In mathematics, the exterior algebra, or Grassmann algebra, named after Hermann Grassmann,^{[3]} is an algebra that uses the exterior product or wedge product as its multiplication. In mathematics, the exterior product or wedge product of vectors is an algebraic construction used in geometry to study areas, volumes, and their higherdimensional analogues. The exterior product of two vectors and denoted by is called a bivector and lives in a space called the exterior square, a vector space that is distinct from the original space of vectors. The magnitude^{[4]} of can be interpreted as the area of the parallelogram with sides and which in three dimensions can also be computed using the cross product of the two vectors. More generally, all parallel plane surfaces with the same orientation and area have the same bivector as a measure of their oriented area. Like the cross product, the exterior product is anticommutative, meaning that for all vectors and but, unlike the cross product, the exterior product is associative.
When regarded in this manner, the exterior product of two vectors is called a 2blade. More generally, the exterior product of any number k of vectors can be defined and is sometimes called a kblade. It lives in a space known as the kth exterior power. The magnitude of the resulting kblade is the oriented hypervolume of the kdimensional parallelotope whose edges are the given vectors, just as the magnitude of the scalar triple product of vectors in three dimensions gives the volume of the parallelepiped generated by those vectors.
The exterior algebra provides an algebraic setting in which to answer geometric questions. For instance, blades have a concrete geometric interpretation, and objects in the exterior algebra can be manipulated according to a set of unambiguous rules. The exterior algebra contains objects that are not only kblades, but sums of kblades; such a sum is called a kvector.^{[5]} The kblades, because they are simple products of vectors, are called the simple elements of the algebra. The rank of any kvector is defined to be the smallest number of simple elements of which it is a sum. The exterior product extends to the full exterior algebra, so that it makes sense to multiply any two elements of the algebra. Equipped with this product, the exterior algebra is an associative algebra, which means that for any elements The kvectors have degree k, meaning that they are sums of products of k vectors. When elements of different degrees are multiplied, the degrees add like multiplication of polynomials. This means that the exterior algebra is a graded algebra.
The definition of the exterior algebra makes sense for spaces not just of geometric vectors, but of other vectorlike objects such as vector fields or functions. In full generality, the exterior algebra can be defined for modules over a commutative ring, and for other structures of interest in abstract algebra. It is one of these more general constructions where the exterior algebra finds one of its most important applications, where it appears as the algebra of differential forms that is fundamental in areas that use differential geometry. The exterior algebra also has many algebraic properties that make it a convenient tool in algebra itself. The association of the exterior algebra to a vector space is a type of functor on vector spaces, which means that it is compatible in a certain way with linear transformations of vector spaces. The exterior algebra is one example of a bialgebra, meaning that its dual space also possesses a product, and this dual product is compatible with the exterior product. This dual algebra is precisely the algebra of alternating multilinear forms, and the pairing between the exterior algebra and its dual is given by the interior product.
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Motivating examples
The first two examples assume a metric tensor field and an orientation; the third example does not assume either.
Areas in the plane
The Cartesian plane is a real vector space equipped with a basis consisting of a pair of unit vectors
 with the orientation and with the metric
Suppose that
are a pair of given vectors in written in components. There is a unique parallelogram having v and w as two of its sides. The area of this parallelogram is given by the standard determinant formula:
Consider now the exterior product of v and w:
where the first step uses the distributive law for the exterior product, and the last uses the fact that the exterior product is alternating, and in particular (The fact that the exterior product is alternating also forces ) Note that the coefficient in this last expression is precisely the determinant of the matrix [v w]. The fact that this may be positive or negative has the intuitive meaning that v and w may be oriented in a counterclockwise or clockwise sense as the vertices of the parallelogram they define. Such an area is called the signed area of the parallelogram: the absolute value of the signed area is the ordinary area, and the sign determines its orientation.
The fact that this coefficient is the signed area is not an accident. In fact, it is relatively easy to see that the exterior product should be related to the signed area if one tries to axiomatize this area as an algebraic construct. In detail, if A(v, w) denotes the signed area of the parallelogram of which the pair of vectors v and w form two adjacent sides, then A must satisfy the following properties:
 A(rv, sw) = rsA(v, w) for any real numbers r and s, since rescaling either of the sides rescales the area by the same amount (and reversing the direction of one of the sides reverses the orientation of the parallelogram).
 A(v, v) = 0, since the area of the degenerate parallelogram determined by v (i.e., a line segment) is zero.
 A(w, v) = −A(v, w), since interchanging the roles of v and w reverses the orientation of the parallelogram.
 A(v + rw, w) = A(v, w) for any real number r, since adding a multiple of w to v affects neither the base nor the height of the parallelogram and consequently preserves its area.
 A(e_{1}, e_{2}) = 1, since the area of the unit square is one.
