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Template:Short description In mathematics and abstract algebra, a Bol loop is an algebraic structure generalizing the notion of group. Bol loops are named for the Dutch mathematician Gerrit Bol who introduced them in Template:Harv.

A loop, L, is said to be a left Bol loop if it satisfies the identity

a(b(ac))=(a(ba))c, for every a,b,c in L,

while L is said to be a right Bol loop if it satisfies

((ca)b)a=c((ab)a), for every a,b,c in L.

These identities can be seen as weakened forms of associativity, or a strengthened form of (left or right) alternativity.

A loop is both left Bol and right Bol if and only if it is a Moufang loop. Alternatively, a right or left Bol loop is Moufang if and only if it satisfies the flexible identity a(ba) = (ab)a . Different authors use the term "Bol loop" to refer to either a left Bol or a right Bol loop.

Properties

The left (right) Bol identity directly implies the left (right) alternative property, as can be shown by setting b to the identity.

It also implies the left (right) inverse property, as can be seen by setting b to the left (right) inverse of a, and using loop division to cancel the superfluous factor of a. As a result, Bol loops have two-sided inverses.

Bol loops are also power-associative.

Bruck loops

A Bol loop where the aforementioned two-sided inverse satisfies the automorphic inverse property, (ab)−1 = a−1 b−1 for all a,b in L, is known as a (left or right) Bruck loop or K-loop (named for the American mathematician Richard Bruck). The example in the following section is a Bruck loop.

Bruck loops have applications in special relativity; see Ungar (2002). Left Bruck loops are equivalent to Ungar's (2002) gyrocommutative gyrogroups, even though the two structures are defined differently.

Example

Let L denote the set of n x n positive definite, Hermitian matrices over the complex numbers. It is generally not true that the matrix product AB of matrices A, B in L is Hermitian, let alone positive definite. However, there exists a unique P in L and a unique unitary matrix U such that AB = PU; this is the polar decomposition of AB. Define a binary operation * on L by A * B = P. Then (L, *) is a left Bruck loop. An explicit formula for * is given by A * B = (A B2 A)1/2, where the superscript 1/2 indicates the unique positive definite Hermitian square root.

Bol algebra

A (left) Bol algebra is a vector space equipped with a binary operation [a,b]+[b,a]=0 and a ternary operation {a,b,c} that satisfies the following identities:[1]

{a,b,c}+{b,a,c}=0

and

{a,b,c}+{b,c,a}+{c,a,b}=0

and

[{a,b,c},d][{a,b,d},c]+{c,d,[a,b]}{a,b,[c,d]}+[[a,b],[c,d]]=0

and

{a,b,{c,d,e}}{{a,b,c},d,e}{c,{a,b,d},e}{c,d,{a,b,e}}=0.

Note that {.,.,.} acts as a Lie triple system. If Template:Math is a left or right alternative algebra then it has an associated Bol algebra Template:Math, where [a,b]=abba is the commutator and {a,b,c}=b,c,a is the Jordan associator.

References

Template:Reflist

  1. Irvin R. Hentzel, Luiz A. Peresi, "Special identities for Bol algebras",  Linear Algebra and its Applications 436(7) · April 2012