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In mathematics a Yetter–Drinfeld category is a special type of
braided monoidal category In mathematics, a ''commutativity constraint'' \gamma on a monoidal category ''\mathcal'' is a choice of isomorphism \gamma_ : A\otimes B \rightarrow B\otimes A for each pair of objects ''A'' and ''B'' which form a "natural family." In partic ...
. It consists of
module Module, modular and modularity may refer to the concept of modularity. They may also refer to: Computing and engineering * Modular design, the engineering discipline of designing complex devices using separately designed sub-components * Mo ...
s over a
Hopf algebra Hopf is a German surname. Notable people with the surname include: * Eberhard Hopf (1902–1983), Austrian mathematician * Hans Hopf (1916–1993), German tenor * Heinz Hopf (1894–1971), German mathematician * Heinz Hopf (actor) (1934–2001), Sw ...
which satisfy some additional axioms.


Definition

Let ''H'' be a Hopf algebra over a
field Field may refer to: Expanses of open ground * Field (agriculture), an area of land used for agricultural purposes * Airfield, an aerodrome that lacks the infrastructure of an airport * Battlefield * Lawn, an area of mowed grass * Meadow, a grass ...
''k''. Let \Delta denote the
coproduct In category theory, the coproduct, or categorical sum, is a construction which includes as examples the disjoint union of sets and of topological spaces, the free product of groups, and the direct sum of modules and vector spaces. The cop ...
and ''S'' the
antipode Antipode or Antipodes may refer to: Mathematics * Antipodal point, the diametrically opposite point on a circle or ''n''-sphere, also known as an antipode * Antipode, the convolution inverse of the identity on a Hopf algebra Geography * Antipode ...
of ''H''. Let ''V'' be a
vector space In mathematics and physics, a vector space (also called a linear space) is a set whose elements, often called '' vectors'', may be added together and multiplied ("scaled") by numbers called '' scalars''. Scalars are often real numbers, but ...
over ''k''. Then ''V'' is called a (left left) Yetter–Drinfeld module over ''H'' if * (V,\boldsymbol) is a left ''H''-
module Module, modular and modularity may refer to the concept of modularity. They may also refer to: Computing and engineering * Modular design, the engineering discipline of designing complex devices using separately designed sub-components * Mo ...
, where \boldsymbol: H\otimes V\to V denotes the left action of ''H'' on ''V'', * (V,\delta\;) is a left ''H''-
comodule In mathematics, a comodule or corepresentation is a concept dual to a module. The definition of a comodule over a coalgebra is formed by dualizing the definition of a module over an associative algebra. Formal definition Let ''K'' be a field, ...
, where \delta : V\to H\otimes V denotes the left coaction of ''H'' on ''V'', * the maps \boldsymbol and \delta satisfy the compatibility condition :: \delta (h\boldsymbolv)=h_v_S(h_) \otimes h_\boldsymbolv_ for all h\in H,v\in V, :where, using Sweedler notation, (\Delta \otimes \mathrm)\Delta (h)=h_\otimes h_ \otimes h_ \in H\otimes H\otimes H denotes the twofold coproduct of h\in H , and \delta (v)=v_\otimes v_ .


Examples

* Any left ''H''-module over a cocommutative Hopf algebra ''H'' is a Yetter–Drinfeld module with the trivial left coaction \delta (v)=1\otimes v. * The trivial module V=k\ with h\boldsymbolv=\epsilon (h)v, \delta (v)=1\otimes v, is a Yetter–Drinfeld module for all Hopf algebras ''H''. * If ''H'' is the group algebra ''kG'' of an
abelian group In mathematics, an abelian group, also called a commutative group, is a group in which the result of applying the group operation to two group elements does not depend on the order in which they are written. That is, the group operation is com ...
''G'', then Yetter–Drinfeld modules over ''H'' are precisely the ''G''-graded ''G''-modules. This means that :: V=\bigoplus _V_g, :where each V_g is a ''G''-submodule of ''V''. * More generally, if the group ''G'' is not abelian, then Yetter–Drinfeld modules over ''H=kG'' are ''G''-modules with a ''G''-gradation :: V=\bigoplus _V_g, such that g.V_h\subset V_. * Over the base field k=\mathbb\; all finite-dimensional, irreducible/simple Yetter–Drinfeld modules over a (nonabelian) group ''H=kG'' are uniquely given through a
conjugacy class In mathematics, especially group theory, two elements a and b of a group are conjugate if there is an element g in the group such that b = gag^. This is an equivalence relation whose equivalence classes are called conjugacy classes. In other w ...
subset G\; together with \chi,X\; (character of) an irreducible group representation of the
centralizer In mathematics, especially group theory, the centralizer (also called commutant) of a subset ''S'' in a group ''G'' is the set of elements \mathrm_G(S) of ''G'' such that each member g \in \mathrm_G(S) commutes with each element of ''S'', ...
Cent(g)\; of some representing g\in /math>: *:V=\mathcal_^\chi=\mathcal_^\qquad V=\bigoplus_V_=\bigoplus_X ** As ''G''-module take \mathcal_^\chi to be the induced module of \chi,X\;: *::Ind_^G(\chi)=kG\otimes_X *:(this can be proven easily not to depend on the choice of ''g'') ** To define the ''G''-graduation (comodule) assign any element t\otimes v\in kG\otimes_X=V to the graduation layer: *::t\otimes v\in V_ ** It is very custom to directly construct V\; as direct sum of ''X''´s and write down the ''G''-action by choice of a specific set of representatives t_i\; for the Cent(g)\;-
coset In mathematics, specifically group theory, a subgroup of a group may be used to decompose the underlying set of into disjoint, equal-size subsets called cosets. There are ''left cosets'' and ''right cosets''. Cosets (both left and right) ...
s. From this approach, one often writes *::h\otimes v\subset times X \;\; \leftrightarrow \;\; t_i\otimes v\in kG\otimes_X \qquad\text\;\;h=t_igt_i^ *:(this notation emphasizes the graduationh\otimes v\in V_h, rather than the module structure)


Braiding

Let ''H'' be a Hopf algebra with invertible antipode ''S'', and let ''V'', ''W'' be Yetter–Drinfeld modules over ''H''. Then the map c_:V\otimes W\to W\otimes V, ::c(v\otimes w):=v_\boldsymbolw\otimes v_, :is invertible with inverse ::c_^(w\otimes v):=v_\otimes S^(v_)\boldsymbolw. :Further, for any three Yetter–Drinfeld modules ''U'', ''V'', ''W'' the map ''c'' satisfies the braid relation ::(c_\otimes \mathrm_U)(\mathrm_V\otimes c_)(c_\otimes \mathrm_W)=(\mathrm_W\otimes c_) (c_\otimes \mathrm_V) (\mathrm_U\otimes c_):U\otimes V\otimes W\to W\otimes V\otimes U. A
monoidal category In mathematics, a monoidal category (or tensor category) is a category \mathbf C equipped with a bifunctor :\otimes : \mathbf \times \mathbf \to \mathbf that is associative up to a natural isomorphism, and an object ''I'' that is both a left ...
\mathcal consisting of Yetter–Drinfeld modules over a Hopf algebra ''H'' with bijective antipode is called a Yetter–Drinfeld category. It is a braided monoidal category with the braiding ''c'' above. The category of Yetter–Drinfeld modules over a Hopf algebra ''H'' with bijective antipode is denoted by ^H_H\mathcal.


References

* {{DEFAULTSORT:Yetter-Drinfeld category Hopf algebras Quantum groups Monoidal categories