- Hopf algebra
In
mathematics , a Hopf algebra, named afterHeinz Hopf , is a structure that is simultaneously a (unital associative) algebra, acoalgebra , and has anantiautomorphism , with these structures compatible.Hopf algebras occur naturally in
algebraic topology , where they originated and are related to theH-space concept, ingroup scheme theory, ingroup theory (via the concept of agroup ring ), and in numerous other places, making them probably the most familiar type ofbialgebra . Hopf algebras are also studied in their own right, with much work on specific classes of examples on the one hand and classification problems on the other.Formal definition
Formally, a Hopf algebra is a
bialgebra "H" over a field "K" together with a "K"-linear map (called the antipode) such that the following diagram commutes:Here Δ is the comultiplication of the bialgebra, ∇ its multiplication, η its unit and ε its counit. In the sumlessSweedler notation , this property can also be expressed as:As for algebras, one can replace the underlying field "K" with a
commutative ring "R" in the above definition.The definition of Hopf algebra is self-dual (as reflected in the symmetry of the above diagram), so if one can define a dual of "H" (which is always possible if "H" is finite-dimensional), then it is automatically a Hopf algebra.
Properties of the antipode
"S" is sometimes required to have a "K"-linear inverse, which is automatic in the finite-dimensional case, or if "H" is
commutative orcocommutative (or more generally quasitriangular).In general, "S" is an
antihomomorphism , so is ahomomorphism , which is therefore an automorphism if "S" was invertible (as may be required).If , then the Hopf algebra is said to be involutive (and the underlying algebra with involution is a
*-algebra ). If "H" is finite-dimensional, commutative, or cocommutative, then it is involutive.If a bialgebra "B" admits an antipode "S", then "S" is unique ("a bialgebra admits at most 1 Hopf algebra structure").
The antipode is an analog to the inversion map on a group that sends to . [ [http://www.mathematik.uni-muenchen.de/~pareigis/Vorlesungen/QuantGrp/ln2_1.pdf Quantum groups lecture notes] ]
Examples
Group algebra. Suppose "G" is a group. The
group algebra "KG" is aunital associative algebra over "K". It turns into a Hopf algebra if we define
* Δ : "KG" → "KG" dirprod "KG" by Δ("g") = "g" dirprod "g" for all "g" in "G"
* ε : "KG" → "K" by ε("g") = 1 for all "g" in "G"
* "S" : "KG" → "KG" by "S"("g") = "g" -1 for all "g" in "G".Functions on a finite group. Suppose now that "G" is a "finite" group. Then the set "K""G" of all functions from "G" to "K" with pointwise addition and multiplication is a unital associative algebra over "K", and "K""G" dirprod "K""G" is naturally isomorphic to "K""G"x"G" (for "G" infinite, "K""G" dirprod "K""G" is a proper subset of "K""G"x"G"). The set "K""G" becomes a Hopf algebra if we define
* Δ : "K""G" → "K""G"x"G" by Δ("f")("x","y") = "f"("xy") for all "f" in "K""G" and all "x","y" in "G"
* ε : "K""G" → "K" by ε("f") = "f"("e") for every "f" in "K""G" [here "e" is theidentity element of "G"]
* "S" : "K""G" → "K""G" by "S"("f")("x") = "f"("x"-1) for all "f" in "K""G" and all "x" in "G".Regular functions on an algebraic group. Generalizing the previous example, we can use the same formulas to show that for a given
algebraic group "G" over "K", the set of allregular function s on "G" forms a Hopf algebra.Universal enveloping algebra. Suppose "g" is a
Lie algebra over the field "K" and "U" is itsuniversal enveloping algebra . "U" becomes a Hopf algebra if we define
* Δ : "U" → "U" dirprod "U" by Δ("x") = "x" dirprod 1 + 1 dirprod "x" for every "x" in "g" (this rule is compatible withcommutator s and can therefore be uniquely extended to all of "U").
