)' title='N_{K/F}(a)' class='latex' />. Notice that we can view K as a vector sapce over F, so <img src='http://l.wordpress.com/latex.php?latex=t_a%3A+K%5Cto+K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='t_a: K\to K' title='t_a: K\to K' class='latex' /> by <img src='http://l.wordpress.com/latex.php?latex=u%5Cmapsto+au&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='u\mapsto au' title='u\mapsto au' class='latex' /> is a linear transformation. So we want a norm, so we define <img src='http://l.wordpress.com/latex.php?latex=N_%7BK%2FF%7D%28a%29%3D%5Cdet+%28t_a%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='N_{K/F}(a)=\det (t_a)' title='N_{K/F}(a)=\det (t_a)' class='latex' />. i.e. the determinant of the matrix that represents that linear transformation. Thus, we get all our nice results from linear algebra like independence of basis choice. If we fight with definitions and linear algebra for a bit we also get that if the extension is Galois, <img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+N_%7BK%2FF%7D%28a%29%3D%5Cprod_%7B%5Cphi%5Cin+Gal%28K%2FF%29%7D+%5Cphi+%28a%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle N_{K/F}(a)=\prod_{\phi\in Gal(K/F)} \phi (a)' title='\displaystyle N_{K/F}(a)=\prod_{\phi\in Gal(K/F)} \phi (a)' class='latex' />. This is left as an (not required) exercise to familiarize yourself with the terms before moving on. Note that we can determine <img src='http://l.wordpress.com/latex.php?latex=Tr_%7BK%2FF%7D%28a%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Tr_{K/F}(a)' title='Tr_{K/F}(a)' class='latex' /> similarly to be the trace of <img src='http://l.wordpress.com/latex.php?latex=t_a&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='t_a' title='t_a' class='latex' />.</p>
<p>Proof of the theorem: Let&#8217;s do the backwards way first (I&#8217;m going to suppress the norm notation since we know where it is happening). Suppose <img src='http://l.wordpress.com/latex.php?latex=a%3Db%2F%5Csigma%28b%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a=b/\sigma(b)' title='a=b/\sigma(b)' class='latex' /> for some <img src='http://l.wordpress.com/latex.php?latex=b%5Cin+K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='b\in K' title='b\in K' class='latex' />. Then let&#8217;s simply use the result (that you proved!) to see that <img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+N%28a%29%3D%5Cleft%28%5Cfrac%7Bb%7D%7B%5Csigma%28b%29%7D%5Cright%29%5Cleft%28%5Cfrac%7B%5Csigma%28b%29%7D%7B%5Csigma%5E2%28b%29%7D%5Cright%29%5Ccdots+%5Cleft%28%5Cfrac%7B%5Csigma%5E%7Bn-1%7D%28b%29%7D%7B%5Csigma%5En%28b%29%7D%5Cright%29%3D1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle N(a)=\left(\frac{b}{\sigma(b)}\right)\left(\frac{\sigma(b)}{\sigma^2(b)}\right)\cdots \left(\frac{\sigma^{n-1}(b)}{\sigma^n(b)}\right)=1' title='\displaystyle N(a)=\left(\frac{b}{\sigma(b)}\right)\left(\frac{\sigma(b)}{\sigma^2(b)}\right)\cdots \left(\frac{\sigma^{n-1}(b)}{\sigma^n(b)}\right)=1' class='latex' /> since <img src='http://l.wordpress.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma' title='\sigma' class='latex' /> has order n.</p>
<p>Now for the forwards direction. Suppose <img src='http://l.wordpress.com/latex.php?latex=N%28a%29%3D1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='N(a)=1' title='N(a)=1' class='latex' />. Again using a standard linear algebra argument we know that <img src='http://l.wordpress.com/latex.php?latex=1%2C+%5Csigma%2C+%5Cldots%2C+%5Csigma%5E%7Bn-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1, \sigma, \ldots, \sigma^{n-1}' title='1, \sigma, \ldots, \sigma^{n-1}' class='latex' /> are K-linearly independent (in fact, any set of field automorphisms of K are K-linearly independent over the vector space of all functions from K to K).</p>
