In mathematics, the split-octonions are an 8-dimensional nonassociative algebra over the real numbers. Unlike the standard octonions, they contain non-zero elements which are non-invertible. Also the signatures of their quadratic forms differ: the split-octonions have a split-signature (4,4) whereas the octonions have a positive-definite signature (8,0).
The octonions and the split-octonions can be obtained from the Cayley–Dickson construction by defining a multiplication on pairs of quaternions. We introduce a new imaginary unit ℓ and write a pair of quaternions (a, b) in the form a + ℓb. The product is defined by the rule:
If λ is chosen to be −1, we get the octonions. If, instead, it is taken to be +1 we get the split-octonions. One can also obtain the split-octonions via a Cayley–Dickson doubling of the split-quaternions. Here either choice of λ (±1) gives the split-octonions.
with real coefficients xa. By linearity, multiplication of split-octonions is completely determined by the following multiplication table:
A convenient mnemonic is given by the diagram at the right which represents the multiplication table for the split-octonions. This one is derived from its parent octonion (one of 480 possible), which is defined by:
where is a completely antisymmetric tensor with value +1 when ijk = 123, 154, 176, 264, 257, 374, 365, and:
with e0 the scalar element, and i, j, k = 1 ... 7.
The red arrows indicate possible direction reversals imposed by negating the lower right quadrant of the parent creating a split octonion with this multiplication table.
Conjugate, norm and inverse
The conjugate of a split-octonion x is given by
just as for the octonions. The quadratic form (or square norm) on x is given by
This norm is the standard pseudo-Euclidean norm on R4,4. Due to the split signature the norm N is isotropic, meaning there are nonzero x for which N(x) = 0. An element x has an (two-sided) inverse x−1 if and only if N(x) ≠ 0. In this case the inverse is given by
The split-octonions, like the octonions, are noncommutative and nonassociative. Also like the octonions, they form a composition algebra since the quadratic form N is multiplicative. That is,
The split-octonions satisfy the Moufang identities and so form an alternative algebra. Therefore, by Artin's theorem, the subalgebra generated by any two elements is associative. The set of all invertible elements (i.e. those elements for which N(x) ≠ 0) form a Moufang loop.
Zorn's vector-matrix algebra
Since the split-octonions are nonassociative they cannot be represented by ordinary matrices (matrix multiplication is always associative). Zorn found a way to represent them as "matrices" containing both scalars and vectors using a modified version of matrix multiplication. Specifically, define a vector-matrix to be a 2×2 matrix of the form
where a and b are real numbers and v and w are vectors in R3. Define multiplication of these matrices by the rule
where · and × are the ordinary dot product and cross product of 3-vectors. With addition and scalar multiplication defined as usual the set of all such matrices forms a nonassociative unital 8-dimensional algebra over the reals, called Zorn's vector-matrix algebra.
Define the "determinant" of a vector-matrix by the rule
This determinant is a quadratic form on the Zorn's algebra which satisfies the composition rule:
Zorn's vector-matrix algebra is, in fact, isomorphic to the algebra of split-octonions. Write an octonion x in the form
where and b are real numbers and a and b are pure quaternions regarded as vectors in R3. The isomorphism from the split-octonions to the Zorn's algebra is given by
This isomorphism preserves the norm since .
Split-octonions are used in the description of physical law. For examples, (a) the Dirac equation in physics (the equation of motion of a free spin 1/2 particle, like e.g. an electron or a proton) can be expressed on native split-octonion arithmetic, (b) the supersymmetric quantum mechanics has an octonionic extension.
- Kevin McCrimmon (2004) A Taste of Jordan Algebras, page 158, Universitext, Springer ISBN 0-387-95447-3 MR2014924
- Max Zorn (1931) "Alternativekörper und quadratische Systeme", Abhandlungen aus dem Mathematischen Seminar der Universität Hamburg 9(3/4): 395–402
- Nathan Jacobson (1962) Lie Algebras, page 142, Interscience Publishers.
- Richard D. Schafer (1966) An Introduction to Nonassociative Algebras, pp 52–6, Academic Press
- Lowell J. Page (1963) "Jordan Algebras", pages 144–186 in Studies in Modern Algebra edited by A.A. Albert, Mathematics Association of America : Zorn’s vector-matrix algebra on page 180
- M. Gogberashvili (2006) "Octonionic Electrodynamics", Journal of Physics A 39: 7099-7104. doi:10.1088/0305-4470/39/22/020
- V. Dzhunushaliev (2008) "Non-associativity, supersymmetry and hidden variables", Journal of Mathematical Physics 49: 042108 doi:10.1063/1.2907868; arXiv:0712.1647