Multilinear map

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Short description: Vector-valued function of multiple vectors, linear in each argument

In linear algebra, a multilinear map is a function of several variables that is linear separately in each variable. More precisely, a multilinear map is a function

f:V1×⋯×Vn→W,

where V1,…,Vn (n∈ℤ≥0) and W are vector spaces (or modules over a commutative ring), with the following property: for each i, if all of the variables but vi are held constant, then f(v1,…,vi,…,vn) is a linear function of vi.[1] One way to visualize this is to imagine two orthogonal vectors; if one of these vectors is scaled by a factor of 2 while the other remains unchanged, the cross product likewise scales by a factor of two. If both are scaled by a factor of 2, the cross product scales by a factor of 22.

A multilinear map of one variable is a linear map, and of two variables is a bilinear map. More generally, for any nonnegative integer k, a multilinear map of k variables is called a k-linear map. If the codomain of a multilinear map is the field of scalars, it is called a multilinear form. Multilinear maps and multilinear forms are fundamental objects of study in multilinear algebra.

If all variables belong to the same space, one can consider symmetric, antisymmetric and alternating k-linear maps. The latter two coincide if the underlying ring (or field) has a characteristic different from two, else the former two coincide.

Examples

Coordinate representation

Let

f:V1×⋯×Vn→W,

be a multilinear map between finite-dimensional vector spaces, where Vi has dimension di, and W has dimension d. If we choose a basis {ei1,…,eidi} for each Vi and a basis {b1,…,bd} for W (using bold for vectors), then we can define a collection of scalars Aj1⋯jnk by

f(e1j1,…,enjn)=Aj1⋯jn1b1+⋯+Aj1⋯jndbd.

Then the scalars {Aj1⋯jnk∣1≤ji≤di,1≤k≤d} completely determine the multilinear function f. In particular, if

vi=∑j=1divijeij

for 1≤i≤n, then

f(v1,…,vn)=∑j1=1d1⋯∑jn=1dn∑k=1dAj1⋯jnkv1j1⋯vnjnbk.

Example

Let's take a trilinear function

g:R2×R2×R2→R, where Vi = R2, di = 2, i = 1,2,3, and W = R, d = 1.

A basis for each Vi is {ei1,…,eidi}={e1,e2}={(1,0),(0,1)}. Let

g(e1i,e2j,e3k)=f(ei,ej,ek)=Aijk, where i,j,k∈{1,2}. In other words, the constant Aijk is a function value at one of the eight possible triples of basis vectors (since there are two choices for each of the three Vi), namely: {e1,e1,e1},{e1,e1,e2},{e1,e2,e1},{e1,e2,e2},{e2,e1,e1},{e2,e1,e2},{e2,e2,e1},{e2,e2,e2}.

Each vector vi∈Vi=R2 can be expressed as a linear combination of the basis vectors

vi=∑j=12vijeij=vi1×e1+vi2×e2=vi1×(1,0)+vi2×(0,1).

The function value at an arbitrary collection of three vectors vi∈R2 can be expressed as g(v1,v2,v3)=∑i=12∑j=12∑k=12Aijkv1iv2jv3k, or in expanded form as g((a,b),(c,d),(e,f))=ace×g(e1,e1,e1)+acf×g(e1,e1,e2)+ade×g(e1,e2,e1)+adf×g(e1,e2,e2)+bce×g(e2,e1,e1)+bcf×g(e2,e1,e2)+bde×g(e2,e2,e1)+bdf×g(e2,e2,e2).

Relation to tensor products

There is a natural one-to-one correspondence between multilinear maps

f:V1×⋯×Vn→W,

and linear maps

F:V1⊗⋯⊗Vn→W,

where V1⊗⋯⊗Vn denotes the tensor product of V1,…,Vn. The relation between the functions f and F is given by the formula

f(v1,…,vn)=F(v1⊗⋯⊗vn).

Multilinear functions on n×n matrices

One can consider multilinear functions, on an n×n matrix over a commutative ring K with identity, as a function of the rows (or equivalently the columns) of the matrix. Let A be such a matrix and ai, 1 ≤ i ≤ n, be the rows of A. Then the multilinear function D can be written as

D(A)=D(a1,…,an),

satisfying

D(a1,…,cai+ai′,…,an)=cD(a1,…,ai,…,an)+D(a1,…,ai′,…,an).

If we let e^j represent the jth row of the identity matrix, we can express each row ai as the sum

ai=∑j=1nA(i,j)e^j.

Using the multilinearity of D we rewrite D(A) as

D(A)=D(∑j=1nA(1,j)e^j,a2,…,an)=∑j=1nA(1,j)D(e^j,a2,…,an).

Continuing this substitution for each ai we get, for 1 ≤ i ≤ n,

D(A)=∑1≤k1≤n…∑1≤ki≤n…∑1≤kn≤nA(1,k1)A(2,k2)…A(n,kn)D(e^k1,…,e^kn).

Therefore, D(A) is uniquely determined by how D operates on e^k1,…,e^kn.

Example

In the case of 2×2 matrices, we get

D(A)=A1,1A1,2D(e^1,e^1)+A1,1A2,2D(e^1,e^2)+A1,2A2,1D(e^2,e^1)+A1,2A2,2D(e^2,e^2),

where e^1=[1,0] and e^2=[0,1]. If we restrict D to be an alternating function, then D(e^1,e^1)=D(e^2,e^2)=0 and D(e^2,e^1)=−D(e^1,e^2)=−D(I). Letting D(I)=1, we get the determinant function on 2×2 matrices:

D(A)=A1,1A2,2−A1,2A2,1.

Properties

  • A multilinear map has a value of zero whenever one of its arguments is zero.

See also

References

  1. ↑ Lang, Serge (2005). "XIII. Matrices and Linear Maps §S Determinants". Algebra. Graduate Texts in Mathematics. 211 (3rd ed.). Springer. pp. 511–. ISBN 978-0-387-95385-4. https://books.google.com/books?id=Fge-BwqhqIYC&pg=PA511.