The region 𝑏𝜇 <𝑎 and the
base 31/4
The rational-base calculation compares a gain in the remainder with
the cost of making its coefficients integral. If the original
coefficient has degree 𝐾𝑛 and the
cancelled coefficient has degree 𝑊𝑛, the leading balance is
𝑏𝑊𝑛(𝑎/𝑏)−(𝐾𝑛−𝑊𝑛)=𝑏𝐾𝑛𝑎−(𝐾𝑛−𝑊𝑛).(1)
The polynomial identities and remainder
estimates below justify this balance, including its lower-order factors.
With 𝐾𝑛/𝑛2 →𝐶1 and (𝐾𝑛 −𝑊𝑛)/𝑛2 →𝐶0, the cleared
remainder tends to zero when 𝐶1log𝑏 <𝐶0log𝑎. The degree drop has two effects: it improves
the real remainder and changes the denominator needed to make its
coefficients integral. Both effects concern the same cancelled form.
This is why one must calculate the degree before rational evaluation,
rather than borrow a denominator bound from the uncancelled family.
We evaluate Zudilin’s 2004 forms at 𝑎/𝑏 after cancelling their common
polynomial factors. His direction (14,12,14;27) [8] gives the constants below; the
comparison between decay and the remaining degree determines the
irrationality region:
𝐶1=(14+12+14)27−12(122+142+272)=10912,𝐶0=266−3𝜋2(225−𝐽),
𝐽=13∑𝑖=1(𝜓1(𝑢𝑖)−𝜓1(𝑣𝑖)),𝜓1(𝑥)=∑𝑘≥01(𝑘+𝑥)2,
where 𝜓1 is the trigamma function, used
only for positive arguments, and the thirteen half-open intervals [𝑢𝑖,𝑣𝑖) are [1/14,1/12), [1/7,1/6), [3/14,1/4), [2/7,1/3), [5/14,2/5), [3/7,7/15), [1/2,8/15), [4/7,3/5), [9/14,2/3), [5/7,11/15), [11/14,4/5), [6/7,13/15), [13/14,14/15). The intervals are disjoint
and lie in [1/14,1), so 0 ≤𝐽 ≤𝜓1(1/14) −𝜓1(1) <196:
in the defining series, 𝜓1(1/14) =196 +∑𝑘≥1(𝑘 +1/14)−2 <196 +𝜓1(1).
Since 𝜋 >3, it follows that
191 <𝐶0 <266 <𝐶1/2. In
particular, the reciprocal constants below are positive without using
decimal approximations. The accompanying rational certificate gives
77.94318445520543<𝐽<77.94318449473569,221.30008815898543<𝐶0<221.30008817100119,0.40568302137302<𝜃∗:=𝐶0/𝐶1<0.40568302139506.
Put 𝜇 =1/𝜃∗. These parameter ratios,
intervals and constants, including 𝐶1/𝐶0 =2.46497868…, occur in [8]; that ratio is the
integer-base exponent bound in its Theorem 1, not a new optimised
constant. The displayed interval endpoints are rounded outwards from
rational bounds; no digits beyond their certified accuracy are
required.
The proof below needs 𝐽 in its
combinatorial form as well. Put
𝜔(𝜉)=max{0,⌊14𝜉⌋+⌊13𝜉⌋−⌊12𝜉⌋−⌊15𝜉⌋,2⌊14𝜉⌋−⌊13𝜉⌋−⌊15𝜉⌋},
the weight that [8]
attaches to the six-tuple 𝑐 =(13,14,12,14,15,13) for the chosen
parameter ratios; it gives the exponents 𝜈𝑙 =𝜔(𝑛/𝑙) of the source’s (22)
and enters its limit (26). Zudilin lists the support of 𝜔 in the same place; the next lemma
verifies that list by exact evaluation. Since 14 +13 =12 +15 and 2 ⋅14 =13 +15, each floor difference is
unchanged by 𝜉 ↦𝜉 +1. Thus
𝜔 has period 1, and the lemma also determines every
value 𝜔(𝑛/𝑙) needed for the
cyclotomic exponents.
Lemma 2.1 (the weight is an indicator). On [0,1) the function 𝜔 takes only the values 0 and 1, and 𝜔 =1 exactly on the union of the
thirteen half-open intervals listed above.
Proof. Each of the three expressions inside the maximum is
constant on every interval between consecutive elements of {𝑘/𝑐 :𝑐 ∈{12,13,14,15}, 0 ≤𝑘 ≤𝑐}, since those are the only points at which one of the four
floor functions changes. There are 48 such intervals in [0,1); evaluating 𝜔 at the midpoint of each gives the
value 1 on the thirteen listed
half-open intervals and 0
elsewhere, and the thirteen listed intervals are unions of consecutive
cells. Each floor function is right-continuous, so a cell has the same
value at its left endpoint as at its midpoint. This also verifies the
half-open endpoint convention. All evaluations use exact rational
arithmetic. ◻
Lemma 2.1 and
termwise integration of the positive series −𝜓′1(𝜉) =∑𝑘≥02(𝑘 +𝜉)−3
give the two forms of 𝐽 used below,
𝐽=∫10𝜔(𝜉)∑𝑘≥02(𝑘+𝜉)3𝑑𝜉=13∑𝑖=1(𝜓1(𝑢𝑖)−𝜓1(𝑣𝑖)),
the
first being the integral ∫10𝜔 𝑑( −𝜓1) of [8]. Since 𝜔 vanishes near 0, both are finite.
For 𝑏 =1 the logarithmic ratio is
zero, so the condition includes every integer base. For 𝑏 >1 it requires 𝑎 >𝑏2.46497868…, substantially
more than 𝑎 >𝑏. There are still
infinitely many admissible coprime numerators for each fixed
denominator. The base 31/4 is
included, whereas 3/2 is excluded.
Taking positive integral powers does not change the ratio. At equality
with the cutoff, the estimates give no conclusion.
Theorem 2.2 (rational-base region). Let 𝑎 >𝑏 ≥1 be coprime integers with
𝑏𝜇<𝑎,equivalentlylog𝑏log𝑎<𝜃∗=0.40568302138406054…
Then 𝐹(𝑎/𝑏) =∑𝑚≥1((𝑎/𝑏)𝑚 −1)−1 is irrational.
The proof has three steps. We cancel the common polynomial factors
using Zudilin’s integrality argument [8]. We then compute the degree of the
remaining polynomials, using his cyclotomic limits and the
reciprocal-interval method of [7]. Finally, we evaluate at 𝑎/𝑏 and show that the positive remainder
still decays after multiplication by the required power of 𝑏. These steps occupy Sections 2.1–2.4. The
construction, direction and constants are Zudilin’s; the rational
specialisation and its degree and remainder estimates are proved
below.
The polynomial forms and their common factors
We construct 𝑈𝑛,𝑉𝑛 as integral
polynomials before evaluating them. Cancelling their common factors at
this stage lowers the degree and hence the power of 𝑏 required at a rational base 𝑎/𝑏.
For each 𝑛 ≥1, the coefficient
formulas below are rational functions of an indeterminate 𝑋. We evaluate them at real 𝑥 >1 and put 𝑞 =𝑥−1 when using the convergent
series. Set
𝑎0=14𝑛+1,𝑎1=12𝑛+1,𝑎2=14𝑛+1,𝛽𝑛=27𝑛+2,𝑁=15𝑛,𝑀𝑛=266𝑛2+34𝑛+1.
The symbol 𝛽𝑛 is the parameter 𝑏 of [8], the exponent in the lower parameter
𝑞𝑏 of the Heine series (13) on
p. 157; the letter 𝑏 continues to
denote the denominator of the base. In this construction alone, 𝑁 =15𝑛 is the cyclotomic cutoff. The
exponent 𝑀𝑛 is the integer of that
paper’s (16) on p. 157. Write (𝑧;𝑞)𝑚 =∏𝑚−1𝑗=0(1 −𝑧𝑞𝑗) for
the 𝑞-Pochhammer symbol (the
shifted 𝑞-factorial). Zudilin’s
positive remainder is
𝐻𝑛(𝑥)=∑𝑡≥0(𝑞𝑡+1;𝑞)𝑎1−1(𝑞;𝑞)𝑎1−1(𝑞;𝑞)𝛽𝑛−𝑎2−1(𝑞𝑎2+𝑡;𝑞)𝛽𝑛−𝑎2𝑞𝑎0𝑡.(2)
The denominator length 𝛽𝑛 −𝑎2 agrees with the gamma
expression (7) and residues (8) of [8]. The unnumbered display of 𝑅(𝑇) on that page instead has length
𝛽𝑛 −𝑎2 −1; we use the
normalisation fixed by the numbered identities. Then [8] gives 𝐻𝑛 =𝐴𝑛𝐹 −𝐵𝑛 with 𝐴𝑛,𝐵𝑛 ∈ℚ(𝑋). We need their explicit
formulas to compute degrees and bound coefficients. Let [𝑚𝑟]𝑋 =∏𝑟𝑗=1(1 −𝑋𝑚−𝑟+𝑗)/(1 −𝑋𝑗)
for 0 ≤𝑟 ≤𝑚. This Gaussian
binomial, or 𝑞-binomial, polynomial
has degree 𝑟(𝑚 −𝑟) and nonnegative
coefficients summing to (𝑚𝑟). For 𝑎2 ≤𝑘 ≤𝛽𝑛 −1 put
𝑐𝑛,𝑘(𝑋)=(−1)𝑎1+𝑎2+𝑘+1𝑋𝑒𝑛,𝑘[𝑘−1𝑎1−1]𝑋[𝛽𝑛−𝑎2−1𝛽𝑛−𝑘−1]𝑋,(3)
𝑒𝑛,𝑘=𝑎1(𝑎1−1)2−(𝛽𝑛−𝑎2)(𝛽𝑛−𝑎2−1)2+(𝛽𝑛−𝑘)(𝛽𝑛−𝑘−1)2.
Then
𝐴𝑛(𝑋)=𝛽𝑛−1∑𝑘=𝑎2𝑐𝑛,𝑘(𝑋)𝑋𝑎0𝑘,𝐵𝑛(𝑋)=𝛽𝑛−1∑𝑘=𝑎2𝑐𝑛,𝑘(𝑋)𝑋𝑎0𝑘(𝑘−𝑎1∑𝑙=11𝑋𝑙−1+𝑎0−1∑𝑗=1𝑋−𝑗(𝑘−𝑎1)𝑋𝑗−1).(4)(5)
Put
𝐷𝑁(𝑋)=𝑁∏𝑙=1Φ𝑙(𝑋),𝜈𝑛,𝑙=𝜔(𝑛/𝑙),Ω𝑛(𝑋)=𝑁∏𝑙=2Φ𝑙(𝑋)𝜈𝑛,𝑙,(6)
with Φ𝑙
the 𝑙th cyclotomic polynomial; by
Lemma 2.1 every
𝜈𝑛,𝑙 is 0 or 1, and 𝜈𝑛,𝑙 =0 for 𝑙 >15𝑛 because the intervals all begin
at or above 1/14.
Zudilin’s Lemma 7 [8] applies at the parameters above: the
tuple is 𝑐 =𝑛 ⋅(13,14,12,14,15,13) with maximum
𝑚(𝑐) =15𝑛 and difference 𝑠(𝑐) =𝑛 >0, and the source’s (14) on
p. 157 holds because 12𝑛 +1 ≤14𝑛 +1
and 26𝑛 +2 ≤27𝑛 +2 ≤28𝑛 +2. Its
conclusion is the inclusion
𝑈𝑛:=𝑋−𝑀𝑛𝐷𝑁Ω𝑛𝐴𝑛∈ℤ[𝑋],𝑉𝑛:=𝑋−𝑀𝑛𝐷𝑁Ω𝑛𝐵𝑛∈ℤ[𝑋].(7)
Two points about that citation matter. First,
the conclusion used is the one in ℤ[𝑋], not integrality at integer
arguments: an integer-valued polynomial such as 𝑋(𝑋 −1)/2 shows that the two statements
differ. The source’s proof supplies the polynomial form. Its Lemma 4
(pp. 157–159) clears the two rational coefficients separately by
Gaussian-binomial identities in ℤ[𝑋]. Lemma 5 (p. 160) makes the
normalised series invariant under the order-twelve group generated by
Heine’s parameter transformation and the exchange of 𝑎1 and 𝑎2. For the divisibility argument,
however, only its order-six subgroup preserving 𝑠 >0 is used: one application of
Heine’s transformation reverses the sign of 𝑠. Under that subgroup the normalising
factorial product takes the three forms displayed in the source.
Comparing their cyclotomic valuations gives the maximum of three terms
in 𝜔. Lemma 7 (p. 161) removes
the resulting common cyclotomic factors by polynomial divisibility; the
divisor Ω𝑛 is monic. These
steps take place before the integer specialisation in (24) on
p. 162.
