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	<title>The Other Side of Moon</title>
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		<title>The Other Side of Moon</title>
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		<title>vim-latex for MacVim</title>
		<link>http://dualm.wordpress.com/2012/01/26/vim-latex-for-macvim/</link>
		<comments>http://dualm.wordpress.com/2012/01/26/vim-latex-for-macvim/#comments</comments>
		<pubDate>Thu, 26 Jan 2012 15:36:43 +0000</pubDate>
		<dc:creator>dualm</dc:creator>
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		<description><![CDATA[See http://code.google.com/p/macvim/wiki/FAQ for instructions on how to install vim-latex(or known as latex-suite) on macvim. However, on my Mac OS X Lion, there seems to be a problem with \lv using the default setting. When commanding \lv a pile of error messages jumped out. The fix I found is the following: go to ftplugin/latex-suite, open texrc,  uncomment the [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=308&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>See <a href="http://code.google.com/p/macvim/wiki/FAQ" target="_blank">http://code.google.com/p/macvim/wiki/FAQ</a> for instructions on how to install vim-latex(or known as latex-suite) on macvim.</p>
<p>However, on my Mac OS X Lion, there seems to be a problem with \lv using the default setting. When commanding \lv a pile of error messages jumped out. The fix I found is the following: go to ftplugin/latex-suite, open texrc,  uncomment the line</p>
<p>TexLet g:Tex_TreatMacViewerAsUNIX = 1</p>
<p>and add here or to .vimrc the following:</p>
<p>TexLet g:Tex_ViewRule_pdf = &#8216;open -a Skim&#8217;</p>
<p>I use Skim as my pdf viewer. These two resolve the problem.</p>
<p>&nbsp;</p>
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		<title>Computing Determinant in Fortran</title>
		<link>http://dualm.wordpress.com/2012/01/06/computing-determinant-in-fortran/</link>
		<comments>http://dualm.wordpress.com/2012/01/06/computing-determinant-in-fortran/#comments</comments>
		<pubDate>Fri, 06 Jan 2012 23:59:21 +0000</pubDate>
		<dc:creator>dualm</dc:creator>
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		<description><![CDATA[It may seem that one should go to LAPACK and find a routine that does just this job. However, it turns out that LAPACK does not really have such a routine. So a little bit of detour is needed. If you want to deal with a general, complex matrix, not symmetric, not Hermitian, then the [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=300&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>It may seem that one should go to LAPACK and find a routine that does just this job. However, it turns out that LAPACK does not really have such a routine. So a little bit of detour is needed. If you want to deal with a general, complex matrix, not symmetric, not Hermitian, then the way to go is using Gauss elimination(GE). LAPACK provides routines to find the LU decomposition of a matrix, which is essentially GE and can be used to compute the determinant. Here is the code snippet:</p>
<pre>
<font face="monospace">
<font color="#804040">&nbsp;1 </font><font color="#2e8b57"><b>complex</b></font>(<font color="#2e8b57"><b>kind</b></font><font color="#804040"><b>=</b></font><font color="#ff00ff">8</font>) <font color="#a020f0">function</font>&nbsp;det(N, mat)
<font color="#804040">&nbsp;2 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#2e8b57"><b>implicit</b></font>&nbsp;<font color="#2e8b57"><b>none</b></font>
<font color="#804040">&nbsp;3 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#2e8b57"><b>integer</b></font>(<font color="#2e8b57"><b>kind</b></font><font color="#804040"><b>=</b></font><font color="#ff00ff">8</font>), <font color="#2e8b57"><b>intent</b></font>(<font color="#2e8b57"><b>in</b></font>) :: N 
