Complete homogeneous symmetric polynomial
In mathematics, specifically in algebraic combinatorics and commutative algebra, the complete homogeneous symmetric polynomials are a specific kind of symmetric polynomials. Every symmetric polynomial can be expressed as a polynomial expression in complete homogeneous symmetric polynomials. Definition
The complete homogeneous symmetric polynomial of degree  in  variables , written  for , is the sum of all monomials of total degree  in the variables. Formally,

The formula can also be written as:

Indeed,  is just the multiplicity of  in the sequence . The first few of these polynomials are

Thus, for each nonnegative integer , there exists exactly one complete homogeneous symmetric polynomial of degree  in  variables. Another way of rewriting the definition is to take summation over all sequences , without condition of ordering :

here  is the multiplicity of number  in the sequence . For example

The polynomial ring formed by taking all integral linear combinations of products of the complete homogeneous symmetric polynomials is a commutative ring. Examples
The following lists the  basic (as explained below) complete homogeneous symmetric polynomials for the first three positive values of . For :

For :

For :

Properties

Generating function
The complete homogeneous symmetric polynomials are characterized by the following identity of formal power series in :

(this is called the generating function, or generating series, for the complete homogeneous symmetric polynomials). Here each fraction in the final expression is the usual way to represent the formal geometric series that is a factor in the middle expression. The identity can be justified by considering how the product of those geometric series is formed: each factor in the product is obtained by multiplying together one term chosen from each geometric series, and every monomial in the variables  is obtained for exactly one such choice of terms, and comes multiplied by a power of  equal to the degree of the monomial. The formula above can be seen as a special case of the MacMahon master theorem. The right hand side can be interpreted as  where  and . On the left hand side, one can identify the complete homogeneous symmetric polynomials as special cases of the multinomial coefficient that appears in the MacMahon expression. Performing some standard computations, we can also write the generating function as which is the power series expansion of the plethystic exponential of  (and note that  is precisely the j-th power sum symmetric polynomial). Relation with the elementary symmetric polynomials

There is a fundamental relation between the elementary symmetric polynomials and the complete homogeneous ones:

which is valid for all , and any number of variables . The easiest way to see that it holds is from an identity of formal power series in  for the elementary symmetric polynomials, analogous to the one given above for the complete homogeneous ones, which can also be written in terms of plethystic exponentials as:

(this is actually an identity of polynomials in , because after  the elementary symmetric polynomials become zero). Multiplying this by the generating function for the complete homogeneous symmetric polynomials, one obtains the constant series 1 (equivalently, plethystic exponentials satisfy the usual properties of an exponential), and the relation between the elementary and complete homogeneous polynomials follows from comparing coefficients of . A somewhat more direct way to understand that relation is to consider the contributions in the summation involving a fixed monomial  of degree . For any subset  of the variables appearing with nonzero exponent in the monomial, there is a contribution involving the product  of those variables as term from , where , and the monomial  from ; this contribution has coefficient . The relation then follows from the fact that

by the binomial formula, where  denotes the number of distinct variables occurring (with nonzero exponent) in . Since  and  are both equal to 1, one can isolate from the relation either the first or the last terms of the summation. The former gives a sequence of equations:

and so on, that allows to recursively express the successive complete homogeneous symmetric polynomials in terms of the elementary symmetric polynomials; the latter gives a set of equations

and so forth, that allows doing the inverse. The first  elementary and complete homogeneous symmetric polynomials play perfectly similar roles in these relations, even though the former polynomials then become zero, whereas the latter do not. This phenomenon can be understood in the setting of the ring of symmetric functions. It has a ring automorphism that interchanges the sequences of the  elementary and first  complete homogeneous symmetric functions. The set of complete homogeneous symmetric polynomials of degree 1 to  in  variables generates the ring of symmetric polynomials in  variables. More specifically, the ring of symmetric polynomials with integer coefficients equals the integral polynomial ring 

This can be formulated by saying that 

form a transcendence basis of the ring of symmetric polynomials in  with integral coefficients (as is also true for the elementary symmetric polynomials). The same is true with the ring  of integers replaced by any other commutative ring. These statements follow from analogous statements for the elementary symmetric polynomials, due to the indicated possibility of expressing either kind of symmetric polynomials in terms of the other kind. Relation with the Stirling numbers

The evaluation at integers of complete homogeneous polynomials and elementary symmetric polynomials is related to Stirling numbers:

Relation with the monomial symmetric polynomials

The polynomial  is also the sum of all distinct monomial symmetric polynomials of degree  in , for instance

Relation with power sums

Newton's identities for homogeneous symmetric polynomials give the simple recursive formula

where  and pk is the k-th power sum symmetric polynomial:  , as above. For small  we have

Relation with symmetric tensors

Consider an -dimensional vector space  and a linear operator  with eigenvalues . Denote by  its th symmetric tensor power and  the induced operator . Proposition:

The proof is easy: consider an eigenbasis  for . The basis in  can be indexed by sequences , indeed, consider the symmetrizations of 
. All such vectors are eigenvectors for  with eigenvalues 
 
hence this proposition is true. Similarly one can express elementary symmetric polynomials via traces over antisymmetric tensor powers. Both expressions are subsumed in expressions of Schur polynomials as traces over Schur functors, which can be seen as the Weyl character formula for . Complete homogeneous symmetric polynomial with variables shifted by 1

If we replace the variables  for , 
the symmetric polynomial 

can be written as a linear combination of
the , 
for ,

The proof, as found in Lemma 3.5 of, relies on the combinatorial properties of increasing -tuples  where . See also
Symmetric polynomial
Elementary symmetric polynomial
Schur polynomial
Newton's identities
MacMahon Master theorem
Symmetric function
Representation theory

References

 Macdonald, I.G. (1979), Symmetric Functions and Hall Polynomials. Oxford Mathematical Monographs. Oxford: Clarendon Press. Macdonald, I.G. (1995), Symmetric Functions and Hall Polynomials, second ed. Oxford: Clarendon Press. (paperback, 1998). Richard P. Stanley (1999), Enumerative Combinatorics, Vol. 2. Cambridge: Cambridge University Press. Homogeneous polynomials
Symmetric functions