R-matrix

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imported>Pythagoras0님의 2014년 2월 26일 (수) 10:24 판
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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 \(\bar R=p\circ R\) instead of the \(R\) matrix where \(p\) is the permutation map
  • this is what makes the module category into braided monoidal category


YBE

$$R_{12}(u)R_{13}(u+v)R_{23}(v)=R_{23}(v)R_{13}(u+v)R_{12}(u)$$

  • $R(u,\eta)$
    • $u$ is called the spectral parameter
    • $\eta$ quantum paramter (or semi-classical parameter)
  • ignoring $\eta$, we get the classical R-matrix $R(u)$ in $U(\mathfrak{g})$
  • ignoring $u$, we get $R(\eta)$ in $U_{q}(\mathfrak{g})$ where $q=e^{\eta}$


permuted R-matrix

  • For \(R\) matrix on \(V \otimes V\), define the permuted R-matrix \(\bar R=p\circ R\) where \(p\) is the permutation map.
  • define \(\bar R_i\) sitting in i and i+1 th slot by

\[\bar R_i=1\otimes \cdots \otimes\bar R \cdots \otimes 1\]

  • whenever \(|i-j| \geq 2 \), we have \(\bar R_i\bar R_j =\bar R_j\bar R_i\)
  • the YBE reduces to

\[\bar R_i\bar R_{i+1}\bar R_i= \bar R_{i+1}\bar R_i \bar R_{i+1} \label{braid}\]


derivation of \ref{braid} from the YBE

  • $\bar R_{2}(u)\bar R_1(u+v) \bar R_{2}(v)$ corresponding to $R_{12}(u)R_{13}(u+v)R_{23}(v)$ can be written as

$$ (1,2,3) \xrightarrow{R_{23}} (1,2',3') \xrightarrow{P_{23}} (1,3',2') \xrightarrow{R_{12}} (1',3'',2') \xrightarrow{P_{12}} (3'',1',2')\xrightarrow{R_{23}} (3'',1'',2'')\xrightarrow{P_{23}} (3'',2'',1'') $$

  • $\bar R_{1}(v)\bar R_2(u+v) \bar R_{1}(u)$ corresponding to $R_{23}(v)R_{13}(u+v)R_{12}(u)$ can be written as

$$ (1,2,3) \xrightarrow{R_{12}} (1',2',3) \xrightarrow{P_{12}} (2',1',3) \xrightarrow{R_{23}} (2,1'',3') \xrightarrow{P_{23}} (2,3',1'')\xrightarrow{R_{12}} (2'',3'',1'')\xrightarrow{P_{12}} (3'',2'',1'') $$

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

$$ \left( \begin{array}{cccc} u+1 & 0 & 0 & 0 \\ 0 & u & 1 & 0 \\ 0 & 1 & u & 0 \\ 0 & 0 & 0 & u+1 \end{array} \right) $$

  • trigonometric R-matrix

$$ \left( \begin{array}{cccc} \sin (u+\eta ) & 0 & 0 & 0 \\ 0 & \sin (u) & \sin (\eta ) & 0 \\ 0 & \sin (\eta ) & \sin (u) & 0 \\ 0 & 0 & 0 & \sin (u+\eta ) \end{array} \right) $$


explicit R-matrices

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.


related items


computational resource


encyclopedia


articles

  • R-matrix arising from affine Hecke algebras and its application to Macdonald's difference operators