Details of the construction of the classical real algebras are as follows:
Complex numbers as ordered pairs The
complex numbers can be written as
ordered pairs of
real numbers and , with the addition operator being component-wise and with multiplication defined by : (a, b) (c, d) = (a c - b d, a d + b c).\, A complex number whose second component is zero is associated with a real number: the complex number is associated with the real number . The
complex conjugate of is given by : (a, b)^* = (a^*, -b) = (a, -b) since is a real number and is its own conjugate. The conjugate has the property that : (a, b)^* (a, b) = (a a + b b, a b - b a) = \left(a^2 + b^2, 0\right),\, which is a non-negative real number. In this way, conjugation defines a
norm, making the complex numbers a
normed vector space over the real numbers: the norm of a complex number is : |z| = \left(z^* z\right)^\frac12.\, Furthermore, for any non-zero complex number , conjugation gives a
multiplicative inverse, : z^{-1} = \frac{z^*}{|z|^2}. As a complex number consists of two independent real numbers, they form a two-dimensional
vector space over the real numbers. Besides being of higher dimension, the complex numbers can be said to lack one algebraic property of the real numbers: a real number is its own conjugate.
Quaternions File:Cayley_Q8_multiplication_graph.svg|thumb|link=|Cayley Q8 graph of quaternion multiplication showing cycles of multiplication of
i (red),
j (green) and
k (blue). In [ the SVG file,] hover over or click a path to highlight it. The next step in the construction is to generalize the multiplication and conjugation operations. Form ordered pairs of complex numbers and , with multiplication defined by : (a, b) (c, d) = (a c - d^* b, d a + b c^*).\, Slight variations on this formula are possible; the resulting constructions will yield structures identical up to the signs of bases. The order of the factors seems odd now, but will be important in the next step. Define the conjugate of by : (a, b)^* = (a^*, -b).\, These operators are direct extensions of their complex analogs: if and are taken from the real subset of complex numbers, the appearance of the conjugate in the formulas has no effect, so the operators are the same as those for the complex numbers. The product of a nonzero element with its conjugate is a non-negative real number: : \begin{align} (a, b)^* (a, b) &= (a^*, -b) (a, b) \\ &= (a^* a + b^* b, b a^* - b a^*) \\ &= \left(|a|^2 + |b|^2, 0 \right).\, \end{align} As before, the conjugate thus yields a norm and an inverse for any such ordered pair. So in the sense we explained above, these pairs constitute an algebra something like the real numbers. They are the
quaternions, named by
Hamilton in 1843. As a quaternion consists of two independent complex numbers, they form a four-dimensional vector space over the real numbers. The multiplication of quaternions is not quite like the multiplication of real numbers, though; it is not
commutative – that is, if and are quaternions, it is not always true that .
Octonions All the steps to create further algebras are the same from octonions onwards. This time, form ordered pairs of quaternions and , with multiplication and conjugation defined exactly as for the quaternions: : (p, q) (r, s) = (p r - s^* q, s p + q r^*).\, Note, however, that because the quaternions are not commutative, the order of the factors in the multiplication formula becomes important—if the last factor in the multiplication formula were rather than , the formula for multiplication of an element by its conjugate would not yield a real number. For exactly the same reasons as before, the conjugation operator yields a norm and a multiplicative inverse of any nonzero element. This algebra was discovered by
John T. Graves in 1843, and is called the
octonions or the "
Cayley numbers". As an octonion consists of two independent quaternions, they form an eight-dimensional vector space over the real numbers. The multiplication of octonions is even stranger than that of quaternions; besides being non-commutative, it is not
associative – that is, if , , and are octonions, it is not always true that . For the reason of this non-associativity, octonions have
no matrix representation.
Sedenions The algebra immediately following the octonions is called the
sedenions. It retains the algebraic property of
power associativity, meaning that if is a sedenion, , but loses the property of being an
alternative algebra and hence cannot be a
composition algebra. It is also at this point that the algebras formed by the Cayley-Dickson construction begin to have nontrivial
zero divisors, in that this and every further algebra created by the construction will have pairs of nonzero values (for example, {{tmath|(e_3 + e_{10})}} and {{tmath|(e_6 - e_{15})}}) which when multiplied give 0.
Trigintaduonions The algebra immediately following the
sedenions is the
trigintaduonions, which form a 32-
dimensional algebra over the
real numbers and can be represented by
blackboard bold \mathbb T.
Further algebras The Cayley–Dickson construction can be carried on
ad infinitum, at each step producing a power-associative algebra whose dimension is double that of the algebra of the preceding step. These include the 64-dimensional sexagintaquatronions (or 64-nions), the 128-dimensional centumduodetrigintanions (or 128-nions), the 256-dimensional ducentiquinquagintasexions (or 256-nions), and
ad infinitum. All the algebras generated in this way over a field are
quadratic: that is, each element satisfies a quadratic equation with coefficients from the field. == Modified Cayley–Dickson construction ==