With the exception of the last property, the exterior product of two vectors satisfies the same properties as the area. In a certain sense, the exterior product generalizes the final property by allowing the area of a parallelogram to be compared to that of any chosen parallelogram in a parallel plane (here, the one with sides e_{1} and e_{2}). In other words, the exterior product provides a basisindependent formulation of area.^{[6]}
Cross and triple products
For vectors in a 3dimensional oriented vector space with a bilinear scalar product, the exterior algebra is closely related to the cross product and triple product. Using a standard basis (e_{1}, e_{2}, e_{3}), the exterior product of a pair of vectors
and
is
where (e_{1} ∧ e_{2}, e_{2} ∧ e_{3}, e_{3} ∧ e_{1}) is a basis for the threedimensional space The coefficients above are the same as those in the usual definition of the cross product of vectors in three dimensions with a given orientation, the only differences being that the exterior product is not an ordinary vector, but instead is a 2vector, and that the exterior product does not depend on the choice of orientation^{[clarification needed]}.
Bringing in a third vector
the exterior product of three vectors is
where e_{1} ∧ e_{2} ∧ e_{3} is the basis vector for the onedimensional space The scalar coefficient is the triple product of the three vectors.
The cross product and triple product in a three dimensional Euclidean vector space each admit both geometric and algebraic interpretations, via Hodge star duality. The cross product u × v can be interpreted as a vector which is perpendicular to both u and v and whose magnitude is equal to the area of the parallelogram determined by the two vectors. It can also be interpreted as the vector consisting of the minors of the matrix with columns u and v. The triple product of u, v, and w is a signed scalar representing a geometric oriented volume. Algebraically, it is the determinant of the matrix with columns u, v, and w. The exterior product in three dimensions allows for similar interpretations: it, too, can be identified with oriented lines, areas, volumes, etc., that are spanned by one, two or more vectors. The exterior product generalizes these geometric notions to all vector spaces and to any number of dimensions, even in the absence of a scalar product.
Electromagnetic field
In Einstein's theories of relativity, the electromagnetic field is generally given as a differential 2form in 4space or as the equivalent alternating tensor field the electromagnetic tensor. Then or the equivalent Bianchi identity None of this requires a metric.
Adding the Lorentz metric and an orientation provides the Hodge star operator and thus makes it possible to define or the equivalent tensor divergence where
Formal definitions and algebraic properties
The exterior algebra of a vector space V over a field K is defined as the quotient algebra of the tensor algebra T(V) by the twosided ideal I generated by all elements of the form x ⊗ x for x ∈ V (i.e. all tensors that can be expressed as the tensor product of a vector in V by itself).^{[7]} The ideal I contains the ideal J generated by elements of the form and these ideals coincide if (if these ideals are different except for the zero vector space).
So,
is an associative algebra. Its multiplication is called the exterior product, and denoted ∧. This means that the product of is induced by the tensor product ⊗ of T(V).
As T^{0} = K, T^{1} = V, and the inclusions of K and V in T(V) induce injections of K and V into These injections are commonly considered as inclusions, and called natural embeddings, natural injections or natural inclusions. The word canonical is also commonly used in place of natural.
Alternating product
The exterior product is by construction alternating on elements of which means that for all by the above construction. It follows that the product is also anticommutative on elements of for supposing that
hence
More generally, if σ is a permutation of the integers [1, ..., k], and x_{1}, x_{2}, ..., x_{k} are elements of V, it follows that
where sgn(σ) is the signature of the permutation σ.^{[8]}
In particular, if x_{i} = x_{j} for some i ≠ j, then the following generalization of the alternating property also holds:
Together with the distributive property of the exterior product, one further generalization is that if and only if is a linearly dependent set of vectors, then
Exterior power
The kth exterior power of V, denoted is the vector subspace of spanned by elements of the form
If then α is said to be a kvector. If, furthermore, α can be expressed as an exterior product of k elements of V, then α is said to be decomposable. Although decomposable kvectors span not every element of is decomposable. For example, in the following 2vector is not decomposable:
(This is a symplectic form, since α ∧ α ≠ 0.^{[9]})
Basis and dimension
If the dimension of V is n and { e_{1}, …, e_{n} } is a basis for V, then the set
is a basis for The reason is the following: given any exterior product of the form
every vector v_{j} can be written as a linear combination of the basis vectors e_{i}; using the bilinearity of the exterior product, this can be expanded to a linear combination of exterior products of those basis vectors. Any exterior product in which the same basis vector appears more than once is zero; any exterior product in which the basis vectors do not appear in the proper order can be reordered, changing the sign whenever two basis vectors change places. In general, the resulting coefficients of the basis kvectors can be computed as the minors of the matrix that describes the vectors v_{j} in terms of the basis e_{i}.
By counting the basis elements, the dimension of is equal to a binomial coefficient:
where n is the dimension of the vectors, and k is the number of vectors in the product. The binomial coefficient produces the correct result, even for exceptional cases; in particular, for k > n.
Any element of the exterior algebra can be written as a sum of kvectors. Hence, as a vector space the exterior algebra is a direct sum
(where by convention the field underlying V, and ), and therefore its dimension is equal to the sum of the binomial coefficients, which is 2^{n}.
