"Algebraic structure → Group theory "Group theory 


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"Modular groups


"Infinite dimensional Lie group


In "mathematics and "theoretical physics, the term quantum group denotes various kinds of "noncommutative algebras with additional structure. In general, a quantum group is some kind of "Hopf algebra. There is no single, allencompassing definition, but instead a family of broadly similar objects.^{["clarification needed]}
The term "quantum group" first appeared in the theory of "quantum integrable systems, which was then formalized by "Vladimir Drinfeld and "Michio Jimbo as a particular class of "Hopf algebra. The same term is also used for other Hopf algebras that deform or are close to classical "Lie groups or "Lie algebras, such as a `bicrossproduct' class of quantum groups introduced by "Shahn Majid a little after the work of Drinfeld and Jimbo.
In Drinfeld's approach, quantum groups arise as "Hopf algebras depending on an auxiliary parameter q or h, which become "universal enveloping algebras of a certain Lie algebra, frequently "semisimple or "affine, when q = 1 or h = 0. Closely related are certain dual objects, also Hopf algebras and also called quantum groups, deforming the algebra of functions on the corresponding semisimple "algebraic group or a "compact Lie group.
Just as groups often appear as symmetries, quantum groups act on many other mathematical objects.^{["clarification needed]}. It has become fashionable^{["citation needed]} to introduce the adjective quantum in cases where quantum groups act on objects. For example, there are quantum planes and quantum Grassmannians.^{["further explanation needed]}
The discovery of quantum groups was quite unexpected, since it was known for a long time that compact groups and semisimple Lie algebras are "rigid" objects, in other words, they cannot be "deformed". One of the ideas behind quantum groups is that if we consider a structure that is in a sense equivalent but larger, namely a "group algebra or a "universal enveloping algebra, then a group or enveloping algebra can be "deformed", although the deformation will no longer remain a group or enveloping algebra. More precisely, deformation can be accomplished within the category of "Hopf algebras that are not required to be either "commutative or "cocommutative. One can think of the deformed object as an algebra of functions on a "noncommutative space", in the spirit of the "noncommutative geometry of "Alain Connes. This intuition, however, came after particular classes of quantum groups had already proved their usefulness in the study of the quantum "YangBaxter equation and "quantum inverse scattering method developed by the Leningrad School ("Ludwig Faddeev, "Leon Takhtajan, "Evgeny Sklyanin, "Nicolai Reshetikhin and "Vladimir Korepin) and related work by the Japanese School.^{[1]} The intuition behind the second, bicrossproduct, class of quantum groups was different and came from the search for selfdual objects as an approach to "quantum gravity.^{[2]}
One type of objects commonly called a "quantum group" appeared in the work of Vladimir Drinfeld and Michio Jimbo as a deformation of the "universal enveloping algebra of a "semisimple Lie algebra or, more generally, a "Kac–Moody algebra, in the category of "Hopf algebras. The resulting algebra has additional structure, making it into a "quasitriangular Hopf algebra.
Let A = (a_{ij}) be the "Cartan matrix of the Kac–Moody algebra, and let q ≠ 0, 1 be a complex number, then the quantum group, U_{q}(G), where G is the Lie algebra whose Cartan matrix is A, is defined as the "unital "associative algebra with generators k_{λ} (where λ is an element of the "weight lattice, i.e. 2(λ, α_{i})/(α_{i}, α_{i}) is an integer for all i), and e_{i} and f_{i} (for "simple roots, α_{i}), subject to the following relations:
And for i ≠ j we have the qSerre relations, which are deformations of the "Serre relations:
where the "qfactorial, the "qanalog of the ordinary "factorial, is defined recursively using "qnumber:
In the limit as q → 1, these relations approach the relations for the universal enveloping algebra U(G), where
and t_{λ} is the element of the Cartan subalgebra satisfying (t_{λ}, h) = λ(h) for all h in the Cartan subalgebra.
There are various "coassociative coproducts under which these algebras are Hopf algebras, for example,
where the set of generators has been extended, if required, to include k_{λ} for λ which is expressible as the sum of an element of the weight lattice and half an element of the "root lattice.
In addition, any Hopf algebra leads to another with reversed coproduct T o Δ, where T is given by T(x ⊗ y) = y ⊗ x, giving three more possible versions.
The "counit on U_{q}(A) is the same for all these coproducts: ε(k_{λ}) = 1, ε(e_{i}) = ε(f_{i}) = 0, and the respective "antipodes for the above coproducts are given by
Alternatively, the quantum group U_{q}(G) can be regarded as an algebra over the field C(q), the field of all "rational functions of an indeterminate q over C.
Similarly, the quantum group U_{q}(G) can be regarded as an algebra over the field Q(q), the field of all "rational functions of an indeterminate q over Q (see below in the section on quantum groups at q = 0). The center of quantum group can be described by quantum determinant.
