elementary symmetric polynomial in terms of power sums


Elementary symmetric polynomials can be expressed as polynomialsMathworldPlanetmathPlanetmathPlanetmath in sums of powers. For instance, one can use the binomial identity (x+y)2=x2+y2+2xy to re-express the elementary symmetric polynomial of power 2 in 2 variables:

x1x2=12(k=12xi)2-12k=12(xi)2

Similarly, one has the following identitiesPlanetmathPlanetmathPlanetmath:

1i<jnxixj=12(k=1nxk)2-12k=1n(xi)2
1i<j<knxixjxk=16(k=1nxk)3-12(k=1nxk2)(k=1nxk)+13k=1nxk3

Note that the algebraic form of these expressions does not depend on n, the number of variables; this is true in general. In fact, it is possible to take n to infinity and obtain an identity for infinite series under suitable circumstances, but that lies beyond the scope of the current entry.

These formulae can be derived using the Newton-Girard recursion relations. Moreover, these recursions can be used to provide an inductive proof that any elementary symmetric polynomial can be expressed in terms of sums of powers. It might also be worth pointing out that Waring’s formula allows one to do the opposite — express sums of powers in terms of symmetric polynomialsMathworldPlanetmath.

Whilst these recursions may be used to derive these formulae, they can be tedious to use; for deriving a particular such relation, it may be easier to determine coefficients by substituting particular values for the variables and solving linear equations, as will be demonstrated with an example. Suppose that we want to express the elementary symmetric polynomial of power 5,

1a<b<c<d<enxaxbxcxdxe

in terms of power sums. Since this is of the fifth order, we shall only require sums of powers less than or equal to 5. Furthermore, we shall only have terms of the fifth order in the expression, so we only need to consider products of these five power sums whose total orderMathworldPlanetmath is five. To determine these possible sums, we consider the possible partitionsMathworldPlanetmath of the number 5:

5,4+1,3+2,3+1+1,2+2+1,2+1+1+1,1+1+1+1+1

Corresponding to these partitions, we have the following ansatz:

1a<b<c<d<enxaxbxcxdxe = c5k=1nxk5+c41(k=1nxk4)(k=1nxk)+c32(k=1nxk3)(k=1nxk2)
+ c311(k=1nxk3)(k=1nxk)2+c221(k=1nxk2)2(k=1nxk)
+ c2111(k=1nxk2)(k=1nxk)3+c11111(k=1nxk)5

Now it remains to determine the c’s. This can be done by substituting particular values for the x’s to obtain 7 equations for the 7 coefficients. By choosing these values strategically, the equations can be made relatively simple so as to reduce the work of solving them. One possibility is the following:

1.n = 1  x1=1:
0 = c5+c41+c32+c311+c221+c2111+c11111
2.n = 2  x1=1x2=1:
0 = 2c5+4c41+4c32+8c311+8c221+16c2111+32c11111
3.n = 3  x1=1x2=1x3=1:
0 = 3c5+9c41+9c32+27c311+27c221+81c2111+243c11111
4.n = 3  x1=1x2=1x3=-1:
0 = c5+3c41+3c32+c311+9c221+3c2111+c11111
5.n = 3  x1=2x2=-1x3=-1:
0 = 5c5+6c32
6.n = 4  x1=1x2=1x3=1x4=1:
0 = 4c5+16c41+16c32+64c311+64c221+256c2111+1024c11111
7.n = 5  x1=1x2=1x3=1x4=1x5=1:
1 = 5c5+25c41+25c32+125c311+125c221+625c2111+3125c11111

By combining equations 1,2,3,6, the following sparse system may be derived:

c5 = 24c11111
c41+c32 = -50c11111
c311+c221 = 35c11111
c2111 = -10c11111

Likewise, subtracting equation 1 from equation 4 yields

c41+c32+4c221+c2111=0

Combining these equations with the already sparse eqnation 5 yeilds the following equations which express everyting else in terms of c11111:

c5 = 24c11111
c41 = -70c11111
c32 = 20c11111
c311 = 5c11111
c221 = 30c11111
c2111 = -10c11111

Substituting this into equation 7, we learn that c11111=1/120, from which the values of the remaining coefficients follow immediately:

c5 = 15
c41 = -712
c32 = 16
c311 = 124
c221 = 14
c2111 = -112

Hence the desired formula is the following:

1a<b<c<d<enxaxbxcxdxe = 15k=1nxk5-712(k=1nxk4)(k=1nxk)+16(k=1nxk3)(k=1nxk2)
+ 124(k=1nxk3)(k=1nxk)2+14(k=1nxk2)2(k=1nxk)
- 112(k=1nxk2)(k=1nxk)3+1120(k=1nxk)5
Title elementary symmetric polynomial in terms of power sums
Canonical name ElementarySymmetricPolynomialInTermsOfPowerSums
Date of creation 2013-03-22 15:57:11
Last modified on 2013-03-22 15:57:11
Owner rspuzio (6075)
Last modified by rspuzio (6075)
Numerical id 9
Author rspuzio (6075)
Entry type Result
Classification msc 05E05
Related topic NewtonGirardFormulaSymmetricPolynomials