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		<title>Degree of Separation in Finite Graphs: Part 1</title>
		<link>http://josephzambrano.wordpress.com/2010/11/28/degree-of-separation-in-finite-graphs-part-1/</link>
		<comments>http://josephzambrano.wordpress.com/2010/11/28/degree-of-separation-in-finite-graphs-part-1/#comments</comments>
		<pubDate>Sun, 28 Nov 2010 23:47:05 +0000</pubDate>
		<dc:creator>josephzambrano</dc:creator>
				<category><![CDATA[Mathematics]]></category>

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		<description><![CDATA[This post was inspired by the concept of six degrees of separation. This concept basically states that every two people are, in a sense, connected through at most six people. In this post, we will attempt to formalize and generalize the concept via graph theory. First we must choose a finite set of vertices for [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=josephzambrano.wordpress.com&amp;blog=12635463&amp;post=33&amp;subd=josephzambrano&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>This post was inspired by the concept of <em>six degrees of separation</em>. This concept basically states that every two people are, in a sense, connected through at most six people. In this post, we will attempt to formalize and generalize the concept via graph theory.</p>
<p>First we must choose a finite set <img src='http://s0.wp.com/latex.php?latex=V&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='V' title='V' class='latex' /> of vertices for our graph <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='G' title='G' class='latex' />. Furthermore, we must introduce the notion of distance between these vertices. The most convenient way of do this is to embed <img src='http://s0.wp.com/latex.php?latex=V&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='V' title='V' class='latex' /> into <img src='http://s0.wp.com/latex.php?latex=%5Cmathbb%7BR%7D%5E2&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;mathbb{R}^2' title='&#92;mathbb{R}^2' class='latex' /> via a mapping <img src='http://s0.wp.com/latex.php?latex=%5Cphi%3AV%5Chookrightarrow%5Cmathbb%7BR%7D%5E2&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;phi:V&#92;hookrightarrow&#92;mathbb{R}^2' title='&#92;phi:V&#92;hookrightarrow&#92;mathbb{R}^2' class='latex' />. This embedding associates each <img src='http://s0.wp.com/latex.php?latex=v%5Cin+V&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='v&#92;in V' title='v&#92;in V' class='latex' /> to some point <img src='http://s0.wp.com/latex.php?latex=%5Cphi%28v%29%3D%28x_v%2Cy_v%29%5Cin%5Cmathbb%7BR%7D%5E2&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;phi(v)=(x_v,y_v)&#92;in&#92;mathbb{R}^2' title='&#92;phi(v)=(x_v,y_v)&#92;in&#92;mathbb{R}^2' class='latex' />. This allows us to utilize the Euclidean metric:</p>
<p><img src='http://s0.wp.com/latex.php?latex=%5Cdelta%28u%2Cv%29%3D%5Csqrt%7B%28x_u-x_v%29%5E2%2B%28y_u-y_v%29%5E2%7D%3Au%2Cv%5Cin+V&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;delta(u,v)=&#92;sqrt{(x_u-x_v)^2+(y_u-y_v)^2}:u,v&#92;in V' title='&#92;delta(u,v)=&#92;sqrt{(x_u-x_v)^2+(y_u-y_v)^2}:u,v&#92;in V' class='latex' /></p>
<p>We now impose a condition on our graph <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='G' title='G' class='latex' />:</p>
<p>(i.) Given the edge set <img src='http://s0.wp.com/latex.php?latex=E&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='E' title='E' class='latex' /> of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='G' title='G' class='latex' />, the probability <img src='http://s0.wp.com/latex.php?latex=%5Crho&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;rho' title='&#92;rho' class='latex' /> that <img src='http://s0.wp.com/latex.php?latex=%5C%7Bu%2Cv%5C%7D%5Cin+E&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;{u,v&#92;}&#92;in E' title='&#92;{u,v&#92;}&#92;in E' class='latex' /> is dependent on <img src='http://s0.wp.com/latex.php?latex=%5Cdelta%28u%2Cv%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;delta(u,v)' title='&#92;delta(u,v)' class='latex' />. </p>
<p>(ii.) The probability of an edge belonging to <img src='http://s0.wp.com/latex.php?latex=E&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='E' title='E' class='latex' /> is independent of all other edges.</p>
