Группа авторов

Algebra and Applications 2


Скачать книгу

a k-vector space A together with a bilinear map m : AAA which is associative. The associativity is expressed by the commutativity of the following diagram:

      The algebra A is unital if there is a unit 1 in it. This is expressed by the commutativity of the following diagram:

      where u is the map from k to A defined by u(λ) = λ1. The algebra A is commutative if

, where
: AAAA is the flip, defined by
.

      With any vector space V, we can associate its tensor algebra T(V). As a vector space, it is defined by:

      with V⊗0 = k and V⊗ k+1 := VV⊗k. The product is given by the concatenation:

      The embedding of k = V⊗0 into T(V) gives the unit map u. The tensor algebra T(V) is also called the free (unital) algebra generated by V. This algebra is characterized by the following universal property: for any linear map φ from V to a unital algebra A, there is a unique unital algebra morphism

from T(V) to A extending φ.

      Let A and B be the unital k-algebras. We put a unital algebra structure on AB in the following way:

      The unit element 1A⊗B is given by 1A1B, and the associativity is clear. This multiplication is thus given by:

      where

: ABABAABB is defined by the flip of the two middle factors:

      1.2.2. Coalgebras

      Coalgebras are the objects which are somehow dual to algebras: axioms for coalgebras are derived from axioms for algebras by reversing the arrows of the corresponding diagrams:

      A k-coalgebra is by definition a k-vector space C together with a bilinear map Δ : CCC, which is coassociative. The coassociativity is expressed by the commutativity of the following diagram:

      A subspace JC is called a subcoalgebra (respectively a left coideal, right coideal and two-sided coideal) of C if Δ(J) is contained in JJ (respectively CJ, JC, JC + CJ) is included in J. The duality alluded to above can be made more precise:

      PROPOSITION 1.1.–

      1 1) The linear dual C* of a counital coalgebra C is a unital algebra, with product (respectively unit map) the transpose of the coproduct (respectively of the counit).

      2 2) Let J be a linear subspace of C. Denote by J⊥ the orthogonal of J in C*.Then:– J is a two-sided coideal if and only if J⊥ is a subalgebra of C*.– J is a left coideal if and only if J⊥ is a left ideal of C*.– J is a right coideal if and only if J⊥ is a right ideal of C*.– J is a subcoalgebra if and only if J⊥ is a two-sided ideal of C*.

      PROOF.– For any subspace K of C*, we will denote by K the subspace of those elements of C on which any element of K vanishes. It coincides with the intersection of the orthogonal of K with C, via the canonical embedding CC**. Therefore, for any linear subspaces JC and KC* we have:

      Suppose that J is a two-sided coideal. Take any ξ, η in J. For any xJ, we have:

      which proves the first assertion. We leave the reader to prove the three other assertions along the same lines. □

      Dually, we have the following:

      PROPOSITION 1.2.– Let K be a linear subspace of C*. Then:

       – K⊥ is a two-sided coideal if and only if K is a subalgebra of C*.

       – K⊥ is a left coideal if and only if K is a left ideal of C*.

       – K⊥ is a right coideal if and only if K is a right ideal of C*.

       – K⊥ is a subcoalgebra if and only if K is a two-sided ideal of C*.

      PROOF.– The linear dual (CC)* naturally contains the tensor product C*C*. Take as a multiplication the restriction of tΔ to C*C*:

      and put u = : kC*. It is easily seen, by just reverting the arrows of the corresponding diagrams, that the coassociativity of Δ implies the associativity of m, and that the counit property for ε implies that u is a unit. □

      Note that the duality property is not perfect: