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Quasitriangular Hopf algebra : ウィキペディア英語版
Quasitriangular Hopf algebra

In mathematics, a Hopf algebra, ''H'', is quasitriangular〔Montgomery & Schneider (2002), (p. 72 ).〕 if there exists an invertible element, ''R'', of H \otimes H such that
:
*R \ \Delta(x)R^ = (T \circ \Delta)(x) \ R for all x \in H, where \Delta is the coproduct on ''H'', and the linear map T : H \otimes H \to H \otimes H is given by T(x \otimes y) = y \otimes x,
:
*(\Delta \otimes 1)(R) = R_ \ R_,
:
*(1 \otimes \Delta)(R) = R_ \ R_,
where R_ = \phi_(R), R_ = \phi_(R), and R_ = \phi_(R), where \phi_ : H \otimes H \to H \otimes H \otimes H, \phi_ : H \otimes H \to H \otimes H \otimes H, and \phi_ : H \otimes H \to H \otimes H \otimes H, are algebra morphisms determined by
:\phi_(a \otimes b) = a \otimes b \otimes 1,
:\phi_(a \otimes b) = a \otimes 1 \otimes b,
:\phi_(a \otimes b) = 1 \otimes a \otimes b.
''R'' is called the R-matrix.
As a consequence of the properties of quasitriangularity, the R-matrix, ''R'', is a solution of the Yang-Baxter equation (and so a module ''V'' of ''H'' can be used to determine quasi-invariants of braids, knots and links). Also as a consequence of the properties of quasitriangularity, (\epsilon \otimes 1) R = (1 \otimes \epsilon) R = 1 \in H; moreover
R^ = (S \otimes 1)(R), R = (1 \otimes S)(R^), and (S \otimes S)(R) = R. One may further show that the
antipode ''S'' must be a linear isomorphism, and thus ''S2'' is an automorphism. In fact, ''S2'' is given by conjugating by an invertible element: S^2(x)= u x u^ where u := m (S \otimes 1)R^ (cf. Ribbon Hopf algebras).
It is possible to construct a quasitriangular Hopf algebra from a Hopf algebra and its dual, using the Drinfeld quantum double construction.
==Twisting==
The property of being a quasi-triangular Hopf algebra is preserved by twisting via an invertible element F = \sum_i f^i \otimes f_i \in \mathcal such that (\varepsilon \otimes id )F = (id \otimes \varepsilon)F = 1 and satisfying the cocycle condition
: (F \otimes 1) \circ (\Delta \otimes id) F = (1 \otimes F) \circ (id \otimes \Delta) F
Furthermore, u = \sum_i f^i S(f_i) is invertible and the twisted antipode is given by S'(a) = u S(a)u^, with the twisted comultiplication, R-matrix and co-unit change according to those defined for the quasi-triangular quasi-Hopf algebra. Such a twist is known as an admissible (or Drinfeld) twist.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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