<p>We now impose conditions on <img src='http://s0.wp.com/latex.php?latex=%5Crho&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;rho' title='&#92;rho' class='latex' />:</p>
<p>(i.) <img src='http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%5Clim_%7Bx%5Cto+0%7D%5Crho%28%5Cdelta%29%3D1&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;displaystyle&#92;lim_{x&#92;to 0}&#92;rho(&#92;delta)=1' title='&#92;displaystyle&#92;lim_{x&#92;to 0}&#92;rho(&#92;delta)=1' class='latex' /></p>
<p>(ii.) <img src='http://s0.wp.com/latex.php?latex=%5Cdisplaystyle%5Clim_%7Bx%5Cto%5Cinfty%7D%5Crho%28%5Cdelta%29%3D0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;displaystyle&#92;lim_{x&#92;to&#92;infty}&#92;rho(&#92;delta)=0' title='&#92;displaystyle&#92;lim_{x&#92;to&#92;infty}&#92;rho(&#92;delta)=0' class='latex' /></p>
<p>(iii.) <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7Bd%5Crho%7D%7Bd%5Cdelta%7D%3C0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;frac{d&#92;rho}{d&#92;delta}&lt;0' title='&#92;frac{d&#92;rho}{d&#92;delta}&lt;0' class='latex' /> <img src='http://s0.wp.com/latex.php?latex=%5Cforall+%5Cdelta%5Cin+%5B0%2C%5Cinfty%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;forall &#92;delta&#92;in [0,&#92;infty)' title='&#92;forall &#92;delta&#92;in [0,&#92;infty)' class='latex' /></p>
<p>Clearly the function <img src='http://s0.wp.com/latex.php?latex=%5Crho%28%5Cdelta%29%3De%5E%7B-%5Cdelta%7D&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;rho(&#92;delta)=e^{-&#92;delta}' title='&#92;rho(&#92;delta)=e^{-&#92;delta}' class='latex' /> satisfies these conditions. Since <img src='http://s0.wp.com/latex.php?latex=%5Cdelta%3AV%5Ctimes+V%5Crightarrow+%5B0%2C%5Cinfty%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;delta:V&#92;times V&#92;rightarrow [0,&#92;infty)' title='&#92;delta:V&#92;times V&#92;rightarrow [0,&#92;infty)' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Crho%3A%5B0%2C%5Cinfty%29%5Crightarrow+%5B0%2C1%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;rho:[0,&#92;infty)&#92;rightarrow [0,1)' title='&#92;rho:[0,&#92;infty)&#92;rightarrow [0,1)' class='latex' />, we know <img src='http://s0.wp.com/latex.php?latex=%5Crho%5Ccirc%5Cdelta%3AV%5Ctimes+V%5Crightarrow+%5B0%2C1%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;rho&#92;circ&#92;delta:V&#92;times V&#92;rightarrow [0,1)' title='&#92;rho&#92;circ&#92;delta:V&#92;times V&#92;rightarrow [0,1)' class='latex' />.</p>
<p>We now define the <em>separation</em>, <img src='http://s0.wp.com/latex.php?latex=%5Comega%28u%2Cv%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;omega(u,v)' title='&#92;omega(u,v)' class='latex' />, of <img src='http://s0.wp.com/latex.php?latex=u&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='u' title='u' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=v&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='v' title='v' class='latex' /> as the length of the minimal path between <img src='http://s0.wp.com/latex.php?latex=u&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='u' title='u' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=v&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='v' title='v' class='latex' />. Clearly <img src='http://s0.wp.com/latex.php?latex=%5Comega%28u%2Cu%29%3D0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;omega(u,u)=0' title='&#92;omega(u,u)=0' class='latex' /> and given a disconnected vertice <img src='http://s0.wp.com/latex.php?latex=v%5Cin+V&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='v&#92;in V' title='v&#92;in V' class='latex' />, we define <img src='http://s0.wp.com/latex.php?latex=%5Comega%28u%2Cv%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;omega(u,v)' title='&#92;omega(u,v)' class='latex' /> to be <em>immeasurable</em>. We also define the <em>degree of separation</em> of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='G' title='G' class='latex' />, <img src='http://s0.wp.com/latex.php?latex=%5Comega%28G%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;omega(G)' title='&#92;omega(G)' class='latex' /> as the average value of <img src='http://s0.wp.com/latex.php?latex=%5Comega%28u%2Cv%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;omega(u,v)' title='&#92;omega(u,v)' class='latex' />, as <img src='http://s0.wp.com/latex.php?latex=u&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='u' title='u' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=v&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='v' title='v' class='latex' /> range over all vertices. We know that <img src='http://s0.wp.com/latex.php?latex=%5Comega%28u%2Cv%29%3D%5Comega%28v%2Cu%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;omega(u,v)=&#92;omega(v,u)' title='&#92;omega(u,v)=&#92;omega(v,u)' class='latex' /> for all vertices. We can now pose the following questions:</p>
