Octonion

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In mathematics, the octonions are a nonassociative extension of the quaternions. Their 8-dimensional normed division algebra over the real numbers is the widest possible that can be obtained from the Cayley-Dickson construction. The octonion algebra is often denoted O, or in blackboard bold by .

Possibly because they don't offer an associative multiplication, the octonions receive at times less attention than the quaternions. Despite this lack of popularity, they are related to a number of exceptional structures in mathematics, among them the exceptional Lie groups. Additionally, octonions have applications in fields such as string theory, special relativity, and quantum logic.

Contents 1 History 2 Definition 2.1 Cayley-Dickson construction 2.2 Fano plane mnemonic 2.3 Conjugate, norm, and inverse 3 Properties 3.1 Automorphisms 4 Applications in physics 5 Quotes 6 See also 7 References

[edit] History

The octonions were discovered in 1843 by John T. Graves, a friend of William Hamilton, who called them octaves. They were discovered independently by Arthur Cayley, who published the first paper on them in 1845. They are sometimes referred to as Cayley numbers or the Cayley algebra.

[edit] Definition

The octonions can be thought of as octets (or 8-tuples) of real numbers. Every octonion is a real linear combination of the unit octonions {1, i, j, k, l, il, jl, kl}. That is, every octonion x can be written in the form

with real coefficients x_a.

Addition of octonions is accomplished by adding corresponding coefficients, as with the complex numbers and quaternions. By linearity, multiplication of octonions is completely determined by the multiplication table for the unit octonions given below.

1	i	j	k	l	il	jl	kl
i	−1	k	−j	il	−l	−kl	jl
j	−k	−1	i	jl	kl	−l	−il
k	j	−i	−1	kl	−jl	il	−l
l	−il	−jl	−kl	−1	i	j	k
il	l	−kl	jl	−i	−1	−k	j
jl	kl	l	−il	−j	k	−1	−i
kl	−jl	il	l	−k	−j	i	−1

The basis for the octonions given here is not nearly as universal as the standard basis for the quaternions; however, nearly all other choices differ from this one only in order and sign.

[edit] Cayley-Dickson construction

A more systematic way of defining the octonions is via the Cayley-Dickson construction. Just as quaternions can be defined as pairs of complex numbers, the octonions can be defined as pairs of quaternions. Addition is defined pairwise. The product of two pairs of quaternions (a, b) and (c, d) is defined by

(a,b)(c,d) = (ac − d ^* b,da + bc ^* )

where z ^* denotes the conjugate of the quaternion z. This definition is equivalent to the one given above when the eight unit octonions are identified with the pairs

(1,0), (i,0), (j,0), (k,0), (0,1), (0,i), (0,j), (0,k)

[edit] Fano plane mnemonic

A convenient mnemonic for remembering the products of unit octonions is given by the following diagram at the right. This diagram with seven points and seven lines (the circle through i, j, and k is considered a line) is called the Fano plane. The lines are oriented in this diagram. The seven points correspond to the seven standard basis elements of Im(O). Each pair of distinct points lies on a unique line and each line runs through exactly three points.

Let (a, b, c) be an ordered triple of points lying on a given line with the order specified by the direction of the arrow. Then multiplication is given by

ab = c and ba = −c

together with cyclic permutations. These rules together with

• 1 is the multiplicative identity,
• e² = − 1 for each point in the diagram

completely defines the multiplicative structure of the octonions. Each of the seven lines generates a subalgebra of O isomorphic to the quaternions H.

[edit] Conjugate, norm, and inverse

The conjugate of an octonion

is given by

Conjugation is an involution of O and satisfies (xy) ^* = y ^* x ^* (note the change in order).

The real part of x is defined as ½(x + x^*) = x₀ and the imaginary part as ½(x - x^*). The set of all purely imaginary octonions span a 7 dimension subspace of O, denoted Im(O).

The norm of the octonion x is defined as

The square root is well-defined here as x ^* x = xx ^* is always a nonnegative real number:

This norm agrees with the standard Euclidean norm on R⁸.

The existence of a norm on O implies the existence of inverses for every nonzero element of O. The inverse of x ≠ 0 is given by

It satisfies xx ^{− 1} = x ^{− 1}x = 1.

[edit] Properties

Octonionic multiplication is neither commutative:

nor associative:

The octonions do satisfy a weaker form of associativity: they are alternative. This means that the subalgebra generated by any two elements is associative. Actually, one can show that the subalgebra generated by any two elements of O is isomorphic to R, C, or H, all of which are associative.

The octonions do retain one important property shared by R, C, and H: the norm on O satisfies

This implies that the octonions form a nonassociative normed division algebra. The higher-dimensional algebras defined by the Cayley-Dickson construction (e.g. the sedenions) all fail to satisfy this property. They all have zero divisors.

Wider number systems exist which have a multiplicative modulus (e.g. 16 dimensional conic sedenions from the Musean hypernumbers program). Their modulus is defined differently from their norm, and they also contain zero divisors.

It turns out that the only normed division algebras over the reals are R, C, H, and O. These four algebras also form the only alternative, finite-dimensional division algebras over the reals (up to isomorphism).

Not being associative, the nonzero elements of O do not form a group. They do, however, form a loop, indeed a Moufang loop.

[edit] Automorphisms

An automorphism, A, of the octonions is an invertible linear transformation of O which satisfies

The set of all automorphisms of O forms a group called G₂. The group G₂ is a simply connected, compact, real Lie group of dimension 14. This group is the smallest of the exceptional Lie groups.

See also: PSL(2,7) - the automorphism group of the Fano plane.

[edit] Applications in physics

Octonions are used for a nonassociative generalization of quantum mechanics. For example, the Heisenberg equation of motion is modified using a nonassociative commutator (see references below).

[edit] Quotes

The real numbers are the dependable breadwinner of the family, the complete ordered field we all rely on. The complex numbers are a slightly flashier but still respectable younger brother: not ordered, but algebraically complete. The quaternions, being noncommutative, are the eccentric cousin who is shunned at important family gatherings. But the octonions are the crazy old uncle nobody lets out of the attic: they are nonassociative. — John Baez

[edit] See also

[edit] References

• John Baez, The Octonions, Bull. Amer. Math. Soc. 39 (2002), 145-205. Online HTML version at http://math.ucr.edu/home/baez/octonions/.
• Conway, John Horton, and Smith, Derek A., (2003) On Quaternions and Octonions: Their Geometry, Arithmetic, and Symmetry, A. K. Peters, Ltd. ISBN 1-56881-134-9. (Review).

For physics on octonion arithmetic see e.g.

• V. Dzhunushaliev, Toy Models of a Nonassociative Quantum Mechanics, Advances in High Energy Physics, vol. 2007, Article ID 12387, 10 pages, 2007. doi:10.1155/2007/12387; arXiv:0706.2398 [quant-ph].

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