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		<summary type="html">&lt;p&gt;more specific stub type&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;In [[mathematics]] the &amp;#039;&amp;#039;&amp;#039;Lawrence–Krammer representation&amp;#039;&amp;#039;&amp;#039; is a [[group representation|representation]] of the [[braid group]]s.  It fits into a family of representations called the Lawrence representations.  The 1st Lawrence representation is the [[Burau representation]] and the 2nd is the Lawrence–Krammer representation.&lt;br /&gt;
&lt;br /&gt;
The Lawrence–Krammer representation is named after [[Ruth Lawrence]] and Daan Krammer.&amp;lt;ref&amp;gt;{{cite arXiv |author=Stephen Bigelow |authorlink= |eprint=math/0204057 |title=The Lawrence–Krammer representation |class= |year=2002 |version=v1 |accessdate=2008-09-08 }}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Definition ==&lt;br /&gt;
&lt;br /&gt;
Consider the [[braid group]] &amp;lt;math&amp;gt;B_n&amp;lt;/math&amp;gt; to be the [[mapping class group]] of a disc with &amp;#039;&amp;#039;n&amp;#039;&amp;#039; marked points &amp;lt;math&amp;gt;P_n&amp;lt;/math&amp;gt;.  The Lawrence–Krammer representation is defined as the action of &amp;lt;math&amp;gt;B_n&amp;lt;/math&amp;gt; on the homology of a certain [[covering map|covering]] space of the [[configuration space]] &amp;lt;math&amp;gt;C_2 P_n&amp;lt;/math&amp;gt;.  Specifically, &amp;lt;math&amp;gt;H_1 C_2 P_n \simeq \mathbb Z^{n+1}&amp;lt;/math&amp;gt;, and the subspace of &amp;lt;math&amp;gt; H_1 C_2 P_n&amp;lt;/math&amp;gt; invariant under the action of &amp;lt;math&amp;gt;B_n&amp;lt;/math&amp;gt; is primitive, free and of rank 2.  Generators for this invariant subspace are denoted by &amp;lt;math&amp;gt;q, t&amp;lt;/math&amp;gt;.  &lt;br /&gt;
&lt;br /&gt;
The covering space of &amp;lt;math&amp;gt;C_2 P_n&amp;lt;/math&amp;gt; corresponding to the kernel of the projection map &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\pi_1 C_2 P_n \to \mathbb Z^2 \langle q,t \rangle &amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
is called the Lawrence–Krammer cover and is denoted &amp;lt;math&amp;gt;\overline{C_2 P_n}&amp;lt;/math&amp;gt;. [[Diffeomorphism]]s of&amp;lt;math&amp;gt;P_n&amp;lt;/math&amp;gt; act on &amp;lt;math&amp;gt;P_n&amp;lt;/math&amp;gt;, thus also on &amp;lt;math&amp;gt;C_2 P_n&amp;lt;/math&amp;gt;, moreover they lift uniquely to diffeomorphisms of &amp;lt;math&amp;gt;\overline{C_2 P_n}&amp;lt;/math&amp;gt; which restrict to identity on the co-dimension two boundary stratum (where both points are on the boundary circle).  The action of &amp;lt;math&amp;gt;B_n&amp;lt;/math&amp;gt; on &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;H_2 \overline{C_2 P_n},&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
thought of as a &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathbb Z\langle t^{\pm},q^{\pm}\rangle&amp;lt;/math&amp;gt;-module, &lt;br /&gt;
&lt;br /&gt;
is the Lawrence–Krammer representation. &amp;lt;math&amp;gt;H_2 \overline{C_2 P_n}&amp;lt;/math&amp;gt; is known to be a free &amp;lt;math&amp;gt;\mathbb Z\langle t^{\pm},q^{\pm}\rangle&amp;lt;/math&amp;gt;-module, of rank &amp;lt;math&amp;gt;n \choose 2&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Matrices ==&lt;br /&gt;
&lt;br /&gt;