Rank of a kvector
If then it is possible to express α as a linear combination of decomposable kvectors:
where each α^{(i)} is decomposable, say
The rank of the kvector α is the minimal number of decomposable kvectors in such an expansion of α. This is similar to the notion of tensor rank.
Rank is particularly important in the study of 2vectors (Sternberg 1964, §III.6) (Bryant et al. 1991). The rank of a 2vector α can be identified with half the rank of the matrix of coefficients of α in a basis. Thus if e_{i} is a basis for V, then α can be expressed uniquely as
where a_{ij} = −a_{ji} (the matrix of coefficients is skewsymmetric). The rank of the matrix a_{ij} is therefore even, and is twice the rank of the form α.
In characteristic 0, the 2vector α has rank p if and only if
 and
Graded structure
The exterior product of a kvector with a pvector is a (k + p)vector, once again invoking bilinearity. As a consequence, the direct sum decomposition of the preceding section
gives the exterior algebra the additional structure of a graded algebra, that is
Moreover, if K is the base field, we have
 and
The exterior product is graded anticommutative, meaning that if and then
In addition to studying the graded structure on the exterior algebra, Bourbaki (1989) studies additional graded structures on exterior algebras, such as those on the exterior algebra of a graded module (a module that already carries its own gradation).
Universal property
Let V be a vector space over the field K. Informally, multiplication in is performed by manipulating symbols and imposing a distributive law, an associative law, and using the identity for v ∈ V. Formally, is the "most general" algebra in which these rules hold for the multiplication, in the sense that any unital associative Kalgebra containing V with alternating multiplication on V must contain a homomorphic image of In other words, the exterior algebra has the following universal property:^{[10]}
Given any unital associative Kalgebra A and any Klinear map such that for every v in V, then there exists precisely one unital algebra homomorphism such that j(v) = f(i(v)) for all v in V (here i is the natural inclusion of V in see above).
To construct the most general algebra that contains V and whose multiplication is alternating on V, it is natural to start with the most general associative algebra that contains V, the tensor algebra T(V), and then enforce the alternating property by taking a suitable quotient. We thus take the twosided ideal I in T(V) generated by all elements of the form v ⊗ v for v in V, and define as the quotient
(and use ∧ as the symbol for multiplication in ). It is then straightforward to show that contains V and satisfies the above universal property.
As a consequence of this construction, the operation of assigning to a vector space V its exterior algebra is a functor from the category of vector spaces to the category of algebras.
Rather than defining first and then identifying the exterior powers as certain subspaces, one may alternatively define the spaces first and then combine them to form the algebra This approach is often used in differential geometry and is described in the next section.
Generalizations
Given a commutative ring R and an Rmodule M, we can define the exterior algebra just as above, as a suitable quotient of the tensor algebra T(M). It will satisfy the analogous universal property. Many of the properties of also require that M be a projective module. Where finite dimensionality is used, the properties further require that M be finitely generated and projective. Generalizations to the most common situations can be found in Bourbaki (1989).
Exterior algebras of vector bundles are frequently considered in geometry and topology. There are no essential differences between the algebraic properties of the exterior algebra of finitedimensional vector bundles and those of the exterior algebra of finitely generated projective modules, by the Serre–Swan theorem. More general exterior algebras can be defined for sheaves of modules.
Alternating tensor algebra
If K is a field of characteristic 0,^{[11]} then the exterior algebra of a vector space V over K can be canonically identified with the vector subspace of T(V) consisting of antisymmetric tensors. Recall that the exterior algebra is the quotient of T(V) by the ideal I generated by elements of the form x ⊗ x.
Let T^{r}(V) be the space of homogeneous tensors of degree r. This is spanned by decomposable tensors
The antisymmetrization (or sometimes the skewsymmetrization) of a decomposable tensor is defined by
where the sum is taken over the symmetric group of permutations on the symbols {1, ..., r}. This extends by linearity and homogeneity to an operation, also denoted by Alt, on the full tensor algebra T(V). The image Alt(T(V)) is the alternating tensor algebra, denoted A(V). This is a vector subspace of T(V), and it inherits the structure of a graded vector space from that on T(V). It carries an associative graded product defined by
Although this product differs from the tensor product, the kernel of Alt is precisely the ideal I (again, assuming that K has characteristic 0), and there is a canonical isomorphism
Index notation
Suppose that V has finite dimension n, and that a basis e_{1}, ..., e_{n} of V is given. Then any alternating tensor t ∈ A^{r}(V) ⊂ T^{r}(V) can be written in index notation as
where t^{i1⋅⋅⋅ir} is completely antisymmetric in its indices.
The exterior product of two alternating tensors t and s of ranks r and p is given by
The components of this tensor are precisely the skew part of the components of the tensor product s ⊗ t, denoted by square brackets on the indices:
The interior product may also be described in index notation as follows. Let be an antisymmetric tensor of rank r. Then, for α ∈ V^{∗}, i_{α}t is an alternating tensor of rank r − 1, given by
where n is the dimension of V.