<font color="#804040">&nbsp;4 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#2e8b57"><b>complex</b></font>(<font color="#2e8b57"><b>kind</b></font><font color="#804040"><b>=</b></font><font color="#ff00ff">8</font>), <font color="#2e8b57"><b>intent</b></font>(<font color="#2e8b57"><b>inout</b></font>), <font color="#2e8b57"><b>dimension</b></font>(:,:) :: mat
<font color="#804040">&nbsp;5 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#2e8b57"><b>integer</b></font>(<font color="#2e8b57"><b>kind</b></font><font color="#804040"><b>=</b></font><font color="#ff00ff">8</font>) :: i, info
<font color="#804040">&nbsp;6 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#2e8b57"><b>integer</b></font>, <font color="#2e8b57"><b>allocatable</b></font>&nbsp;:: ipiv(:)
<font color="#804040">&nbsp;7 </font><font color="#2e8b57"><b>&nbsp;&nbsp;&nbsp;&nbsp;real</b></font>(<font color="#2e8b57"><b>kind</b></font><font color="#804040"><b>=</b></font><font color="#ff00ff">8</font>) :: sgn
<font color="#804040">&nbsp;8 </font>
<font color="#804040">&nbsp;9 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#804040"><b>allocate</b></font>(ipiv(N))
<font color="#804040">10 </font>
<font color="#804040">11 </font>&nbsp;&nbsp;&nbsp;&nbsp;ipiv <font color="#804040"><b>=</b></font>&nbsp;<font color="#ff00ff">0</font>
<font color="#804040">12 </font>&nbsp;&nbsp;&nbsp;&nbsp;
<font color="#804040">13 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#a020f0">call</font>&nbsp;zgetrf(N, N, mat, N, ipiv, info)
<font color="#804040">14 </font>&nbsp;&nbsp;&nbsp;&nbsp;
<font color="#804040">15 </font>&nbsp;&nbsp;&nbsp;&nbsp;det <font color="#804040"><b>=</b></font>&nbsp;ONE
<font color="#804040">16 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#804040"><b>do</b></font>&nbsp;i <font color="#804040"><b>=</b></font>&nbsp;<font color="#ff00ff">1</font>, N
<font color="#804040">17 </font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;det <font color="#804040"><b>=</b></font>&nbsp;det<font color="#804040"><b>*</b></font>mat(i, i)
<font color="#804040">18 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#804040"><b>end do</b></font>
<font color="#804040">19 </font>&nbsp;&nbsp;&nbsp;&nbsp;sgn <font color="#804040"><b>=</b></font>&nbsp;ONE
<font color="#804040">20 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#804040"><b>do</b></font>&nbsp;i <font color="#804040"><b>=</b></font>&nbsp;<font color="#ff00ff">1</font>, N
<font color="#804040">21 </font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;<font color="#804040"><b>if</b></font>(ipiv(i) <font color="#804040"><b>/=</b></font>&nbsp;i) <font color="#804040"><b>then</b></font>
<font color="#804040">22 </font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;sgn <font color="#804040"><b>=</b></font>&nbsp;<font color="#804040"><b>-</b></font>sgn
<font color="#804040">23 </font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;<font color="#804040"><b>end if</b></font>
<font color="#804040">24 </font>&nbsp;&nbsp;&nbsp;&nbsp;<font color="#804040"><b>end do</b></font>
<font color="#804040">25 </font>&nbsp;&nbsp;&nbsp;&nbsp;det <font color="#804040"><b>=</b></font>&nbsp;sgn<font color="#804040"><b>*</b></font>det&nbsp;&nbsp; 
<font color="#804040">26 </font><font color="#a020f0">end function</font>&nbsp;det
</font></pre>
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		<title>Innocence</title>
		<link>http://dualm.wordpress.com/2011/12/02/innocence/</link>
		<comments>http://dualm.wordpress.com/2011/12/02/innocence/#comments</comments>
		<pubDate>Fri, 02 Dec 2011 08:41:54 +0000</pubDate>
