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Baltic Way 2017 · Problem 4

Algebra

A linear form in kk variables is an expression of the form P(x1,…,xk)=a1x1+…+akxkP\left(x_{1}, \ldots, x_{k}\right)=a_{1} x_{1}+\ldots+a_{k} x_{k} with real constants a1,…,aka_{1}, \ldots, a_{k}. Prove that there exist a positive integer nn and linear forms P1,…,PnP_{1}, \ldots, P_{n} in 2017 variables such that the equation

x1⋅x2⋅…⋅x2017=P1(x1,…,x2017)2017+…+Pn(x1,…,x2017)2017x_{1} \cdot x_{2} \cdot \ldots \cdot x_{2017}=P_{1}\left(x_{1}, \ldots, x_{2017}\right)^{2017}+\ldots+P_{n}\left(x_{1}, \ldots, x_{2017}\right)^{2017}

holds for all real numbers x1,…,x2017x_{1}, \ldots, x_{2017}.

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Topics

Sequences and recurrences · Equations and inequalities

Solutions

Solution 1

For every ε=(ε1,…,εn)∈{±1}2017\varepsilon=\left(\varepsilon_{1}, \ldots, \varepsilon_{n}\right) \in\{ \pm 1\}^{2017} let

Pε(X1,…,X2017)=ε1X1+⋯+ε2017X2017P_{\varepsilon}\left(X_{1}, \ldots, X_{2017}\right)=\varepsilon_{1} X_{1}+\cdots+\varepsilon_{2017} X_{2017}

and βε=ε1⋯ε2017\beta_{\varepsilon}=\varepsilon_{1} \cdots \varepsilon_{2017}. Consider

g(X1,…,Xk):=∑ε(βεPε(X1,…,X2017))2017=∑ε1,…,ε2017ε1⋯ε2017(ε1X1+⋯+ε2017X2017)2017\begin{aligned} g\left(X_{1}, \ldots, X_{k}\right) & :=\sum_{\varepsilon}\left(\beta_{\varepsilon} P_{\varepsilon}\left(X_{1}, \ldots, X_{2017}\right)\right)^{2017} \\ & =\sum_{\varepsilon_{1}, \ldots, \varepsilon_{2017}} \varepsilon_{1} \cdots \varepsilon_{2017}\left(\varepsilon_{1} X_{1}+\cdots+\varepsilon_{2017} X_{2017}\right)^{2017} \end{aligned}

If we choose X1=0X_{1}=0, then every combination (ε2X2+⋯+ε2017X2017)2017\left(\varepsilon_{2} X_{2}+\cdots+\varepsilon_{2017} X_{2017}\right)^{2017} occurs exactly twice and with opposite signs in the above sum. Hence, g(0,X2,…,X2017)≡0g\left(0, X_{2}, \ldots, X_{2017}\right) \equiv 0. The analogous statements are true for all other variables. Consequently, gg is divisible by X1…X2017X_{1} \ldots X_{2017}, and thereby of the form cX1…X2017c X_{1} \ldots X_{2017} for some real constant cc. If c≠0c \neq 0, then both sides can be divided by cc, and we obtain a representation with n=22017n=2^{2017} linear forms.

With X1=⋯=X2017=1X_{1}=\cdots=X_{2017}=1 we get

c=∑εε1⋅…⋅ε2017(ε1+…+ε2017)2017=∑ε∑k1,…,k2017k1+…+k2017=2017(2017k1,…,k2017)ε1k1+1⋅…⋅ε2017k2017+1\begin{aligned} c & =\sum_{\varepsilon} \varepsilon_{1} \cdot \ldots \cdot \varepsilon_{2017}\left(\varepsilon_{1}+\ldots+\varepsilon_{2017}\right)^{2017} \\ & =\sum_{\varepsilon} \sum_{\substack{k_{1}, \ldots, k_{2017} \\ k_{1}+\ldots+k_{2017}=2017}}\left(\begin{array}{c} 2017 \\ k_{1}, \ldots, k_{2017} \end{array}\right) \varepsilon_{1}^{k_{1}+1} \cdot \ldots \cdot \varepsilon_{2017}^{k_{2017}+1} \end{aligned}

The part of the sum with k1k_{1} even is zero since

∑k1 even,.,.,k k1+…+k2017=2017(2017k1,…,k2017)(∑ε,ε1=1ε2k2+1⋅…⋅ε2017k2017+1+∑ε,ε1=−1(−1)k1+1⋅…⋅ε2017k2017+1)=0\sum_{\substack{k_{1} \text { even,.,.,k } \\ k_{1}+\ldots+k_{2017}=2017}}\left(\begin{array}{c} 2017 \\ k_{1}, \ldots, k_{2017} \end{array}\right)\left(\sum_{\varepsilon, \varepsilon_{1}=1} \varepsilon_{2}^{k_{2}+1} \cdot \ldots \cdot \varepsilon_{2017}^{k_{2017}+1}+\sum_{\varepsilon, \varepsilon_{1}=-1}(-1)^{k_{1}+1} \cdot \ldots \cdot \varepsilon_{2017}^{k_{2017}+1}\right)=0

Now we may consider the part of the sum with k1k_{1} odd. Similarly the part of this new sum with k2k_{2} even equals 0 . Doing this for all the variables we get

c=∑ε=1∑k1 odd, ,…,k2017 odd k1+…+k2017=2017(2017k1,…,k2017)=22017(20171,…,1)=22017⋅2017!≠0c=\sum_{\varepsilon=1} \sum_{\substack{k_{1} \text { odd, }, \ldots, k_{2017} \text { odd } \\ k_{1}+\ldots+k_{2017}=2017}}\left(\begin{array}{c} 2017 \\ k_{1}, \ldots, k_{2017} \end{array}\right)=2^{2017}\left(\begin{array}{c} 2017 \\ 1, \ldots, 1 \end{array}\right)=2^{2017} \cdot 2017 ! \neq 0

forms.

