<?xml version='1.0' encoding='UTF-8'?><?xml-stylesheet href='static/style.xsl' type='text/xsl'?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-09-19T19:22:32Z</responseDate><request verb="GetRecord" identifier="oai:ecommons.cornell.edu:1813/31119" metadataPrefix="dim">https://ecommons.cornell.edu/server/oai/request</request><GetRecord><record><header><identifier>oai:ecommons.cornell.edu:1813/31119</identifier><datestamp>2026-05-14T13:52:23Z</datestamp><setSpec>com_1813_35</setSpec><setSpec>col_1813_47</setSpec></header><metadata><dim:dim xmlns:dim="http://www.dspace.org/xmlns/dspace/dim" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.dspace.org/xmlns/dspace/dim http://www.dspace.org/schema/dim.xsd">
   <dim:field mdschema="dc" element="contributor" qualifier="author" lang="en_US">Samuelson, Peter</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="chair" lang="en_US">Berest, Yuri</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="committeeMember" lang="en_US">Knutson, Allen</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="committeeMember" lang="en_US">Sjamaar, Reyer</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="accessioned">2013-01-31T19:44:23Z</dim:field>
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   <dim:field mdschema="dc" element="date" qualifier="issued" lang="en_US">2012-08-20</dim:field>
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   <dim:field mdschema="dc" element="identifier" qualifier="bibid">7959867</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="abstract" lang="en_US">If M is a 3-manifold, the Kauffman bracket skein module is a vector space Kq (M ) functorially associated to M that depends on a parameter q ∈ C* . If F is a surface, then Kq (F x [0, 1]) is an algebra, and Kq (M ) is a module over Kq ((∂M ) x [0, 1]). One motivation for the definition is that if L [SUBSET OF] S 3 is a knot, then the (colored) Jones polynomials Jn (L) ∈ C[q ±1 ] can be computed from Kq (S 3 \ L). It was shown in [14] that Kq (T 2 x [0, 1]) ~ AZ2 , the subalgebra of the quantum =q torus XY = q 2 Y X which is invariant under the involution X [RIGHTWARDS ARROW] X [-]1 , Y [RIGHTWARDS ARROW] Y [-]1 . Our starting point is the observation that the category of AZ2 -modules is equivalent q to the category of modules over a simpler algebra, the crossed product Aq Z2 . We write ML for the image of Kq (S 3 \ L) under this equivalence. Theorem 5.2.1 gives a simple formula showing Jn (L) can be computed from ML , and Corollary 5.3.3 shows a recursion relation for Jn (L) can be computed from ML (if ML is f.g. over C[X ±1 ]). In Chapter 6 we give an explicit description of ML when L is the trefoil. Conjecture 4.3.4 conjectures the general structure of ML for torus knots. The algebra Aq Z2 is the t = 1 subfamily of the double affine Hecke algebra Hq,t of type A1 . In Chapter 8 we give a new skein-theoretic realization of the + + spherical subalgebra Hq,t , and we also give a construction associating an Hq,t - module ML (t) to each knot L. In Chapter 9 we construct algebraic deformations of the skein module ML to a family of modules ML (t) over Hq,t . In the case when L is the trefoil, we use these deformations to give example calculations of 2-variable polynomials Jn (q, t) that specialize to the colored Jones polynomials when t = 1.</dim:field>
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   <dim:field mdschema="dc" element="subject" lang="en_US">knot theory</dim:field>
   <dim:field mdschema="dc" element="subject" lang="en_US">quantum algebra</dim:field>
   <dim:field mdschema="dc" element="title" lang="en_US">Kauffman Bracket Skein Modules And The Quantum Torus</dim:field>
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   <dim:field mdschema="cris" element="virtual" qualifier="author" lang="en_US">Samuelson, Peter</dim:field>
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   	&lt;Title>Kauffman Bracket Skein Modules And The Quantum Torus&lt;/Title>
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   	&lt;PublicationDate>2012-08-20&lt;/PublicationDate>
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        	&lt;DisplayName>Samuelson, Peter&lt;/DisplayName>
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    &lt;Keyword>knot theory&lt;/Keyword>
    &lt;Keyword>quantum algebra&lt;/Keyword>
   	&lt;Abstract>If M is a 3-manifold, the Kauffman bracket skein module is a vector space Kq (M ) functorially associated to M that depends on a parameter q ∈ C* . If F is a surface, then Kq (F x [0, 1]) is an algebra, and Kq (M ) is a module over Kq ((∂M ) x [0, 1]). One motivation for the definition is that if L [SUBSET OF] S 3 is a knot, then the (colored) Jones polynomials Jn (L) ∈ C[q ±1 ] can be computed from Kq (S 3 \ L). It was shown in [14] that Kq (T 2 x [0, 1]) ~ AZ2 , the subalgebra of the quantum =q torus XY = q 2 Y X which is invariant under the involution X [RIGHTWARDS ARROW] X [-]1 , Y [RIGHTWARDS ARROW] Y [-]1 . Our starting point is the observation that the category of AZ2 -modules is equivalent q to the category of modules over a simpler algebra, the crossed product Aq Z2 . We write ML for the image of Kq (S 3 \ L) under this equivalence. Theorem 5.2.1 gives a simple formula showing Jn (L) can be computed from ML , and Corollary 5.3.3 shows a recursion relation for Jn (L) can be computed from ML (if ML is f.g. over C[X ±1 ]). In Chapter 6 we give an explicit description of ML when L is the trefoil. Conjecture 4.3.4 conjectures the general structure of ML for torus knots. The algebra Aq Z2 is the t = 1 subfamily of the double affine Hecke algebra Hq,t of type A1 . In Chapter 8 we give a new skein-theoretic realization of the + + spherical subalgebra Hq,t , and we also give a construction associating an Hq,t - module ML (t) to each knot L. In Chapter 9 we construct algebraic deformations of the skein module ML to a family of modules ML (t) over Hq,t . In the case when L is the trefoil, we use these deformations to give example calculations of 2-variable polynomials Jn (q, t) that specialize to the colored Jones polynomials when t = 1.&lt;/Abstract>
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