Second, the module inclusion gives a polynomial coefficient pair, and
uniqueness identifies it with the displayed cancelled source pair. If
two pairs differed, subtracting their identities would express 𝐹 as a rational function of 𝑋. This is impossible: as ℎ ↓0, splitting the original
Lambert sum 𝐹(𝑒ℎ) =∑𝑚≥1(𝑒ℎ𝑚 −1)−1 at
𝐿 =⌊1/ℎ⌋ gives an
initial sum ℎ−1∑𝑚≤𝐿𝑚−1 +𝑂(𝐿), since 𝑦−1 −1 ≤(𝑒𝑦 −1)−1 ≤𝑦−1 for
0 <𝑦 ≤1. The remaining sum is at
most 𝑒−ℎ(𝐿+1)/((1 −𝑒−1)(1 −𝑒−ℎ)) =𝑂(ℎ−1).
Hence 𝐹(𝑒ℎ) =ℎ−1log(1/ℎ) +𝑂(ℎ−1), so
(𝑋 −1)𝐹(𝑋) →∞ and (𝑋 −1)2𝐹(𝑋) →0 as 𝑋 ↓1, which no rational function
does. Thus the source’s module inclusion yields the specific pair
in (7),
not merely some unspecified polynomial representation of the same
function. This functional nonrationality says nothing about an
individual value. For 𝑥 >1, write
the cancelled remainder as
Λ𝑛(𝑥)=𝑈𝑛(𝑥)𝐹(𝑥)−𝑉𝑛(𝑥)=𝑥−𝑀𝑛𝐷𝑁(𝑥)Ω𝑛(𝑥)𝐻𝑛(𝑥).
Exact degrees
The final summand of 𝐴𝑛 has
strictly larger degree than all the others. We use it to determine the
leading coefficient as well as the degree. After cancellation, this will
give the least common power of the base denominator that clears the
pair.
Let 𝑑𝑛,𝑘 =deg(𝑐𝑛,𝑘(𝑋)𝑋𝑎0𝑘).
The Gaussian factors are monic of degrees (𝑎1 −1)(𝑘 −𝑎1) and (𝛽𝑛 −𝑘 −1)(𝑘 −𝑎2). Adding these to the
monomial exponent gives
𝑑𝑛,𝑘=𝑒𝑛,𝑘+𝑎0𝑘+(𝑎1−1)(𝑘−𝑎1)+(𝛽𝑛−𝑘−1)(𝑘−𝑎2)=−𝑘2+80𝑘𝑛+3𝑘−340𝑛2−26𝑛2.
Taking the difference
at consecutive indices, we obtain
𝑑𝑛,𝑘+1−𝑑𝑛,𝑘=40𝑛+1−𝑘>0(𝑎2≤𝑘≤𝛽𝑛−2),
the inequality because 𝑘 ≤𝛽𝑛 −2 =27𝑛 and 27𝑛 <40𝑛 +1. The summand of top degree
is therefore the one at 𝑘 =𝛽𝑛 −1
alone, no cancellation occurs there, and
𝐾𝑛:=deg𝐴𝑛=𝑑𝑛,𝛽𝑛−1=1091𝑛2+81𝑛+22,𝑊𝑛:=deg𝑈𝑛=𝐾𝑛−𝑀𝑛+∑𝑙≤𝑁𝜑(𝑙)−∑2≤𝑙≤𝑁𝜈𝑛,𝑙𝜑(𝑙),(8)
the second equality because deg𝐷𝑁 =∑𝑙≤𝑁𝜑(𝑙) and
degΩ𝑛 =∑2≤𝑙≤𝑁𝜈𝑛,𝑙𝜑(𝑙), and because 𝑈𝑛 is a polynomial by (7),
so subtracting 𝑀𝑛 from the degree
of 𝐷𝑁𝐴𝑛/Ω𝑛 is legitimate.
In particular 𝑈𝑛 ≠0. There is
also no integer leading-coefficient factor to cancel: the top summand
has leading coefficient ( −1)𝑎1+𝑎2+𝛽𝑛 =( −1)𝑛, and both
Gaussian factors and 𝐷𝑁/Ω𝑛
are monic. Thus the leading coefficient of 𝑈𝑛 is ( −1)𝑛.
The net decrease in degree is
𝐾𝑛−𝑊𝑛=𝑀𝑛−deg(𝐷𝑁/Ω𝑛).
Dividing
by 𝑋𝑀𝑛 lowers the degree by
𝑀𝑛, but multiplying by the
remaining cyclotomic factors increases it by deg(𝐷𝑁/Ω𝑛). This is why the
remainder estimate below involves 𝐾𝑛 −𝑊𝑛, rather than 𝑀𝑛 alone.
For a reduced fraction 𝑎/𝑏, the
unit leading coefficient also gives the exact denominator of 𝑈𝑛(𝑎/𝑏), not just an upper bound. For
every prime 𝑝 ∣𝑏,
𝑏𝑊𝑛𝑈𝑛(𝑎/𝑏)≡(−1)𝑛𝑎𝑊𝑛≢0(mod𝑝).
No prime dividing 𝑏 cancels from the cleared numerator, so
the reduced denominator is exactly 𝑏𝑊𝑛. In particular every common
integer divisor of the cleared row is coprime to 𝑏. This excludes cancelling a factor of
𝑏 from this row, not cancellation
at other primes or a saving from a different pair.
The formal arithmetic checks cover the value
of 2𝑀𝑛 from the source’s
formula (16), the degree
difference 𝑑𝑛,𝑘+1 −𝑑𝑛,𝑘 =40𝑛 +1 −𝑘, its positivity
for 𝑎2 ≤𝑘 ≤𝛽𝑛 −2, and
the top
degree 2𝐾𝑛 =1091𝑛2 +81𝑛 +2.
These statements check the polynomial degree calculation, not the
analytic estimates used later.
For the second coefficient, fix 𝑛 and let 𝑥 →∞. For 𝑥 ≥2, every finite product in (2)
lies between ∏𝑗≥1(1 −2−𝑗) >0 and 1, independently of 𝑡. Also ∑𝑡≥0𝑥−𝑎0𝑡 ≤2. These bounds
give 𝐻𝑛(𝑥) =𝑂(1) for the whole sum,
not just each summand. Also 𝐹(𝑥) =𝑥−1 +𝑂(𝑥−2), because 𝜏(1) =1 and ∑𝑚≥2𝑚𝑥−𝑚 =𝑂(𝑥−2). The monic
normalising factor at infinity gives Λ𝑛(𝑥) =𝑂(𝑥𝑊𝑛−𝐾𝑛). Since 𝐾𝑛 ≥2 and 𝑈𝑛 has leading coefficient ( −1)𝑛,
𝑉𝑛(𝑥)=𝑈𝑛(𝑥)𝐹(𝑥)−Λ𝑛(𝑥)=(−1)𝑛𝑥𝑊𝑛−1+𝑂(𝑥𝑊𝑛−2).
The degree formula gives
𝑊𝑛 ≥𝐾𝑛 −𝑀𝑛 =(559𝑛2 +13𝑛)/2 >0.
Polynomial integrality was established earlier, so the displayed
asymptotic proves the exact statement
deg𝑉𝑛=𝑊𝑛−1,lc𝑉𝑛=(−1)𝑛.(9)
In particular 𝑉𝑛 is not the zero polynomial. Applying
the same prime-by-prime reduction at its own degree shows that 𝑉𝑛(𝑎/𝑏) has reduced denominator exactly
𝑏𝑊𝑛−1. Thus 𝑏𝑊𝑛 is the least common clearing
denominator, although the second coordinate alone needs one fewer power
of 𝑏. In the common normalisation,
gcd(𝑏𝑊𝑛𝑉𝑛(𝑎/𝑏),𝑏𝑊𝑛)=𝑏.
Indeed 𝑏𝑊𝑛𝑉𝑛(𝑎/𝑏) is 𝑏 times an integer coprime to 𝑏. These facts concern the fixed source
pair, not all approximants. The degree calculation fixes 𝑛 and varies 𝑥; the decay calculation fixes 𝑥 and varies 𝑛.
The cyclotomic limit
We prove the cyclotomic limits of Zudilin [8] by summing over reciprocal intervals,
following [7]. The
summatory totient estimate handles each finite set of intervals. A bound
on the remaining small indices permits passage to their infinite
union.
Write Σ𝑛 =∑2≤𝑙≤𝑁𝜈𝑛,𝑙𝜑(𝑙). The elementary summatory estimate is
∑𝑙≤𝑦𝜑(𝑙) =3𝜋−2𝑦2 +𝑂(𝑦log(2𝑦)). Fix one half-open
interval [𝑢,𝑣) of Lemma 2.1. The
condition {𝑛/𝑙} ∈[𝑢,𝑣) holds
exactly on the blocks
𝑛𝑘+𝑣<𝑙≤𝑛𝑘+𝑢,𝑘=0,1,2,…,
so the summatory estimate gives, for each fixed
𝑘, 𝑛−2∑𝑙 in block 𝑘𝜑(𝑙) →3𝜋−2((𝑘 +𝑢)−2 −(𝑘 +𝑣)−2). For
𝐿 ≥1, all blocks with 𝑘 ≥𝐿 lie below 𝑛/(𝐿 +𝑢). For every 𝑦 ≥0,
∑𝑙≤𝑦𝜑(𝑙)≤𝑦2.
For
𝑦 <1 the sum is empty; otherwise
it is at most ⌊𝑦⌋(⌊𝑦⌋ +1)/2 ≤𝑦2. Hence the normalised contribution of the
omitted blocks is at most (𝐿 +𝑢)−2, uniformly in 𝑛. This is the bound needed to pass from
finitely many blocks to all of them. Taking 𝑛 →∞ first and then 𝐿 →∞ justifies the infinite block
sum, and summing the thirteen half-open intervals gives 𝑛−2Σ𝑛 →3𝐽/𝜋2. With ∑𝑙≤15𝑛𝜑(𝑙) =3𝜋−2225𝑛2 +𝑂(𝑛log𝑛), equation (8) yields
𝐾𝑛𝑛2→𝐶1,𝐾𝑛−𝑊𝑛𝑛2=𝑀𝑛−∑𝑙≤𝑁𝜑(𝑙)+Σ𝑛𝑛2→266−3𝜋2(225−𝐽)=𝐶0,(10)
and hence 𝑊𝑛/𝑛2 →𝐶1 −𝐶0. These are the
rational-base degree limits built on Zudilin’s cyclotomic limits [8].
For the real size estimate, fix 𝑥 >1. The Möbius product formula and
reindexing the divisors give
∑𝑙≤𝑁|logΦ𝑙(𝑥)−𝜑(𝑙)log𝑥|≤∑𝑑≤𝑁⌊𝑁/𝑑⌋[−log(1−𝑥−𝑑)]≤𝑁∑𝑑≥1−log(1−𝑥−𝑑)𝑑.
The bound −log(1 −𝑥−𝑑) ≤𝑥−𝑑/(1 −𝑥−1)
shows that the series on the right is finite for each fixed 𝑥 >1. Since 𝜈𝑛,𝑙 ∈{0,1}, this proves the
bound
log𝐷𝑁(𝑥)Ω𝑛(𝑥)=(∑𝑙≤𝑁𝜑(𝑙)−Σ𝑛)log𝑥+𝑂𝑥(𝑁).(11)
Here 𝑁 =15𝑛,
so the error is 𝑂𝑥(𝑛) =𝑜(𝑛2). The
bracket equals 𝑊𝑛 −𝐾𝑛 +𝑀𝑛 by (8). No
uniform constant as 𝑥 ↓1 is
asserted.
Positive linear forms with integer coefficients
We now specialise at 𝑥 =𝑎/𝑏 >1.
Put 𝑞 =1/𝑥 and 𝑃𝑞 =(𝑞;𝑞)∞. Every finite 𝑞-Pochhammer product in (2)
has factors 1 −𝑞𝑗 with 𝑗 ≥1, so it lies between 𝑃𝑞 and 1. Each of the two ratios therefore lies
between 𝑃𝑞 and 𝑃−1𝑞. Summing the resulting geometric
bounds gives
𝑃2𝑞≤𝐻𝑛(𝑥)≤𝑃−2𝑞1−𝑞𝑎0≤𝑃−2𝑞1−𝑞,
whence 𝐻𝑛(𝑥) >0 and log𝐻𝑛(𝑥) =𝑂𝑥(1) uniformly in 𝑛. The cyclotomic factors are positive on
(1,∞), so the cancelled
remainder Λ𝑛(𝑥) is positive
as well, by (7).
