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Bol loop

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Algebraic structure

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 (Bol 1937).

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

a ( b ( a c ) ) = ( a ( b a ) ) c {\displaystyle 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

( ( c a ) b ) a = c ( ( a b ) a ) {\displaystyle ((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) = a b 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 B A), 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 {\displaystyle +=0} and a ternary operation { a , b , c } {\displaystyle \{a,b,c\}} that satisfies the following identities:

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

and

{ a , b , c } + { b , c , a } + { c , a , b } = 0 {\displaystyle \{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 {\displaystyle -+\{c,d,\}-\{a,b,\}+,]=0}

and

{ a , b , { c , d , e } } { { a , b , c } , d , e } { c , { a , b , d } , e } { c , d , { a , b , e } } = 0 {\displaystyle \{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 A is a left or right alternative algebra then it has an associated Bol algebra A, where [ a , b ] = a b b a {\displaystyle =ab-ba} is the commutator and { a , b , c } = b , c , a {\displaystyle \{a,b,c\}=\langle b,c,a\rangle } is the Jordan associator.

References

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