Non-associative algebra

A **non-associative algebra** (or **distributive algebra**) is an algebra over a field where the binary multiplication operation is not assumed to be associative. That is, an algebraic structure *A* is a non-associative algebra over a field *K* if it is a vector space over *K* and is equipped with a *K*-bilinear binary multiplication operation *A* × *A* → *A* which may or may not be associative. Examples include Lie algebras, Jordan algebras, the octonions, and three-dimensional Euclidean space equipped with the cross product operation. Since it is not assumed that the multiplication is associative, using parentheses to indicate the order of multiplications is necessary. For example, the expressions (*ab*)(*cd*), (*a*(*bc*))*d* and *a*(*b*(*cd*)) may all yield different answers.

While this use of *non-associative* means that associativity is not assumed, it does not mean that associativity is disallowed. In other words, "non-associative" means "not necessarily associative", just as "noncommutative" means "not necessarily commutative" for noncommutative rings.

An algebra is *unital* or *unitary* if it has an identity element *I* with *Ix* = *x* = *xI* for all *x* in the algebra. For example, the octonions are unital, but Lie algebras never are.

The nonassociative algebra structure of *A* may be studied by associating it with other associative algebras which are subalgebra of the full algebra of *K*-endomorphisms of *A* as a *K*-vector space. Two such are the **derivation algebra** and the **(associative) enveloping algebra**, the latter being in a sense "the smallest associative algebra containing *A*".

More generally, some authors consider the concept of a non-associative algebra over a commutative ring *R*: An *R*-module equipped with an *R*-bilinear binary multiplication operation. If a structure obeys all of the ring axioms apart from associativity (for example, any *R*-algebra), then it is naturally a

Z

{\displaystyle \mathbb{Z}}

-algebra, so some authors refer to non-associative

Z

{\displaystyle \mathbb{Z}}

-algebras as **non-associative rings**.

## Algebras satisfying identities

Ring-like structures with two binary operations and no other restrictions are a broad class, one which is too general to study. For this reason, the best-known kinds of non-associative algebras satisfy identities which simplify multiplication somewhat. These include the following identities.

In the list, *x*, *y* and *z* denote arbitrary elements of an algebra.

* Associative: (*xy*)*z* = *x*(*yz*).
* Commutative: *xy* = *yx*.
* Anticommutative: *xy* = −*yx*.
* Jacobi identity: (*xy*)*z* + (*yz*)*x* + (*zx*)*y* = 0.
* Jordan identity: (*xy*)(*x*2) = *x*(*y*(*x*2)).
* Power associative: For all *x*, any three nonnegative powers of *x* associate. That is if *a*, *b* and *c* are nonnegative powers of *x*, then *a*(*bc*) = (*ab*)*c*. This is equivalent to saying that *x**m* *x**n* = *x**n+m* for all non-negative integers *m* and *n*.
* Alternative: (*xx*)*y* = *x*(*xy*) and (*yx*)*x* = *y*(*xx*).
* Flexible: *x*(*yx*) = (*xy*)*x*.
* Elastic: Flexible and (*xy*)(*xx*) = *x*(*y*(*xx*)), *x*(*xx*)*y* = (*xx*)(*xy*).

These properties are related by

1. *associative* implies *alternative* implies *power associative*;
2. *associative* implies *Jordan identity* implies *power associative*;
3. Each of the properties *associative*, *commutative*, *anticommutative*, *Jordan identity*, and *Jacobi identity* individually imply *flexible*, which implies *power associative*.
4. For a field with characteristic not two, being both commutative and anticommutative implies the algebra is just {0}.
5. *alternative* implies *flexible*. If the algebra is not commutative, any two out of the three following properties: *left-alternative*, *right-alternative*, *flexible*, imply the third one.

### Associator

Main articles: Associator
The **associator** on *A* is the *K*-multilinear map

[
⋅
,
⋅
,
⋅
]
:
A
×
A
×
A
→
A

{\displaystyle [\cdot,\cdot,\cdot] : A \times A \times A \to A}

 given by

[
x
,
y
,
z
# ]
(
x
y
)
z
−
x
(
y
z
)
.

