MHB Symmetric Polynomials s1,s2,s3

Click For Summary
SUMMARY

The discussion focuses on expressing the sum of squares of variables, specifically r12 + r22 + ... + rn2, as a polynomial in the elementary symmetric polynomials s1, s2, and s3. The key conclusion is that this expression can be simplified to s12 - 2s2, where s1 is the sum of the variables, s2 is the sum of the products of the variables taken two at a time, and s3 is the product of all variables. The derivation involves recognizing the relationship between the squared sum and the symmetric polynomials.

PREREQUISITES
  • Understanding of elementary symmetric polynomials
  • Familiarity with polynomial algebra
  • Knowledge of combinatorial notation for sums
  • Basic concepts of symmetric functions
NEXT STEPS
  • Study the properties of symmetric polynomials in algebra
  • Learn about polynomial rings and their applications
  • Explore the theory of symmetric functions and their combinatorial interpretations
  • Investigate advanced topics in algebra related to symmetric groups
USEFUL FOR

Mathematicians, algebra students, and anyone interested in the theory of symmetric polynomials and their applications in combinatorics and algebraic structures.

mathjam0990
Messages
28
Reaction score
0
Express r12+r22+...+rn2 as a polynomial in the elementary symmetric polynomials s1, s2, . . . ,sn.

I'm sure the equation we are dealing with is (r1+r2+...+rn)2 which is very large to factor out but should yield r12+r22+...+rn2+(other terms)

I believe s1=r1+r2+...+rn

s2=Σri1ri2 for 1≤i1≤i2≤n

s3=r1r2⋅⋅⋅⋅⋅⋅rn

So the answer should be r12+r22+...+rn2 = s12 - (something with s2,...sn) Sorry I am not sure what to employ here to break this all the way down.

If there is anyone who could provide an explanation, that would be amazing. Thank you!
 
Physics news on Phys.org
mathjam0990 said:
Express r12+r22+...+rn2 as a polynomial in the elementary symmetric polynomials s1, s2, . . . ,sn.

I'm sure the equation we are dealing with is (r1+r2+...+rn)2 which is very large to factor out but should yield r12+r22+...+rn2+(other terms)

I believe s1=r1+r2+...+rn

s2=Σri1ri2 for 1≤i1≤i2≤n

s3=r1r2⋅⋅⋅⋅⋅⋅rn

So the answer should be r12+r22+...+rn2 = s12 - (something with s2,...sn) Sorry I am not sure what to employ here to break this all the way down.

If there is anyone who could provide an explanation, that would be amazing. Thank you!
.

now $s_1 = r_1 + r_2 + r_3 + r_ 4 ...\cdots r_n$
because we need to evaluate $r_1^2 + r_2^2 + ..\cdots + r_n^2$ I am tempted to sqaure $S_1$ which shall give
square terms and additional ones

As we get $s_1^2 = r_1^2 + r_2^2 + r_3^2 + r_ 4 ...\cdots r_n^2 + r_1 r_2 + r_1 r_3 + ...$
$= r_1^2 + r_2^2 + r_3^2 + r_ 4 ...\cdots r_n^2 + 2 \sum_{p=1}^{m-1} \sum_{m=1}^{n} r_p r_m$ (one comes from $r_p r_m$ and another from $r_m r_p$ for $p \ne m$
$= r_1^2 + r_2^2 + r_3^2 + r_ 4 ...\cdots r_n^2 + 2 s_2$

hence given sum = $s_1^2 - 2s_2$
 
mathjam0990 said:
Express r12+r22+...+rn2 as a polynomial in the elementary symmetric polynomials s1, s2, . . . ,sn.

I'm sure the equation we are dealing with is (r1+r2+...+rn)2 which is very large to factor out but should yield r12+r22+...+rn2+(other terms)

I believe s1=r1+r2+...+rn

s2=Σri1ri2 for 1≤i1≤i2≤n

s3=r1r2⋅⋅⋅⋅⋅⋅rn

So the answer should be r12+r22+...+rn2 = s12 - (something with s2,...sn) Sorry I am not sure what to employ here to break this all the way down.

If there is anyone who could provide an explanation, that would be amazing. Thank you!

It's easier to illustrate what the $s_i$ are with a particular $n$. Let's use $n = 4$. Suppose our variables are $r_1,r_2,r_3,r_4$. Then our polynomials are in the polynomial ring:

$F[r_1,r_2,r_3,r_4]$ (where $F$ is our underlying field).

Given $f \in F[r_1,r_2,r_3,r_4]$, we can have $\sigma \in S_4$ operate on $F[r_1,r_2,r_3,r_4]$ by:

$\sigma(f(r_1,r_2,r_3,r_4)) = f(r_{\sigma(1)},r_{\sigma(2)},r_{\sigma(3)},r_{\sigma(4)})$.

We say a polynomial $f \in F[r_1,r_2,r_3,r_4]$ is *symmetric* if $\sigma(f) = f$.

The ELEMENTARY symmetric polynomials are the "basic" symmetric polynomials of any given degree > 0. Let's see how they are constructed, for $n = 4$, by seeing what they ought to be (note we don't care about constant terms, since $\sigma$ never affects them, so for simplicity's sake, we'll always assume all constant terms are 0).

For degree $1$, our polynomials are just linear combinations of the $r_i$. So the "simplest" symmetric combination would be:

$s_1 = r_1 + r_2 + r_3 + r_4$.

This can't be improved on, eliminating any term would break the symmetry.

for degree $2$, our polynomials would be linear combinations of $r_ir_j$ ($i = j$ might happen) + terms of lower degree. since we can capture symmetric terms of lower degree by the polynomial above, we will only look at symmetric combinations of $r_ir_j$.

At first, it might seem the best candidate would be:

$f = r_1^2 + r_1r_2 + r_1r_3 + r_1r_4 + r_2^2 + r_2r_3 + r_2r_4 + r_3^2 + r_3r_4 + r_4^2$ (all possible degree 2 terms summed).

However, note that:

$s_1^2 = (r_1 + r_2 + r_3 + r_4)^2 =$

$ r_1^2 + r_1r_2 + r_1r_3 + r_1r_4 + r_2r_1 + r_2^2 + r_2r_3 + r_2r_4 + r_3r_1 + r_3r_2r_3^2 + r_4r_1 + r_4r_2 + r_4r_3 + r_4^2$

$= r_1^2 + r_2^2 + r_3^2 + r_4^2 + 2(r_1r_2 + r_1r_3 + r_1r_4 + r_2r_3 + r_2r_4 + r_3r_4)$

If we call the "cross-terms" $2g$, we have:

$f = s_1^2 - 2g + g$ where the $s_1^2 - 2g$ gives us just the degree 2 terms in $f$ that are squares.

Thus all we need to get $f$ is $s_1$ and $g$ (both of these are still symmetric) and $g$ is "more minimal" than $f$ (fewer terms). So we should pick $g$ as $s_2$:

$s_2 = r_1r_2 + r_1r_3 + r_1r_4 + r_2r_3 + r_2r_4 + r_3r_4$

The same sort of logic applies to the higher terms (but the algebra is horrendous), so:

$s_3 = r_1r_2r_3 + r_1r_2r_4 + r_1r_3r_4 + r_2r_3r_4$

(Do you see the pattern? We pick $s_k = \sum\limits_{i_1 < i_2 < \cdots < i_k} r_{i_1}r_{i_2}\cdots r_{i_k}$)

and finally $s_4 = r_1r_2r_3r_4$.
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

Similar threads

  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 2 ·
Replies
2
Views
4K