		<dc:creator>dualm</dc:creator>
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		<description><![CDATA[In our acquisition of knowledge of the Universe (whether mathematical or otherwise) that which renovates the quest is nothing more nor less than complete innocence. It is in this state of complete innocence that we receive everything from the moment of our birth. Although so often the object of our contempt and of our private [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=297&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<blockquote><p>In our acquisition of knowledge of the Universe (whether mathematical or otherwise) that which renovates the quest is nothing more nor less than complete innocence. It is in this state of complete innocence that we receive everything from the moment of our birth. Although so often the object of our contempt and of our private fears, it is always in us. It alone can unite humility with boldness so as to allow us to penetrate to the heart of things, or allow things to enter us and taken possession of us.</p>
<p>This unique power is in no way a privilege given to “exceptional talents” – persons of incredible brain power (for example), who are better able to manipulate, with dexterity and ease, an enormous mass of data, ideas and specialized skills. Such gifts are undeniably valuable, and certainly worthy of envy from those who (like myself) were not so “endowed at birth, far beyond the ordinary”.</p>
<p>Yet it is not these gifts, nor the most determined ambition combined with irresistible will-power, that enables one to surmount the “invisible yet formidable boundaries” that encircle our universe. Only innocence can surmount them, which mere knowledge doesn’t even take into account, in those moments when we find ourselves able to listen to things, totally and intensely absorbed in child’s play.</p>
<p>— Alexander Grothendieck</p></blockquote>
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		<title>RG=GR</title>
		<link>http://dualm.wordpress.com/2011/11/15/rggr/</link>
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		<pubDate>Tue, 15 Nov 2011 07:53:07 +0000</pubDate>
		<dc:creator>dualm</dc:creator>
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		<description><![CDATA[今天听黑哥们Philip Phillips的报告，印象比较深的就是他介绍AdS/CFT的时候说RG=GR……黑哥们笑话的质量还是相当不赖的。<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=286&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>今天听黑哥们Philip Phillips的报告，印象比较深的就是他介绍AdS/CFT的时候说RG=GR……黑哥们笑话的质量还是相当不赖的。</p>
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		<title>Scattered Thoughts</title>
		<link>http://dualm.wordpress.com/2011/11/14/scattered-thoughts/</link>
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		<pubDate>Mon, 14 Nov 2011 00:32:22 +0000</pubDate>
		<dc:creator>dualm</dc:creator>
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		<description><![CDATA[Conformal field theories in even space-time dimensions(e.g. 1+1, 3+1,&#8230;) have trace anomaly and one can define a central charge for the theory which effectively counts how many degrees of freedom there are in the theory. This is related to the stability of  topologically-ordered phases in odd space-time dimensions, since their boundaries are described by CFT [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=283&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>Conformal field theories in even space-time dimensions(e.g. 1+1, 3+1,&#8230;) have trace anomaly and one can define a central charge for the theory which effectively counts how many degrees of freedom there are in the theory. This is related to the stability of  topologically-ordered phases in odd space-time dimensions, since their boundaries are described by CFT in even space-time dimensions. Therefore, we can understand the IQHE in 2+1 and 4+1 dimensions. Relation to chiral anomaly?</p>
