Baer correspondence: Difference between revisions

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==Definition==
==Definition==


===The two sides of the correspondence===
===The setup of the correspondence===


The '''Baer correspondence''' is a special case of the [[Lazard correspondence]], and is a correspondence as follows:
The '''Baer correspondence''' is a special case of the [[Lazard correspondence]], and is a correspondence as follows:
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The Baer correspondence preserves underlying sets, i.e., a group and Lie ring that are in Baer correspondence have the same underlying set.
The Baer correspondence preserves underlying sets, i.e., a group and Lie ring that are in Baer correspondence have the same underlying set.


The ''Lie ring'' of any given Baer Lie group (i.e., 2-powered class two group) can be viewed as the same set with Lie ring operations defined using a fixed formula in terms of group operations, and the ''Lie group'' of any given Baer Lie ring (i.e., 2-powered class two Lie ring) is defined using a fixed formula in terms of the Lie ring operations. The procedures for going from a group to a Lie ring and a Lie ring to a group are inverses of each other.
The mapping in the direction from groups to Lie rings will be denoted <math>\log</math> and the mapping in the direction from Lie rings to groups will be denoted <math>\exp</math>. Explicitly:
 
* For any Baer Lie group <math>G</math>, we define its Baer Lie ring <math>\log(G)</math> as having the same underlying set and with the Lie ring operations defined using fixed formulas of the group operations.
* For any Baer Lie ring <math>L</math>, we define its Baer Lie group <math>\exp(L)</math> as having the same underlying set and with the group operations defined using fixed formulas of the group operations.
 
It will further be true that:
 
* <math>\exp(\log(G)) = G</math> for any Baer Lie group <math>G</math>.
* <math>\log(\exp(L)) = L</math> for any Baer Lie ring <math>L</math>.


===The finite p-group case===
===The finite p-group case===

Revision as of 02:41, 15 November 2013

This article states and (possibly) proves a fact that is true for odd-order p-groups: groups of prime power order where the underlying prime is odd. The statement is false, in general, for groups whose order is a power of two.
View other such facts for p-groups|View other such facts for finite groups

Definition

The setup of the correspondence

The Baer correspondence is a special case of the Lazard correspondence, and is a correspondence as follows:

Baer Lie groups Baer Lie rings

Here:

The Baer correspondence preserves underlying sets, i.e., a group and Lie ring that are in Baer correspondence have the same underlying set.

The mapping in the direction from groups to Lie rings will be denoted log and the mapping in the direction from Lie rings to groups will be denoted exp. Explicitly:

  • For any Baer Lie group G, we define its Baer Lie ring log(G) as having the same underlying set and with the Lie ring operations defined using fixed formulas of the group operations.
  • For any Baer Lie ring L, we define its Baer Lie group exp(L) as having the same underlying set and with the group operations defined using fixed formulas of the group operations.

It will further be true that:

  • exp(log(G))=G for any Baer Lie group G.
  • log(exp(L))=L for any Baer Lie ring L.

The finite p-group case

For any fixed odd prime number p, any p-group is uniquely 2-divisible, and so is any p-Lie ring, so the Baer correspondence restricts to a correspondence:

Class two p-groups Class two p-Lie rings

From group to Lie ring

For proof that this construction works, refer: Proof of Baer construction of Lie ring for Baer Lie group

Suppose G is a Baer Lie group, i.e., a 2-powered group of nilpotency class (at most) two. Let [,] denote the commutator of two elements. Note that we can adopt either the left or the right convention -- the two definitions are equal because the group has class two. Denote by the function that takes an element and returns the unique element whose square is that element. If g has finite order m, then g=g(m+1)/2. We give the underlying set of G the structure of a Lie ring, denoted logG, as follows:

Lie ring operation that we need to define Definition in terms of the group operations Further comments
Addition, i.e., define x+y for x,yG x+y:=xy[x,y]=xyx=xy2x Since G has class two, [x,y] is central. Since center is local powering-invariant, applied to the prime 2, we get that [x,y] is central. Thus, it makes sense to divide by this element without specifying whether the division occurs on the left or on the right.
The other two definitions are equivalent, but this requires some algebraic manipulation to show. These definitions are significant because they show that the additive group operation is the same as the twisted multiplication defined for generic 2-powered groups.
Identity element for addition, denoted 0. Same as identity element for group multiplication, denoted e or 1. This automatically follows from the way addition is defined.
Additive inverse, i.e., define x for xG. Same as x1, i.e., the multiplicative inverse in the group. This automatically follows from the way addition is defined.
Lie bracket, i.e., the [,] map in the Lie ring. Same as the group commutator [x,y]=xyx1y1.