By (8)
and (9)
both polynomial degrees are at most 𝑊𝑛, so
ˆ𝑈𝑛=𝑏𝑊𝑛𝑈𝑛(𝑎/𝑏),ˆ𝑉𝑛=𝑏𝑊𝑛𝑉𝑛(𝑎/𝑏)
are integers, and ˆΛ𝑛 :=𝑏𝑊𝑛Λ𝑛(𝑎/𝑏) =ˆ𝑈𝑛𝐹(𝑎/𝑏) −ˆ𝑉𝑛 is positive and lies in ℤ𝐹(𝑎/𝑏) +ℤ. This follows by multiplying
each polynomial value by 𝑏𝑊𝑛.
The integer coefficients and the earlier cancellation of a common
cyclotomic factor are separate inputs. Combining the size estimates,
logˆΛ𝑛=𝑊𝑛log𝑏−𝑀𝑛log𝑥+(∑𝑙≤𝑁𝜑(𝑙)−Σ𝑛)log𝑥+𝑂𝑥(𝑛)=𝐾𝑛log𝑏−(𝐾𝑛−𝑊𝑛)log𝑎+𝑜(𝑛2),
the second equality by log𝑥 =log𝑎 −log𝑏 and (8).
With (10) this
proves
lim𝑛→∞logˆΛ𝑛𝑛2=𝐶1log𝑏−𝐶0log𝑎.(12)
Proof of Theorem 2.2. The
hypothesis log𝑏/log𝑎 <𝜃∗ =𝐶0/𝐶1 makes the right side of (12) negative,
so ˆΛ𝑛 >0 and ˆΛ𝑛 →0. Suppose 𝐹(𝑎/𝑏) =𝑃/𝑄 with integers 𝑃 and 𝑄 ≥1. Then 𝑄ˆΛ𝑛 =𝑃ˆ𝑈𝑛 −𝑄ˆ𝑉𝑛 is a positive integer for every 𝑛 and tends to 0, which is impossible. ◻
Above the threshold (12) says that
these same homogenised forms grow like 𝑒𝑐𝑛2 with 𝑐 >0, and at equality the limit decides
nothing. Both statements are about the displayed family.
The hypothesis 𝑏 ≥1 admits
𝑏 =1, where the statement reduces to
the known integer-base theorem. Coprimality fixes the reduced
representation of the base. It is used in the exact-denominator
assertion above, but is not needed for the sufficient irrationality
implication once the displayed logarithmic inequality holds. Negative
bases are excluded, because the proof uses positivity for real bases
greater than 1.
Theorem 2.3 (the base 31/4 outside the Bundschuh–Väänänen
region). 𝐹(31/4) is
irrational, and so is 𝐹((31/4)𝑟) for every integer
𝑟 ≥1. Here
log4log31=0.4036981731641997…<81200<𝜃∗,
while
4𝜇=30.483515…<31<4𝜇BV=32.369642…
with 𝜇BV =2𝜋2/(𝜋2 −2) =2.508284761994…,
so 31/4 lies outside the region
log𝑏/log𝑎 <1/2 −1/𝜋2 =0.3986788163576622… of [6] and inside the region of
Theorem 2.2.
Proof. The comparison log4/log31 <81/200 is the integer
certificate 4200 <3181,
which Lean checks,
and Lean also checks that it places 31/4 in the region log𝑏/log𝑎 <81/200. The ratio
log𝑏/log𝑎 is invariant under
(𝑎,𝑏) ↦(𝑎𝑟,𝑏𝑟), which
places every
power of 31/4 in the same
region, and (31𝑟,4𝑟) are
coprime. Lean also checks that 31/4 lies outside the earlier region.
That exclusion also has a two-line rational certificate: 312 <45 gives log4/log31 >2/5, and 𝜋2 <10 gives 1/2 −1/𝜋2 <2/5, so
12−1𝜋2<25<log4log31<81200<𝜃∗.
The remaining comparison 81/200 <𝜃∗ is proved in
Section 2.5.
Theorem 2.2
then applies. ◻
Corollary 2.4 (an irrationality measure uniform over
powers). For coprime 𝑎 >𝑏 ≥1 with 𝜃 =log𝑏/log𝑎 <𝜃∗ and
every integer 𝑟 ≥1,
𝜇irr(𝐹((𝑎/𝑏)𝑟))≤1−𝜃𝜃∗−𝜃.
Here 𝜇irr(𝜉) is the supremum of the
exponents 𝜈 for which |𝜉 −𝑝/𝑞| <𝑞−𝜈 has infinitely many
reduced rational solutions. In particular, 𝜇irr(𝐹((31/4)𝑟)) <301 for
every 𝑟 ≥1.
Proof. For the irrationality exponent, bound 𝐴𝑛 in (4): its 𝑂(𝑛) Laurent monomials multiply two
Gaussian binomial polynomials, each with nonnegative coefficients
summing to at most 227𝑛+2. Thus
its absolute coefficient sum is exp(𝑂(𝑛)), and its largest exponent
𝐾𝑛 gives |𝐴𝑛(𝑥)| ≤𝑥𝐾𝑛exp(𝑂(𝑛)) for fixed
𝑥 >1. The cyclotomic estimate in
Section 2.4 bounds
the multiplier 𝑥−𝑀𝑛𝐷𝑁(𝑥)/Ω𝑛(𝑥) by 𝑥𝑊𝑛−𝐾𝑛exp(𝑂𝑥(𝑛)). Therefore
|𝑈𝑛(𝑥)|≤𝑥𝑊𝑛exp(𝑂𝑥(𝑛))(𝑥>1 fixed).
Set 𝜉 =𝐹(𝑎/𝑏), 𝑄𝑛 =𝑏𝑊𝑛𝑈𝑛(𝑎/𝑏) and 𝑃𝑛 =𝑏𝑊𝑛𝑉𝑛(𝑎/𝑏). With
𝛼=(𝐶1−𝐶0)log𝑎,𝜏=𝐶0log𝑎−𝐶1log𝑏>0,
we have log(𝑄𝑛𝜉 −𝑃𝑛) = −𝜏𝑛2 +𝑜(𝑛2) and
|𝑄𝑛| ≤exp(𝛼𝑛2 +𝑜(𝑛2)).
For integers 𝐴,𝐵,𝑝,𝑞 with 𝑞 >0, if 𝐿 =𝐴𝜉 −𝐵 and 2𝑞|𝐿| ≤1, then
|𝐿|≤|𝐴||𝜉−𝑝/𝑞|.
When 𝐴𝑝 −𝐵𝑞 =0 this is equality. Otherwise the
nonzero integer 𝐴𝑝 −𝐵𝑞 gives 1/𝑞 ≤|𝐿| +|𝐴| |𝜉 −𝑝/𝑞|, which proves
the inequality. Fix 0 <𝜂 <𝜏. For all sufficiently
large 𝑛, the estimates above give
𝑒−(𝜏+𝜂)𝑛2≤𝑄𝑛𝜉−𝑃𝑛≤𝑒−(𝜏−𝜂)𝑛2,|𝑄𝑛|≤𝑒(𝛼+𝜂)𝑛2.
For every sufficiently
large denominator 𝑞, the upper
remainder bound suggests choosing 𝑛 =⌈√log(2𝑞)/(𝜏−𝜂)⌉.
Then 2𝑞(𝑄𝑛𝜉 −𝑃𝑛) ≤1, so the
preceding integer argument applies to (𝐴,𝐵) =(𝑄𝑛,𝑃𝑛) for every numerator 𝑝. Also 𝑄𝑛 ≠0: otherwise 𝑄𝑛𝜉 −𝑃𝑛 would be an integer strictly
between 0 and 1. The lower remainder bound and the
coefficient bound now give
|𝜉−𝑝/𝑞|≥𝑒−(𝛼+𝜏+2𝜂)𝑛2=𝑞−(𝛼+𝜏+2𝜂)/(𝜏−𝜂)−𝑜(1),
since
𝑛2 =log(2𝑞)/(𝜏 −𝜂) +𝑂𝜂(√log𝑞 +1).
Let 𝜂 ↓0. The
resulting bound is 1 +𝛼/𝜏 =(1 −𝜃)/(𝜃∗ −𝜃).
Taking a common power multiplies 𝛼,𝜏 by 𝑟, leaving this quotient unchanged; the
constants in the approximation inequality may depend on 𝑟. For 31/4, the exact rational interval
calculation below gives
0.40568302137302<𝜃∗<0.40568302139506,0.40369817316419<log4log31<0.40369817316420.
For each trigamma difference, sum 𝑘 =0,…,255 exactly and bound the
remaining decreasing positive summand 𝑓𝑢,𝑣(𝑥) =(𝑥 +𝑢)−2 −(𝑥 +𝑣)−2 by its
integral from 256 to infinity and
that integral plus 𝑓𝑢,𝑣(256).
Bound 𝜋 with Machin’s identity
and alternating arctangent series, and logarithms with the positive
arctanh series and a
geometric tail bound. Outward rational interval operations then place
(1 −𝜌)/(𝜃∗ −𝜌), where
𝜌 =log4/log31, between 300.4269130 and 300.4269164, hence below 301. All endpoints are rational. For the
bound 301 alone, the coarser
inequalities 𝜌 <0.4036982 and
𝜃∗ >0.40568 suffice:
1−𝜌𝜃∗−𝜌<1−0.40369820.40568−0.4036982=29815099909<301.
Here the quotient is increasing
in 𝜌 and decreasing in 𝜃∗ because 𝜌 <𝜃∗ <1. The finer
enclosure also certifies the displayed decimal approximation. Lean
checks the coarser calculation, including 2981509/9909 <301, and proves
enclosures of 𝜃∗ and 𝜌 sharper than the finer ones
displayed above (Section 2.5 and
Theorem 2.3); the 256-summand calculation is an exact
computation outside Lean. ◻
The rational bracket around 𝜃∗
Rational bounds for the trigamma differences locate 𝜃∗ without a numerical
approximation to the full sums. Their first terms already place 31/4 inside the region and 3/2 outside it. A sharper enclosure then
gives the irrationality-exponent bound 301.
For the lower bound, keep only the 𝑘 =0 term of each of the thirteen
differences 𝜓1(𝑢𝑖) −𝜓1(𝑣𝑖). All later terms
are positive, so
𝐽 ≥ 13∑𝑖=1(1𝑢2𝑖−1𝑣2𝑖)=201564069025125971865920>77610.
Since 𝜋 >157/50 and 225 −𝐽 <225,
𝐶0>266−3(225−776/10)(157/50)2=545113424649>88371400=81200𝐶1,
so 81/200 <𝜃∗. For the upper bound
the thirteen half-open intervals are disjoint and ordered and 𝜓1 is positive and decreasing, so the
sum telescopes below its first term:
𝐽<𝜓1(1/14)=196+∑𝑘≥11(𝑘+1/14)2<196+𝜋26<198<225,
whence 𝐶0 <266 and 𝜃∗ <532/1091 <1/2. So
81200<𝜃∗<12.
Lean checks the definitions of 𝐶0, 𝐶1 and 𝜃∗ together with the lower
bound on 𝐽, rational
lower bound on 𝐶0, and the two
comparisons 81/200 <𝜃∗ and 𝜃∗ <1/2. It also checks that
31/4 belongs to the region, that every
positive integral power does too, and that 3/2 is excluded. These comparisons
use the defined constant; the analytic estimates belong to the proof of
Theorem 2.2,
which Lean also checks. Lean also proves 0.40568302138406054100 ≤𝜃∗ ≤0.40568302138406054104
and enclosures of 𝐽 and 𝐶0 (evidence record, Theorem 2.2). The sharper
interval in the preceding proof comes from the stated exact-arithmetic
certificate with 256 summands per
trigamma difference. It does not rely on the historical thousand-term
decimal evaluation reported in Section 2.7.
The shorter interval above suffices for the bound 301 but does not certify all digits
printed in the cutoff. Lean’s enclosure of 𝜃∗ implies the following bounds,
and a separate integer-arithmetic calculation reproduces them
independently of Lean:
0.4056830213840605403<𝜃∗<0.4056830213840605417,2.4649786835749750334<𝜇<2.4649786835749750415.
Here is the complete error bound used in that
calculation. For each of the thirteen intervals, put 𝑓𝑢,𝑣(𝑘) =(𝑘 +𝑢)−2 −(𝑘 +𝑣)−2. Round
each of the first 𝑀 =65536 positive
rational summands down to a multiple of 10−50. Their true sum is between this
rounded sum and that sum plus 𝑀10−50. Since 𝑓𝑢,𝑣 is positive and decreasing, the
remaining tail lies between its integral from 𝑀 to infinity and that integral plus
𝑓𝑢,𝑣(𝑀). The integral is (𝑀 +𝑢)−1 −(𝑀 +𝑣)−1. Summing these
rational intervals and using Machin’s alternating-series bounds for
𝜋 gives the displayed bounds on
𝜃∗ and its reciprocal. The
coefficient 225 −𝐽 is positive, so
the interval endpoints for 𝐶0 have
the claimed order. This verifies the displayed decimal truncations; the
program and its recorded
result are public. The proofs use the exact definitions and never
these decimal values.
