A multiplication matrix of an element in a finite-dimensional associative commutative algebra
with multiplicative
identity over a field
is the matrix, in a chosen vector
basis, of the
-linear transformation
|
(1)
|
Changing the vector basis replaces by a similar matrix.
For elements
,
the matrices satisfy
|
(2)
|
For polynomial equations, let , where
is a zero-dimensional
ideal. Choose polynomial representatives
, ...,
of a vector basis of this
quotient ring. The
th column of
is determined by
|
(3)
|
A Gröbner basis computes these expressions by polynomial division when the are the monomials not divisible
by any of its leading monomials (Sturmfels 2002,
p. 17).
When ,
let
be the finite set of common zeros of
. For
, the evaluation vector
satisfies
|
(4)
|
Thus the eigenvalues of are the values
. More precisely, its characteristic
polynomial is
|
(5)
|
where
is the identity matrix and
is the dimension over
of the localization
of
at the maximal ideal corresponding to
(Cox 2021). Common left eigenvectors
of
,
...,
give consistent coordinate tuples. Separate lists of eigenvalues
do not in general determine which coordinates belong to the same solution. If
, where
is the ideal radical,
these matrices can be diagonalized in a common vector
basis (Sturmfels 2002, pp. 17-18). This gives an eigenvalue
method for solving finite systems of polynomial
equations (Auzinger and Stetter 1988, Trott 2006).
In one variable, multiplication by on
, for a monic
polynomial
of polynomial degree
, gives the standard companion
matrix in the vector basis
,
, ...,
.