The concept of supergroup is a generalization of that of group. In other words, every supergroup carries a natural group structure, but there may be more than one way to structure a given group as a supergroup. A supergroup is like a Lie group in that there is a well defined notion of smooth function defined on them.
However the functions may have even and odd parts. Moreover, a supergroup has a super Lie algebra which plays a role similar to that of a Lie algebra for Lie groups in that they determine most of the representation theory and which is the starting point for classification.
More formally, a Lie supergroup is a supermanifold G together with a multiplication morphism , an inversion morphism and a unit morphism which makes G a group object in the of supermanifolds. This means that, formulated as commutative diagrams, the usual associativity and inversion axioms of a group continue to hold. Since every manifold is a supermanifold, a Lie supergroup generalises the notion of a Lie group.
There are many possible supergroups. The ones of most interest in theoretical physics are the ones which extend the Poincaré group or the conformal group. Of particular interest are the orthosymplectic groups Osp(M|N) and the superunitary groups SU(M|N).
An equivalent algebraic approach starts from the observation that a supermanifold is determined by its ring of supercommutative smooth functions, and that a morphism of supermanifolds corresponds one to one with an algebra homomorphism between their functions in the opposite direction, i.e. that the category of supermanifolds is opposite to the category of algebras of smooth graded commutative functions. Reversing all the arrows in the commutative diagrams that define a Lie supergroup then shows that functions over the supergroup have the structure of a Z2-graded Hopf algebra. Likewise the representations of this Hopf algebra turn out to be Z2-graded comodules. This Hopf algebra gives the global properties of the supergroup.
There is another related Hopf algebra which is the dual of the previous Hopf algebra.
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Une superalgèbre de Lie est une extension de la notion d'algèbre de Lie par l'ajout d'une Z-graduation. Cette graduation sépare la superalgèbre en la somme directe d'une partie paire et d'une partie impaire. Cette structure est utilisée en physique théorique pour décrire la supersymétrie. Les éléments de l'algèbre peuvent y être représentés par des opérateurs différentiels. Dans la plupart de ces théories, les éléments pairs correspondent aux bosons et les éléments impairs aux fermions.
Superspace is the coordinate space of a theory exhibiting supersymmetry. In such a formulation, along with ordinary space dimensions x, y, z, ..., there are also "anticommuting" dimensions whose coordinates are labeled in Grassmann numbers rather than real numbers. The ordinary space dimensions correspond to bosonic degrees of freedom, the anticommuting dimensions to fermionic degrees of freedom. The word "superspace" was first used by John Wheeler in an unrelated sense to describe the configuration space of general relativity; for example, this usage may be seen in his 1973 textbook Gravitation.
En mathématiques, on peut construire l'algèbre enveloppante d'une algèbre de Lie . Il s'agit d'une algèbre associative unitaire qui permet de rendre compte de la plupart des propriétés de . Algèbre de Lie Soit K un corps commutatif de caractéristique différente de 2. Une algèbre de Lie sur K est un espace vectoriel muni d'une application bilinéaire de dans qui vérifie les propriétés suivantes : Tout espace vectoriel peut être muni d'une structure d'algèbre de Lie, en posant .
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