Divided power structure explained

In mathematics, specifically commutative algebra, a divided power structure is a way of introducing items with similar properties as expressions of the form

xn/n!

have, also when it is not possible to actually divide by

n!

.

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

\gamman:I\toA

for n = 0, 1, 2, ... such that:

\gamma0(x)=1

and

\gamma1(x)=x

for

x\inI

, while

\gamman(x)\inI

for n > 0.

\gamman(x+y)=

n
\sum
i=0

\gamman-i(x)\gammai(y)

for

x,y\inI

.

\gamman(λx)=λn\gamman(x)

for

λ\inA,x\inI

.

\gammam(x)\gamman(x)=((m,n))\gammam+n(x)

for

x\inI

, where

((m,n))=

(m+n)!
m!n!
is an integer.

\gamman(\gammam(x))=Cn,\gammamn(x)

for

x\inI

and

m>0

, where

Cn,=

(mn)!
(m!)nn!
is an integer.

For convenience of notation,

\gamman(x)

is often written as

x[n]

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.

Homomorphisms of divided power algebras are ring homomorphisms that respects the divided power structure on its source and target.

Examples

\Z

on one generator:

\Z\langle{x}\rangle:=\Z\left[x,\tfrac{x2}{2},\ldots,\tfrac{xn}{n!},\ldots\right]\subset\Q[x].

\Q,

then every ideal I has a unique divided power structure where

\gamman(x)=\tfrac{1}{n!}xn.

[1] Indeed, this is the example which motivates the definition in the first place.

S\bulletM

denote the symmetric algebra of M over A. Then its dual

(S\bulletM)\vee=

\bullet
Hom
A(S

M,A)

has a canonical structure of divided power ring. In fact, it is canonically isomorphic to a natural completion of

\GammaA(\check{M})

(see below) if M has finite rank.

Constructions

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

A\langlex1,x2,\ldots,xn\rangle

consisting of divided power polynomials in the variables

x1,x2,\ldots,xn,

that is sums of divided power monomials of the form

c

[i1]
x
1
[i2]
x
2

[in]
x
n

with

c\inA

. 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

\GammaA(M),

with PD ideal

\Gamma+(M)

and an A-linear map

M\to\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.

The divided power functor is used in the construction of co-Schur functors.

See also

References

Notes and References

  1. The uniqueness follows from the easily verified fact that in general,

    xn=n!\gamman(x)

    .