<p>FQHE can be understood from parton(or slave particle) construction as the IQHE of partons. This approach has been developed by Wen to derive the effective field theories of various non-Abelian QHS. Recently discovered FQHE in flat-band lattice models can also be understood using this approach. An interesting question is what if the mean-field ansatz breaks the internal gauge symmetry(i.e. the mean-field ansatz has nontrivial internal gauge fluxes). The most extreme case would be that the gauge group is completely broken to its center, which is usually a discrete group(i.e. Z_n). Does the topological order remain the same? The Abelian case is studied by Lu &amp; Ran. The non-Abelian case is still an open question.</p>
<p>A deep result due to Dijkgraaf and Witten states that the Chern-Simons actions for a compact gauge group G are in one–to–one correspondence with the elements of the cohomology group <img src='http://s0.wp.com/latex.php?latex=H%5E4%28BG%2C+Z%29&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='H^4(BG, Z)' title='H^4(BG, Z)' class='latex' /> of the classifying space BG with integer coeﬃcients Z. In particular, this classiﬁcation includes the case of ﬁnite groups H. The isomorphism <img src='http://s0.wp.com/latex.php?latex=H%5E4%28BH%2C+Z%29%5Csimeq+H%5E3%28H%2C+U%281%29%29&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='H^4(BH, Z)&#92;simeq H^3(H, U(1))' title='H^4(BH, Z)&#92;simeq H^3(H, U(1))' class='latex' /> which is only valid for ﬁnite H then implies that the diﬀerent CS theories for a ﬁnite gauge group H correspond to the diﬀerent<br />
elements <img src='http://s0.wp.com/latex.php?latex=%5Comega+%5Cin+H%5E3%28H%2C+U%281%29%29&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='&#92;omega &#92;in H^3(H, U(1))' title='&#92;omega &#92;in H^3(H, U(1))' class='latex' />, i.e. algebraic 3-cocycles ω taking values in U(1).</p>
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		<title>周作人《希腊女诗人》一文中所译萨福诗句</title>
		<link>http://dualm.wordpress.com/2011/07/02/%e5%91%a8%e4%bd%9c%e4%ba%ba%e3%80%8a%e5%b8%8c%e8%85%8a%e5%a5%b3%e8%af%97%e4%ba%ba%e3%80%8b%e4%b8%80%e6%96%87%e4%b8%ad%e6%89%80%e8%af%91%e8%90%a8%e7%a6%8f%e8%af%97%e5%8f%a5/</link>
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		<pubDate>Sat, 02 Jul 2011 06:57:29 +0000</pubDate>
		<dc:creator>dualm</dc:creator>
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		<description><![CDATA[周作人《希腊女诗人》一文中所译萨福诗句： 其一： 凉风嗫嚅，过棠棣枝间，睡意自流，自颤叶而下。 其二： 月落星沉，良夜已半，光阴自逝，而吾今独卧。 其三： 满月已升，女伴绕神坛而立，或作雅舞，践弱草之芳华。 其四： 甘棠色赤于枝头，为采者所忘，              ——非敢忘也，但不能及耳。 其五： 如山上水仙，为牧人所践，花萎于地。 其六： 爱摇吾心，如山风降于栎树。 （见钟叔河编辑《周作人文类编》第八卷《希腊之余光》，湖南文艺出版社1998年版）<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=277&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>周作人《希腊女诗人》一文中所译萨福诗句：</p>
<p>其一： 凉风嗫嚅，过棠棣枝间，睡意自流，自颤叶而下。</p>
<p>其二： 月落星沉，良夜已半，光阴自逝，而吾今独卧。</p>
<p>其三： 满月已升，女伴绕神坛而立，或作雅舞，践弱草之芳华。</p>
<p>其四： 甘棠色赤于枝头，为采者所忘，<br />              ——非敢忘也，但不能及耳。</p>
<p>其五： 如山上水仙，为牧人所践，花萎于地。</p>
<p>其六： 爱摇吾心，如山风降于栎树。</p>
<p>（见钟叔河编辑《周作人文类编》第八卷《希腊之余光》，湖南文艺出版社1998年版）</p>
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		<title>Recent arXiv Digest</title>
		<link>http://dualm.wordpress.com/2011/05/28/recent-arxiv-digest/</link>
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		<pubDate>Sat, 28 May 2011 17:26:06 +0000</pubDate>