{\displaystyle [x,y,z] = (xy)z - x(yz).\,}

It measures the degree of nonassociativity of

A

{\displaystyle A}

, and can be used to conveniently express some possible identities satisfied by *A*.

* Associative: the associator is identically zero;
* Alternative: the associator is alternating, interchange of any two terms changes the sign;
* Flexible:

[
x
,
y
,
x
# ]
0

{\displaystyle [x,y,x] = 0}

;
* Jordan:

[
x
,
y
,

x
2

# ]
0

{\displaystyle [x, y, x^2] = 0}

.

The **nucleus** is the set of elements that associate with all others: that is, the *n* in *A* such that

[
n
,
A
,
A
# ]
[
A
,
n
,
A
# ]
[
A
,
A
,
n
# ]
{
0
}

.

{\displaystyle [n,A,A] = [A,n,A] = [A,A,n] = \{0\} \ . }

The nucleus is an associative subring of *A*.

### Center

The **center** of a *A* is the set of elements that commute and associate with everything in *A*, that is the intersection of

C
(
A
# )
{
n
∈
A

n
# r
r
n

∀
r
∈
A

}

{\displaystyle C(A) = \{ n \in A \ | \ nr=rn \, \forall r \in A \, \} }

with the nucleus. It turns out that for elements of *C(A)* it is enough that two of the sets

(
[
n
,
A
,
A
]
,
[
A
,
n
,
A
]
,
[
A
,
A
,
n
]
)

{\displaystyle ([n,A,A], [A,n,A] , [A,A,n])}

 are

{
0
}

{\displaystyle \{0\}}

 for the third to also be the zero set.

## Examples

* Euclidean space **R**3 with multiplication given by the vector cross product is an example of an algebra which is anticommutative and not associative. The cross product also satisfies the Jacobi identity.
* Lie algebras are algebras satisfying anticommutativity and the Jacobi identity.
* Algebras of vector fields on a differentiable manifold (if *K* is **R** or the complex numbers **C**) or an algebraic variety (for general *K*);
* Jordan algebras are algebras which satisfy the commutative law and the Jordan identity.
* Every associative algebra gives rise to a Lie algebra by using the commutator as Lie bracket. In fact every Lie algebra can either be constructed this way, or is a subalgebra of a Lie algebra so constructed.
* Every associative algebra over a field of characteristic other than 2 gives rise to a Jordan algebra by defining a new multiplication *x\*y* = (1/2)(*xy* + *yx*). In contrast to the Lie algebra case, not every Jordan algebra can be constructed this way. Those that can are called *special*.
* Alternative algebras are algebras satisfying the alternative property. The most important examples of alternative algebras are the octonions (an algebra over the reals), and generalizations of the octonions over other fields. All associative algebras are alternative. Up to isomorphism, the only finite-dimensional real alternative, division algebras (see below) are the reals, complexes, quaternions and octonions.
* Power-associative algebras, are those algebras satisfying the power-associative identity. Examples include all associative algebras, all alternative algebras, Jordan algebras, and the sedenions.
* The hyperbolic quaternion algebra over **R**, which was an experimental algebra before the adoption of Minkowski space for special relativity.

More classes of algebras:

* Graded algebras. These include most of the algebras of interest to multilinear algebra, such as the tensor algebra, symmetric algebra, and exterior algebra over a given vector space. Graded algebras can be generalized to filtered algebras.
* Division algebras, in which multiplicative inverses exist. The finite-dimensional alternative division algebras over the field of real numbers have been classified. They are the real numbers (dimension 1), the complex numbers (dimension 2), the quaternions (dimension 4), and the octonions (dimension 8). The quaternions and octonions are not commutative. Of these algebras, all are associative except for the octonions.
* Quadratic algebras, which require that *xx* = *re* + *sx*, for some elements *r* and *s* in the ground field, and *e* a unit for the algebra. Examples include all finite-dimensional alternative algebras, and the algebra of real 2-by-2 matrices. Up to isomorphism the only alternative, quadratic real algebras without divisors of zero are the reals, complexes, quaternions, and octonions.
* The Cayley–Dickson algebras (where *K* is **R**), which begin with:
	+ **C** (a commutative and associative algebra);
	+ the quaternions **H** (an associative algebra);
	+ the octonions (an alternative algebra);
	+ the sedenions, and the infinite sequence of Cayley-Dickson algebras (power-associative algebras).
* The Poisson algebras are considered in geometric quantization. They carry two multiplications, turning them into commutative algebras and Lie algebras in different ways.
* Genetic algebras are non-associative algebras used in mathematical genetics.
* Triple systems