Duality
Alternating operators
Given two vector spaces V and X and a natural number k, an alternating operator from V^{k} to X is a multilinear map
such that whenever v_{1}, ..., v_{k} are linearly dependent vectors in V, then
The map
which associates to vectors from their exterior product, i.e. their corresponding vector, is also alternating. In fact, this map is the "most general" alternating operator defined on given any other alternating operator there exists a unique linear map with This universal property characterizes the space and can serve as its definition.
Alternating multilinear forms
The above discussion specializes to the case when X = K, the base field. In this case an alternating multilinear function
is called an alternating multilinear form. The set of all alternating multilinear forms is a vector space, as the sum of two such maps, or the product of such a map with a scalar, is again alternating. By the universal property of the exterior power, the space of alternating forms of degree k on V is naturally isomorphic with the dual vector space If V is finitedimensional, then the latter is naturally isomorphic^{[clarification needed]} to In particular, if V is ndimensional, the dimension of the space of alternating maps from V^{k} to K is the binomial coefficient
Under such identification, the exterior product takes a concrete form: it produces a new antisymmetric map from two given ones. Suppose ω : V^{k} → K and η : V^{m} → K are two antisymmetric maps. As in the case of tensor products of multilinear maps, the number of variables of their exterior product is the sum of the numbers of their variables. Depending on the choice of identification of elements of exterior power with multilinear forms, the exterior product is defined as
or as
where, if the characteristic of the base field K is 0, the alternation Alt of a multilinear map is defined to be the average of the signadjusted values over all the permutations of its variables:
When the field K has finite characteristic, an equivalent version of the second expression without any factorials or any constants is welldefined:
where here Sh_{k,m} ⊂ S_{k+m} is the subset of (k,m) shuffles: permutations σ of the set {1, 2, ..., k + m} such that σ(1) < σ(2) < ⋯ < σ(k), and σ(k + 1) < σ(k + 2) < ⋯ < σ(k + m).
Interior product
Suppose that V is finitedimensional. If V^{∗} denotes the dual space to the vector space V, then for each α ∈ V^{∗}, it is possible to define an antiderivation on the algebra
This derivation is called the interior product with α, or sometimes the insertion operator, or contraction by α.
Suppose that Then w is a multilinear mapping of V^{∗} to K, so it is defined by its values on the kfold Cartesian product V^{∗} × V^{∗} × ... × V^{∗}. If u_{1}, u_{2}, ..., u_{k−1} are k − 1 elements of V^{∗}, then define
Additionally, let i_{α}f = 0 whenever f is a pure scalar (i.e., belonging to ).
Axiomatic characterization and properties
The interior product satisfies the following properties:
 For each k and each α ∈ V^{∗}, (By convention, )
 If v is an element of V (), then i_{α}v = α(v) is the dual pairing between elements of V and elements of V^{∗}.
 For each α ∈ V^{∗}, i_{α} is a graded derivation of degree −1:
These three properties are sufficient to characterize the interior product as well as define it in the general infinitedimensional case.
Further properties of the interior product include:
Hodge duality
Suppose that V has finite dimension n. Then the interior product induces a canonical isomorphism of vector spaces
by the recursive definition
In the geometrical setting, a nonzero element of the top exterior power (which is a onedimensional vector space) is sometimes called a volume form (or orientation form, although this term may sometimes lead to ambiguity). The name orientation form comes from the fact that a choice of preferred top element determines an orientation of the whole exterior algebra, since it is tantamount to fixing an ordered basis of the vector space. Relative to the preferred volume form σ, the isomorphism is given explicitly by
If, in addition to a volume form, the vector space V is equipped with an inner product identifying V with V^{∗}, then the resulting isomorphism is called the Hodge star operator, which maps an element to its Hodge dual:
The composition of with itself maps → and is always a scalar multiple of the identity map. In most applications, the volume form is compatible with the inner product in the sense that it is an exterior product of an orthonormal basis of V. In this case,
where id is the identity mapping, and the inner product has metric signature (p, q) — p pluses and q minuses.
Inner product
For V a finitedimensional space, an inner product (or a pseudoEuclidean inner product) on V defines an isomorphism of V with V^{∗}, and so also an isomorphism of with The pairing between these two spaces also takes the form of an inner product. On decomposable kvectors,
the determinant of the matrix of inner products. In the special case v_{i} = w_{i}, the inner product is the square norm of the kvector, given by the determinant of the Gramian matrix (⟨v_{i}, v_{j}⟩). This is then extended bilinearly (or sesquilinearly in the complex case) to a nondegenerate inner product on If e_{i}, i = 1, 2, ..., n, form an orthonormal basis of V, then the vectors of the form
constitute an orthonormal basis for , a statement equivalent to the Cauchy–Binet formula.