<p>(i.) Given any number <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='n' title='n' class='latex' />, what embedding <img src='http://s0.wp.com/latex.php?latex=%5Cphi&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;phi' title='&#92;phi' class='latex' />, if any, will ensure <img src='http://s0.wp.com/latex.php?latex=%5Comega%28G%29%3Dn&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;omega(G)=n' title='&#92;omega(G)=n' class='latex' />? Moreover, is this embedding necessarily unique? If not, then does the condition <img src='http://s0.wp.com/latex.php?latex=%5Comega%28G%29%3Dn&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;omega(G)=n' title='&#92;omega(G)=n' class='latex' /> induce an equivalence class on such embeddings?</p>
<p>(ii.) Does there exist a algorithm to express <img src='http://s0.wp.com/latex.php?latex=%5Comega%28G%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;omega(G)' title='&#92;omega(G)' class='latex' /> given <img src='http://s0.wp.com/latex.php?latex=%7CV%7C&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='|V|' title='|V|' class='latex' />? If so, what is its computational complexity?</p>
<p>In the next post, we will begin to explore these questions in great detail.</p>
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		<title>Algebraic Topology: Part 2</title>
		<link>http://josephzambrano.wordpress.com/2010/03/18/algebraic-topology-post-2/</link>
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		<pubDate>Thu, 18 Mar 2010 20:48:22 +0000</pubDate>
		<dc:creator>josephzambrano</dc:creator>
				<category><![CDATA[Mathematics]]></category>

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		<description><![CDATA[In the last post, we established the notion of a path and loop in a topological space . A path is a continuous image of the interval into . A loop is a path such that the endpoints of the mapping are equal. Remember that a continuous map takes open sets to open sets. We [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=josephzambrano.wordpress.com&amp;blog=12635463&amp;post=17&amp;subd=josephzambrano&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>In the last post, we established the notion of a path and loop in a topological space <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' />. A path is a continuous image of the interval <img src='http://s0.wp.com/latex.php?latex=I%3D%5B0%2C1%5D&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='I=[0,1]' title='I=[0,1]' class='latex' /> into <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' />. A loop is a path such that the endpoints of the mapping are equal. Remember that a continuous map takes open sets to open sets. We also established the idea of a homotopy. A homotopy is a continuous deformation of a space into another. A path homotopy <img src='http://s0.wp.com/latex.php?latex=H%3AI%5Ctimes+I%5Cdisplaystyle%5Crightarrow+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='H:I&#92;times I&#92;displaystyle&#92;rightarrow X' title='H:I&#92;times I&#92;displaystyle&#92;rightarrow X' class='latex' /> deforms one path in <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> to another. Two paths are homotopic if there exists a homotopy between them. Moreover, the existence of such a homotopy is an equivalence relation on paths in a space. We denote a set of homotopic paths in <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> as <img src='http://s0.wp.com/latex.php?latex=%5Bf%5D&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='[f]' title='[f]' class='latex' />. We then said that the fundemental group <img src='http://s0.wp.com/latex.php?latex=%5Cpi_1%28X%2Cx_0%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;pi_1(X,x_0)' title='&#92;pi_1(X,x_0)' class='latex' /> of <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> based at <img src='http://s0.wp.com/latex.php?latex=x_0%5Cin+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0&#92;in X' title='x_0&#92;in X' class='latex' /> is the set of equivalence classes of homotopic loops at <img src='http://s0.wp.com/latex.php?latex=x_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0' title='x_0' class='latex' /> under the group operation of concatenation. Also, recall that we said that the fundemental group essentially counts the number of 1-dimensional holes in the space. For higher dimensional holes, we use the higher homotopy groups, but thats a post for another day.</p>