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		<description><![CDATA[Topological Field Theory for p-wave Superconductors T.H. Hansson, A. Karlhede, Masatoshi Sato Functional renormalization group approach to correlated fermion systems Walter Metzner, Manfred Salmhofer, Carsten Honerkamp, Volker Meden, Kurt Schoenhammer The effects of interaction on quantum spin Hall insulators Dung-Hai Lee Observation of topologically protected bound states in a one dimensional photonic system Takuya Kitagawa, [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=270&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p><a href="http://arxiv.org/abs/1105.5031">Topological Field Theory for p-wave Superconductors</a><br />
T.H. Hansson, A. Karlhede, Masatoshi Sato</p>
<p><a href="http://arxiv.org/abs/1105.5289">Functional renormalization group approach to correlated fermion systems</a><br />
Walter Metzner, Manfred Salmhofer, Carsten Honerkamp, Volker Meden, Kurt Schoenhammer</p>
<p><a href="http://arxiv.org/abs/1105.4900">The effects of interaction on quantum spin Hall insulators</a><br />
Dung-Hai Lee</p>
<p><a href="http://arxiv.org/abs/1105.5334">Observation of topologically protected bound states in a one dimensional photonic system</a><br />
Takuya Kitagawa, Matthew A. Broome, Alessandro Fedrizzi, Mark S. Rudner, Erez Berg, Ivan Kassal, Alán Aspuru-Guzik, Eugene Demler, Andrew G. White</p>
<p><a href="http://arxiv.org/abs/1105.5375">The Fate of the Photon in Topological Matter: Superconductivity, Confinement and the Vortex Quantum Hall Effect</a><br />
M.C. Diamantini, C.A. Trugenberger</p>
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		<title>数列极限题之后续</title>
		<link>http://dualm.wordpress.com/2011/01/26/%e6%95%b0%e5%88%97%e6%9e%81%e9%99%90%e9%a2%98%e4%b9%8b%e5%90%8e%e7%bb%ad/</link>
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		<pubDate>Wed, 26 Jan 2011 23:26:19 +0000</pubDate>
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		<description><![CDATA[在之前一篇post里我讨论了一个数列极限问题，题目如下：设有数列满足 . 研究的极限。题目本身不难，很容易证明极限存在并且为1。比较值得注意的是这个数列收敛速度非常快（可以估计出数列是以指数的指数这样的速度收敛的）。这个题目看起来像一个普通的高等数学练习，但实际上背景很不简单：历史上最早研究这个问题的是Gauss。可以想象，能引起了Gauss兴趣的问题必定不是泛泛。Gauss问的是：给定初始值, 极限是多少？他特别考虑了的情形。记. Gauss证明了下面的结论： 事实上，有如下更一般的结论： 也即可以用椭圆积分来表示！ 是所谓的第一类完全椭圆积分：<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=240&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p style="text-align:left;">在之前一篇<a href="http://dualm.wordpress.com/2010/09/15/%E6%95%B0%E5%88%97%E6%9E%81%E9%99%90%E9%97%AE%E9%A2%98%E4%B8%80%E5%88%99/">post</a>里我讨论了一个数列极限问题，题目如下：设有数列<img src='http://s0.wp.com/latex.php?latex=a_n%2C+b_n&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='a_n, b_n' title='a_n, b_n' class='latex' />满足</p>
<p style="text-align:center;"><img src='http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+a_%7Bn%2B1%7D%3D%5Cfrac%7Ba_n%2Bb_n%7D%7B2%7D%2C+b_%7Bn%2B1%7D%3D%5Csqrt%7Ba_n+b_n%7D&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='&#92;displaystyle a_{n+1}=&#92;frac{a_n+b_n}{2}, b_{n+1}=&#92;sqrt{a_n b_n}' title='&#92;displaystyle a_{n+1}=&#92;frac{a_n+b_n}{2}, b_{n+1}=&#92;sqrt{a_n b_n}' class='latex' />.</p>
<p style="text-align:left;">研究<img src='http://s0.wp.com/latex.php?latex=a_n%2Fb_n&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='a_n/b_n' title='a_n/b_n' class='latex' />的极限。题目本身不难，很容易证明极限存在并且为1。比较值得注意的是这个数列收敛速度非常快（可以估计出数列是以指数的指数这样的速度收敛的）。这个题目看起来像一个普通的高等数学练习，但实际上背景很不简单：历史上最早研究这个问题的是Gauss。可以想象，能引起了Gauss兴趣的问题必定不是泛泛。Gauss问的是：给定初始值<img src='http://s0.wp.com/latex.php?latex=a_0%3Da%2C+b_0%3Db&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='a_0=a, b_0=b' title='a_0=a, b_0=b' class='latex' />, 极限<img src='http://s0.wp.com/latex.php?latex=%5Clim_%7Bn%5Crightarrow+%5Cinfty%7Da_n&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='&#92;lim_{n&#92;rightarrow &#92;infty}a_n' title='&#92;lim_{n&#92;rightarrow &#92;infty}a_n' class='latex' />是多少？他特别考虑了<img src='http://s0.wp.com/latex.php?latex=a%3D1%2C+b%3D%5Csqrt%7B2%7D&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='a=1, b=&#92;sqrt{2}' title='a=1, b=&#92;sqrt{2}' class='latex' />的情形。记<img src='http://s0.wp.com/latex.php?latex=%5Clim_%7Bn%5Crightarrow+%5Cinfty%7Da_n%3DM%28a%2C+b%29&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='&#92;lim_{n&#92;rightarrow &#92;infty}a_n=M(a, b)' title='&#92;lim_{n&#92;rightarrow &#92;infty}a_n=M(a, b)' class='latex' />. Gauss证明了下面的结论：</p>