With respect to the inner product, exterior multiplication and the interior product are mutually adjoint. Specifically, for and
where x^{♭} ∈ V^{∗} is the musical isomorphism, the linear functional defined by
for all y ∈ V. This property completely characterizes the inner product on the exterior algebra.
Indeed, more generally for and iteration of the above adjoint properties gives
where now is the dual lvector defined by
for all
Bialgebra structure
There is a correspondence between the graded dual of the graded algebra and alternating multilinear forms on V. The exterior algebra (as well as the symmetric algebra) inherits a bialgebra structure, and, indeed, a Hopf algebra structure, from the tensor algebra. See the article on tensor algebras for a detailed treatment of the topic.
The exterior product of multilinear forms defined above is dual to a coproduct defined on giving the structure of a coalgebra. The coproduct is a linear function Δ : → ⊗ which is given by
on elements v∈V. The symbol 1 stands for the unit element of the field K. Recall that K ⊂ , so that the above really does lie in ⊗ . This definition of the coproduct is lifted to the full space by (linear) homomorphism. The correct form of this homomorphism is not what one might naively write, but has to be the one carefully defined in the coalgebra article. In this case, one obtains
Expanding this out in detail, one obtains the following expression on decomposable elements:
where the second summation is taken over all (p+1, k−p)shuffles. The above is written with a notational trick, to keep track of the field element 1: the trick is to write and this is shuffled into various locations during the expansion of the sum over shuffles. The shuffle follows directly from the first axiom of a coalgebra: the relative order of the elements is preserved in the riffle shuffle: the riffle shuffle merely splits the ordered sequence into two ordered sequences, one on the left, and one on the right.
Observe that the coproduct preserves the grading of the algebra. Extending to the full space one has
The tensor symbol ⊗ used in this section should be understood with some caution: it is not the same tensor symbol as the one being used in the definition of the alternating product. Intuitively, it is perhaps easiest to think it as just another, but different, tensor product: it is still (bi)linear, as tensor products should be, but it is the product that is appropriate for the definition of a bialgebra, that is, for creating the object ⊗ . Any lingering doubt can be shaken by pondering the equalities (1 ⊗ v) ∧ (1 ⊗ w) = 1 ⊗ (v ∧ w) and (v ⊗ 1) ∧ (1 ⊗ w) = v ⊗ w, which follow from the definition of the coalgebra, as opposed to naive manipulations involving the tensor and wedge symbols. This distinction is developed in greater detail in the article on tensor algebras. Here, there is much less of a problem, in that the alternating product ∧ clearly corresponds to multiplication in the bialgebra, leaving the symbol ⊗ free for use in the definition of the bialgebra. In practice, this presents no particular problem, as long as one avoids the fatal trap of replacing alternating sums of ⊗ by the wedge symbol, with one exception. One can construct an alternating product from ⊗, with the understanding that it works in a different space. Immediately below, an example is given: the alternating product for the dual space can be given in terms of the coproduct. The construction of the bialgebra here parallels the construction in the tensor algebra article almost exactly, except for the need to correctly track the alternating signs for the exterior algebra.
In terms of the coproduct, the exterior product on the dual space is just the graded dual of the coproduct:
where the tensor product on the righthand side is of multilinear linear maps (extended by zero on elements of incompatible homogeneous degree: more precisely, α ∧ β = ε ∘ (α ⊗ β) ∘ Δ, where ε is the counit, as defined presently).
The counit is the homomorphism ε : → K that returns the 0graded component of its argument. The coproduct and counit, along with the exterior product, define the structure of a bialgebra on the exterior algebra.
With an antipode defined on homogeneous elements by the exterior algebra is furthermore a Hopf algebra.^{[14]}
Functoriality
Suppose that V and W are a pair of vector spaces and f : V → W is a linear map. Then, by the universal property, there exists a unique homomorphism of graded algebras
such that
In particular, preserves homogeneous degree. The kgraded components of are given on decomposable elements by
Let
The components of the transformation relative to a basis of V and W is the matrix of k × k minors of f. In particular, if V = W and V is of finite dimension n, then is a mapping of a onedimensional vector space to itself, and is therefore given by a scalar: the determinant of f.
Exactness
If is a short exact sequence of vector spaces, then
is an exact sequence of graded vector spaces,^{[15]} as is
 ^{[16]}
Direct sums
In particular, the exterior algebra of a direct sum is isomorphic to the tensor product of the exterior algebras:
This is a graded isomorphism; i.e.,
In greater generality, for a short exact sequence of vector spaces there is a natural filtration
where for is spanned by elements of the form for and The corresponding quotients admit a natural isomorphism
 given by
In particular, if U is 1dimensional then
is exact, and if W is 1dimensional then
is exact.^{[17]}
Applications
Linear algebra
In applications to linear algebra, the exterior product provides an abstract algebraic manner for describing the determinant and the minors of a matrix. For instance, it is well known that the determinant of a square matrix is equal to the volume of the parallelotope whose sides are the columns of the matrix (with a sign to track orientation). This suggests that the determinant can be defined in terms of the exterior product of the column vectors. Likewise, the k × k minors of a matrix can be defined by looking at the exterior products of column vectors chosen k at a time. These ideas can be extended not just to matrices but to linear transformations as well: the determinant of a linear transformation is the factor by which it scales the oriented volume of any given reference parallelotope. So the determinant of a linear transformation can be defined in terms of what the transformation does to the top exterior power. The action of a transformation on the lesser exterior powers gives a basisindependent way to talk about the minors of the transformation.