Finally, we can even merge the two forms with opposite choices of the signs to obtain a representation with 220162^{2016} linear

Solution 2

We show by induction that for every integer k≥1k \geq 1 there exist an n=nkn=n_{k}, real numbers λ1,…,λnk\lambda_{1}, \ldots, \lambda_{n_{k}} and linear forms Pk,1,…,Pk,nkP_{k, 1}, \ldots, P_{k, n_{k}} in kk variables such that

x1…xk=λ1Pk,1(x1,…,xk)k+⋯+λnkPk,nk(x1,…,xk)k.x_{1} \ldots x_{k}=\lambda_{1} P_{k, 1}\left(x_{1}, \ldots, x_{k}\right)^{k}+\cdots+\lambda_{n_{k}} P_{k, n_{k}}\left(x_{1}, \ldots, x_{k}\right)^{k} .

For k=1k=1 we can choose n=n1=1n=n_{1}=1 and P1,1(x1)=x1P_{1,1}\left(x_{1}\right)=x_{1}. Now for the induction step, we observe that

x1…xky=λ1Pk,1(x1,…,xk)ky+⋯+λkPk,nk(x1,…,xk)kyx_{1} \ldots x_{k} y=\lambda_{1} P_{k, 1}\left(x_{1}, \ldots, x_{k}\right)^{k} y+\cdots+\lambda_{k} P_{k, n_{k}}\left(x_{1}, \ldots, x_{k}\right)^{k} y

Thus it suffices to write XkYX^{k} Y as a linear combination of (k+1)(k+1)-th powers of linear forms in XX and YY. The set-up

XkY=∑i=1mαi(X+βiY)k+1X^{k} Y=\sum_{i=1}^{m} \alpha_{i}\left(X+\beta_{i} Y\right)^{k+1}

leads to the equations ∑iαiβi=1k+1\sum_{i} \alpha_{i} \beta_{i}=\frac{1}{k+1} and ∑iαiβid=0\sum_{i} \alpha_{i} \beta_{i}^{d}=0 for d=0,2,3,…,k+1d=0,2,3, \ldots, k+1. Choosing m=k+2m=k+2 and distinct values for the βi\beta_{i} 's, this becomes a system of k+2k+2 linear equations in the k+2k+2 variables αi\alpha_{i}. If the system had no solution, then the lefthand sides of the equations would be linearly dependent. On the other hand, given cj,j=0,1,…,k+1c_{j}, j=0,1, \ldots, k+1 with ∑jcjβij=0\sum_{j} c_{j} \beta_{i}^{j}=0 for all ii, the polynomial P(x)=∑jcjxjP(x)=\sum_{j} c_{j} x^{j} has degree at most k+1k+1 and the k+2k+2 distinct zeros b1,…,bk+2b_{1}, \ldots, b_{k+2} and, hence, is the zero polynomial. Consequently, the system has a solution, and we can choose nk+1=(k+2)nkn_{k+1}=(k+2) n_{k} and the induction is complete.

The above gives us

x1…x2017=λ1P2017,1(x1,…,x2017)2017+⋯+λn2017P2017,n2017(x1,…,x2017)2017=(λ11/2017P2017,1(x1,…,x2017))2017+⋯+(λn20171/2017P2017,n2017(x1,…,x2017))2017,\begin{aligned} x_{1} \ldots x_{2017} & =\lambda_{1} P_{2017,1}\left(x_{1}, \ldots, x_{2017}\right)^{2017}+\cdots+\lambda_{n_{2017}} P_{2017, n_{2017}}\left(x_{1}, \ldots, x_{2017}\right)^{2017} \\ & =\left(\lambda_{1}^{1 / 2017} P_{2017,1}\left(x_{1}, \ldots, x_{2017}\right)\right)^{2017}+\cdots+\left(\lambda_{n_{2017}}^{1 / 2017} P_{2017, n_{2017}}\left(x_{1}, \ldots, x_{2017}\right)\right)^{2017}, \end{aligned}

as wanted.

Remark: Of course, the consistency of the system of linear equations also follows by the fact that the determinant of the coefficient matrix does not vanish as it is of Vandermonde's type.

Contest context

Results from Baltic Way 2017

11 teams

Mean score
1.1 / 5
Scores of 4 or 5
2 / 11
Estonia
0 / 5

Score distribution

08
10
20
31
41
51
All team scores
TeamScore
St. Petersburg4 / 5
Germany3 / 5
Poland5 / 5
Denmark0 / 5
Estonia0 / 5
Lithuania0 / 5
Sweden0 / 5
Norway0 / 5
Finland0 / 5
Iceland0 / 5
Latvia0 / 5