<p style="text-align:center;"><img src='http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+%5Cfrac%7B%5Cpi%7D%7B2M%281%2C%5Csqrt%7B2%7D%29%7D%3D%5Cint_0%5E1%5Cfrac%7B%5Cmathrm%7Bd%7D+x%7D%7B%5Csqrt%7B1-x%5E4%7D%7D&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='&#92;displaystyle &#92;frac{&#92;pi}{2M(1,&#92;sqrt{2})}=&#92;int_0^1&#92;frac{&#92;mathrm{d} x}{&#92;sqrt{1-x^4}}' title='&#92;displaystyle &#92;frac{&#92;pi}{2M(1,&#92;sqrt{2})}=&#92;int_0^1&#92;frac{&#92;mathrm{d} x}{&#92;sqrt{1-x^4}}' class='latex' /></p>
<p style="text-align:left;">事实上，有如下更一般的结论：</p>
<p style="text-align:center;"><img src='http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+%5Cfrac%7B%5Cpi%7D%7B2M%281%2Cy%29%7D%3DK%28%5Csqrt%7By%5E2-1%7D%29&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='&#92;displaystyle &#92;frac{&#92;pi}{2M(1,y)}=K(&#92;sqrt{y^2-1})' title='&#92;displaystyle &#92;frac{&#92;pi}{2M(1,y)}=K(&#92;sqrt{y^2-1})' class='latex' /></p>
<p style="text-align:left;">也即<img src='http://s0.wp.com/latex.php?latex=M%28a%2C+b%29&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='M(a, b)' title='M(a, b)' class='latex' />可以用椭圆积分来表示！<img src='http://s0.wp.com/latex.php?latex=K%28k%29&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='K(k)' title='K(k)' class='latex' /> 是所谓的第一类完全椭圆积分：</p>
<p style="text-align:center;"><img src='http://s0.wp.com/latex.php?latex=%5Cdisplaystyle+K%28k%29%3D+%5Cint_0%5E%7B%5Cpi%2F2%7D%5Cfrac%7B%5Cmathrm%7Bd%7D+%5Ctheta%7D%7B%5Csqrt%7B1-k%5E2%5Csin%5E2%5Ctheta%7D%7D%3D%5Cint_0%5E1+%5Cfrac%7B%5Cmathrm%7Bd%7D+u%7D%7B%5Csqrt%7B%281-u%5E2%29%281-k%5E2u%5E2%29%7D%7D&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='&#92;displaystyle K(k)= &#92;int_0^{&#92;pi/2}&#92;frac{&#92;mathrm{d} &#92;theta}{&#92;sqrt{1-k^2&#92;sin^2&#92;theta}}=&#92;int_0^1 &#92;frac{&#92;mathrm{d} u}{&#92;sqrt{(1-u^2)(1-k^2u^2)}}' title='&#92;displaystyle K(k)= &#92;int_0^{&#92;pi/2}&#92;frac{&#92;mathrm{d} &#92;theta}{&#92;sqrt{1-k^2&#92;sin^2&#92;theta}}=&#92;int_0^1 &#92;frac{&#92;mathrm{d} u}{&#92;sqrt{(1-u^2)(1-k^2u^2)}}' class='latex' /></p>
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		<title>arXiv Digest 12/17/10</title>
		<link>http://dualm.wordpress.com/2010/12/17/arxiv-digest-121710/</link>
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		<pubDate>Fri, 17 Dec 2010 15:45:44 +0000</pubDate>
		<dc:creator>dualm</dc:creator>
				<category><![CDATA[arXiv Digest]]></category>

		<guid isPermaLink="false">http://dualm.wordpress.com/?p=232</guid>
		<description><![CDATA[The landscape of the Hubbard model Authors: Subir Sachdev Electron-Electron Interactions in Graphene: Current Status and Perspectives Authors: Valeri N. Kotov, Bruno Uchoa, Vitor M. Pereira, A. H. Castro Neto, F. Guinea Fractional quantum Hall effect in a U(1)xSU(2) gauge field Authors: Rebecca N. Palmer, Jiannis K. Pachos Localization of preformed Cooper-pairs in disordered superconductors [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=232&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p><a href="http://arxiv.org/abs/1012.0299">The landscape of the Hubbard model</a><br />
Authors: Subir Sachdev</p>
<p><a href="http://arxiv.org/abs/1012.3484">Electron-Electron Interactions in Graphene: Current Status and Perspectives</a><br />