Technical details: Definitions
Let^{[18]} be an ndimensional vector space over field with basis
 For define on simple tensors by and expand the definition linearly to all tensors. More generally, we can define on simple tensors byi.e. choose k components on which A would act, then sum up all results obtained from different choices. If define Since is 1dimensional with basis we can identify with the unique number satisfying
 For define the exterior transpose to be the unique operator satisfying for any and
 For define These are equivalent to the previous definitions.
Basic properties
All results obtained from other definitions of the determinant, trace and adjoint can be obtained from this definition (since these definitions are equivalent). Here are some basic properties related to these new definitions:
 is linear.
 We have a canonical isomorphism However, there is no canonical isomorphism between and
 The entries of the transposed matrix of are minors of
 For all In particular,and hence
 In particular,
 The characteristic polynomial of can be given by Similarly,
Leverrier's algorithm
are the coefficients of the terms in the characteristic polynomial. They also appear in the expressions of and Leverrier's Algorithm^{[19]} is an economical way of computing and
 Set
 For
Physics
In physics, many quantities are naturally represented by alternating operators. For example, if the motion of a charged particle is described by velocity and acceleration vectors in fourdimensional spacetime, then normalization of the velocity vector requires that the electromagnetic force must be an alternating operator on the velocity. Its six degrees of freedom are identified with the electric and magnetic fields.
Linear geometry
The decomposable kvectors have geometric interpretations: the bivector u ∧ v represents the plane spanned by the vectors, "weighted" with a number, given by the area of the oriented parallelogram with sides u and v. Analogously, the 3vector u ∧ v ∧ w represents the spanned 3space weighted by the volume of the oriented parallelepiped with edges u, v, and w.
Projective geometry
Decomposable kvectors in correspond to weighted kdimensional linear subspaces of V. In particular, the Grassmannian of kdimensional subspaces of V, denoted Gr_{k}(V), can be naturally identified with an algebraic subvariety of the projective space This is called the Plücker embedding.
Differential geometry
The exterior algebra has notable applications in differential geometry, where it is used to define differential forms.^{[20]} Differential forms are mathematical objects that evaluate the length of vectors, areas of parallelograms, and volumes of higherdimensional bodies, so they can be integrated over curves, surfaces and higher dimensional manifolds in a way that generalizes the line integrals and surface integrals from calculus. A differential form at a point of a differentiable manifold is an alternating multilinear form on the tangent space at the point. Equivalently, a differential form of degree k is a linear functional on the kth exterior power of the tangent space. As a consequence, the exterior product of multilinear forms defines a natural exterior product for differential forms. Differential forms play a major role in diverse areas of differential geometry.
An alternate approach defines differential forms in terms of germs of functions.
In particular, the exterior derivative gives the exterior algebra of differential forms on a manifold the structure of a differential graded algebra. The exterior derivative commutes with pullback along smooth mappings between manifolds, and it is therefore a natural differential operator. The exterior algebra of differential forms, equipped with the exterior derivative, is a cochain complex whose cohomology is called the de Rham cohomology of the underlying manifold and plays a vital role in the algebraic topology of differentiable manifolds.
Representation theory
In representation theory, the exterior algebra is one of the two fundamental Schur functors on the category of vector spaces, the other being the symmetric algebra. Together, these constructions are used to generate the irreducible representations of the general linear group; see fundamental representation.
Superspace
The exterior algebra over the complex numbers is the archetypal example of a superalgebra, which plays a fundamental role in physical theories pertaining to fermions and supersymmetry. A single element of the exterior algebra is called a supernumber^{[21]} or Grassmann number. The exterior algebra itself is then just a onedimensional superspace: it is just the set of all of the points in the exterior algebra. The topology on this space is essentially the weak topology, the open sets being the cylinder sets. An ndimensional superspace is just the nfold product of exterior algebras.
Lie algebra homology
Let L be a Lie algebra over a field K, then it is possible to define the structure of a chain complex on the exterior algebra of L. This is a Klinear mapping
defined on decomposable elements by
The Jacobi identity holds if and only if ∂∂ = 0, and so this is a necessary and sufficient condition for an anticommutative nonassociative algebra L to be a Lie algebra. Moreover, in that case is a chain complex with boundary operator ∂. The homology associated to this complex is the Lie algebra homology.
Homological algebra
The exterior algebra is the main ingredient in the construction of the Koszul complex, a fundamental object in homological algebra.
