octonion
Let ℍ be the quaternions over the reals ℝ. Apply the
Cayley-Dickson construction to ℍ once, and we obtain an algebra
,
variously called Cayley algebra, the octonion algebra, or simply the octonions, over ℝ. Specifically the construction is carried out as follows:
-
1.
Form the vector space 𝕆=ℍ⊕ℍ𝐤; any element of 𝕆 can be written as a+b𝐤, where a,b∈ℍ;
-
2.
Define a binary operation
on 𝕆 called the multiplication in O by
(a+b𝐤)(c+d𝐤):=(ac-ˉdb)+(da+bˉc)𝐤, where a,b,c,d∈ℍ, and ˉc is the quaternionic conjugation
of c∈ℍ. When b=d=0, the multiplication is reduced the multiplication in ℍ. In addition, the multiplication rule above imply the following:
a(d𝐤)=(da)𝐤 (1) (b𝐤)c=(bˉc)𝐤 (2) (b𝐤)(d𝐤)=-ˉdb. (3) In particular, in the last equation, if b=d=1, 𝐤2=-1.
-
3.
Define a unary operation on 𝕆 called the octonionic conjugation in O by
¯a+b𝐤:=ˉa-b𝐤, where a,b∈ℍ. Clearly, the octonionic conjugation is an involution
(http://planetmath.org/Involution2) (ˉˉx=x).
-
4.
Finally, define a unary operation N on 𝕆 called the norm in O by N(x):=xˉx, where x∈𝕆. Write x=a+b𝐤, then
N(x)=(a+b𝐤)(ˉa-b𝐤)=(aˉa+ˉbb)+(-ba+bˉˉa)𝐤=aˉa+bˉb≥0. It is not hard to see that N(x)=0 iff x=0.
The above four (actually, only the first two suffice) steps makes
𝕆 into an 8-dimensional algebra over ℝ such that ℍ is
embedded as a subalgebra.
With the last two steps, one can define the inverse of a non-zero
element x∈𝕆 by
x-1:=ˉxN(x) |
so that
xx-1=x-1x=1. Since x is arbitrary, 𝕆 has no zero
divisors. Upon checking that x-1(xy)=y=(yx)x-1, the non-associative algebra 𝕆 is turned into a division algebra
.
Since N(x)≥0 for any x∈𝕆, we can define a non-negative
real-valued function ∥⋅∥ on 𝕆 by ∥x∥=√N(x). This is clearly well-defined and ∥x∥=0 iff
x=0. In addition, it is not hard to see that, for any r∈ℝ
and x∈𝕆, ∥rx∥=|r|∥x∥, and that ∥⋅∥
satisfies the triangular inequality. This makes 𝕆 into a normed
division algebra.
Since the multiplication in ℍ is noncommutative, 𝕆 is
noncommutative. In fact, if we write ℍ=ℂ⊕ℂ𝐣,
where ℂ are the complex numbers and 𝐣2=-1, then
B={1,𝐢,𝐣,𝐢𝐣} is a basis
for the vector space ℍ over ℝ. With the introduction
of 𝐤∈𝕆, we quickly check that 𝐤
anti-commute with the non-real basis elements in B:
𝐢𝐤=-𝐤𝐢,𝐣𝐤=-𝐤𝐣,(𝐢𝐣)𝐤=-𝐤(𝐢𝐣). |
Furthermore, one checks that 𝐢(𝐣𝐤)=(𝐣𝐢)𝐤=-(𝐢𝐣)𝐤, so that
𝕆 is not associative.
Since 𝕆=ℍ⊕ℍ𝐤, the set {1,𝐢,𝐣,𝐢𝐣,𝐤,𝐢𝐤,𝐣𝐤,(𝐢𝐣)𝐤}(=B∪B𝐤) is a
basis for 𝕆 over ℝ. A less messy way to represent these basis
elements is done the following assignment:
Title | octonion |
---|---|
Canonical name | Octonion |
Date of creation | 2013-03-22 15:21:42 |
Last modified on | 2013-03-22 15:21:42 |
Owner | CWoo (3771) |
Last modified by | CWoo (3771) |
Numerical id | 15 |
Author | CWoo (3771) |
Entry type | Definition |
Classification | msc 17A75 |
Classification | msc 17D05 |
Synonym | Cayley algebra |
Related topic | TheoremsOnSumsOfSquares |
Related topic | DivisionAlgebra |
Defines | octonion algebra |
\@unrecurse |