Authors: Valeri N. Kotov, Bruno Uchoa, Vitor M. Pereira, A. H. Castro Neto, F. Guinea</p>
<p><a href="http://arxiv.org/abs/1012.3581">Fractional quantum Hall effect in a U(1)xSU(2) gauge field</a><br />
Authors: Rebecca N. Palmer, Jiannis K. Pachos</p>
<p><a href="http://arxiv.org/abs/1012.3630">Localization of preformed Cooper-pairs in disordered superconductors</a><br />
Authors: B. Sacepe, T. Dubouchet, C. Chapelier, M. Sanquer, M. Ovadia, D. Shahar, M. Feigel&#8217;man, L. Ioffe</p>
<p><a href="http://arxiv.org/abs/1012.3459">Anomalous Hall response of topological insulators</a><br />
Authors: Dimitrie Culcer, S. Das Sarma</p>
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		<title>arXiv Digest 12/01/10</title>
		<link>http://dualm.wordpress.com/2010/12/02/arxiv-digest-120110/</link>
		<comments>http://dualm.wordpress.com/2010/12/02/arxiv-digest-120110/#comments</comments>
		<pubDate>Thu, 02 Dec 2010 21:10:53 +0000</pubDate>
		<dc:creator>dualm</dc:creator>
				<category><![CDATA[arXiv Digest]]></category>
		<category><![CDATA[Uncategorized]]></category>

		<guid isPermaLink="false">http://dualm.wordpress.com/?p=215</guid>
		<description><![CDATA[Non-Abelian s-wave superconductivity in spin-orbit coupled systems: Bulk phases and quantum phase transitions Sumanta Tewari, Tudor D. Stanescu, Jay D. Sau, S. Das Sarma Evidence for electron-electron interaction in topological insulator thin films Jian Wang, Ashley M. DaSilva, Cui-Zu Chang, Ke He, J. K. Jain, Nitin Samarth, Xu-Cun Ma, Qi-Kun Xue, Moses H. W. Chan [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=dualm.wordpress.com&amp;blog=12155841&amp;post=215&amp;subd=dualm&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p><a href="http://arxiv.org/abs/1012.0057">Non-Abelian s-wave superconductivity in spin-orbit coupled systems: Bulk phases and quantum phase transitions<br />
</a>Sumanta Tewari, Tudor D. Stanescu, Jay D. Sau, S. Das Sarma</p>
<p><a href="http://arxiv.org/abs/1012.0271">Evidence for electron-electron interaction in topological insulator thin films</a><br />
Jian Wang, Ashley M. DaSilva, Cui-Zu Chang, Ke He, J. K. Jain, Nitin Samarth, Xu-Cun Ma, Qi-Kun Xue, Moses H. W. Chan</p>
<p><a href="http://arxiv.org/abs/1012.0296">Majorana fermion exchange in quasi-one-dimensional networks<br />
</a>David J Clarke, Jay D. Sau, Sumanta Tewari</p>
<p><a href="http://arxiv.org/abs/1012.0046">Fractionalization via <img src='http://s0.wp.com/latex.php?latex=%5Cmathbb%7BZ%7D_%7B2%7D&amp;bg=ffffff&amp;fg=555555&amp;s=0' alt='&#92;mathbb{Z}_{2}' title='&#92;mathbb{Z}_{2}' class='latex' /> Gauge Fields at a Cold Atom Quantum Hall Transition</a><br />
Yafis Barlas, Kun Yang</p>
<p>Two earlier preprints:</p>
<p><a href="http://arxiv.org/abs/1011.6371">Majorana End-States in Multi-band Microstructures with Rashba Spin-Orbit Coupling<br />
</a>Andrew C. Potter, Patrick A. Lee</p>
<p><a href="http://arxiv.org/abs/1011.6422">Topological superconductivity and Majorana fermions in half-metal / superconductor heterostructure<br />
</a>Suk Bum Chung, Hai-Jun Zhang, Xiao-Liang Qi, Shou-Cheng Zhang</p>
<p>Several more related</p>
<p><a href="http://arxiv.org/abs/1012.0317">Phase transitions in topological lattice models via topological symmetry breaking</a><br />
F. J. Burnell, Steven H. Simon, J. K. Slingerland</p>
<p><a href="http://arxiv.org/abs/1012.0330">Majorana modes at the ends of superconductor vortices in doped topological insulators</a><br />
Pavan Hosur, Pouyan Ghaemi, Roger S. K. Mong, Ashvin Vishwanath</p>
<p><a href="http://arxiv.org/abs/1012.0561">Controlling non-Abelian statistics of Majorana fermions in quasi-one-dimensional wire networks</a><br />
Jay D. Sau, D. J. Clarke, S. Tewari</p>
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