History
The exterior algebra was first introduced by Hermann Grassmann in 1844 under the blanket term of Ausdehnungslehre, or Theory of Extension.^{[22]} This referred more generally to an algebraic (or axiomatic) theory of extended quantities and was one of the early precursors to the modern notion of a vector space. SaintVenant also published similar ideas of exterior calculus for which he claimed priority over Grassmann.^{[23]}
The algebra itself was built from a set of rules, or axioms, capturing the formal aspects of Cayley and Sylvester's theory of multivectors. It was thus a calculus, much like the propositional calculus, except focused exclusively on the task of formal reasoning in geometrical terms.^{[24]} In particular, this new development allowed for an axiomatic characterization of dimension, a property that had previously only been examined from the coordinate point of view.
The import of this new theory of vectors and multivectors was lost to mid 19th century mathematicians,^{[25]} until being thoroughly vetted by Giuseppe Peano in 1888. Peano's work also remained somewhat obscure until the turn of the century, when the subject was unified by members of the French geometry school (notably Henri Poincaré, Élie Cartan, and Gaston Darboux) who applied Grassmann's ideas to the calculus of differential forms.
A short while later, Alfred North Whitehead, borrowing from the ideas of Peano and Grassmann, introduced his universal algebra. This then paved the way for the 20th century developments of abstract algebra by placing the axiomatic notion of an algebraic system on a firm logical footing.
See also
 Alternating algebra
 Exterior calculus identities
 Clifford algebra, a generalization of exterior algebra using a nonzero quadratic form
 Geometric algebra
 Koszul complex
 Multilinear algebra
 Symmetric algebra, the symmetric analog
 Tensor algebra
 Weyl algebra, a quantum deformation of the symmetric algebra by a symplectic form
Notes
 ^ ^{a} ^{b} Penrose, R. (2007). The Road to Reality. Vintage books. ISBN 9780679776314.
 ^ Wheeler, Misner & Thorne 1973, p. 83
 ^ Grassmann (1844) introduced these as extended algebras (cf. Clifford 1878). He used the word äußere (literally translated as outer, or exterior) only to indicate the produkt he defined, which is nowadays conventionally called exterior product, probably to distinguish it from the outer product as defined in modern linear algebra.
 ^ Strictly speaking, the magnitude depends on some additional structure, namely that the vectors be in a Euclidean space. We do not generally assume that this structure is available, except where it is helpful to develop intuition on the subject.
 ^ The term kvector is not equivalent to and should not be confused with similar terms such as 4vector, which in a different context could mean an element of a 4dimensional vector space. A minority of authors use the term kmultivector instead of kvector, which avoids this confusion.
 ^ This axiomatization of areas is due to Leopold Kronecker and Karl Weierstrass; see Bourbaki (1989b, Historical Note). For a modern treatment, see Mac Lane & Birkhoff (1999, Theorem IX.2.2). For an elementary treatment, see Strang (1993, Chapter 5).
 ^ Mac Lane & Birkhoff (1999)
 ^ A proof of this can be found in more generality in Bourbaki (1989).
 ^ See Sternberg (1964, §III.6).
 ^ See Bourbaki (1989, §III.7.1), and Mac Lane & Birkhoff (1999, Theorem XVI.6.8). More detail on universal properties in general can be found in Mac Lane & Birkhoff (1999, Chapter VI), and throughout the works of Bourbaki.
 ^ See Bourbaki (1989, §III.7.5) for generalizations.
 ^ Note: The orientations shown here are not correct; the diagram simply gives a sense that an orientation is defined for every kform.
 ^ Wheeler, J.A.; Misner, C.; Thorne, K.S. (1973). Gravitation. W.H. Freeman & Co. pp. 58–60, 83, 100–9, 115–9. ISBN 0716703440.
 ^ Indeed, the exterior algebra of V is the enveloping algebra of the abelian Lie superalgebra structure on V.
 ^ This part of the statement also holds in greater generality if V and W are modules over a commutative ring: That converts epimorphisms to epimorphisms. See Bourbaki (1989, Proposition 3, §III.7.2).
 ^ This statement generalizes only to the case where V and W are projective modules over a commutative ring. Otherwise, it is generally not the case that converts monomorphisms to monomorphisms. See Bourbaki (1989, Corollary to Proposition 12, §III.7.9).
 ^ Such a filtration also holds for vector bundles, and projective modules over a commutative ring. This is thus more general than the result quoted above for direct sums, since not every short exact sequence splits in other abelian categories.
 ^ Winitzki 2010
 ^ Kahan, W. (2000). "Jordan's normal form" (PDF). Math. H110.
 ^ James, A.T. (1983). "On the Wedge Product". In Karlin, Samuel; Amemiya, Takeshi; Goodman, Leo A. (eds.). Studies in Econometrics, Time Series, and Multivariate Statistics. Academic Press. pp. 455–464. ISBN 0123987504.
 ^ DeWitt, Bryce (1984). "Chapter 1". Supermanifolds. Cambridge University Press. p. 1. ISBN 0521423775.
 ^ Kannenberg (2000) published a translation of Grassmann's work in English; he translated Ausdehnungslehre as Extension Theory.
