Moufang loop
From Free net encyclopedia
In mathematics, a Moufang loop is a special kind of algebraic structure. It is similar to a group in many ways but may fail to be associative. Moufang loops were introduced by Ruth Moufang.
Contents |
Definition
A Moufang loop is a loop Q that satisfies any one of the following identities (the binary operation in Q is denoted by juxtaposition):
- z(x(zy)) = ((zx)z)y
- x(z(yz)) = ((xz)y)z
- (zx)(yz) = (z(xy))z
for all x, y, z in Q. These identities—known as Moufang identities—are, in fact, equivalent in any loop. Therefore if Q satisfies one of them it satisfies all of them.
Examples
- Any group is associative loop and therefore a Moufang loop.
- The nonzero octonions form a nonassociative Moufang loop under octonion multiplication.
- The subset of unit norm octonions (forming a 7-sphere in O) is closed under multiplication and therefore forms a Moufang loop.
- The basis octonions and their additive inverses form a finite Moufang loop of order 16.
- The set of invertible split-octonions form a nonassociative Moufang loop, as do the set of unit norm split-octonions. More generally, the set of invertible elements in any octonion algebra over a field F form a Moufang loop, as do the subset of unit norm elements.
- For any field F let M(F) denote the Moufang loop of unit norm elements in the (unique) split-octonion algebra over F. Let Z denote the center of M(F). If the characteristic of F is 2 then Z = {e}, otherwise Z = {±e}. The Paige loop over F is the loop M*(F) = M(F)/Z. Paige loops are nonassociative simple Moufang loops. All finite nonassociative simple Moufang loops are Paige loops over finite fields. The smallest Paige loop M*(2) has order 120.
- A large class of nonassociative Moufang loops can be constructed as follows. Let G be an arbitrary group. Define a new element u not in G and let M(G,2) = G ∪ (G u). The product in M(G,2) is given by the usual product of elements in G together with
- <math>(gu)h = (gh^{-1})u</math>
- <math>g(hu) = (hg)u</math>
- <math>(gu)(hu) = h^{-1}g</math>
- It follows that <math>u^2 = 1</math> and <math>ug = g^{-1}u</math>. With the above product M(G,2) is a Moufang loop. It is associative iff G is abelian.
- The smallest nonassociative Moufang loop is M(S3,2) which has order 12.
Properties
Associativity
Moufang loops differ from groups in that they need not be associative. A Moufang loop that is associative is a group. The Moufang identities may be viewed as weaker forms of associativity.
By setting various elements to the identity, the Moufang identities imply
- x(xy) = (xx)y left alternative identity
- (xy)y = x(yy) right alternative identity
- x(yx) = (xy)x flexible identity
Moufang's theorem states that when three elements x, y, and z in a Moufang loop obey the associative law: (xy)z = x(yz) then they generate an associative subloop; that is, a group. A corollary of this is that all Moufang loops are di-associative (i.e. the subloop generated by any two elements of a Moufang loop is associative and therefore a group). In particular, Moufang loops are power associative, so that exponents xn are well-defined. When working with Moufang loops, it is common to drop the parenthesis in expressions with only two distinct elements. For example, the Moufang identities may be written unambigously as
- z(x(zy)) = (zxz)y
- ((xz)y)z = x(zyz)
- (zx)(yz) = z(xy)z
Left and right multiplication
The Moufang identites can be written in terms of the left and right multiplication operaters on Q. The first two identities state that
- <math>L_xL_yL_x = L_{xyx}</math>
- <math>R_xR_yR_x = R_{xyx}</math>
while the third identity says
- <math>L_z(x)R_z(y) = B_z(xy)</math>
for all <math>x,y,z</math> in <math>Q</math>. Here <math>B_z = L_zR_z = R_zL_z</math> is bimultiplication by <math>z</math>. The third Moufang identity is therefore equivalent to the statement that the triple <math>(L_z, R_z, B_z)</math> is an autotopy of <math>Q</math> for all <math>z</math> in <math>Q</math>.
Inverse properties
All Moufang loops have the inverse property, which means that each element x has a two-sided inverse x−1 which satisfies the identities:
- <math>x^{-1}(xy) = y = (yx)x^{-1}</math>
for all x and y. It follows that <math>(xy)^{-1} = y^{-1}x^{-1}</math> and <math>x(yz) = e</math> if and only if <math>(xy)z = e</math>.
Moufang loops are universal among inverse property loops; that is, a loop Q is a Moufang loop iff every loop isotope of Q has the inverse property. If follows that every loop isotope of a Moufang loop is a Moufang loop.
Moufang quasigroups
Any quasigroup which satisfies one of the Moufang identities must, in fact, have an identity element and therefore be a Moufang loop. We give a proof here for the third identity:
- Let a be any element of Q, and let e be the unique element such that ae = a. Then for any x in Q, (xa)x = (x(ae))x = (xa)(ex). Cancelling gives x = ex so that e is a left identity element. Now let f be the element such that fe = e. Then (yf)e = (e(yf))e = (ey)(fe) = (ey)e = ye. Cancelling gives yf = y, so f is a right identity element. Lastly, e = ef = f, so e is a two-sided identity element.
The proofs for first two identities are somewhat more difficult.
See also
References
- Jonathan D. H. Smith and Anna B. Romanowska (1999) Post-Modern Algebra, Wiley-Interscience. ISBN 0-471-12738-8.
- Template:Planetmath reference