Earlier criteria and changes of direction
Zudilin’s parameters and constants give a rational-base condition
that can be compared directly with the earlier height criterion. We make
that comparison before varying the parameter direction. A single family
valid at every real base greater than 1 is subject to the degree restriction
proved below.
Attribution.
Bundschuh and Väänänen proved the irrationality of 𝐹(𝑎/𝑏) on the region log𝑏/log𝑎 <1/2 −1/𝜋2 =0.3986788163576622… [6], and every base of
Theorem 2.2
with 𝑏 ≤3 is already theirs. Their
printed hypothesis for 𝛼 = −1 is
𝜆 <(1/2 +1/𝜋2)−1
with 𝜆 =logℎ(𝑞)/log|𝑞|.
Here the source uses 𝑞 for the
base, not its reciprocal, and
𝐸𝑞(𝑧)=∏𝑗≥1(1+𝑧𝑞−𝑗),𝐿𝑞(𝑧)=𝐸′𝑞(𝑧)𝐸𝑞(𝑧)=∑𝑗≥11𝑞𝑗+𝑧.
For 𝑞 =𝑎/𝑏 >1, 𝐸𝑞( −1) >0 and 𝐿𝑞( −1) =𝐹(𝑎/𝑏); in particular 𝛼 = −1 is not one of the excluded
zeros −𝑞𝑗. Since 𝑎,𝑏 are coprime and 𝑎 >𝑏 >0, the rational height is ℎ(𝑞) =𝑎. Thus 𝜆 =log𝑎/log(𝑎/𝑏) =1/(1 −log𝑏/log𝑎), and the printed hypothesis is equivalent to the displayed
inequality. Duverney proved another, strictly smaller, region for the
same series [14].
Zudilin remarked that his generalized 𝑞-logarithm results can be given at
non-integer rational bases under an assumption log|𝑟| >𝑐log|𝑠| for a computable
𝑐 >0, without computing a value
[9]. Zudilin’s 2004
paper supplies the forms and the exponent 𝜇 under the standing hypothesis 𝑝 =1/𝑞 ∈ℤ\{0, ±1},
and it states no rational-base result [8]. The contribution here is the rational
specialisation of the 2004 forms, with the denominator accounting and
the limit passage carried out in full, which identifies the printed
𝜇 as an admissible 𝑐 for 𝐹 itself, together with the region that
constant defines and its application to 31/4.
Where the earlier criterion stops.
Both regions are cut out by the same quantity. The published cutoff
1/2 −1/𝜋2 of [6] is the reciprocal of 𝜇BV =2𝜋2/(𝜋2 −2),
the constant Van Assche later recovered as an integer-base
irrationality-exponent bound for 𝐹(𝑝) [18], and the cutoff 𝜃∗ of Theorem 2.2 is the
reciprocal of the smaller integer-base bound 𝜇 =𝐶1/𝐶0 printed at [8]. For Zudilin’s family
this reciprocal relation uses both the exact degree limit 𝑑 =𝐶1 −𝐶0 and the stronger evaluation
bound |𝑈𝑛(𝑝)| ≤𝑝𝑊𝑛exp(𝑂𝑝(𝑛)) proved in Corollary 2.4,
together with decay exponent 𝜎 =𝐶0. A general exponential
coefficient-height bound would contribute an additional term to the
integer-base exponent estimate; it cannot simply be discarded. The
discussion following Theorem 2.5 makes that
distinction explicit. The rational-base proof clears the denominators of
the already cancelled polynomials. It does not infer value irrationality
merely by taking the reciprocal of a published exponent bound. The bases
gained are exactly the strip 𝑠𝜇 <𝑟 ≤𝑠𝜇BV, which is empty for 𝑠 =2 and 𝑠 =3 and is first occupied at 𝑠 =4 by the single coprime numerator 31. The integer comparisons and rational
bracket in Section 2.5
establish membership in the region. The irrationality conclusion in
Theorem 2.3
also uses the constructed forms and their proved analytic estimates.
This application does not improve either inherited integer-base exponent
bound.
What a larger region would require.
At 3/2 the logarithmic parameter
is
log2log3=0.6309297535714574…,
which exceeds 𝜃∗ by 0.2252467…. Theorem 2.2 gives no
conclusion when log𝑏/log𝑎 ≥𝜃∗. The same argument can apply to another family
once its polynomial integrality, degrees and fixed-base remainder
estimates are proved. A smaller ratio of the resulting constants 𝐶1/𝐶0 would enlarge the
reciprocal-cutoff region. For example, 𝐶1/𝐶0 ≤2.4234 would give a cutoff
greater than 0.4126 and admit 29/4. An integer-base
irrationality-exponent bound alone does not supply the polynomial data
needed for this specialisation. The existing formal proofs establish
irrationality and measure bounds for the constructed forms; they do not
supply a different family whose divided remainder is small and nonzero
at 3/2.
The next restriction concerns one polynomial family whose estimates
hold at every fixed 𝑥 >1, with
the same leading constants but possibly base-dependent error terms. This
quantifier is essential: the proof chooses a large integer base at which
remainder decay would outpace coefficient growth. Estimates only at
3/2, or for a different family at
each base, do not permit that choice. The 2004 family satisfies the
hypotheses. The conclusion concerns forms in 𝐹(𝑥) and 1, not simultaneous forms in several
independent target values. Here height means the largest absolute
coefficient. To compare it with the sum of the absolute coefficients,
note that for a polynomial of degree at most 𝑑,
max𝑗|𝑝𝑗|≤∑𝑗|𝑝𝑗|≤(𝑑+1)max𝑗|𝑝𝑗|.
For a nonzero polynomial of degree 𝑑 =𝑂(𝑛2), the logarithms of these norms
differ by 𝑂(log𝑛). They have the
same leading quadratic growth rate, but the literal zero-height
conditions are not identical: 1 +𝑋
has maximum coefficient 1 and
coefficient sum 2. In particular,
when ℎ =0, the displayed bound ℎ𝑛2(1 +𝑜(1)) is zero, not an arbitrary
𝑜(𝑛2) term. The proof below also
works with the additive bound ℎ𝑛2 +𝑜(𝑛2); its evaluation estimate
absorbs the 𝑂(log𝑛) difference.
Alternatively, either norm convention implies the hypothesis for the
other norm after replacing ℎ by any
larger positive constant. The degree conclusion is independent of that
replacement. In the rational-base conclusions, write 𝑎/𝑏 with integers 𝑎 >𝑏 ≥1. The estimates hold without
coprimality; a reduced representation gives the smaller
denominator-clearing factor.
Theorem 2.5 (a degree restriction for estimates valid
at every base). Let (𝑈𝑛,𝑉𝑛) ∈ℤ[𝑥]2 be a sequence such
that, for constants 𝜎,𝛿 >0 and ℎ ≥0 independent of 𝑛 and of the base,
Λ𝑛(𝑥) :=𝑈𝑛(𝑥)𝐹(𝑥) −𝑉𝑛(𝑥) ≠0 for
every real 𝑥 >1;
deg𝑈𝑛,deg𝑉𝑛 ≤𝛿𝑛2(1 +𝑜(1));
the coefficient heights satisfy
logmax(𝐻(𝑈𝑛),𝐻(𝑉𝑛))≤ℎ𝑛2(1+𝑜(1)),
where 𝐻(𝑃)
is the largest absolute value of a coefficient of 𝑃;
the remainders satisfy
log|Λ𝑛(𝑥)|=−𝜎𝑛2log𝑥(1+𝑜(1))
for every real 𝑥 >1.
Put 𝑑𝑛 :=max(deg𝑈𝑛,deg𝑉𝑛). Then 𝜎 ≤𝛿, and for every fixed
rational base 𝑎/𝑏 >1,
lim sup𝑛→∞𝑛−2log|
|
|𝑏𝑑𝑛Λ𝑛(𝑎/𝑏)|
|
|≤𝛿log𝑏−𝜎log(𝑎/𝑏).
Consequently the homogenised
forms tend to zero whenever log𝑏/log𝑎 <𝜎/(𝜎 +𝛿), a sufficient region whose cutoff
is at most 1/2. If the actual
degrees satisfy 𝑑𝑛/𝑛2 →𝑑,
then 𝑑 ≥𝜎 and the limit
exists and equals 𝑑log𝑏 −𝜎log(𝑎/𝑏); in that case the forms tend to zero below
log𝑏/log𝑎 =𝜎/(𝜎 +𝑑) and
their absolute values tend to infinity above it, so the exact-degree
case has no decaying homogenised forms at 3/2.
Proof. The coefficient-height bound controls evaluation at
an integer base. For every fixed 𝑝 >1,
|𝑈𝑛(𝑝)|,|𝑉𝑛(𝑝)|≤(𝑑𝑛+1)max(𝐻(𝑈𝑛),𝐻(𝑉𝑛))𝑝𝑑𝑛≤exp((ℎ+𝛿log𝑝)𝑛2+𝑜(𝑛2)).
Here log(𝑑𝑛 +1) =𝑜(𝑛2) by the degree bound.
This is where the coefficient-height hypothesis is needed.
Suppose 𝜎 >𝛿. To
make remainder decay beat coefficient growth, choose an integer 𝑝 ≥2 with (𝜎 −𝛿)log𝑝 >ℎ and put 𝑢𝑛 =𝑈𝑛(𝑝), 𝑣𝑛 =𝑉𝑛(𝑝) and ℓ𝑛 =𝑢𝑛𝐹(𝑝) −𝑣𝑛. The integer
determinant eliminates 𝐹(𝑝); the
evaluation bound and hypothesis (4) give
𝑢𝑛𝑣𝑛+1−𝑢𝑛+1𝑣𝑛=𝑢𝑛+1ℓ𝑛−𝑢𝑛ℓ𝑛+1=𝑜(1).
Indeed, each product on the right has absolute value at most exp((ℎ +(𝛿 −𝜎)log𝑝)𝑛2 +𝑜(𝑛2)). The expression on the left is an integer, so it
is eventually zero. Also 𝑢𝑛 ≠0
eventually, since 𝑢𝑛 =0 would make
ℓ𝑛 = −𝑣𝑛 a nonzero integer of
absolute value less than 1. Thus
𝑣𝑛/𝑢𝑛 is eventually a fixed
rational number 𝑟. If 𝐹(𝑝) =𝑟, then ℓ𝑛 =0; otherwise |ℓ𝑛| =|𝑢𝑛| |𝐹(𝑝) −𝑟| ≥|𝐹(𝑝) −𝑟|. Both
contradict the nonzero remainders tending to zero. Hence 𝜎 ≤𝛿.
For a fixed rational base 𝑎/𝑏 >1, taking logarithms gives
𝑛−2log|𝑏𝑑𝑛Λ𝑛(𝑎/𝑏)|=𝑑𝑛𝑛2log𝑏−𝜎log(𝑎/𝑏)+𝑜(1).
Hypothesis (2)
yields the stated upper limit and sufficient region. Since 𝜎 ≤𝛿, its cutoff is at most
1/2. If 𝑑𝑛/𝑛2 →𝑑, apply the preceding
integer-base argument with 𝑑 +𝜀 in place of 𝛿 for every 𝜀 >0 to obtain 𝑑 ≥𝜎. The displayed identity then
gives the exact limit. Its sign is that of (𝜎 +𝑑)log𝑏 −𝜎log𝑎, which
proves both assertions away from equality. At 3/2 this sign is positive because log2/log3 >1/2 ≥𝜎/(𝜎 +𝑑). ◻
Corollary 2.6 (nondecay when 𝑏 <𝑎 <𝑏2). Under the hypotheses
of Theorem 2.5, for positive
integers 𝑎,𝑏 with 𝑏 <𝑎 <𝑏2, the undivided forms 𝑏𝑑𝑛Λ𝑛(𝑎/𝑏) do not tend to
zero. No limit of 𝑑𝑛/𝑛2 is
assumed.
Proof. Write 𝑥 =𝑎/𝑏 and
suppose 𝐶𝑛 =𝑏𝑑𝑛Λ𝑛(𝑥) →0. Since 𝐶𝑛 ≠0 and |𝐶𝑛| ≤1 eventually, logarithms and the
remainder asymptotic at 𝑥 give the
degree bound
𝑑𝑛log𝑏≤−log|Λ𝑛(𝑥)|=𝜎log𝑥𝑛2+𝑜(𝑛2).
