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Locally compact quantum group : ウィキペディア英語版
Locally compact quantum group

A locally compact quantum group is a relatively new C
*-algebra
ic approach toward quantum groups that generalizes the Kac-algebra, compact-quantum-group and Hopf-algebra approaches. Earlier attempts at a unifying definition of quantum groups using, for example, multiplicative unitaries have enjoyed some success but have also encountered several technical problems.
One of the main features distinguishing this new approach from its predecessors is the axiomatic existence of left and right invariant weights. This gives a noncommutative analogue of left and right Haar measures on a locally compact Hausdorff group.
== Definitions ==
Before we can even begin to properly define a locally compact quantum group, we first need to define a number of preliminary concepts and also state a few theorems.
Definition (weight). Let A be a C
*-algebra
, and let A_ denote the set of positive elements of A . A weight on A is a function \phi: A_ \to () such that
* \phi(a_ + a_) = \phi(a_) + \phi(a_) for all a_,a_ \in A_ , and
* \phi(r \cdot a) = r \cdot \phi(a) for all r \in a weight on A . We say that \phi is a K.M.S. weight ('K.M.S.' stands for 'Kubo-Martin-Schwinger') on A if and only if \phi is a ''proper weight'' on A and there exists a norm-continuous one-parameter group (\sigma_)_ = \phi for all t \in \mathbb , and
* for every a \in \text(\sigma_) , we have \phi(a^ a) = \phi(\sigma_(a) () B is a dense subset of B ), then we can uniquely extend \pi to a
*-homomorphism \overline: M(A) \to M(B) .
Theorem 3. If \omega: A \to \mathbb is a state (i.e., a positive linear functional of norm 1 ) on A , then we can uniquely extend \omega to a state \overline: M(A) \to \mathbb on M(A) .
Definition (Locally compact quantum group). A (C
*-algebraic) locally compact quantum group is an ordered pair \mathcal = (A,\Delta) , where A is a C
*-algebra and \Delta: A \to M(A \otimes A) is a ''non-degenerate''
*-homomorphism called the co-multiplication, that satisfies the following four conditions:
* The co-multiplication is co-associative, i.e., \overline \circ \Delta = \overline \circ \Delta .
* The sets \left\, ~ a \in A \right\} and \left\(\Delta(a)) ~ \big| ~ \omega \in A^, ~ a \in A \right\} are linearly dense subsets of A .
* There exists a faithful K.M.S. weight \phi on A that is left-invariant, i.e., \phi \! \left( \overline(1_) \cdot \phi(a) for all \omega \in A^ and a \in \mathcal_^ .
* There exists a K.M.S. weight \psi on A that is right-invariant, i.e., \psi \! \left( \overline(\Delta(a)) \right) = \overline(1_) \cdot \psi(a) for all \omega \in A^ and a \in \mathcal_^ .
From the definition of a locally compact quantum group, it can be shown that the right-invariant K.M.S. weight \psi is automatically faithful. Therefore, the faithfulness of \psi is a redundant condition and does not need to be postulated.

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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