The difficult cofactor configuration can be restricted using the actual
column j. The following result is uniform in the row; it does not search
through finitely many rows.
Proposition. Suppose (n,8,j) is bad, put h=n−7, and choose maximal
small-prime positions with
(r2,r3,r5,r7)=(1,3,0,2).
Write Pp=pvp(n−rp) and up=(n−rp)/Pp. Assume
u2,u3,u5≥h3/10.(1)
There is no hypothesis on u7. If h≥10850001, then
Thus the low-residue Lucas branch cannot realize this cofactor region at
large height. The alternative in (2) remains possible; this proposition
does not make the whole index effective.
An exact column valuation identity
Here is a general lemma independent of badness. Let p be prime,
0≤r<p, r<j≤n, and write
n−r=pAu,A≥1,p∤u.
Then
pvp(jn)[j(j−1)⋯(j−r)]p≤n−r.(4)
To prove it, use
(j)r+1(jn)=(n)r+1(j−r−1n−r−1).
Exactly one numerator factor in (n)r+1 is divisible by p, so its
valuation is A. The bottom A base-p digits of
n−r−1=pAu−1 are all p−1. Kummer therefore gives
vp(j−r−1n−r−1)=vp(⌊(j−r−1)/pA⌋u−1)≤⌊logpu⌋.
For u=1 the middle valuation is zero, as required. Taking valuations in
the displayed binomial identity proves (4). The same bound holds with
j replaced by n−j whenever that column exceeds r.
In particular, if jmodpA≤r, the falling factorial on the left
contains a multiple of pA. Hence pvp(jn)≤u. For
Ep=pmin{A,vp(jn)},
this implies
Ep≤min(pA,u)≤n−r.(5)
Equation (4) also retains information in the other Lucas branch, where
(5) need not hold.
At a grid point x+y=t<8, prescribe residual multiplicity
Rxy=max{0,mt−hx−hy}.
The degree-84 symmetric jet matrix is 1845×1849 and has full row
rank modulo 251. The
nonvanishing interpolation lemma
therefore provides a finite integer family G of degree at most 85 with
these residual multiplicities, at least one of which is nonzero at every
physical point (j,c) with j+c>7. Coordinate factors cannot vanish
there, since j,c≥9.
Consequently one of the corresponding F=HG is nonzero, has degree at
most
D=2∑ha+85=283,
and has the row multiplicities mt. The integer data and the exact rank
calculation are retained in the
checker and
certificate.
Put B=(jn) and
E7=7min{v7(n−2),v7(B)}.
The exact localization inequality, retaining this actual overlap, gives
The contribution of every nonmaximal small-prime power is covered by the
factor (7!)102. The prime threshold remains the original p≥8,
which here means primes at least 11.
The sum of the row multiplicities is 487. By (1), each of P2,P3,P5
is at most 2h7/10. Also n≤2h. A deliberately generous coefficient
bound obtained from a nonzero maximal jet minor gives
h367/10≤10169000E773.(7)
For completeness, a jet entry is smaller than 2⋅884.
Hadamard, adjugates, and the generator construction bound the coefficient
norm of G by 101845(84+6)+50. The logarithmic bounds for H,
(7!)102, and the replacements n≤2h add respectively
198, 408, and 283+239. Their total is 167228<169000.
The remaining height exponent in (6) is exactly
487−283−107(81+56+102)=10367.
If the low-residue branch in (2) held, (5) would give
E7≤n−2≤2h. Then (7) would imply
h1/5≤10169000273/2<10170000,
contrary to h≥10850001. This proves (2).
Finally, (7) gives
E7≥10−169000/73h367/730.
Combine this with (4), first at j and then at c. Since
7v7(B)≥E7 and n−2≤2h,
[(j)3]7,[(c)3]7≤2⋅10169000/73h363/730.
At the stated height these quantities are strictly below h;
the preceding lower bound for E7 is strictly above h.
This proves (3).