See also: list of algebras
## Properties

There are several properties that may be familiar from ring theory, or from associative algebras, which are not always true for non-associative algebras. Unlike the associative case, elements with a (two-sided) multiplicative inverse might also be a zero divisor. For example, all non-zero elements of the sedenions have a two-sided inverse, but some of them are also zero divisors.

## Free non-associative algebra

The **free non-associative algebra** on a set *X* over a field *K* is defined as the algebra with basis consisting of all non-associative monomials, finite formal products of elements of *X* retaining parentheses. The product of monomials *u*, *v* is just (*u*)(*v*). The algebra is unital if one takes the empty product as a monomial.

Kurosh proved that every subalgebra of a free non-associative algebra is free.

## Associated algebras

An algebra *A* over a field *K* is in particular a *K*-vector space and so one can consider the associative algebra End*K*(*A*) of *K*-linear vector space endomorphism of *A*. We can associate to the algebra structure on *A* two subalgebras of End*K*(*A*), the **derivation algebra** and the **(associative) enveloping algebra**.

### Derivation algebra

Main articles: Derivation algebra
A *derivation* on *A* is a map *D* with the property

D
(
x
⋅
y
# )
D
(
x
)
⋅
y
x
⋅
D
(
y
)

.

{\displaystyle D(x \cdot y) = D(x) \cdot y + x \cdot D(y) \ . }

The derivations on *A* form a subspace Der*K*(*A*) in End*K*(*A*). The commutator of two derivations is again a derivation, so that the Lie bracket gives Der*K*(*A*) a structure of Lie algebra.

### Enveloping algebra

There are linear maps *L* and *R* attached to each element *a* of an algebra *A*:

L
(
a
)
:
x
↦
a
x
;

R
(
a
)
:
x
↦
x
a

.

{\displaystyle L(a) : x \mapsto ax ; \ \ R(a) : x \mapsto xa \ . }

The *associative enveloping algebra* or *multiplication algebra* of *A* is the associative algebra generated by the left and right linear maps. The *centroid* of *A* is the centraliser of the enveloping algebra in the endomorphism algebra End*K*(*A*). An algebra is *central* if its centroid consists of the *K*-scalar multiples of the identity.

Some of the possible identities satisfied by non-associative algebras may be conveniently expressed in terms of the linear maps:

* Commutative: each *L*(*a*) is equal to the corresponding *R*(*a*);
* Associative: any *L* commutes with any *R*;
* Flexible: every *L*(*a*) commutes with the corresponding *R*(*a*);
* Jordan: every *L*(*a*) commutes with *R*(*a*2);
* Alternative: every *L*(*a*)2 = *L*(*a*2) and similarly for the right.

The *quadratic representation* *Q* is defined by

Q
(
a
)
:
x
↦
2
a
⋅
(
a
⋅
x
)
−
(
a
⋅
a
)
⋅
x

{\displaystyle Q(a) : x \mapsto 2a \cdot (a \cdot x) - (a \cdot a) \cdot x \ }

or equivalently

Q
(
a
# )
2

L
2

(
a
)
−
L
(

a
2

)

.

{\displaystyle Q(a) = 2 L^2(a) - L(a^2) \ . }

The article on universal enveloping algebras describes the canonical construction of enveloping algebras, as well as the PBW-type theorems for them. For Lie algebras, such enveloping algebras have a universal property, which does not hold, in general, for non-associative algebras. The best-known example is, perhaps the Albert algebra, an exceptional Jordan algebra that is not enveloped by the canonical construction of the enveloping algebra for Jordan algebras.