Power-sum relation for arbitrary homogeneous symmetric polynomials

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Let xm={x1,…,xm}{\bf x}^m=\{x_1,\ldots,x_m\} and ym={y1,…,ym}{\bf y}^m=\{y_1,\ldots,y_m\}. For an arbitrary homogeneous symmetric polynomial Sn(xm)S_n({\bf x}^m) of degree nn, write

Sn(xm)=∑kCn,kPn,k(xm),Pn,k(xm)=∏l=1npl(xm)kl,S_n({\bf x}^m)=\sum_{\bf k}C_{n,\bf k}P_{n,\bf k}({\bf x}^m),\qquad P_{n,\bf k}({\bf x}^m)=\prod_{l=1}^n p_l({\bf x}^m)^{k_l},

where ∑i=1niki=n\sum_{i=1}^n i k_i=n, and let π(xm)=∏j=1mxj\pi({\bf x}^m)=\prod_{j=1}^m x_j. Define

Vn(xm)=Sn(xm)π(xm),Un(xm,ym)=Vn(xm)−∑i=1myim−k−1Vn(sim),V_n({\bf x}^m)=\frac{S_n({\bf x}^m)}{\pi({\bf x}^m)},\qquad U_n({\bf x}^m,{\bf y}^m)=V_n({\bf x}^m)-\sum_{i=1}^m y_i^{m-k-1}V_n({\bf s}_i^m),

where sim{\bf s}_i^m has entries si,jm=yixj−yjxi+xiδijs^m_{i,j}=y_i x_j-y_j x_i+x_i\delta_{ij}. Power-sum relation. The relation

Un(xm,ym)=0,U_n({\bf x}^m,{\bf y}^m)=0,

holds for 0≤n≤m−10\leq n\leq m-1. Moreover, at ym=1m{\bf y}^m={\bf 1}^m,

Un(xm,1m)=Yn−m(xm),n≥m,U_n({\bf x}^m,{\bf 1}^m)=Y_{n-m}({\bf x}^m),\qquad n\geq m,

where Yn−mY_{n-m} is homogeneous symmetric of degree n−mn-m and

Yn−m(xm)=∑kCn,kYn−m,k(xm).Y_{n-m}({\bf x}^m)=\sum_{\bf k}C_{n,\bf k}Y_{n-m,\bf k}({\bf x}^m).

This packages the proposed relations for arbitrary power-sum expansions; the source gives no resolution status.

References

Primary source

Boris Y. Rubinstein, “A New Class of Relations for Homogeneous Symmetric Polynomials”, arXiv:2510.25749 (2025).

Progress summary

Refreshed
Claimed solved

A 2025 paper claims the relation works for every homogeneous symmetric polynomial, and a later posted argument claims a complete proof, but neither has been independently verified.

Rubinstein's 2025 preprint claims that the relations previously obtained for Bernoulli symmetric polynomials remain valid for arbitrary homogeneous symmetric polynomials, including the power-sum formulation considered here.

October 2025 general-validity claim

Rubinstein states that the relations are valid in the arbitrary-polynomial setting and derives consequences for Bernoulli numbers. The retrieved record does not independently verify the exact displayed formulation or establish a published proof.

Posted attempt

A posted argument claims a complete proof after correcting the exponent from m−k−1m-k-1 to m−n−1m-n-1. It uses cancellation of residues at xi=0x_i=0 and Dij=0D_{ij}=0, then polynomiality, degree bounds, and symmetry; the attempt has not been independently verified.

Current status (as of August 2026): The general relation is claimed in Rubinstein's 2025 preprint and in a complete posted proof attempt, but independent verification is absent.

Sources

Solutions 1

ProofThis solution needs a summarySee full solutionHide full solution

In the primary source, equations (25) and (27) use the exponent m−n−1m-n-1; the displayed m−k−1m-k-1 contains an unbound kk and must be corrected accordingly.

