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Divided Power Structure





DEFINITION


Let ''A'' be a Commutative Ring with an Ideal ''I''. A ''divided power structure'' (or PD-structure, after the French ''puissances divisées'') on ''I'' is a collection of maps \gamma_n : I o A for ''n''=0, 1, 2, ... such that:

#\gamma_0(x) = 1 and \gamma_1(x) = x for x \in I, while \gamma_n(x) \in I for ''n'' > 0.
#\gamma_n(x + y) = \sum_{i=0}^n \gamma_{n-i}(x) \gamma_i(y) for x, y \in I.
#\gamma_n(\lambda x) = \lambda^n \gamma_n(x) for \lambda \in A, x \in I.
#\gamma_m(x) \gamma_n(x) = ((m, n)) \gamma_{m+n}(x) for x \in I, where ((m, n)) = rac{(m+n)!}{m! n!} is an integer.
#\gamma_n(\gamma_m(x)) = C_{n, m} \gamma_{mn}(x) for x \in I, where C_{n, m} = rac{(mn)!}{(m!)^n n!} is an integer.

For convenience of notation, \gamma_n(x) is often written as x^{ {Link without Title} } when it is clear what divided power structure is meant.

The term ''divided power ideal'' refers to an ideal with a given divided power structure, and ''divided power ring'' refers to a ring with a given ideal with divided power structure.


EXAMPLES


  • If ''A'' is an algebra over the rational numbers Q, then every ideal ''I'' has a unique divided power structure where \gamma_n(x) = rac{1}{n!} \cdot x^n. (The uniqueness follows from the easily verified fact that in general, x^n = n! \gamma_n(x).) Indeed, this is the example which motivates the definition in the first place.


  • If ''A'' is a ring of Characteristic p > 0, where ''p'' is prime, and ''I'' is an ideal such that I^p = 0, then we can define a divided power structure on ''I'' where \gamma_n(x) = rac{1}{n!} x^n if ''n'' < ''p'', and \gamma_n(x) = 0 if n \geq p. (Note the distinction between I^p and the ideal generated by x^p for x \in I; the latter is always zero if a divided power structure exists, while the former is not necessarily zero.)


  • If ''M'' is an ''A''-module, let S^\cdot M denote the Symmetric Algebra of ''M'' over ''A''. Then its dual (S^\cdot M) \check{~} = Hom_A(S^\cdot M, A) has a canonical structure of divided power ring. In fact, it is canonically isomorphic to a natural Completion of \Gamma_A(\check{M}) (see below) if ''M'' has finite rank.




CONSTRUCTIONS


If ''A'' is any ring, there exists a divided power ring

:A \langle x_1, x_2, \ldots, x_n angle

consisting of ''divided power polynomials'' in the variables

:x_1, x_2, \ldots, x_n,

that is sums of ''divided power monomials'' of the form

:c x_1^{ x_2^{[i_2 } \cdots x_n^{[i_n]}

with c \in A. Here the divided power ideal is the set of divided power polynomials with constant coefficient 0.

More generally, if ''M'' is an ''A''-module, there is a Universal ''A''-algebra, called

:\Gamma_A(M),

with PD ideal

:\Gamma_+(M)

and an ''A''-linear map

:M o \Gamma_+(M).

(The case of divided power polynomials is the special case in which ''M'' is a Free Module over ''A'' of finite rank.)

If ''I'' is any ideal of a ring ''A'', there is a Universal Construction which extends ''A'' with divided powers of elements of ''I'' to get a ''divided power envelope'' of ''I'' in ''A''.


APPLICATIONS


The divided power envelope is a fundamental tool in the theory of PD Differential Operators and Crystalline Cohomology , where it is used to overcome technical difficulties which arise in positive Characteristic .


REFERENCES


  • Pierre Berthelot and Arthur Ogus, ''Notes on Crystalline Cohomology.'' Annals of Mathematics Studies. Princeton University Press, 1978.