In mathematics, the Cayley–Dickson construction, named after Arthur Cayley and Leonard Eugene Dickson, produces a sequence of algebras over the field of real numbers, each with twice the dimension of the previous one. The algebras produced by this process are known as Cayley–Dickson algebras, for example complex numbers, quaternions, and octonions. These examples are useful composition algebras frequently applied in mathematical physics.
The Cayley–Dickson construction defines a new algebra as a Cartesian product of an algebra with itself, with multiplication defined in a specific way (different from the componentwise multiplication) and an involution known as conjugation. The product of an element and its conjugate (or sometimes the square root of this product) is called the norm.
The symmetries of the real field disappear as the Cayley–Dickson construction is repeatedly applied: first losing order, then commutativity of multiplication, associativity of multiplication, and finally alternativity.
More generally, the Cayley–Dickson construction takes any algebra with involution to another algebra with involution of twice the dimension.
Hurwitz's theorem (composition algebras) states that the reals, complex numbers, quaternions, and octonions are the only (normed) division algebras (over the real numbers).
| Algebra | Multiplication properties | Nontriv. zero divisors | |||||
|---|---|---|---|---|---|---|---|
| Power-assoc. | |||||||
| Real numbers | 1 | ||||||
| Complex num. | 2 | ||||||
| Quaternions | 4 | ||||||
| Octonions | 8 | ||||||
| Sedenions | 16 | rowspan=2 | rowspan=2 | rowspan=2 | rowspan=2 | rowspan=2 | rowspan=2 |
| ≥ 32 | |||||||
The Cayley–Dickson construction is due to Leonard Dickson in 1919 showing how the octonions can be constructed as a two-dimensional algebra over quaternions. In fact, starting with a field F, the construction yields a sequence of F-algebras of dimension 2n. For n = 2 it is an associative algebra called a quaternion algebra, and for n = 3 it is an alternative algebra called an octonion algebra. These instances n = 1, 2 and 3 produce composition algebras as shown below.
The case n = 1 starts with elements (a, b) in F × F and defines the conjugate (a, b)* to be (a*, –b) where a* = a in case n = 1, and subsequently determined by the formula. The essence of the F-algebra lies in the definition of the product of two elements (a, b) and (c, d):
(a,b) x (c,d)=(ac-d*b,da+bc*).
z=(a,b)
w=(c,d),
w*z*=(zw)*.
proof:
(c*,-d)(a*,-b)=(c*a*+b*(-d),-bc*-da)=(zw)*.
N(z)=zz*
N(zw)=N(z)N(w).
proof:
N(zw)=(ac-d*b,da+bc*)(c*a*-b*d,-da-bc*)=(aa*+bb*)(cc*+dd*)
Details of the construction of the classical real algebras are as follows:
See main article: Complex number. 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)=(ac-bd,ad+bc).
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)=(aa+bb,ab-ba)=\left(a2+b2,0\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) |
Furthermore, for any non-zero complex number , conjugation gives a multiplicative inverse,
z-1=
| 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.
See main article: Quaternion.
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)=(ac-d*b,da+bc*).
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,ba*-ba*)\ &=\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 .
See main article: Octonion. All the steps to create further algebras are the same from octonions on.
This time, form ordered pairs of quaternions and, with multiplication and conjugation defined exactly as for the quaternions:
(p,q)(r,s)=(pr-s*q,sp+qr*).
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.
The algebra immediately following the octonions is called the sedenions. It retains an algebraic property called power associativity, meaning that if is a sedenion,, but loses the property of being an alternative algebra and hence cannot be a composition algebra.
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. 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.
In 1954 R. D. Schafer examined the algebras generated by the Cayley–Dickson process over a field and showed they satisfy the flexible identity. He also proved that any derivation algebra of a Cayley–Dickson algebra is isomorphic to the derivation algebra of Cayley numbers, a 14-dimensional Lie algebra over .[1]
The Cayley–Dickson construction, starting from the real numbers
R
C
H
O
When this modified construction is applied to
R
R x R;
gave a slight generalization, defining the product and involution on for an algebra with involution (with) to be
\begin{align}(p,q)(r,s)&=(pr-\gammas*q,sp+qr*)\ (p,q)*&=(p*,-q)\end{align}
The algebra produced by the Cayley–Dickson construction is also an algebra with involution.
inherits properties from unchanged as follows.
Other properties of only induce weaker properties of :