R-matrix
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introduction
- R-matrix has entries from Boltzman weights.
- From quantum group point of view, R-matrix naturally appears as intertwiners of tensor product of two evaluation modules
- from this intertwining property we need to consider <math>\bar R=p\circ R</math> instead of the <math>R</math> matrix where <math>p</math> is the permutation map
- this is what makes the module category into braided monoidal category
YBE
- R-matrix is a solution of the Yang-Baxter equation (YBE)
- <math>R_{12}(u)R_{13}(u+v)R_{23}(v)=R_{23}(v)R_{13}(u+v)R_{12}(u)</math>
- <math>R(u,\eta)</math>
- <math>u</math> is called the spectral parameter
- <math>\eta</math> quantum paramter (or semi-classical parameter)
- ignoring <math>\eta</math>, we get the classical R-matrix <math>R(u)</math> in <math>U(\mathfrak{g})</math>
- ignoring <math>u</math>, we get <math>R(\eta)</math> in <math>U_{q}(\mathfrak{g})</math> where <math>q=e^{\eta}</math>
- found by Drinfeld and Jimbo
- see Drinfeld-Jimbo quantum groups (quantized UEA)
permuted R-matrix
- For <math>R</math> matrix on <math>V \otimes V</math>, define the permuted R-matrix <math>\bar R=p\circ R</math> where <math>p</math> is the permutation map.
- define <math>\bar R_i</math> sitting in i and i+1 th slot by
- <math>\bar R_i=1\otimes \cdots \otimes\bar R\otimes \cdots \otimes 1</math>
- whenever <math>|i-j| \geq 2 </math>, we have <math>\bar R_i\bar R_j =\bar R_j\bar R_i</math>
- the YBE reduces to
- <math>\bar R_i\bar R_{i+1}\bar R_i= \bar R_{i+1}\bar R_i \bar R_{i+1} \label{braid}</math>
- these are the Braid group relations.
derivation of \ref{braid} from the YBE
- <math>\bar R_{2}(u)\bar R_1(u+v) \bar R_{2}(v)</math> corresponding to <math>R_{12}(u)R_{13}(u+v)R_{23}(v)</math> can be written as
- <math>
(1,2,3) \xrightarrow{R_{23}} (1,2',3') \xrightarrow{P_{23}} (1,3',2') \xrightarrow{R_{12}} (1',3,2') \xrightarrow{P_{12}} (3,1',2')\xrightarrow{R_{23}} (3,1,2)\xrightarrow{P_{23}} (3,2,1) </math>
- <math>\bar R_{1}(v)\bar R_2(u+v) \bar R_{1}(u)</math> corresponding to <math>R_{23}(v)R_{13}(u+v)R_{12}(u)</math> can be written as
- <math>
(1,2,3) \xrightarrow{R_{12}} (1',2',3) \xrightarrow{P_{12}} (2',1',3) \xrightarrow{R_{23}} (2,1,3') \xrightarrow{P_{23}} (2,3',1)\xrightarrow{R_{12}} (2,3,1)\xrightarrow{P_{12}} (3,2,1) </math>
R-matrix and Braid groups
- with an R-matrix satisfying the YBE, we obtain a representation of the Braid group, which then gives a link invariant in Knot theory
examples of R-matrix
- rational R-matrix
- <math>
\left( \begin{array}{cccc} u+1 & 0 & 0 & 0 \\ 0 & u & 1 & 0 \\ 0 & 1 & u & 0 \\ 0 & 0 & 0 & u+1 \end{array} \right) </math>
- trigonometric R-matrix
- <math>
\left( \begin{array}{cccc} \sin (u+\eta ) & 0 & 0 & 0 \\ 0 & \sin (u) & \sin (\eta ) & 0 \\ 0 & \sin (\eta ) & \sin (u) & 0 \\ 0 & 0 & 0 & \sin (u+\eta ) \end{array} \right) </math>
explicit R-matrices
- taken from http://mathoverflow.net/questions/5103/solutions-of-the-quantum-yang-baxter-equation
- The general theory (due to Jimbo) is that each irreducible finite dimensional representation of the quantised enveloping algebra of a Kac-Moody algebra (not of finite type) gives a trigonometric R-matrix.
- There is substantial information on these representations but the R-matrices are not explicit.
tensor product graph method
- There is a special case which is explicit and is given by the "tensor product graph" method (this was worked out by Niall MacKay and Gustav Delius).
- I used this in my paper: R-matrices and the magic square. J. Phys. A, 36(7):1947–1959, 2003. and you can find the references there.
- If you want to go beyond this special case and be explicit then you can use "cabling" a.k.a "fusion".
beyond the tensor product graph method
- The only papers which deal with R-matrices not covered by the tensor product graph method that I know of are
- Vyjayanthi Chari and Andrew Pressley. Fundamental representations of Yangians and singularities of R-matrices. J. Reine Angew. Math., 417:87–128, 1991.
- G'abor Tak'acs. The R-matrix of the Uq(d(3)4 ) algebra and g(1)2 affine Toda field theory. Nuclear Phys. B, 501(3):711–727, 1997.
- Bruce W. Westbury. An R-matrix for D(3) 4 . J. Phys. A, 38(2):L31–L34, 2005
- Deepak Parashar, Bruce W. Westbury R-matrices for the adjoint representations of Uq(so(n)) arXiv:0906.3419
- The Chari & Pressley paper deals with rational R-matrices.
- The last preprint was an incomplete attempt to try and find the trigonometric analogues of these R-matrices.
computational resource
encyclopedia
articles
- Lentner, Simon, and Daniel Nett. “New <math>R</math>-Matrices for Small Quantum Groups.” arXiv:1409.5824 [math], September 19, 2014. http://arxiv.org/abs/1409.5824.
- R-matrix arising from affine Hecke algebras and its application to Macdonald's difference operators
메타데이터
위키데이터
- ID : Q2993305
메타데이터
위키데이터
- ID : Q2993305
Spacy 패턴 목록
- [{'LOWER': 'baum'}, {'OP': '*'}, {'LOWER': 'connes'}, {'LEMMA': 'conjecture'}]