Let SS be any symmetric homogeneous polynomial of degree nn in mm variables. Set

Dij=yixj−yjxi,(si)j={xi,j=i,Dij,j≠i,π(x)=∏ixi,D_{ij}=y_ix_j-y_jx_i, \qquad (s_i)_j= \begin{cases} x_i,&j=i,\\ D_{ij},&j\ne i, \end{cases} \qquad \pi(x)=\prod_i x_i,

and define

U=S(x)π(x)−∑iyim−n−1S(si)xi∏j≠iDij.U= \frac{S(x)}{\pi(x)} - \sum_i \frac{y_i^{m-n-1}S(s_i)} {x_i\prod_{j\ne i}D_{ij}}.

Over the coefficient field generated by the yiy_i, the only possible xx-poles are xix_i and DijD_{ij}. On xi=0x_i=0,

S(si)=yinS(x∣xi=0),∏j≠iDij=yim−1∏j≠ixj,S(s_i)=y_i^nS(x|_{x_i=0}), \qquad \prod_{j\ne i}D_{ij} =y_i^{m-1}\prod_{j\ne i}x_j,

so the residue of the ii-th summand cancels the residue of S(x)/π(x)S(x)/\pi(x).

On Dij=0D_{ij}=0, write c=yj/yic=y_j/y_i. Then

xj=cxi,Djr=cDir,sj=c τij(si),x_j=cx_i, \qquad D_{jr}=cD_{ir}, \qquad s_j=c\,\tau_{ij}(s_i),

and hence S(sj)=cnS(si)S(s_j)=c^nS(s_i). The two corresponding residues have ratio

−c(m−n−1)+n−(m−1)=−1,-c^{(m-n-1)+n-(m-1)}=-1,

so they cancel. Therefore UU is a polynomial in xx, homogeneous of degree n−mn-m. In particular,

U=0(n<m).U=0\qquad(n<m).

For n≥mn\ge m, put d=n−m+1d=n-m+1. Multiplication by π(y)d\pi(y)^d removes all explicit yy-denominators. With

H=π(x)∏i<jDij,C=(m2),H=\pi(x)\prod_{i<j}D_{ij}, \qquad C=\binom m2,

the residue cancellations show that the numerator over the common denominator HH is divisible by every pairwise nonassociated irreducible factor xi,Dijx_i,D_{ij}. Thus

R=π(y)dU∈Q[x1,…,xm,y1,…,ym],U=Rπ(y)d.R=\pi(y)^dU\in\mathbb Q[x_1,\ldots,x_m,y_1,\ldots,y_m], \qquad U=\frac{R}{\pi(y)^d}.

Moreover,

deg⁡xR=n−m.\deg_x R=n-m.

The first term of HRHR has yy-degree at most md+Cmd+C; each remaining term has degree at most

(m−1)d+n+C−(m−1)=md+C.(m-1)d+n+C-(m-1)=md+C.

Since HH is homogeneous of yy-degree CC, it follows that

deg⁡yR≤md=m(n−m+1).\deg_yR\le md=m(n-m+1).

Simultaneously permuting the pairs (xi,yi)(x_i,y_i) leaves UU, π(y)d\pi(y)^d, and therefore RR invariant. Specializing y1=⋯=ym=1y_1=\cdots=y_m=1 consequently gives a symmetric homogeneous polynomial

Yn−m(x)=R(x,1).Y_{n-m}(x)=R(x,\mathbf1).

Finally, linearity in SS gives the asserted decomposition

S=∑kCn,kPn,k⟹Yn−m=∑kCn,kYn−m,k.S=\sum_{\mathbf k}C_{n,\mathbf k}P_{n,\mathbf k} \quad\Longrightarrow\quad Y_{n-m} =\sum_{\mathbf k}C_{n,\mathbf k}Y_{n-m,\mathbf k}.

This proves all four source assertions, including the nonspecialized rational form, the degree bound, and simultaneous-permutation symmetry.