 ^ J Itard, Biography in Dictionary of Scientific Biography (New York 1970–1990).
 ^ Authors have in the past referred to this calculus variously as the calculus of extension (Whitehead 1898; Forder 1941), or extensive algebra (Clifford 1878), and recently as extended vector algebra (Browne 2007).
 ^ Bourbaki 1989, p. 661.
References
Mathematical references
 Bishop, R.; Goldberg, S.I. (1980), Tensor analysis on manifolds, Dover, ISBN 0486640396
 Includes a treatment of alternating tensors and alternating forms, as well as a detailed discussion of Hodge duality from the perspective adopted in this article.
 Bourbaki, Nicolas (1989), Elements of mathematics, Algebra I, SpringerVerlag, ISBN 3540642439
 This is the main mathematical reference for the article. It introduces the exterior algebra of a module over a commutative ring (although this article specializes primarily to the case when the ring is a field), including a discussion of the universal property, functoriality, duality, and the bialgebra structure. See §III.7 and §III.11.
 Bryant, R.L.; Chern, S.S.; Gardner, R.B.; Goldschmidt, H.L.; Griffiths, P.A. (1991), Exterior differential systems, SpringerVerlag
 This book contains applications of exterior algebras to problems in partial differential equations. Rank and related concepts are developed in the early chapters.
 Mac Lane, S.; Birkhoff, G. (1999), Algebra, AMS Chelsea, ISBN 0821816462
 Chapter XVI sections 6–10 give a more elementary account of the exterior algebra, including duality, determinants and minors, and alternating forms.
 Sternberg, Shlomo (1964), Lectures on Differential Geometry, Prentice Hall
 Contains a classical treatment of the exterior algebra as alternating tensors, and applications to differential geometry.
Historical references
 Bourbaki (1989, Historical note on chapters II and III)
 Clifford, W. (1878), "Applications of Grassmann's Extensive Algebra", American Journal of Mathematics, The Johns Hopkins University Press, 1 (4): 350–358, doi:10.2307/2369379, JSTOR 2369379
 Forder, H.G. (1941), The Calculus of Extension, Internet Archive
 Grassmann, Hermann (1844), Die Lineale Ausdehnungslehre – Ein neuer Zweig der Mathematik (in German) (The Linear Extension Theory – A new Branch of Mathematics) alternative reference
 Kannenberg, Lloyd (2000), Extension Theory (translation of Grassmann's Ausdehnungslehre), American Mathematical Society, ISBN 0821820311
 Peano, Giuseppe (1888), Calcolo Geometrico secondo l'Ausdehnungslehre di H. Grassmann preceduto dalle Operazioni della Logica Deduttiva; Kannenberg, Lloyd (1999), Geometric calculus: According to the Ausdehnungslehre of H. Grassmann, Birkhäuser, ISBN 9780817641269.
 Whitehead, Alfred North (1898), A Treatise on Universal Algebra, with Applications, Cambridge
Other references and further reading
 Browne, J.M. (2007), Grassmann algebra – Exploring applications of Extended Vector Algebra with Mathematica
 An introduction to the exterior algebra, and geometric algebra, with a focus on applications. Also includes a history section and bibliography.
 Spivak, Michael (1965), Calculus on manifolds, AddisonWesley, ISBN 9780805390216
 Includes applications of the exterior algebra to differential forms, specifically focused on integration and Stokes's theorem. The notation in this text is used to mean the space of alternating kforms on V; i.e., for Spivak is what this article would call Spivak discusses this in Addendum 4.
 Strang, G. (1993), Introduction to linear algebra, WellesleyCambridge Press, ISBN 9780961408855
 Includes an elementary treatment of the axiomatization of determinants as signed areas, volumes, and higherdimensional volumes.
 Onishchik, A.L. (2001) [1994], "Exterior algebra", Encyclopedia of Mathematics, EMS Press
 Wendell, Fleming (2012) [1977], "7. Exterior algebra and differential calculus", Functions of Several Variables (2nd ed.), Springer, pp. 275–320, ISBN 9781468494617
 This textbook in multivariate calculus introduces the exterior algebra of differential forms adroitly into the calculus sequence for colleges.
 Winitzki, S. (2010), Linear Algebra via Exterior Products
 An introduction to the coordinatefree approach in basic finitedimensional linear algebra, using exterior products.
 Shafarevich, I.R.; Remizov, A.O. (2012). Linear Algebra and Geometry. Springer. ISBN 9783642309939.
 Chapter 10: The Exterior Product and Exterior Algebras
 "The Grassmann method in projective geometry" A compilation of English translations of three notes by Cesare BuraliForti on the application of exterior algebra to projective geometry
 C. BuraliForti, "Introduction to Differential Geometry, following the method of H. Grassmann" An English translation of an early book on the geometric applications of exterior algebras
 "Mechanics, according to the principles of the theory of extension" An English translation of one Grassmann's papers on the applications of exterior algebra