Just as there are many different types of representations for Kac–Moody algebras and their universal enveloping algebras, so there are many different types of representation for quantum groups.
As is the case for all Hopf algebras, U_{q}(G) has an "adjoint representation on itself as a module, with the action being given by
where
One important type of representation is a weight representation, and the corresponding "module is called a weight module. A weight module is a module with a basis of weight vectors. A weight vector is a nonzero vector v such that k_{λ} · v = d_{λ}v for all λ, where d_{λ} are complex numbers for all weights λ such that
A weight module is called integrable if the actions of e_{i} and f_{i} are locally nilpotent (i.e. for any vector v in the module, there exists a positive integer k, possibly dependent on v, such that for all i). In the case of integrable modules, the complex numbers d_{λ} associated with a weight vector satisfy ^{["citation needed]}, where ν is an element of the weight lattice, and c_{λ} are complex numbers such that
Of special interest are "highest weight representations, and the corresponding highest weight modules. A highest weight module is a module generated by a weight vector v, subject to k_{λ} · v = d_{λ}v for all weights μ, and e_{i} · v = 0 for all i. Similarly, a quantum group can have a lowest weight representation and lowest weight module, i.e. a module generated by a weight vector v, subject to k_{λ} · v = d_{λ}v for all weights λ, and f_{i} · v = 0 for all i.
Define a vector v to have weight ν if for all λ in the weight lattice.
If G is a Kac–Moody algebra, then in any irreducible highest weight representation of U_{q}(G), with highest weight ν, the multiplicities of the weights are equal to their multiplicities in an irreducible representation of U(G) with equal highest weight. If the highest weight is dominant and integral (a weight μ is dominant and integral if μ satisfies the condition that is a nonnegative integer for all i), then the weight spectrum of the irreducible representation is invariant under the "Weyl group for G, and the representation is integrable.
Conversely, if a highest weight module is integrable, then its highest weight vector v satisfies , where c_{λ} · v = d_{λ}v are complex numbers such that
and ν is dominant and integral.
As is the case for all Hopf algebras, the "tensor product of two modules is another module. For an element x of U_{q}(G), and for vectors v and w in the respective modules, x ⋅ (v ⊗ w) = Δ(x) ⋅ (v ⊗ w), so that , and in the case of coproduct Δ_{1}, and
The integrable highest weight module described above is a tensor product of a onedimensional module (on which k_{λ} = c_{λ} for all λ, and e_{i} = f_{i} = 0 for all i) and a highest weight module generated by a nonzero vector v_{0}, subject to for all weights λ, and for all i.
In the specific case where G is a finitedimensional Lie algebra (as a special case of a Kac–Moody algebra), then the irreducible representations with dominant integral highest weights are also finitedimensional.
In the case of a tensor product of highest weight modules, its decomposition into submodules is the same as for the tensor product of the corresponding modules of the Kac–Moody algebra (the highest weights are the same, as are their multiplicities).
Strictly, the quantum group U_{q}(G) is not quasitriangular, but it can be thought of as being "nearly quasitriangular" in that there exists an infinite formal sum which plays the role of an Rmatrix. This infinite formal sum is expressible in terms of generators e_{i} and f_{i}, and Cartan generators t_{λ}, where k_{λ} is formally identified with q^{tλ}. The infinite formal sum is the product of two factors,^{["citation needed]}
and an infinite formal sum, where λ_{j} is a basis for the dual space to the Cartan subalgebra, and μ_{j} is the dual basis, and η = ±1.
The formal infinite sum which plays the part of the Rmatrix has a welldefined action on the tensor product of two irreducible highest weight modules, and also on the tensor product of two lowest weight modules. Specifically, if v has weight α and w has weight β, then
and the fact that the modules are both highest weight modules or both lowest weight modules reduces the action of the other factor on v ⊗ W to a finite sum.
Specifically, if V is a highest weight module, then the formal infinite sum, R, has a welldefined, and "invertible, action on V ⊗ V, and this value of R (as an element of End(V ⊗ V)) satisfies the "YangBaxter equation, and therefore allows us to determine a representation of the "braid group, and to define quasiinvariants for "knots, "links and "braids.
"Masaki Kashiwara has researched the limiting behaviour of quantum groups as q → 0, and found a particularly well behaved base called a "crystal base.
There has been considerable progress in describing finite quotients of quantum groups such as the above U_{q}(g) for q^{n} = 1; one usually considers the class of pointed "Hopf algebras, meaning that all subcoideals are 1dimensional and thus there sum form a group called coradical:
See also "compact quantum group.
"S. L. Woronowicz introduced compact matrix quantum groups. Compact matrix quantum groups are abstract structures on which the "continuous functions" on the structure are given by elements of a "C*algebra. The geometry of a compact matrix quantum group is a special case of a "noncommutative geometry.
