Homogeneous polynomial

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In mathematics, a homogeneous polynomial, sometimes called quantic in older texts, is a polynomial whose nonzero terms all have the same degree.[1] For example, x5+2x3y2+9xy4 is a homogeneous polynomial of degree 5, in two variables; the sum of the exponents in each term is always 5. The polynomial x3+3x2y+z7 is not homogeneous, because the sum of exponents does not match from term to term. The function defined by a homogeneous polynomial is always a homogeneous function. An algebraic form, or simply form, is a function defined by a homogeneous polynomial.[notes 1] A binary form is a form in two variables. A form is also a function defined on a vector space, which may be expressed as a homogeneous function of the coordinates over any basis. A polynomial of degree 0 is always homogeneous; it is simply an element of the field or ring of the coefficients, usually called a constant or a scalar. A form of degree 1 is a linear form.[notes 2] A form of degree 2 is a quadratic form. In geometry, the Euclidean distance is the square root of a quadratic form. Homogeneous polynomials are ubiquitous in mathematics and physics.[notes 3] They play a fundamental role in algebraic geometry, as a projective algebraic variety is defined as the set of the common zeros of a set of homogeneous polynomials.

Properties

A homogeneous polynomial defines a homogeneous function. This means that, if a multivariate polynomial P is homogeneous of degree d, then

P(λx1,,λxn)=λdP(x1,,xn),

for every λ in any field containing the coefficients of P. Conversely, if the above relation is true for infinitely many λ then the polynomial is homogeneous of degree d. In particular, if P is homogeneous then

P(x1,,xn)=0P(λx1,,λxn)=0,

for every λ. This property is fundamental in the definition of a projective variety. Any nonzero polynomial may be decomposed, in a unique way, as a sum of homogeneous polynomials of different degrees, which are called the homogeneous components of the polynomial. Given a polynomial ring R=K[x1,,xn] over a field (or, more generally, a ring) K, the homogeneous polynomials of degree d form a vector space (or a module), commonly denoted Rd. The above unique decomposition means that R is the direct sum of the Rd (sum over all nonnegative integers). The dimension of the vector space (or free module) Rd is the number of different monomials of degree d in n variables (that is the maximal number of nonzero terms in a homogeneous polynomial of degree d in n variables). It is equal to the binomial coefficient

(d+n1n1)=(d+n1d)=(d+n1)!d!(n1)!.

Homogeneous polynomial satisfy Euler's identity for homogeneous functions. That is, if P is a homogeneous polynomial of degree d in the indeterminates x1,,xn, one has, whichever is the commutative ring of the coefficients,

dP=i=1nxiPxi,

where Pxi denotes the formal partial derivative of P with respect to xi.

Homogenization

A non-homogeneous polynomial P(x1,...,xn) can be homogenized by introducing an additional variable x0 and defining the homogeneous polynomial sometimes denoted hP:[2]

hP(x0,x1,,xn)=x0dP(x1x0,,xnx0),

where d is the degree of P. For example, if

P(x1,x2,x3)=x33+x1x2+7,

then

hP(x0,x1,x2,x3)=x33+x0x1x2+7x03.

A homogenized polynomial can be dehomogenized by setting the additional variable x0 = 1. That is

P(x1,,xn)=hP(1,x1,,xn).

See also

Notes

  1. However, as some authors do not make a clear distinction between a polynomial and its associated function, the terms homogeneous polynomial and form are sometimes considered as synonymous.
  2. Linear forms are defined only for finite-dimensional vector space, and have thus to be distinguished from linear functionals, which are defined for every vector space. "Linear functional" is rarely used for finite-dimensional vector spaces.
  3. Homogeneous polynomials in physics often appear as a consequence of dimensional analysis, where measured quantities must match in real-world problems.

References

  1. Cox, David A.; Little, John; O'Shea, Donal (2005). Using Algebraic Geometry. Graduate Texts in Mathematics. Vol. 185 (2nd ed.). Springer. p. 2. ISBN 978-0-387-20733-9.
  2. Cox, Little & O'Shea 2005, p. 35

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