<p>Thus, <img src='http://l.wordpress.com/latex.php?latex=%5Cdisplaystyle+%5Cphi+%3D+a%5Ccdot+1%2B%28a%5Csigma%28a%29%29%5Csigma+%2B+%28a%5Csigma%28a%29%5Csigma%5E2%28a%29%29%5Csigma%5E2%2B%5Ccdots+%2B+%5Cleft%28%5Cprod_%7Bi%3D0%7D%5E%7Bn-1%7D%5Csigma%5Ei+%28a%29%5Cright%29%5Csigma%5E%7Bn-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\displaystyle \phi = a\cdot 1+(a\sigma(a))\sigma + (a\sigma(a)\sigma^2(a))\sigma^2+\cdots + \left(\prod_{i=0}^{n-1}\sigma^i (a)\right)\sigma^{n-1}' title='\displaystyle \phi = a\cdot 1+(a\sigma(a))\sigma + (a\sigma(a)\sigma^2(a))\sigma^2+\cdots + \left(\prod_{i=0}^{n-1}\sigma^i (a)\right)\sigma^{n-1}' class='latex' /> from K to K is not 0. By the thing you proved the coefficient on <img src='http://l.wordpress.com/latex.php?latex=%5Csigma%5E%7Bn-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma^{n-1}' title='\sigma^{n-1}' class='latex' /> is <img src='http://l.wordpress.com/latex.php?latex=N%28a%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='N(a)' title='N(a)' class='latex' /> which is 1. More importantly, there is some <img src='http://l.wordpress.com/latex.php?latex=c%5Cin+K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c\in K' title='c\in K' class='latex' /> such that <img src='http://l.wordpress.com/latex.php?latex=%5Cphi%28c%29%5Cneq+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi(c)\neq 0' title='\phi(c)\neq 0' class='latex' />, so let&#8217;s define <img src='http://l.wordpress.com/latex.php?latex=b%3D%5Cphi%28c%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='b=\phi(c)' title='b=\phi(c)' class='latex' />.</p>
<p>But <img src='http://l.wordpress.com/latex.php?latex=%5Csigma%28b%29%3D%5Cfrac%7B1%7D%7Ba%7D%28b-ac%29%2B%5Csigma%5En%28c%29%3D%5Cfrac%7B1%7D%7Ba%7D%28b-ac%29%2Bc%3D%5Cfrac%7Bb%7D%7Ba%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma(b)=\frac{1}{a}(b-ac)+\sigma^n(c)=\frac{1}{a}(b-ac)+c=\frac{b}{a}' title='\sigma(b)=\frac{1}{a}(b-ac)+\sigma^n(c)=\frac{1}{a}(b-ac)+c=\frac{b}{a}' class='latex' />. Thus <img src='http://l.wordpress.com/latex.php?latex=a%3Db%2F%5Csigma%28b%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a=b/\sigma(b)' title='a=b/\sigma(b)' class='latex' />. And we are done.</p>
<p>Does this proof remind anyone of Lagrange resolvents? Eh, whatever, I won&#8217;t dig for a connection now.</p>
<p>I also mentioned that there is a generalization of this.</p>
<p>Statement: If K/F is a finite Galois extension and <img src='http://l.wordpress.com/latex.php?latex=G%3DGal%28K%2FF%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G=Gal(K/F)' title='G=Gal(K/F)' class='latex' />, then <img src='http://l.wordpress.com/latex.php?latex=H%5E1%28G%2C+K%5E%5Ctimes%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H^1(G, K^\times)' title='H^1(G, K^\times)' class='latex' /> is trivial. I&#8217;m debating whether or not to parse and prove this version next time, or to just drop the Hilbert Theorem 90 posts. Suggestions?</p>
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		<title>Property of the Plane</title>
		<link>http://hilbertthm90.wordpress.com/2008/06/22/property-of-the-plane/</link>
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		<pubDate>Sun, 22 Jun 2008 17:25:52 +0000</pubDate>
		<dc:creator>hilbertthm90</dc:creator>
				<category><![CDATA[math]]></category>
		<category><![CDATA[topology]]></category>
		<category><![CDATA[cohomology]]></category>
		<category><![CDATA[connected components]]></category>
		<category><![CDATA[exact sequence]]></category>
		<category><![CDATA[mayer-vietoris]]></category>

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		<description><![CDATA[I was reading the blog topological musings, and the category talk reminded me of this neat thing I posted on AoPS awhile ago.