<p>In general, the fundemental group is determined by the choice of basepoint. However, we can easily show (and it is quite intuitive) that for any path connected space <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> (i.e. a space such that there exists a path between any two points),  the fundemental groups at two unequal points in <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> are isomorphic (they are equal). This fact can be applied to the arguments in the last post about the fundemental groups of euclidean spaces, as well as the circle, since they are path connected.</p>
<p>In the last post, I stated that the fundemental group acts as a functor from the category <img src='http://s0.wp.com/latex.php?latex=Top&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='Top' title='Top' class='latex' /> to the category <img src='http://s0.wp.com/latex.php?latex=Grp&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='Grp' title='Grp' class='latex' />. This means that for any continuous map <img src='http://s0.wp.com/latex.php?latex=f%3AX%5Crightarrow+Y&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f:X&#92;rightarrow Y' title='f:X&#92;rightarrow Y' class='latex' />, every loop in <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> with basepoint <img src='http://s0.wp.com/latex.php?latex=x_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0' title='x_0' class='latex' /> is mapped to a loop in <img src='http://s0.wp.com/latex.php?latex=Y&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='Y' title='Y' class='latex' /> with basepoint <img src='http://s0.wp.com/latex.php?latex=y_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='y_0' title='y_0' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=f%28x_0%29%3Dy_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f(x_0)=y_0' title='f(x_0)=y_0' class='latex' />. This results in a group homomorphism <img src='http://s0.wp.com/latex.php?latex=%5Cpi%28f%29%3A%5Cpi_1%28X%29%5Crightarrow+%5Cpi_1%28Y%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;pi(f):&#92;pi_1(X)&#92;rightarrow &#92;pi_1(Y)' title='&#92;pi(f):&#92;pi_1(X)&#92;rightarrow &#92;pi_1(Y)' class='latex' /> called the induced homomorphism. Also, given any two continuous maps <img src='http://s0.wp.com/latex.php?latex=f%3AX%5Crightarrow+Y&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f:X&#92;rightarrow Y' title='f:X&#92;rightarrow Y' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=g%3AX%5Crightarrow+Y&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='g:X&#92;rightarrow Y' title='g:X&#92;rightarrow Y' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=f%28x_0%29%3Dg%28x_0%29%3Dy_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f(x_0)=g(x_0)=y_0' title='f(x_0)=g(x_0)=y_0' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=f%5Csimeq+g&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f&#92;simeq g' title='f&#92;simeq g' class='latex' /> (homotopic relative to <img src='http://s0.wp.com/latex.php?latex=x_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0' title='x_0' class='latex' />), then <img src='http://s0.wp.com/latex.php?latex=X%5Csimeq+Y%5CRightarrow+%5Cpi_1%28X%2Cx_0%29%5Ccong+%5Cpi_1%28Y%2Cy_0%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X&#92;simeq Y&#92;Rightarrow &#92;pi_1(X,x_0)&#92;cong &#92;pi_1(Y,y_0)' title='X&#92;simeq Y&#92;Rightarrow &#92;pi_1(X,x_0)&#92;cong &#92;pi_1(Y,y_0)' class='latex' />. This means that the functor does not distinguish between homotopic maps at a given bsepoint. Therefore, homotopy equivalent path connected spaces have isomorphic fundemental groups. </p>
<p>I stated that I we would prove a well know result using fundemental groups in this post. But I need something to talk about next time, so it will wait.</p>
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		<title>Algebraic Topology: Part 1</title>
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		<pubDate>Wed, 17 Mar 2010 00:50:11 +0000</pubDate>
		<dc:creator>josephzambrano</dc:creator>
				<category><![CDATA[Mathematics]]></category>

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		<description><![CDATA[If we wish to study algebraic topology, we should first motivate the subject. Therefore we should ask, &#8220;What is algebraic topology (and topology for that matter) and why should we learn it?&#8221;. To answer the first part of the question, topology is the study of spatial properties that are preserved under continuous deformations of an [...]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=josephzambrano.wordpress.com&amp;blog=12635463&amp;post=9&amp;subd=josephzambrano&amp;ref=&amp;feed=1" width="1" height="1" />]]></description>
			<content:encoded><![CDATA[<p>If we wish to study algebraic topology, we should first motivate the subject. Therefore we should ask, &#8220;What is algebraic topology (and topology for that matter) and why should we learn it?&#8221;. To answer the first part of the question, topology is the study of spatial properties that are preserved under continuous deformations of an object (this will be much more clear latter). In algebraic topology, we try to reduce topological questions into questions of algebra, a field which is very well understood. We can do this by introducing algebraic invariants into the mix. As for the second part of the question, topology is simply a language to speak about geometry in a much larger setting. </p>
<p>Now that we have motivated the topic at hand, we can begin. Since this is algebraic topology, I will assume you are already comfortable with some basic point-set topology. If not, I recommend that you search for &#8220;topology notes&#8221; on google. You&#8217;re bound to find a decent reference. </p>
<p>Earlier I spoke about topology being the study of certain objects under continuous deformations. These objects are called <a href="http://en.wikipedia.org/wiki/Topological_spaces">topological spaces</a> and continuous deformations are simply continuous maps or functions. Remember, we call a map <img src='http://s0.wp.com/latex.php?latex=f%3AX%5Cdisplaystyle%5Crightarrow+Y&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f:X&#92;displaystyle&#92;rightarrow Y' title='f:X&#92;displaystyle&#92;rightarrow Y' class='latex' /> from a topological space <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> to a topological space <img src='http://s0.wp.com/latex.php?latex=Y&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='Y' title='Y' class='latex' /> if <img src='http://s0.wp.com/latex.php?latex=f&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f' title='f' class='latex' /> takes open sets in <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> to open sets in <img src='http://s0.wp.com/latex.php?latex=Y&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='Y' title='Y' class='latex' />. For those who study category theory,<a href="http://en.wikipedia.org/wiki/Continuity_(topology)"> continuous maps </a>are the morphisms of the category <img src='http://s0.wp.com/latex.php?latex=Top&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='Top' title='Top' class='latex' />. </p>
<p>In algebraic topology, and especially homotopy theory, we study objects on topological spaces called paths. We will find that paths allow us to define an extremely important construction called the fundemental group. A <a href="http://en.wikipedia.org/wiki/Path_(topology)">path</a> is a continuous function <img src='http://s0.wp.com/latex.php?latex=f%3AI%5Cdisplaystyle%5Crightarrow+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f:I&#92;displaystyle&#92;rightarrow X' title='f:I&#92;displaystyle&#92;rightarrow X' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=I&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='I' title='I' class='latex' /> is the unit interval, <img src='http://s0.wp.com/latex.php?latex=%5B0%2C1%5D&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='[0,1]' title='[0,1]' class='latex' />, and <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> is a topological space. We say a <img