Set 𝑐 =𝜎log𝑥/log𝑏. Since 1 <𝑥 <𝑏, we have 0 <𝑐 <𝜎, and the displayed
inequality gives 𝑑𝑛 ≤(𝑐 +𝜀)𝑛2 eventually for
each 𝜀 >0. Apply
Theorem 2.5
to the same polynomial family with degree upper rate 𝑐: its height bound, nonvanishing and
all-base remainder asymptotics are unchanged. This gives 𝜎 ≤𝑐, contradicting 𝑐 <𝜎. ◻
This strengthens the failure of a sufficient-cutoff test to an
exclusion of decay under the stated all-base hypotheses. It does not
supply an actual-degree limit or assert divergence. If 𝑑𝑛/𝑛2 →𝑑, the separate exact-degree
result gives the stronger conclusion |𝑏𝑑𝑛Λ𝑛(𝑎/𝑏)| →∞ in the
same strict region. Equality 𝑎 =𝑏2
remains unclassified. The corollary concerns the undivided forms; it
does not exclude base-dependent content division or other irrationality
methods outside its hypotheses.
A degree bound alone would not supply the evaluation estimate: even
degree-zero polynomials can have arbitrarily large integer coefficients.
This explains the height hypothesis (3), without establishing that it
cannot be weakened or omitted. At log𝑏/log𝑎 =𝜎/(𝜎 +𝑑), the normalised logarithm is zero
and the hypotheses decide neither behaviour. Theorem 2.5 is a
restriction on the stated families, not on all Padé constructions.
There is also a distinction between the degree cutoff and an
irrationality-exponent estimate at a fixed integer base 𝑝 ≥2. The hypotheses above give
|𝑈𝑛(𝑝)|≤exp((ℎ+𝛿log𝑝)𝑛2+𝑜(𝑛2)),|Λ𝑛(𝑝)|=exp(−𝜎log𝑝𝑛2+𝑜(𝑛2)).
Apply the
integer-form argument in the proof of Corollary 2.4,
with coefficient growth rate ℎ +𝛿log𝑝 and remainder decay rate 𝜎log𝑝. It gives
𝜇irr(𝐹(𝑝))≤1+𝛿𝜎+ℎ𝜎log𝑝.
Thus the
reciprocal 𝜎/(𝜎 +𝛿)
of the degree expression 1 +𝛿/𝜎 is not, under these
hypotheses alone, the reciprocal of the exponent bound furnished by that
argument. To obtain the latter identification it suffices to prove the
stronger evaluated estimate |𝑈𝑛(𝑝)| ≤exp(𝛿log𝑝 𝑛2 +𝑜(𝑛2)). This is separate from bounding the polynomial’s
coefficients by exp(𝑂(𝑛2)).
For the family of Section 2.1 the
fourth hypothesis is the size estimate proved there and the second
is (8). The
third is proved next, so Theorem 2.5 applies to
that family.
Lemma 2.7 (coefficient heights of the constructed
polynomials). There is a constant ℎ with logmax(𝐻(𝑈𝑛),𝐻(𝑉𝑛)) ≤ℎ𝑛2 for every 𝑛 ≥1,
where 𝑈𝑛 and 𝑉𝑛 are the polynomials of (7).
Proof. For a polynomial or Laurent polynomial 𝑃, write ‖𝑃‖ for the sum of the absolute values
of its coefficients. Then ‖𝑃𝑄‖ ≤‖𝑃‖ ‖𝑄‖; for an ordinary
polynomial, 𝐻(𝑃) ≤‖𝑃‖. This
convention includes the Laurent monomials in 𝑐𝑛,𝑘.
By Lemma 2.1 every
𝜈𝑛,𝑙 is 0 or 1, so 𝐷𝑁/Ω𝑛 =∏𝑙∈𝑆Φ𝑙 over a
subset 𝑆 ⊆{1,…,𝑁}. A
monic polynomial with roots 𝜁1,…,𝜁𝑑 on the unit circle
has coefficient norm at most 2𝑑:
expanding its linear factors bounds the sum of the absolute coefficients
by ∏𝑑𝑗=1(1 +|𝜁𝑗|) =2𝑑.
Hence ‖Φ𝑙‖ ≤2𝜑(𝑙)
and
‖
‖
‖𝐷𝑁Ω𝑛‖
‖
‖≤2∑𝑙≤𝑁𝜑(𝑙)≤2225𝑛2.
For 𝐴𝑛, the Gaussian binomial [𝑚𝑟]𝑋 has
nonnegative coefficients summing to (𝑚𝑟), so ‖𝑐𝑛,𝑘‖ ≤(𝑘−1𝑎1−1)(𝛽𝑛−𝑎2−1𝛽𝑛−𝑘−1) ≤22𝛽𝑛
by (3),
and summing the at most 𝛽𝑛
terms of (4) gives
‖𝐴𝑛‖ ≤𝛽𝑛22𝛽𝑛.
Hence ‖𝑈𝑛‖ ≤‖𝐷𝑁/Ω𝑛‖ ‖𝐴𝑛‖ ≤𝑒𝑂(𝑛2) and 𝐻(𝑈𝑛) ≤𝑒𝑂(𝑛2).
For 𝑉𝑛, bound it on the circle
|𝑧| =2 and use Cauchy’s estimate
𝐻(𝑉𝑛) ≤max|𝑧|=2|𝑉𝑛(𝑧)|: each
coefficient satisfies |𝑣𝑖| ≤2−𝑖max|𝑧|=2|𝑉𝑛(𝑧)|. The
bound also holds for the zero polynomial. On that circle |𝑧𝑙 −1| ≥2𝑙 −1 ≥1, so each of the
at most 𝛽𝑛 +𝑎0 inner terms
of (5)
has modulus at most 1; also |𝑐𝑛,𝑘(𝑧)𝑧𝑎0𝑘| ≤‖𝑐𝑛,𝑘‖ 2𝐾𝑛
and |𝐷𝑁(𝑧)/Ω𝑛(𝑧)| ≤‖𝐷𝑁/Ω𝑛‖ 2225𝑛2 ≤𝑒𝑂(𝑛2), while |𝑧−𝑀𝑛| ≤1. There are 𝑂(𝑛) outer summands, each with 𝑂(𝑛) inner terms. After multiplication by
the normalising factor, each term is bounded by 𝑒𝑂(𝑛2), since 𝐾𝑛 =𝑂(𝑛2). Summing the 𝑂(𝑛2) terms preserves this bound. Hence
max|𝑧|=2|𝑉𝑛(𝑧)| ≤𝑒𝑂(𝑛2)
and 𝐻(𝑉𝑛) ≤𝑒𝑂(𝑛2). ◻
With Lemma 2.7,
Zudilin’s family satisfies all four hypotheses of Theorem 2.5, with exact
degree limit 𝑑 =𝐶1 −𝐶0 by (10), and
decay exponent 𝜎 =𝐶0 because
logΛ𝑛(𝑥) = −(𝐾𝑛 −𝑊𝑛)log𝑥 +𝑜(𝑛2) for each fixed real 𝑥 >1 by the size estimate of
Section 2.4. For it
𝜎/(𝜎 +𝑑) =𝜃∗ and
(𝜎 +𝑑)/𝜎 =𝜇. The stronger
bound |𝑈𝑛(𝑝)| ≤𝑝𝑊𝑛exp(𝑂𝑝(𝑛)) from Corollary 2.4
removes the extra height term at each integer base. Within this family
the rational-base threshold is therefore the reciprocal of the proved
integer-base irrationality-exponent bound.
Examples of rational bases.
Among reduced 𝑎/𝑏 with 1 ≤𝑏 <𝑎 ≤60, the region of
Theorem 2.2
has 137 members, of which 78 are non-integral. The two largest
admitted logarithmic ratios belong to 53/5 and 31/4, respectively 0.000313 and 0.001985 below 𝜃∗; the smallest excluded ratio is
that of 52/5, namely 0.4073243836…, which exceeds the
cutoff by 0.001641. A calculation
with rational bounds for logarithms and for the cutoff checks all 1101 reduced fractions in the stated
range, these rounded margins and the four fixed-denominator comparisons
below (program,
result).
The bases in this region and outside the region of [6] are those in the strip
𝑠𝜇 <𝑟 ≤𝑠𝜇BV, which is empty for 𝑠 =2 and 𝑠 =3, is {31} for 𝑠 =4, and is {53,54,56} for 𝑠 =5. The strip is infinite: its width
𝑠𝜇BV −𝑠𝜇
eventually exceeds 𝑠, so for every
large enough denominator it contains an integer congruent to 1 modulo 𝑠. Hence 31/4 is the member of the strip with
least denominator and least numerator.
A certified finite parameter search.
The parameter ratios (14,12,14;27) are Zudilin’s [8]. They maximise 𝐶0/𝐶1 in the following finite box:
positive integer parameters (𝛼0,𝛼1,𝛼2;𝛽) with
every entry at most 30, greatest
common divisor 1, and
𝛼1≤𝛼2,𝛼1+𝛼2<𝛽≤𝛼0+𝛼2.
These are the
source’s parameter inequalities [8], with a bound imposed for enumeration.
The definitions of 𝐶0,𝐶1 and
their floor function are reproduced in Section 10. There are
exactly 37,533 tuples. Exactly
two attain the maximum: (14,12,14;27) and (15,12,13;26). Both give 𝜃∗, although they are distinct
primitive directions.
The enumeration and comparisons are certified by rational intervals.
The fractions 𝑗/𝑐 with 1 ≤𝑐 ≤30 partition [0,1) into 278 half-open intervals. Every floor
function occurring in the search is constant on each interval, and the
first interval contributes zero. On each remaining interval [𝑢,𝑣), the integral is a sum of positive
differences (𝑘 +𝑢)−2 −(𝑘 +𝑣)−2,
weighted by 0 or 1. With 𝑀 =256, the tail lies between
(𝑀+𝑢)−1−(𝑀+𝑣)−1and(𝑀+𝑢)−1−(𝑀+𝑣)−1+(𝑀+𝑢)−2−(𝑀+𝑣)−2.
This follows by
comparing the positive decreasing summand with its integral. Outward
rounding of rational numbers and Machin’s bounds for 𝜋 give, for each of the two maximisers,
0.40568302137302<𝐶0/𝐶1<0.40568302139506.
Every other tuple has 𝐶0/𝐶1 <0.40563943278333. The
intervals therefore separate these two candidates from all other tuples,
without relying on floating-point ordering.
Their exact equality is not inferred from overlapping intervals.
Write 𝜔𝐴,𝜔𝐵 for their
step functions in the order just listed, and let 𝐽𝐴,𝐽𝐵 be their integrals against 𝑑( −𝜓1) on [0,1]. The floor formulas give
𝜔𝐵(𝑢)−𝜔𝐴(𝑢)=⌊13𝑢⌋+⌊15𝑢⌋−2⌊14𝑢⌋.
For
every positive integer 𝑐,
telescoping the 𝑐 intervals and
splitting the defining trigamma series into residue classes gives
∫10⌊𝑐𝑢⌋𝑑(−𝜓1(𝑢))=𝑐−1∑𝑗=1𝜓1(𝑗/𝑐)−(𝑐−1)𝜓1(1)=𝑐(𝑐−1)𝜋26.
Hence 𝐽𝐵 −𝐽𝐴 =𝜋2/3. Both directions have
𝑚 =15 and 𝐶1 =1091/2, while the quadratic part of
𝐶0 before the 3/𝜋2 correction is 266 for 𝐴 and 265 for 𝐵. Its decrease by 1 exactly cancels the increase 3(𝐽𝐵 −𝐽𝐴)/𝜋2 =1. Thus 𝐶0 also agrees.
A calculation compares every tuple of the box with interval bounds,
and a second implementation repeats it with 512 summands before the tail and a
different enumeration order; both are in one
program, with its recorded
result. The calculation proves optimality only in the displayed
finite box. No bound on a direction outside that box follows, and this
calculation is not needed for the irrationality theorem.
The two-coordinate forms in 1
and 𝐹(𝑝) should be distinguished
from simultaneous approximation to two target values. Postelmans and Van
Assche prove the ℚ-linear
independence of 1,𝜁𝑞(1),𝜁𝑞(2) for 𝑞 =1/𝑝 with integer 𝑝 ≥2 [30]. Their confluent multiple
little 𝑞-Jacobi construction has
two orthogonality conditions; its common integer normalisation and
nonvanishing argument are in Section 6, especially (6.1)–(6.4). That
theorem treats two target values and retains the integer inverse-base
restriction. It supplies neither the coefficient pairs nor the all-base
estimates assumed in Theorem 2.5; it is not an
application at 3/2.
