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Depth of noncommutative subrings
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Depth of noncommutative subrings : ウィキペディア英語版
Depth of noncommutative subrings
In ring theory and Frobenius algebra extensions, fields of mathematics, there is a notion of depth two subring or depth of a Frobenius extension. The notion of depth two is important in a certain noncommutative Galois theory, which generates Hopf algebroids in place of the more classical Galois groups, whereas the notion of depth greater than two measures the defect, or distance, from being depth two in a tower of iterated endomorphism rings above the subring. A more recent definition of depth of any unital subring in any associative ring is proposed (see below) in a paper studying the depth of a subgroup of a finite group as group algebras over a commutative ring.
== Definition and first examples ==

A unital subring B \subseteq A has (or is) right depth two if there is a split epimorphism of natural A-B-bimodules from A^n \rightarrow A \otimes_B A for some positive integer n; by switching to natural B-A-bimodules, there is a corresponding definition of left depth two. Here we use the usual notation A^n = A \times \ldots \times A (n times) as well as the common notion, p is a split epimorphism if there is a homomorphism q in the reverse direction such that pq = identity on the image of p. (Sometimes the subring B in A is referred to as the ring extension A over B; the theory works as well for a ring homomorphism B into A, which induces right and left B-modules structures on A.) Equivalently, the condition for left or right depth two may be given in terms of a split monomorphism of bimodules where the domains and codomains above are reversed.
For example, let A be the group algebra of a finite group G (over any commutative base ring k; see the articles on group theory and group ring for the elementary definitions). Let B be the group (sub)algebra of a normal subgroup H of index n in G with coset representatives g_1,\cdots,g_n. Define a split A-B epimorphism p: A^n \rightarrow A \otimes_B A by p((a_1,\cdots,a_n)) = \sum_^n a_i g_i^ \otimes_B g_i . It is split by the mapping q: A \otimes_B A \rightarrow A^n defined by q(a \otimes_B a') = (a \gamma_1(a'),\cdots,a\gamma_n(a')) where \gamma_i(g) = \delta_ g for g in the coset g_jH (and extended linearly to a mapping A into B, a B-B-module homomorphism since H is normal in G): the splitting condition pq = the identity on A \otimes_B A is satisfied. Thus B is right depth two in A.
As another example (perhaps more elementary than the first; see ring theory or module theory for some of the elementary notions), let A be an algebra over a commutative ring B, where B is taken to be in the center of A. Assume A is a finite projective B-module, so there are B-linear mapping f_i: A \rightarrow B and elements x_i \in A (i = 1,...,n) called a projective base for the B-module A if it satisfies \sum_^n x_i f_i(a) = a for all a in A. It follows that B is left depth two in A by defining
p(a_1,\cdots,a_n) = \sum_^n x_i \otimes_B a_i with splitting map q(a \otimes_B a') = (f_1(a)a',\cdots,f_n(a)a') as the reader may verify. A similar argument naturally shows that B is right depth two in A.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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