src='http://s0.wp.com/latex.php?latex=f&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f' title='f' class='latex' /> is a path from <img src='http://s0.wp.com/latex.php?latex=x_0%5Cin+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0&#92;in X' title='x_0&#92;in X' class='latex' /> to <img src='http://s0.wp.com/latex.php?latex=x_1%5Cin+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_1&#92;in X' title='x_1&#92;in X' class='latex' /> if <img src='http://s0.wp.com/latex.php?latex=f%280%29%3Dx_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f(0)=x_0' title='f(0)=x_0' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=f%281%29%3Dx_1&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f(1)=x_1' title='f(1)=x_1' class='latex' />. We call a path a loop if <img src='http://s0.wp.com/latex.php?latex=f%280%29%3Df%281%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f(0)=f(1)' title='f(0)=f(1)' class='latex' />. Given two paths <img src='http://s0.wp.com/latex.php?latex=f%2Cf%27&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='f,f&#039;' title='f,f&#039;' class='latex' /> from <img src='http://s0.wp.com/latex.php?latex=x_0%5Cin+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0&#92;in X' title='x_0&#92;in X' class='latex' /> to <img src='http://s0.wp.com/latex.php?latex=x_1%5Cin+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_1&#92;in X' title='x_1&#92;in X' class='latex' /> on a topological space <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> that share endpoints, we define a path <a href="http://en.wikipedia.org/wiki/Homotopy">homotopy</a> <img src='http://s0.wp.com/latex.php?latex=F%3A+I%5Ctimes+I%5Cdisplaystyle%5Crightarrow+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='F: I&#92;times I&#92;displaystyle&#92;rightarrow X' title='F: I&#92;times I&#92;displaystyle&#92;rightarrow X' class='latex' /> as a continuous map that has the following properties: <img src='http://s0.wp.com/latex.php?latex=F%28s%2C0%29%3Df%28s%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='F(s,0)=f(s)' title='F(s,0)=f(s)' class='latex' />, <img src='http://s0.wp.com/latex.php?latex=F%28s%2C1%29%3Df%27%28s%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='F(s,1)=f&#039;(s)' title='F(s,1)=f&#039;(s)' class='latex' />, <img src='http://s0.wp.com/latex.php?latex=F%280%2Ct%29%3Dx_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='F(0,t)=x_0' title='F(0,t)=x_0' class='latex' />, <img src='http://s0.wp.com/latex.php?latex=F%281%2Ct%29%3Dx_1&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='F(1,t)=x_1' title='F(1,t)=x_1' class='latex' />. Intuitively, this can be viewed as a continuous deformation of the original path to the second one. Also, it is correct to say that homotopy essentially counts the holes in a space.</p>
<p>It is easy to show that path homotopy is an equivalence relation. Therefore, given the set of all loops based at a point <img src='http://s0.wp.com/latex.php?latex=x_0%5Cin+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0&#92;in X' title='x_0&#92;in X' class='latex' /> in a topological space <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' />, we place homotopic loops at <img src='http://s0.wp.com/latex.php?latex=x_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0' title='x_0' class='latex' /> into equivalence classes. In other words, all the loops at <img src='http://s0.wp.com/latex.php?latex=x_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0' title='x_0' class='latex' /> that have a homotopy between then (can be continuously deformed into each other) are put into a single class. We can denote a class of homotopic loops at <img src='http://s0.wp.com/latex.php?latex=x_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0' title='x_0' class='latex' /> as <img src='http://s0.wp.com/latex.php?latex=%5Bf%5D&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='[f]' title='[f]' class='latex' />. If we consider the set of all eqivalence classes of loops based at a single point in a pointed topological space and the operation of concatenation (fancy word for connecting) we obtain a group called the fundemental group, <img src='http://s0.wp.com/latex.php?latex=%5Cpi_1%28X%2Cx_0%29&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;pi_1(X,x_0)' title='&#92;pi_1(X,x_0)' class='latex' />. For example, imagine a topological space <img