Theorem 1 -- the strict one-half lower bound
Statement
Let n≥1 and let z1,…,zn∈C satisfy z1=1. For
j≥1, set
Sj=t=1∑nztj.
Then
1≤j≤nmax∣Sj∣>21.(1)
Consequently the question in Problem 519 has an
affirmative answer with the absolute constant c=1/2.
Newton--Girard interface
We use the following standard algebraic identity. If
P(x)=t=1∏m(x−rt)=xm+c1xm−1+⋯+cm
and pj=∑t=1mrtj, then
pk+c1pk−1+⋯+ck−1p1+kck=0(1≤k≤m),(2)
while
pk+c1pk−1+⋯+cmpk−m=0(k>m).(3)
Equations (2)--(3), with their displayed sign convention, are the complete
external Newton--Girard input used below.
If n=1, then S1=1 and (1) is immediate. Assume henceforth that
n≥2, and write
t=2∏n(x−zt)=xn−1+b1xn−2+⋯+bn−1.
Put
Tj=t=2∑nztj=Sj−1.
Applying (2) with m=n−1 gives, for 1≤k≤n−1,
Tk+b1Tk−1+⋯+bk−1T1+kbk=0.
After substituting Tj=Sj−1 and collecting constants, this becomes
Sk+b1Sk−1+⋯+bk−1S1=1+b1+⋯+bk−1−kbk.(4)
Applying (3) at k=n=m+1 gives
Tn+b1Tn−1+⋯+bn−1T1=0,
and therefore
Sn+b1Sn−1+⋯+bn−1S1=1+b1+⋯+bn−1.(5)
These are equations (1) and (2), respectively, in the source.
Proof of the bound
Fix 0<α<π/2, and set
A0=1,Ak=1+b1+⋯+bk,Wk=1+∣b1∣+⋯+∣bk∣.
For each 1≤k≤n−1, the
[[analysis/biro_1994_problem_turan_concerning_sums_powers_complex/lemma_1|geometric
dichotomy]] says that either
∣Ak−1−kbk∣≥sinα∣Ak−1∣,(6)
or
∣Ak∣≥∣Ak−1∣+cosα∣bk∣.(7)
Let
M=1≤j≤nmax∣Sj∣.
There are two cases.
Case 1: growth persists
Suppose (7) holds for every k=1,…,n−1. The iterated part of the
geometric lemma gives
∣An−1∣>cosαWn−1.(8)
On the other hand, (5) and the triangle inequality give
MWn−1≥∣Sn+b1Sn−1+⋯+bn−1S1∣=∣An−1∣.
Since Wn−1>0, comparison with (8) yields
M>cosα.(9)
Case 2: first failure of growth
Otherwise let k0 be the least index for which (7) fails. If k0>1,
then (7) held through k0−1, so the iterated estimate gives
∣Ak0−1∣>cosαWk0−1.
The same inequality also holds when k0=1, because then its two sides are
1 and cosα. Since (7) fails at k0, the dichotomy forces (6)
there. Using (4), followed by (6), gives
MWk0−1≥∣Sk0+b1Sk0−1+⋯+bk0−1S1∣=∣Ak0−1−k0bk0∣≥sinα∣Ak0−1∣>sinαcosαWk0−1.
Again Wk0−1>0, and hence
M>sinαcosα.(10)
Because 0<sinα<1, (9) also implies (10). Thus (10) holds in both
cases. Taking α=π/4 gives
M>sin4πcos4π=21,
which proves (1).
Source and dependency scope
The theorem and proof are on printed pp. 210--211, physical PDF pp. 224--225,
of the published volume scan.
The definition of Sj and Rn is on printed p. 209, physical p. 223.
Every local inequality in the proof, including the planar geometry, appears
here or on the linked lemma page. Only the standard Newton--Girard interface
(2)--(3) remains external. No assertion about the sharp constant or the
best presently known constant is part of this theorem.
Read depth. Claims checked: the statement, the definitions on p. 209
and equations (1)--(2) of the print were read clause by clause on the
printed pages. The proof above is the paper's argument restated here step
by step, with the case n=1 and the degenerate cases added; it is a
compilation, not an independent review.
The paper's
[[analysis/biro_1994_problem_turan_concerning_sums_powers_complex/theorem_2|Theorem
2]] (p. 212) refines (1) for n≥2 to
max1≤j≤n∣Sj∣>21+8n1+64n23, its case of
one prescribed 1.
Bears on. Problem 519; (1) proves its exact
existence statement with c=1/2.