By using the Mayer-Vietoris sequence in cohomology, we determine whether or not  can be written as the union of two open connected sets, U and V, such that  is disconnected.
Well, it [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=hilbertthm90.wordpress.com&blog=3601932&post=47&subd=hilbertthm90&ref=&feed=1" />]]></description>
			<content:encoded><![CDATA[<div class='snap_preview'><br /><p>I was reading the blog <a href="http://topologicalmusings.wordpress.com/">topological musings</a>, and the category talk reminded me of this neat thing I posted on AoPS awhile ago.</p>
<p>By using the Mayer-Vietoris sequence in cohomology, we determine whether or not <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BR%7D%5E2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{R}^2' title='\mathbb{R}^2' class='latex' /> can be written as the union of two open connected sets, U and V, such that <img src='http://l.wordpress.com/latex.php?latex=U%5Ccap+V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='U\cap V' title='U\cap V' class='latex' /> is disconnected.</p>
<p>Well, it seems that we are concerned with <img src='http://l.wordpress.com/latex.php?latex=H%5E0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H^0' title='H^0' class='latex' /> stuff, since that tells us the number of connected components.</p>
<p>The sequence gives <img src='http://l.wordpress.com/latex.php?latex=0%5Cto+H%5E0%28%5Cmathbb%7BR%7D%5E2%29%5Cto+H%5E0%28U%29%5Coplus+H%5E0%28V%29%5Cto+H%5E0%28U%5Ccap+V%29%5Cto+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0\to H^0(\mathbb{R}^2)\to H^0(U)\oplus H^0(V)\to H^0(U\cap V)\to 0' title='0\to H^0(\mathbb{R}^2)\to H^0(U)\oplus H^0(V)\to H^0(U\cap V)\to 0' class='latex' />, a nice short exact sequence in which we mostly know they are connected, so</p>
<p><img src='http://l.wordpress.com/latex.php?latex=0%5Cto+%5Cmathbb%7BR%7D%5Cto+%5Cmathbb%7BR%7D%5Coplus+%5Cmathbb%7BR%7D%5Cto+H%5E0%28U%5Ccap+V%29%5Cto+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0\to \mathbb{R}\to \mathbb{R}\oplus \mathbb{R}\to H^0(U\cap V)\to 0' title='0\to \mathbb{R}\to \mathbb{R}\oplus \mathbb{R}\to H^0(U\cap V)\to 0' class='latex' />, basically the question reduces to: Is it possible for the second to last term to have dimension greater than 1, but the sequence to remain exact?</p>
<p>Well, no, since the exactness tells us the dimension of <img src='http://l.wordpress.com/latex.php?latex=H%5E0%28U%5Ccap+V%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H^0(U\cap V)' title='H^0(U\cap V)' class='latex' /> is the dimension of <img src='http://l.wordpress.com/latex.php?latex=%5Cfrac%7B%5Cmathbb%7BR%7D%5Coplus%5Cmathbb%7BR%7D%7D%7B%5Cmathbb%7BR%7D%7D%5Ccong+%5Cmathbb%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\frac{\mathbb{R}\oplus\mathbb{R}}{\mathbb{R}}\cong \mathbb{R}' title='\frac{\mathbb{R}\oplus\mathbb{R}}{\mathbb{R}}\cong \mathbb{R}' class='latex' />.</p>
<p>So we have a nifty result: the plane cannot be broken into two connected parts in which the intersection of these two parts is disconnected.</p>
<p>Challenge for the readers: This seems extremely simple and obvious. Find a proof that does not require advanced techniques such as cohomology.</p>
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