Finite calculations
The polynomial reconstruction below determines the forms for 𝑛 =1,2,3,4. Together with the exact
comparison of all directions in the preceding finite box, it provides
small cases against which to check the general formulas. The two
calculations are available, along with the other finite calculations, in
the reproduction
guide, and a single
script reruns them and compares each with its recorded result. The
historical high-precision evaluations were not rerun. None of these
finite calculations proves a statement for all indices, and none is a
Lean proof. The tests for 𝑁 ≤8 and
the rational interval certificate are described separately.
The public
reproduction guide gives the command and dependency pin for the
direction-search program. Run it with --bound 30 and
the output path named there; adding --check compares the
result without replacing the stored
search results. The stored record specifies mpmath 1.3.0 at thirty
decimal digits. Its exact enumeration count is 37,533, but its ordering by 𝐶0/𝐶1 is numerical and has no interval
certificate in that historical record. The separate rational certificate
above verifies the maximisers in the stated finite box; the archived
program itself still uses numerical comparisons.
An exact integer calculation (program,
every
coefficient) reconstructs the forms of Section 2.1 directly
in ℤ[𝑋] from the displayed source
formulas. It checks division by Ω𝑛 and 𝑋𝑀𝑛 with zero remainder and computes
all coefficients of 𝑈𝑛,𝑉𝑛. The
exact degrees are
𝑛1234𝐾𝑛587226450328891𝑊𝑛333131529445220deg𝐷𝑁722786281102degΩ𝑛2594219380.
In each case deg𝑉𝑛 =𝑊𝑛 −1 and both leading coefficients are ( −1)𝑛. Independently expanding 𝐹(1/𝑞) =∑𝑗≥1𝜏(𝑗)𝑞𝑗 checks the
vanishing coefficients below order 𝐾𝑛 −𝑊𝑛 in 𝑈𝑛(1/𝑞)𝐹(1/𝑞) −𝑉𝑛(1/𝑞) and its next
twelve coefficients against the positive source expression. Exact
rational evaluation at 31/4, 3 and 7/2 also checks homogenisation; at the
two noninteger bases, the power 𝑏𝑊𝑛−1 fails to clear 𝑈𝑛(𝑎/𝑏), as predicted by the general
leading-coefficient argument.
A separate historical numerical report evaluated the remainder
identity at those three bases to relative accuracy below 10−39 at 𝑛 =3. It reported positivity of ˆΛ𝑛 and agreement with the
bounds on 𝐻𝑛 in Section 2.4. These
high-precision real evaluations were not reproduced by the exact
polynomial calculation just described.
The historical constant evaluation used 𝜔, the thirteen intervals of
Lemma 2.1 and
forty-digit trigamma values. It reported
𝐽=77.94318447500909…,𝐶0=221.30008816500502…,
and 𝐶1/𝐶0 =2.46497868357497…, agreeing
with the source’s printed precision [8]. The rational interval estimate stated
earlier, rather than these rounded digits, supports the numerical
inequality.
The main term 𝐾𝑛log𝑏 −(𝐾𝑛 −𝑊𝑛)log𝑎 at 31/4 is negative for
every 1 ≤𝑛 ≤400, as verified by
exact rational logarithm enclosures and exact totient sums (program,
result).
Dividing by 𝑛2 gives, to three
decimal places, −58.478, −10.280, −4.297, −3.863 at 𝑛 =1,10,100,400. This finite sign check
does not assert negativity at every index. The proved limit is 𝐶1log4 −𝐶0log31 = −3.718…; the
elementary convergence-rate bound is 𝑂(log2(𝑛 +2)/𝑛). Indeed, summing the
𝑂(𝑦log(2𝑦)) endpoint errors over
the floor blocks with 𝑘 ≤𝑛 gives
𝑂(𝑛log2(𝑛 +2)); the remaining
main-term tail is 𝑂(1) since its
summands are 𝑂(𝑛2/𝑘3). The linear
terms of 𝑀𝑛 add 𝑂(𝑛). The stronger rate 𝑂(1/𝑛) does not follow from these
estimates. Only the limit enters Theorem 2.2.
For orientation, the all-rank order and leading-coefficient formulas
of Theorem 3.4
give the following first seven values:
𝑁1234567ord01514305591lc161084320324000408240008001504000.
Power comparisons and Hankel determinants
Three integer comparisons will be used to estimate residue counts and
scalar exponents. The first gives log3/log2 <65/41 and shows that 65 is the least integer 𝑞 with 341 <2𝑞; the inequality 2129 <382 checks the failure of
the subset count at depth 41 one
row earlier. They determine numerical thresholds, leaving the
coefficient and remainder hypotheses to be checked for any family of
approximants. Readers interested first in the determinant asymptotic may
begin at Section 3.1.
Theorem 3.1 (sharp power bracket). One has
264<341<265.
Consequently
4165<log2log3,log3log2<6541.
Proof. Direct evaluation gives
264=18446744073709551616,341=36472996377170786403,265=36893488147419103232.
Taking logarithms of the upper bound gives 41log3 <65log2. Dividing this
inequality by 65log3 and by 41log2, respectively, gives the two
stated logarithmic bounds; both divisors are positive. ◻
The upper power bound gives log2/log3 >41/65, a sharper lower
bound than 81/200. In particular,
41/65 −2/5 =3/13. Combining this with
1/2 −1/𝜋2 <2/5 gives the first
gap below; the same logarithmic lower bound is then compared with the
rectangular expression.
For 𝜌 ≥0 and 𝜎 ≥1 +𝜌, define
ΘHP(𝜌,𝜎)=(1+𝜌2)/2+𝜎−3𝜎2/𝜋2(1+𝜌)2/2+𝜎(1+𝜌)+(1+𝜌2)/2+𝜎.
The
denominator is positive on this domain.
Corollary 3.2 (gaps between the stated logarithmic
thresholds). For every 𝜌,𝜎 ∈ℝ with 0 ≤𝜌 and 1 +𝜌 ≤𝜎,
313<log2log3−(12−1𝜋2),313<log2log3−ΘHP(𝜌,𝜎),
where ΘHP is the
rectangular exponent threshold. Moreover
log3/log2−13<841.
Proof. The first inequality follows from 41/65 −2/5 =3/13, Theorem 3.1, and
1/2 −1/𝜋2 <2/5. The polynomial
calculation in Section 10 proves ΘHP(𝜌,𝜎) ≤1/2 −1/𝜋2
on the stated domain, which gives the second inequality. The final
inequality is a direct rearrangement of log3/log2 <65/41. ◻
The next inequalities compare two proposed savings in the denominator
exponent with the exponent 4𝑁3 −3𝑁2 before division. Here 𝐸 denotes the exponent saved. The
statement assumes the bounds 𝐸 ≤𝑁3 −𝑁 or 𝐸 ≤2𝑁3 −𝑁; it
does not derive them for a polynomial family. Under either bound, the
saving is less than 39/41 of the
original exponent. Thus these bounds alone cannot justify the reduction
required by this model.
Theorem 3.3 (bounds for two proposed degree savings).
For every integer 𝑁 >0,
41(𝑁3−𝑁)<39(4𝑁3−3𝑁2).
For
every integer 𝑁 ≥2,
41(2𝑁3−𝑁)<39(4𝑁3−3𝑁2).
Hence the
same strict inequalities hold with the left side replaced by 41𝐸 whenever, respectively, 𝐸 ≤𝑁3 −𝑁 or 𝐸 ≤2𝑁3 −𝑁.
Proof. After subtraction, the first inequality is
𝑁(115𝑁2−117𝑁+41)>0,
whose quadratic
factor is 115(𝑁 −1)2 +113(𝑁 −1) +39,
positive for 𝑁 ≥1. The second
becomes
𝑁(74𝑁2−117𝑁+41)>0.
Its
quadratic factor is 74(𝑁 −2)2 +179(𝑁 −2) +103, positive for
𝑁 ≥2. The assertions for 𝐸 follow by monotonicity. ◻
An application of these degree bounds must separately prove that its
proposed divisor satisfies one of the stated bounds. These inequalities
do not rule out additional factors caused by cancellation in a
determinant, a different choice of integral forms, or another proof of
irrationality at 3/2.
The sharp 𝑞-order of the
normalised Hankel determinant
We begin with the formal expansion of Zudilin’s normalised Hankel
determinant at 𝑥 =𝑧 =1. Determining
its first nonzero term is a calculation in power series in 𝑞; an interpretation as a divisor after
integer evaluation would additionally require an integral normalisation
and a divisibility argument. Zudilin constructs the determinant by
combining the Padé-type approximations of Bundschuh and Zudilin [12] with
Bézivin’s method as developed in [13]; see [9]. His passage from the 𝑞-order to the size of the determinant
borrows the proofs of [13], as he notes in [9].
The source writes ℓ𝑝(𝑥,𝑧) =𝑥∑𝑟≥1𝑧𝑟/(𝑝𝑟 −𝑥), so
ℓ𝑝(1,1) =𝐹(𝑝). Here 𝑝 =𝑞−1 and 𝑥,𝑧 are auxiliary parameters, not the
base. Write 𝑁 for the Hankel rank.
With 𝑞 a formal variable, the
moments and determinant in question are
𝑣∗𝑚=∑𝑡≥0𝑞(𝑚+1)𝑡(𝑞;𝑞)3𝑚(𝑞𝑡+1;𝑞)𝑚(𝑞𝑚+𝑡+1;𝑞)𝑚+1,𝑉∗𝑁=det(𝑣∗𝑖+𝑗)0≤𝑖,𝑗<𝑁.
All product
denominators have constant term 1,
so their inverses exist in ℤ[[𝑞]].
The order of a nonzero series is the least exponent of 𝑞 with a nonzero coefficient.
Theorem 3.4 (the first nonzero term at every rank).
For every rank 𝑁, the
normalised Hankel determinant 𝑉∗𝑁 of [9], evaluated at 𝑥 =𝑧 =1, has
ord𝑞𝑉∗𝑁=𝑁(𝑁−1)(2𝑁−1)6,leading coefficient(𝑁!)2(𝑁+1)!2𝑁.
The source proves the order inequality and also gives |𝑉∗𝑁(𝑞)| ≤|𝑞|𝑁3/3exp(𝑂(𝑁2)),
referring to additional estimates for the passage from formal order to
analytic size [9].
Equality in the order bound rules out a further initial power of 𝑞 at 𝑥 =𝑧 =1; it does not itself prove a
fixed-𝑞 estimate. For 0 <𝑞 <1, the positive-measure
argument below gives both positivity and a two-sided comparison with the
leading term, with logarithmic error 𝑂𝑞(𝑁). It refines the subleading
control, not the cubic exponent of 𝑞.
The row identity.
We choose row operations whose first surviving coefficients can be
computed explicitly. The auxiliary lemma applies to more general
products than the moments above; its use here is to identify the
coefficient that remains after each row operation.
Work over 𝐴 =ℤ[[𝑞]]. Let 𝐻(𝑋) =1 +∑𝑠≥1𝑎𝑠(𝑞)𝑋𝑠. For
nonnegative integers 𝑚,𝑡, put
𝑊𝑚(𝑡)=𝑞(𝑚+1)𝑡𝑚∏𝑟=1𝐻(𝑞𝑟),𝐷𝑗=𝑗−1∏𝑟=0(𝐼−𝑞𝑟N),𝐸(𝑚,𝑗)=𝑚𝑗−𝑗(𝑗−1)2,
where N is the backward shift (N𝑓)𝑚 =𝑓𝑚−1 in the index
𝑚. Thus 𝐷𝑗 is Zudilin’s backward-difference
operator in [9].
Write ¯𝐻 =𝐻mod𝑞 and ℎ𝑟 =[𝑋𝑟]¯𝐻(𝑋)−1, with ℎ𝑟 =0 for 𝑟 <0 and ℎ0 =1.
The lemma allows arbitrary coefficients 𝑎𝑠(𝑞) ∈ℤ[[𝑞]]; the only normalisation
imposed on 𝐻 is its constant term
1. It therefore covers the product
series used below, but not an unnormalised series with a different
constant term. All statements here are coefficientwise identities of
formal series, with no analytic convergence assumption. For a general
𝐻, the coefficient in the lemma can
vanish. The application below computes it for the chosen products and
proves the required nonvanishing.
Lemma 3.5 (a coefficient of each transformed row).
For 𝑚 ≥𝑗 ≥0 one has 𝐷𝑗𝑊𝑚(𝑡) ∈𝑞𝐸(𝑚,𝑗)𝐴 and
[𝑞𝐸(𝑚,𝑗)]𝐷𝑗𝑊𝑚(𝑡)=(−1)𝑗ℎ𝑗−𝑡.
Proof. Let 𝑒𝑢 denote a
formal basis vector indexed by 𝑢 ≥0, and suppress the argument 𝑞 in 𝑎𝑠(𝑞). We use the transition rule
Φ𝑒0=∑𝑠≥1𝑎𝑠𝑒𝑠−1,Φ𝑒𝑢=(𝑞𝑢−1)𝑒𝑢−1+𝑞𝑢∑𝑠≥1𝑎𝑠𝑒𝑢+𝑠−1(𝑢>0).