src='http://s0.wp.com/latex.php?latex=X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='X' title='X' class='latex' /> and point <img src='http://s0.wp.com/latex.php?latex=x_0%5Cin+X&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0&#92;in X' title='x_0&#92;in X' class='latex' />. Imagine that there are three equivalence classes of loops at <img src='http://s0.wp.com/latex.php?latex=x_0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='x_0' title='x_0' class='latex' /> (i.e. three sets homotopic of loops). Call them <img src='http://s0.wp.com/latex.php?latex=%5Bf%5D&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='[f]' title='[f]' class='latex' />, <img src='http://s0.wp.com/latex.php?latex=%5Bg%5D&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='[g]' title='[g]' class='latex' />, and <img src='http://s0.wp.com/latex.php?latex=%5Bf%2Ag%5D&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='[f*g]' title='[f*g]' class='latex' />. Then we define the concatenation of loops as <img src='http://s0.wp.com/latex.php?latex=%5Bf%5D%2A%5Bg%5D%3D%5Bf%2Ag%5D&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='[f]*[g]=[f*g]' title='[f]*[g]=[f*g]' class='latex' /> (i.e. concatenation is well-defined). Do note that I am being quite liberal by defining the third equivalence class in this example as the concatenation of the others, but I&#8217;m simply trying to reinforce that this is a group.</p>
<p>Now for a concrete example of the fundamental group. Consider any Euclidean space <img src='http://s0.wp.com/latex.php?latex=R%5En&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='R^n' title='R^n' class='latex' />. Then the fundemental group of <img src='http://s0.wp.com/latex.php?latex=R%5En&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='R^n' title='R^n' class='latex' /> at any basepoint contains only one element. This is due to the fact that all loops in <img src='http://s0.wp.com/latex.php?latex=R%5En&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='R^n' title='R^n' class='latex' /> can be deformed into each other (i.e. they are homotopic). Intuitively this is because there are no &#8220;holes&#8221; in a Euclidean space. Therefore the fundemental group <img src='http://s0.wp.com/latex.php?latex=%5Cpi_1%28R%5En%29%3D0&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;pi_1(R^n)=0' title='&#92;pi_1(R^n)=0' class='latex' /> (i.e. it is the trivial group of one element). </p>
<p>Another great example is that of the circle <img src='http://s0.wp.com/latex.php?latex=S%5E1&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='S^1' title='S^1' class='latex' />. Essentially, we consider loops that wrap around the circle <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='n' title='n' class='latex' /> times. We consider loops that move counter-clockwise as positive and those that move clockwise as negative. It is obvious that loops with the same number of turns are homotopic. Therefore, we get a one-to-one correspondence between the homotopy classes of <img src='http://s0.wp.com/latex.php?latex=S%5E1&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='S^1' title='S^1' class='latex' /> and the integers. Therefore we can conclude that <img src='http://s0.wp.com/latex.php?latex=%5Cpi_1%28S%5E1%29%3DZ&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='&#92;pi_1(S^1)=Z' title='&#92;pi_1(S^1)=Z' class='latex' />. Despite the simple reasoning, we will need a bit more machinery to actually prove this. </p>
<p>Now that we have established the fundemental group as a concrete construction, we examine its properties when acted on by continuous deformations (this is topology after all). Without getting too far into the next post, a homeomorphism of topological spaces induce homomorphism between the underlying fundemental groups. </p>
<p>Next time, we will discuss the implications of the fundemental group in a categorical sense (we will show that the fundemental group is a funtor from the catergory <img src='http://s0.wp.com/latex.php?latex=Top&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='Top' title='Top' class='latex' /> to <img src='http://s0.wp.com/latex.php?latex=Grp&amp;bg=1B1B1B&amp;fg=DDDDDD&amp;s=0' alt='Grp' title='Grp' class='latex' />). We will also prove a very well known result using the fundemental group.</p>
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