* ε : "U" → "K" by ε("x") = 0 for all "x" in "g" (again, extended to "U")
* "S" : "U" → "U" by "S"("x") = -"x" for all "x" in "g".Cohomology of Lie groups
The cohomology algebra of a Lie group is a Hopf algebra: the multiplication is provided by the cup-product, and the comultiplication :by the group multiplication .This observation was actually a source of the notion of Hopf algebra. Using this structure, Hopf proved a structure theorem for the cohomology algebra of Lie groups.
Theorem (Hopf) [ Hopf, 1941.] Let "A" be a finite-dimensional, graded commutative, gradedcocommutative Hopf algebra over a field of characteristic 0. Then "A" (as an algebra) is a free exterior algebra with generators of odd degree.
Quantum groups and non-commutative geometry
All examples above are either commutative (i.e. the multiplication is
commutative ) or co-commutative (i.e. Δ = "T" Δ where "T": "H" dirprod "H" → "H" dirprod "H" is defined by "T"("x" dirprod "y") = "y" dirprod "x"). Other interesting Hopf algebras are certain "deformations" or "quantizations" of those from example 3 which are neither commutative nor co-commutative. These Hopf algebras are often called "quantum groups ", a term that is so far only loosely defined. They are important innoncommutative geometry , the idea being the following: a standard algebraic group is well described by its standard Hopf algebra of regular functions; we can then think of the deformed version of this Hopf algebra as describing a certain "non-standard" or "quantized" algebraic group (which is not an algebraic group at all). While there does not seem to be a direct way to define or manipulate these non-standard objects, one can still work with their Hopf algebras, and indeed one "identifies" them with their Hopf algebras. Hence the name "quantum group".Related concepts
Graded Hopf algebras are often used inalgebraic topology : they are the natural algebraic structure on the direct sum of all homology orcohomology groups of anH-space .Locally compact quantum group s generalize Hopf algebras and carry a topology. The algebra of allcontinuous function s on aLie group is a locally compact quantum group.Quasi-Hopf algebra s are also generalizations of Hopf algebras, where coassociativity only holds up to a twist.Analogy with groups
Groups can be axiomatized by the same diagrams (equivalently, operations) as a Hopf algebra, where "G" is taken to be a set instead of a module. In this case:
* the field "K" is replaced by the 1-point set
* there is a natural counit (map to 1 point)
* there is a natural comultiplication (the diagonal map)
* the unit is the identity element of the group
* the multiplication is the multiplication in the group
* the antipode is the inverseIn this philosophy, a group can be thought of as a Hopf algebra over the "field with one element ". [ [http://sbseminar.wordpress.com/2007/10/07/group-hopf-algebra/ Group = Hopf algebra « Secret Blogging Seminar ] , [http://www.youtube.com/watch?v=p3kkm5dYH-w Group objects and Hopf algebras] , video of Simon Willerton.]See also
*
Quasitriangular Hopf algebra
*Algebra/set analogy
*Representation theory of Hopf algebras
*Ribbon Hopf algebra
*Superalgebra
* Supergroup
*Anyonic Lie algebra Notes
References
* Pierre Cartier, [http://inc.web.ihes.fr/prepub/PREPRINTS/2006/M/M-06-40.pdf "A primer of Hopf algebras"] , IHES preprint, September 2006, 81 pages
* Jurgen Fuchs, "Affine Lie Algebras and Quantum Groups", (1992), Cambridge University Press. ISBN 0-521-48412-X
* H. Hopf, Uber die Topologie der Gruppen-Mannigfaltigkeiten und ihrer Verallgemeinerungen, Ann. of Math. 42 (1941), 22-52. Reprinted in Selecta Heinz Hopf, pp. 119-151, Springer, Berlin (1964). MathSciNet | id = 4784
* Ross Moore, Sam Williams and Ross Talent: [http://www-texdev.ics.mq.edu.au/Quantum/Quantum.ps Quantum Groups: an entrée to modern algebra]
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