In Φ𝑗𝑒𝑡, a coefficient means
the sum of the weights of length-𝑗
paths from 𝑡 to the specified
endpoint. Each step lowers its index by at most one. A path ending at
𝑢 therefore visits only indices at
most max(𝑡,𝑢 +𝑗), so each
coefficient is a finite sum. No action on the algebraic direct sum is
assumed.
For 𝑚 ≥1, a direct expansion
gives
𝑊𝑚(𝑢)−𝑊𝑚−1(𝑢)=𝑞𝑚∑𝑣(Φ𝑒𝑢)𝑣𝑊𝑚−1(𝑣),
since both sides equal
𝑞𝑚𝑢𝑚−1∏𝑟=1𝐻(𝑞𝑟)(𝑞𝑢𝐻(𝑞𝑚)−1).
For the induction step take 𝑚 ≥𝑗 +1 and note that 𝐸(𝑚,𝑗) −𝐸(𝑚 −1,𝑗) =𝑗. Applying 𝐼 −𝑞𝑗N to 𝑞𝐸(𝑚,𝑗)𝑊𝑚−𝑗(𝑢) therefore gives
𝑞𝐸(𝑚,𝑗)(𝑊𝑚−𝑗(𝑢) −𝑊𝑚−𝑗−1(𝑢)). The
preceding identity contributes one further factor 𝑞𝑚−𝑗, and 𝐸(𝑚,𝑗) +𝑚 −𝑗 =𝐸(𝑚,𝑗 +1). Induction, starting
with 𝐷0 =𝐼, gives
𝐷𝑗𝑊𝑚(𝑡)=𝑞𝐸(𝑚,𝑗)∑𝑢(Φ𝑗𝑒𝑡)𝑢𝑊𝑚−𝑗(𝑢).(13)
The endpoint sum is also locally finite: ord𝑊𝑚−𝑗(𝑢) =(𝑚 −𝑗 +1)𝑢, so
only finitely many endpoints contribute to any fixed power of 𝑞.
Modulo 𝑞 the operator
simplifies: ¯Φ𝑒𝑢 = −𝑒𝑢−1
for 𝑢 >0, and ¯Φ𝑒0 =∑𝑠≥1𝑎𝑠(0)𝑒𝑠−1.
Put 𝑐𝑗,𝑡 =(¯Φ𝑗𝑒𝑡)0.
Then 𝑐𝑗+1,𝑡 = −𝑐𝑗,𝑡−1 for 𝑡 >0 and 𝑐𝑗+1,0 =∑𝑗+1𝑠=1𝑎𝑠(0)𝑐𝑗,𝑠−1,
the sum terminating because a state above 𝑗 cannot reach 0 in 𝑗 steps. Now 𝑐0,𝑡 =𝛿𝑡,0 =ℎ−𝑡, and if 𝑐𝑗,𝑡 =( −1)𝑗ℎ𝑗−𝑡 for all 𝑡 then 𝑐𝑗+1,𝑡 =( −1)𝑗+1ℎ𝑗+1−𝑡 for 𝑡 >0 at once, while for 𝑡 =0 the identity ¯𝐻¯𝐻−1 =1 gives ℎ𝑗+1 = −∑𝑠≥1𝑎𝑠(0)ℎ𝑗+1−𝑠 and
hence 𝑐𝑗+1,0 =( −1)𝑗∑𝑠≥1𝑎𝑠(0)ℎ𝑗+1−𝑠 =( −1)𝑗+1ℎ𝑗+1.
So 𝑐𝑗,𝑡 =( −1)𝑗ℎ𝑗−𝑡 for all
𝑗,𝑡. Since ord𝑊𝑚−𝑗(𝑢) =(𝑚 −𝑗 +1)𝑢 and
𝑚 ≥𝑗, in (13) only
the state 𝑢 =0 contributes at degree
𝐸(𝑚,𝑗), which gives both
assertions. ◻
Apply the lemma to a summand of the normalised remainder:
𝑇𝑚,𝑡=𝑞(𝑚+1)𝑡(𝑞;𝑞)3𝑚(𝑞𝑡+1;𝑞)𝑚(𝑞𝑚+𝑡+1;𝑞)𝑚+1.
Set
𝐻𝑡(𝑋)=(1−𝑋)3(1−𝑞𝑡𝑋)2(1−𝑞𝑡𝑋2)(1−𝑞𝑡+1𝑋2).
Then 𝑇𝑚,𝑡 =(1 −𝑞𝑡+1)−1𝑊𝐻𝑡𝑚(𝑡), by
the telescoping identity
𝑚∏𝑟=1𝐻𝑡(𝑞𝑟)=(𝑞;𝑞)3𝑚(1−𝑞𝑡+1)(𝑞𝑡+1;𝑞)𝑚(𝑞𝑚+𝑡+1;𝑞)𝑚+1.
The two denominator products contribute the consecutive factors 1 −𝑞𝑡+2,…,1 −𝑞𝑡+2𝑚+1. Reducing
modulo 𝑞 gives ¯𝐻𝑡 =(1 −𝑋)3 for 𝑡 >0, so ℎ(𝑡)𝑟 =(𝑟+22), and ¯𝐻0 =(1 −𝑋)4/(1 +𝑋), so ℎ(0)𝑟 =(𝑟 +1)(𝑟 +2)(2𝑟 +3)/6. The scalar
factor (1 −𝑞𝑡+1)−1 has
constant term 1. The rows are 𝑣∗𝑚 =∑𝑡≥0𝑇𝑚,𝑡. In 𝐷𝑗 only the shifts 𝑚,𝑚 −1,…,𝑚 −𝑗 occur. Since 𝑚 ≥𝑗 and ord𝑇𝑚−𝑟,𝑡 =(𝑚 −𝑟 +1)𝑡 ≥(𝑚 −𝑗 +1)𝑡,
only finitely many 𝑡 can affect any
fixed coefficient after any of these shifts. This justifies
interchanging the sum and 𝐷𝑗, and
then extracting its coefficient at degree 𝐸(𝑚,𝑗). Terms with 𝑡 >𝑗 contribute ℎ(𝑡)𝑗−𝑡 =0, so Lemma 3.5 at 𝑚 =𝑗 +ℓ, where 𝐸(𝑗 +ℓ,𝑗) =𝑗(𝑗 +1)/2 +𝑗ℓ, gives
𝐷𝑗𝑣∗𝑗+ℓ=(−1)𝑗(𝑗+1)2(𝑗+2)2𝑞𝑗(𝑗+1)/2+𝑗ℓ+𝑂(𝑞𝑗(𝑗+1)/2+𝑗ℓ+1)(𝑗,ℓ≥0).(14)
The coefficient is obtained by summing
ℎ(0)𝑗+𝑗∑𝑡=1ℎ(𝑡)𝑗−𝑡=(𝑗+1)(𝑗+2)(2𝑗+3)6+(𝑗+23)=(𝑗+1)2(𝑗+2)2.
Proof of Theorem 3.4.
The operators 𝐷𝑗 act by lower
unitriangular row operations, so they leave det(𝑣∗𝑖+𝑗)0≤𝑖,𝑗<𝑁
unchanged. By (14) the entry
in row 𝑗 and column ℓ has order 𝑗(𝑗 +1)/2 +𝑗ℓ. For 𝑁 =2, the matrix of entry orders is
(0012).
The off-diagonal product is the unique term of order one. Its
permutation sign cancels the negative leading coefficient of the second
row, giving 6𝑞 +𝑂(𝑞2). At arbitrary
rank the same argument selects the reversed permutation. For a
permutation 𝜍, the
corresponding Leibniz term has weight ∑𝑗(𝑗(𝑗 +1)/2 +𝑗𝜍(𝑗)).
By the rearrangement inequality, ∑𝑗𝑗𝜍(𝑗) is uniquely minimised
by the reversal 𝜍(𝑗) =𝑁 −1 −𝑗,
the values 𝑗 being distinct. The
minimum weight is ∑𝑗<𝑁𝑗2 =𝑁(𝑁 −1)(2𝑁 −1)/6, so
exactly one Leibniz term attains it and no cancellation is possible
there. The sign of the reversal is ( −1)𝑁(𝑁−1)/2, which cancels ∏𝑗<𝑁( −1)𝑗, and the surviving
coefficient is
𝑁−1∏𝑗=0(𝑗+1)2(𝑗+2)2=(𝑁!)2(𝑁+1)!2𝑁.
◻
A separate positive-measure estimate.
We seek positive moment weights comparable to (𝑘 +1)2(𝑘 +2)/2, with constants depending
only on 𝑞. In the determinant
expansion these constants give factors exponential in 𝑁, so they do not change its cubic
exponent of 𝑞. For fixed 0 <𝑞 <1 write 𝑃 =(𝑞;𝑞)∞, 𝑄 =(√𝑞;𝑞)∞, 𝑇 =( −1;𝑞)2∞, and
𝐺𝑞(𝑤)=1(𝑤;𝑞)3∞∑𝑡≥0𝑤𝑡(𝑞;𝑞)𝑡(𝑞𝑡𝑤2;𝑞)∞(𝑞𝑡𝑤;𝑞)2∞,𝛾𝑘=[𝑤𝑘]𝐺𝑞(𝑤),𝑐𝑘=(𝑘+1)2(𝑘+2)2.
The choice 𝑤 =𝑞𝑚+1 collects all
dependence on the moment index. Indeed, the three finite products in the
𝑡th remainder summand become
(𝑞;𝑞)𝑚=𝑃(𝑤;𝑞)∞,(𝑞𝑡+1;𝑞)𝑚=𝑃(𝑞;𝑞)𝑡(𝑞𝑡𝑤;𝑞)∞,(𝑞𝑚+𝑡+1;𝑞)𝑚+1=(𝑞𝑡𝑤;𝑞)∞(𝑞𝑡𝑤2;𝑞)∞.
Their substitution
gives 𝑣∗𝑚 =𝑃4𝐺𝑞(𝑞𝑚+1) term by
term. For fixed 𝑞 and 0 <𝑟 <1, the 𝑡th summand on |𝑤| ≤𝑟 satisfies
|
|
|
|𝑤𝑡(𝑞𝑡𝑤2;𝑞)∞(𝑞;𝑞)𝑡(𝑤;𝑞)3∞(𝑞𝑡𝑤;𝑞)2∞|
|
|
|≤(−𝑟2;𝑞)∞𝑃(𝑟;𝑞)5∞𝑟𝑡.
Indeed, (𝑞;𝑞)𝑡 ≥𝑃, each denominator product in
𝑤 has modulus at least (𝑟;𝑞)∞ >0, and the numerator
product has modulus at most ( −𝑟2;𝑞)∞. The bound is independent
of 𝑡, so the sum converges
uniformly and absolutely on each such disk. The individual products
converge there as well, since their tails are bounded by geometric
series in 𝑞. Thus 𝐺𝑞 is holomorphic for |𝑤| <1, and its Taylor series may be
evaluated at 𝑤 =𝑞𝑚+1 to obtain
the moment expansion. For formal series, the corresponding substitution
is justified coefficient by coefficient, as in the short paper. The
𝑞-binomial theorem [28]
(𝐴𝑤;𝑞)∞(𝑤;𝑞)∞=∑𝑗≥0(𝐴;𝑞)𝑗(𝑞;𝑞)𝑗𝑤𝑗(0≤𝐴≤1)
follows by comparing coefficients in (1 −𝑤)𝑅(𝑤) =(1 −𝐴𝑤)𝑅(𝑞𝑤) with 𝑅(0) =1; the series converges for |𝑤| <1 since its coefficients are at
most 𝑃−1. They are nonnegative,
and at least (𝐴;𝑞)∞ if 𝐴 <1. For 𝐴 =1 the series equals 1. Factor the numerator of the 𝑡th term using
(𝑞𝑡𝑤2;𝑞)∞=(𝑞𝑡/2𝑤;𝑞)∞(−𝑞𝑡/2𝑤;𝑞)∞(𝑞(𝑡+1)/2𝑤;𝑞)∞(−𝑞(𝑡+1)/2𝑤;𝑞)∞.
After pairing
each positive-argument factor with one denominator, the 𝑡th summand of 𝐺𝑞 becomes
𝑤𝑡(𝑞;𝑞)𝑡(𝑞𝑡/2𝑤;𝑞)∞(𝑤;𝑞)∞(𝑞(𝑡+1)/2𝑤;𝑞)∞(𝑤;𝑞)∞×(−𝑞𝑡/2𝑤;𝑞)∞(−𝑞(𝑡+1)/2𝑤;𝑞)∞(𝑤;𝑞)∞(𝑞𝑡𝑤;𝑞)2∞.