Using Bigelow&amp;#039;s conventions for the Lawrence–Krammer representation, generators for &amp;lt;math&amp;gt;H_2 \overline{C_2 P_n}&amp;lt;/math&amp;gt; are denoted &amp;lt;math&amp;gt;v_{j,k}&amp;lt;/math&amp;gt; for &amp;lt;math&amp;gt;1 \leq j &amp;lt; k \leq n&amp;lt;/math&amp;gt;.  Letting &amp;lt;math&amp;gt;\sigma_i&amp;lt;/math&amp;gt; denote the standard Artin generators of the [[braid group]], we get the expression:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\sigma_i\cdot v_{j,k} = \left\{&lt;br /&gt;
\begin{array}{lr}&lt;br /&gt;
v_{j,k} &amp;amp; i\notin \{j-1,j,k-1,k\}, \\&lt;br /&gt;
qv_{i,k} + (q^2-q)v_{i,j} + (1-q)v_{j,k} &amp;amp; i=j-1 \\&lt;br /&gt;
v_{j+1,k} &amp;amp; i=j\neq k-1, \\&lt;br /&gt;
qv_{j,i} + (1-q)v_{j,k} - (q^2-q)tv_{i,k} &amp;amp; i=k-1\neq j,\\&lt;br /&gt;
v_{j,k+1} &amp;amp; i=k,\\&lt;br /&gt;
-tq^2v_{j,k} &amp;amp; i=j=k-1.&lt;br /&gt;
\end{array}&lt;br /&gt;
\right.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Faithfulness ==&lt;br /&gt;
&lt;br /&gt;
Stephen Bigelow and Daan Krammer have independent proofs that the Lawrence–Krammer representation is [[group representation|faithful]].&lt;br /&gt;
&lt;br /&gt;
== Geometry ==&lt;br /&gt;
&lt;br /&gt;
The Lawrence–Krammer representation preserves a non-degenerate [[sesquilinear form]] which is known to be negative-definite Hermitian provided &amp;lt;math&amp;gt;q, t&amp;lt;/math&amp;gt; are specialized to suitable unit complex numbers (&amp;#039;&amp;#039;q&amp;#039;&amp;#039; near &amp;#039;&amp;#039;1&amp;#039;&amp;#039; and &amp;#039;&amp;#039;t&amp;#039;&amp;#039; near &amp;#039;&amp;#039;i&amp;#039;&amp;#039;).  Thus the braid group is a subgroup of the [[unitary group]] of &amp;lt;math&amp;gt;\frac{n(n-1)}{2}&amp;lt;/math&amp;gt;-square matrices. Recently it has been shown that the image of the Lawrence–Krammer representation is [[dense set|dense subgroup]] of the [[unitary group]] in this case. &lt;br /&gt;
&lt;br /&gt;
The sesquilinear form has the explicit description:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \langle v_{i,j}, v_{k,l}\rangle = -(1-t)(1+qt)(q-1)^2t^{-2}q^{-3}&lt;br /&gt;
\left\{&lt;br /&gt;
\begin{array}{lr}&lt;br /&gt;
-q^2t^2(q-1) &amp;amp; i=k&amp;lt;j&amp;lt;l \text{ or } i&amp;lt;k&amp;lt;j=l \\&lt;br /&gt;
-(q-1) &amp;amp; k=i&amp;lt;l&amp;lt;j \text{ or } k&amp;lt;i&amp;lt;j=l \\&lt;br /&gt;
t(q-1) &amp;amp; i&amp;lt;j=k&amp;lt;l \\&lt;br /&gt;
q^2t(q-1) &amp;amp; k&amp;lt;l=i&amp;lt;j \\&lt;br /&gt;
-t(q-1)^2(1+qt) &amp;amp; i&amp;lt;k&amp;lt;j&amp;lt;l \\&lt;br /&gt;
(q-1)^2(1+qt) &amp;amp; k&amp;lt;i&amp;lt;l&amp;lt;j \\&lt;br /&gt;
(1-qt)(1+q^2t) &amp;amp; k=i, j=l \\&lt;br /&gt;
0 &amp;amp; \text{otherwise} \\&lt;br /&gt;
\end{array}&lt;br /&gt;
\right.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* S. Bigelow, &amp;#039;&amp;#039;Braid groups are linear&amp;#039;&amp;#039;, J. Amer. Math. Soc. 14 (2001), 471-486.&lt;br /&gt;
* S. Bigelow, &amp;#039;&amp;#039;The Lawrence–Krammer representation&amp;#039;&amp;#039;, Topology and geometry of manifolds, Proc. Sympos. Pure Math., 71 (2003) &lt;br /&gt;
* R. Budney, &amp;#039;&amp;#039;On the image of the Lawrence–Krammer representation&amp;#039;&amp;#039;, J Knot. Th. Ram. (2005)&lt;br /&gt;
* D. Krammer, &amp;#039;&amp;#039;Braid groups are linear&amp;#039;&amp;#039;, Ann. Math. 155 (2002), 131-156.&lt;br /&gt;
* L. Paoluzzi and L. Paris, &amp;#039;&amp;#039;A note on the Lawrence-Krammer-Bigelow representation&amp;#039;&amp;#039;, Alg. Geom. Topology 2 (2002), 499-518.&lt;br /&gt;
&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Lawrence-Krammer representation}}&lt;br /&gt;
[[Category:Braid groups]]&lt;br /&gt;
[[Category:Representation theory]]&lt;/div&gt;</summary>
		<author><name>en&gt;Qetuth</name></author>
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