The continuous complexvalued functions on a compact Hausdorff topological space form a commutative C*algebra. By the "Gelfand theorem, a commutative C*algebra is isomorphic to the C*algebra of continuous complexvalued functions on a compact Hausdorff topological space, and the topological space is uniquely determined by the C*algebra up to "homeomorphism.
For a compact "topological group, G, there exists a C*algebra homomorphism Δ: C(G) → C(G) ⊗ C(G) (where C(G) ⊗ C(G) is the C*algebra tensor product  the completion of the algebraic tensor product of C(G) and C(G)), such that Δ(f)(x, y) = f(xy) for all f ∈ C(G), and for all x, y ∈ G (where (f ⊗ g)(x, y) = f(x)g(y) for all f, g ∈ C(G) and all x, y ∈ G). There also exists a linear multiplicative mapping κ: C(G) → C(G), such that κ(f)(x) = f(x^{−1}) for all f ∈ C(G) and all x ∈ G. Strictly, this does not make C(G) a Hopf algebra, unless G is finite. On the other hand, a finitedimensional "representation of G can be used to generate a *subalgebra of C(G) which is also a Hopf *algebra. Specifically, if is an ndimensional representation of G, then for all i, j u_{ij} ∈ C(G) and
It follows that the *algebra generated by u_{ij} for all i, j and κ(u_{ij}) for all i, j is a Hopf *algebra: the counit is determined by ε(u_{ij}) = δ_{ij} for all i, j (where δ_{ij} is the "Kronecker delta), the antipode is κ, and the unit is given by
As a generalization, a compact matrix quantum group is defined as a pair (C, fu), where C is a C*algebra and is a matrix with entries in C such that
where I is the identity element of C. Since κ is antimultiplicative, then κ(vw) = κ(w) κ(v) for all v, w in C_{0}.
As a consequence of continuity, the comultiplication on C is coassociative.
In general, C is not a bialgebra, and C_{0} is a Hopf *algebra.
Informally, C can be regarded as the *algebra of continuous complexvalued functions over the compact matrix quantum group, and u can be regarded as a finitedimensional representation of the compact matrix quantum group.
A representation of the compact matrix quantum group is given by a "corepresentation of the Hopf *algebra (a corepresentation of a counital coassociative coalgebra A is a square matrix with entries in A (so v belongs to M(n, A)) such that
for all i, j and ε(v_{ij}) = δ_{ij} for all i, j). Furthermore, a representation v, is called unitary if the matrix for v is unitary (or equivalently, if κ(v_{ij}) = v*_{ij} for all i, j).
An example of a compact matrix quantum group is SU_{μ}(2), where the parameter μ is a positive real number. So SU_{μ}(2) = (C(SU_{μ}(2)), u), where C(SU_{μ}(2)) is the C*algebra generated by α and γ, subject to
and
so that the comultiplication is determined by ∆(α) = α ⊗ α − γ ⊗ γ*, ∆(γ) = α ⊗ γ + γ ⊗ α*, and the coinverse is determined by κ(α) = α*, κ(γ) = −μ^{−1}γ, κ(γ*) = −μγ*, κ(α*) = α. Note that u is a representation, but not a unitary representation. u is equivalent to the unitary representation
Equivalently, SU_{μ}(2) = (C(SU_{μ}(2)), w), where C(SU_{μ}(2)) is the C*algebra generated by α and β, subject to
and
so that the comultiplication is determined by ∆(α) = α ⊗ α − μβ ⊗ β*, Δ(β) = α ⊗ β + β ⊗ α*, and the coinverse is determined by κ(α) = α*, κ(β) = −μ^{−1}β, κ(β*) = −μβ*, κ(α*) = α. Note that w is a unitary representation. The realizations can be identified by equating .
When μ = 1, then SU_{μ}(2) is equal to the algebra C(SU(2)) of functions on the concrete compact group SU(2).
Whereas compact matrix pseudogroups are typically versions of DrinfeldJimbo quantum groups in a dual function algebra formulation, with additional structure, the bicrossproduct ones are a distinct second family of quantum groups of increasing importance as deformations of solvable rather than semisimple Lie groups. They are associated to Lie splittings of Lie algebras or local factorisations of Lie groups and can be viewed as the cross product or Mackey quantisation of one of the factors acting on the other for the algebra and a similar story for the coproduct Δ with the second factor acting back on the first. The very simplest nontrivial example corresponds to two copies of R locally acting on each other and results in a quantum group (given here in an algebraic form) with generators p, K, K^{−1}, say, and coproduct
where h is the deformation parameter. This quantum group was linked to a toy model of Planck scale physics implementing "Born reciprocity when viewed as a deformation of the "Heisenberg algebra of quantum mechanics. Also, starting with any compact real form of a semisimple Lie algebra g its complexification as a real Lie algebra of twice the dimension splits into g and a certain solvable Lie algebra (the Iwasawa decomposition), and this provides a canonical bicrossproduct quantum group associated to g. For su(2) one obtains a quantum group deformation of the "Euclidean group E(3) of motions in 3 dimensions.