The claim is that with these operations, G acquires the structure of a 2-powered class two Lie ring, i.e., a Baer Lie ring.

From Lie ring to group

For proof that this construction works, refer: Proof of Baer construction of Lie group for Baer Lie ring

Suppose L is a Baer Lie ring, i.e., a uniquely 2-divisible class two Lie ring, with addition denoted + and Lie bracket denoted [,]. We give the underlying set of L the structure of a class two group, denoted exp(L), as follows:

Group operation that we need to define Definition in terms of the Lie ring operations Further comments
Group multiplication xy:=x+y+12[x,y] Since center is local powering-invariant in Lie ring, we obtain that the element 12[x,y] is central.
Identity element for multiplication Same as the zero element 0 of the Lie ring.
Multiplicative inverse x1. Same as the additive inverse x.
Group commutator [x,y]=xyx1y1 Same as the Lie bracket [x,y].

The claim is that with these operations, L acquires the structure of a 2-powered class two group.

Mutually inverse nature

Further information: Proof of mutual inverse nature of the Baer constructions between group and Lie ring

The two operations described above are two-sided inverses of each other. Explicitly:

  1. If we start with a Baer Lie group, construct its Baer Lie ring, and then construct the Baer Lie group of that, we return to the original Baer Lie group.
  2. If we start with a Baer Lie ring, construct its Baer Lie group, and then construct the Baer Lie ring of that, we return to the original Baer Lie ring.

Conceptual interpretation

Analogy with center and radius, or mean and mean deviation

Suppose a,bR. The arithmetic mean of a and b is c=(a+b)/2 and the mean deviation is r=|ba|/2. Explicitly, a and b are the endpoints of the interval with center c=(a+b)/2 and radius r=|ba|/2. The diameter is |ba|.

We can do something similar with geometric means. For a,b positive reals, the geometric mean is ab and the geometric deviation is a/b or b/a (depending on how you measure it).

We can understand the construction of the Lie ring similarly. The idea is that we have a group with a (possibly) noncommutative multiplication. We want to separate out the "commutative" part of the multiplication (which we store as the addition of the Lie ring) from the "noncommutative" part of the multiplication (which we store as the Lie bracket of the Lie ring). Explicitly, noting that xy and yx commute on account of the class being two, we get the following:

  • The commutative part of the multiplication can be thought of as obtained by "averaging" out both products. Explicitly, x+y is the geometric mean of xy and yx, i.e., it is the unique central value z such that xyz=zyx. If we work out the formula for this, we obtain that it is xy[x,y]. Note that we can alternatively describe it as x+y=xy2x=yx2y.
  • The noncommutative part of the multiplication can be thought of as the quotient of xy and yx, which is given as the group commutator [x,y]

Twisted product

The Lie ring addition can also be defined as follows:

x+y:=x1/2yx1/2

This is a special case of the twisted multiplication of a 2-powered group.

Examples

In the case of an abelian group, the corresponding Lie ring is an abelian Lie ring and the additive group of the Lie ring coincides with the original abelian group. In other words, abelian groups correspond to abelian Lie rings.

Groups of prime-cube order

The behavior is the same for all odd primes p for groups of order p3.

Group GAP ID (second part) Lie ring Additive group of Lie ring Description of Baer correspondence
unitriangular matrix group:UT(3,p) 3 niltriangular matrix Lie ring:NT(3,p) elementary abelian group of prime-cube order Baer correspondence between UT(3,p) and NT(3,p)
semidirect product of cyclic group of prime-square order and cyclic group of prime order 4 (insert name) direct product of cyclic group of prime-square order and cyclic group of prime order (insert link)

Groups of prime-fourth order

We first consider groups of order 34=81.

Group GAP ID (second part) Lie ring Additive group of Lie ring Description of Baer correspondence
SmallGroup(81,3) 3 (insert link) direct product of Z9 and E9 (insert link)
semidirect product of Z9 and Z9 4 (insert link) direct product of Z9 and Z9 (insert link)
semidirect product of Z27 and Z3 6 (insert link) direct product of Z27 and Z3 (insert link)
direct product of prime-cube order group:U(3,3) and Z3 12 (insert link) elementary abelian group:E81 (insert link)
direct product of semidirect product of Z9 and Z3 and Z3 13 (insert link) direct product of Z9 and E9 (insert link)
central product of prime-cube order group:U(3,3) and Z9 14 (insert link) direct product of Z9 and E9 (insert link)

Generalizations

There are three kinds of generalizations:

References