The 𝑞-binomial identity makes the two ratios
nonnegative coefficientwise; the remaining product also has nonnegative
coefficients. When 𝑡 =0, the first
ratio is 1 and every coefficient of
the second is at least 𝑄. The last
fraction has coefficients at least those of (1 −𝑤)−3. Thus the 𝑡 =0 term alone bounds 𝛾𝑘 below by 𝑄(𝑘+33).
For the upper bound, if 𝑅 has
nonnegative coefficients and 𝑅(1) ≤𝐶 <∞, convolution with a nondecreasing sequence 𝑑𝑘 is bounded by 𝐶𝑑𝑘. At 𝑡 =0, bound the second ratio
coefficientwise by 𝑃−1(1 −𝑤)−1. After extracting (1 −𝑤)−3 from the last fraction, its
remaining factor has value at 𝑤 =1
at most 𝑇𝑃−3. This gives 𝑇𝑃−4(𝑘+33). For 𝑡 ≥1, both ratios are bounded by 𝑃−1(1 −𝑤)−1. Extracting the one
factor (1 −𝑤)−1 from the last
fraction leaves a factor with value at 1 at most 𝑇𝑃−3; also (𝑞;𝑞)−1𝑡 ≤𝑃−1. The 𝑡th summand is therefore bounded
coefficientwise by 𝑇𝑃−6𝑤𝑡(1 −𝑤)−3. Summing 𝑡 ≥1 gives 𝑇𝑃−6(𝑘+23) as the bound for its
𝑘th coefficient. Consequently
𝑄3𝑐𝑘≤𝛾𝑘≤𝑇(𝑃−4+𝑃−6)𝑐𝑘.
Thus ∑𝑘≥0𝑃4𝛾𝑘𝑞𝑘𝛿𝑞𝑘 is
a finite positive measure on [0,1],
with infinitely many distinct support points and moments 𝑣∗𝑚(𝑞). In standard terminology, (𝑣∗𝑚(𝑞))𝑚≥0 is a Hausdorff moment
sequence. This statement fixes 𝑞;
the measure is not a representing measure for the coefficient sequence
𝑠𝑚(𝑝) considered in the next
subsection. A nonzero polynomial of degree less than 𝑁 cannot vanish at all of its first 𝑁 atoms; the associated Gram matrix is
positive definite. Truncate the measure to its first 𝐾 +1 atoms. At fixed rank 𝑁, each matrix entry converges as 𝐾 →∞, and the determinant converges
because it is a polynomial in those entries. Finite Cauchy–Binet and
monotone convergence of the nonnegative tuple sums therefore give
Heine’s expansion, whose integral form is reproved in [10]:
𝑉∗𝑁=∑𝑘0<⋯<𝑘𝑁−1∏𝑖(𝑃4𝛾𝑘𝑖𝑞𝑘𝑖)∏𝑖<𝑗(𝑞𝑘𝑖−𝑞𝑘𝑗)2.
Retaining the tuple 𝑘𝑖 =𝑖 and using
∏𝑁−1𝑑=1(1 −𝑞𝑑)2(𝑁−𝑑) ≥𝑃2𝑁 gives the lower bound below. For the upper bound put
𝑘𝑖 =𝑖 +𝜆𝑖, where the 𝜆𝑖 are nonnegative and
nondecreasing. Factoring the smaller power from each Vandermonde
difference gives the exact exponent
∑𝑖𝑘𝑖+2∑𝑖<𝑗𝑘𝑖=𝐵𝑁+𝑁−1∑𝑖=0(2𝑁−1−2𝑖)𝜆𝑖.
Every weight 2𝑁 −1 −2𝑖 is at least 1. Since 0 <𝑞 <1, the remaining power of 𝑞 is at most 𝑞∑𝑖𝜆𝑖. Also 𝑐𝑖+𝜆/𝑐𝑖 ≤(𝜆 +1)3.
Discard the remaining Vandermonde factors, each bounded by 1, and enlarge the nonnegative sum by
dropping the ordering restriction on the 𝜆𝑖. It now factors into 𝑁 copies of ∑𝜆≥0(𝜆 +1)3𝑞𝜆,
which gives
(𝑃6𝑄/3)𝑁𝐶𝑁𝑞𝐵𝑁≤𝑉∗𝑁(𝑞)≤[𝑃4𝑇(𝑃−4+𝑃−6)1+4𝑞+𝑞2(1−𝑞)4]𝑁𝐶𝑁𝑞𝐵𝑁.
Both
constants are positive and finite, so 𝑉∗𝑁(𝑞) >0 and log(𝑉∗𝑁(𝑞)/(𝐶𝑁𝑞𝐵𝑁)) =𝑂𝑞(𝑁),
including 𝑁 =0 under the empty
determinant convention. Here 𝑁 →∞ with 𝑞 fixed; the constants are not uniform as
𝑞 ↑1. The formal-order
calculation instead fixes 𝑁 and
expands at 𝑞 =0. No joint uniform
limit is asserted. The measure depends on 𝑞, not on the moment index or rank: one
measure represents the whole sequence at that base. This is an analytic
representation, not a denominator factor for the 2004 polynomial forms.
Section 3.2
replaces the band 𝑂𝑞(𝑁) by an
exact asymptotic with an explicit positive constant, using the same
weights.
Earlier work and the unresolved value at 3/2.
The antecedent is the inequality of [9]; the equality and the leading
coefficient are proved here. Lemma 3.5
and (14)
give that row calculation. Nothing in this subsection decides the
arithmetic nature of 𝐹(3/2).
The size of 𝑉∗𝑁 at a fixed
base
The preceding bounds leave an error of order 𝑁 in the logarithm. We now determine its
linear, logarithmic and constant terms. There are two calculations:
compare every node configuration with the first 𝑁 nodes, then multiply the resulting
moment weights. The first is independent of the particular weights under
the hypotheses below; the second produces the Lambert-value correction
for 𝑉∗𝑁. Throughout this
subsection 0 <𝑞 <1 is fixed,
and we write
𝑃=(𝑞;𝑞)∞,M(𝑞)=∏𝑑≥1(1−𝑞𝑑)−𝑑,𝐿=𝐹(1/𝑞)=∑𝑟≥1𝑞𝑟1−𝑞𝑟,
with 𝐵𝑁 =∑𝑗<𝑁𝑗2 and 𝐶𝑁 =∏𝑘<𝑁𝑐𝑘 =(𝑁!)2(𝑁 +1)!/2𝑁 as
above. Both products converge to positive finite values, and the
abbreviation 𝐿 is used only in this
subsection; it is the value at 𝑞 of
the divisor series L of
Section 10.
The estimates in this subsection concern real determinants at fixed
𝑞. Denominator valuations for the
2004 forms were treated separately in Section 2.
For 𝑎𝑘 =1, the moments are (1 −𝑞𝑚+1)−1, so Cauchy’s determinant
formula gives the model calculation
𝐷(0)𝑁:=det(11−𝑞𝑖+𝑗+1)0≤𝑖,𝑗<𝑁=𝑞𝐵𝑁Δ𝑁∏0≤𝑖,𝑗<𝑁(1−𝑞𝑖+𝑗+1),Δ𝑁=𝑁−1∏𝑑=1(1−𝑞𝑑)2(𝑁−𝑑).(15)
The denominator has limiting multiplicity 𝑑 at 1 −𝑞𝑑, while
Δ𝑁𝑃2𝑁=∏𝑑<𝑁(1−𝑞𝑑)−2𝑑∏𝑑≥𝑁(1−𝑞𝑑)−2𝑁⟶M(𝑞)2.
The convergence follows from
∑𝑑|log(1 −𝑞𝑑)| <∞ and
the bound 𝑂𝑞(𝑁𝑞𝑁) for the
logarithm of the second product. Hence
𝐷(0)𝑁∼M(𝑞)3𝑞𝐵𝑁𝑃2𝑁.(16)
Two copies of M(𝑞) come from the squared
Vandermonde and one from the Cauchy denominator. We shall compare
general weights with this exact model. Fixed displacements of the last
few node indices have weight ratios tending to 1; the polynomial bound in the theorem
controls the sum over all displacements.
Theorem 3.6 (determinants of geometric moments).
Let 𝑎𝑘 >0 satisfy, for fixed
constants 𝐶 and 𝜅,
𝑎𝑘+ℎ𝑎𝑘⟶1(𝑘→∞) for each fixed ℎ≥0,𝑎𝑘+ℎ𝑎𝑘≤𝐶(1+ℎ)𝜅(𝑘,ℎ≥0).
Put 𝑀𝑚 =∑𝑘≥0𝑎𝑘𝑞(𝑚+1)𝑘 and 𝐷𝑁 =det(𝑀𝑖+𝑗)0≤𝑖,𝑗<𝑁. Then
𝐷𝑁∼M(𝑞)3𝑞𝐵𝑁𝑃2𝑁𝑁−1∏𝑘=0𝑎𝑘(𝑁→∞).
Proof of Theorem 3.6.
We may increase 𝐶 to at least 1 and 𝜅 to at least 0. The bound 𝑎ℎ ≤𝐶𝑎0(1 +ℎ)𝜅 makes ∑𝑘≥0𝑎𝑘𝑞𝑘𝛿𝑞𝑘 a finite
positive measure with moments 𝑀𝑚.
Apply Cauchy–Binet to finite truncations. Entrywise convergence gives
convergence of their determinants, and monotone convergence applies to
the nonnegative tuple sums. Hence
𝐷𝑁=∑0≤𝑘0<⋯<𝑘𝑁−1∏𝑖<𝑁𝑎𝑘𝑖𝑞𝑘𝑖∏𝑖<𝑗<𝑁(𝑞𝑘𝑖−𝑞𝑘𝑗)2.(17)
The tuple 𝑘𝑖 =𝑖 contributes 𝑞𝐵𝑁Δ𝑁∏𝑖<𝑁𝑎𝑖. It does
not account for the whole asymptotic. For example, replace (0,1,…,𝑁 −2,𝑁 −1) by (0,1,…,𝑁 −2,𝑁). The ratio of its
contribution to that of the original tuple is
𝑞𝑎𝑁𝑎𝑁−1𝑁−1∏𝑑=1(1−𝑞𝑑+11−𝑞𝑑)2=𝑞𝑎𝑁𝑎𝑁−1(1−𝑞𝑁1−𝑞)2⟶𝑞(1−𝑞)2.(18)
Only pairs involving the moved node change, so
the product telescopes. At 𝑞 =1/2
the limiting ratio is 2: the
displaced tuple contributes twice as much asymptotically as (0,1,…,𝑁 −1).
Subtracting (0,1,…,𝑁 −1)
gives the shifts 𝜆𝑖 =𝑘𝑖 −𝑖.
Since 𝑘𝑖+1 ≥𝑘𝑖 +1, these are
nonnegative and weakly increasing; reversing their order gives a
partition. For 𝑁 =4, for example,
(0,1,3,5)⎵⎵⎵⎵(𝑘𝑖)⟼(0,0,1,2)⎵⎵⎵⎵(𝜆𝑖)⟼(2,1,0,0)⎵⎵⎵⎵(𝜇𝑗).
In general, put
𝜇𝑗 =𝜆𝑁−𝑗 for 1 ≤𝑗 ≤𝑁, so that 𝜇1 ≥⋯ ≥𝜇𝑁 ≥0. Division by
the contribution of 𝑘𝑖 =𝑖 turns the
summand for this tuple into
𝑊𝑁(𝜇)=𝑞∑𝑗≤𝑁(2𝑗−1)𝜇𝑗∏𝑗≤𝑁𝑎𝑁−𝑗+𝜇𝑗𝑎𝑁−𝑗⋅∏1≤𝑗<𝑘≤𝑁(1−𝑞𝑘−𝑗+𝜇𝑗−𝜇𝑘1−𝑞𝑘−𝑗)2.(19)
We order the indices increasingly, so their
geometric nodes decrease towards zero. The 𝑗th index from the right contributes once
through 𝑞𝑘𝑖 and twice through
each of its 𝑗 −1 pairs with later
indices in the squared Vandermonde. Its displacement therefore has
exponent 1 +2(𝑗 −1) =2𝑗 −1.
Set 𝑊𝑁(𝜇) =0 when 𝜇 has more than 𝑁 positive parts, so that every sum has
the same index set. Fix a partition with ℓ positive parts. It affects only the
last ℓ indices of (0,1,…,𝑁 −1): for instance, (2,1) affects the last two for every
𝑁 ≥2. Those indices tend to
infinity, so the weight ratios in (19)
tend to 1 by the fixed-shift
hypothesis.
The Vandermonde quotient still contains a growing number of factors,
but its dependence on 𝑁 telescopes.
The factors with 𝑗 <𝑘 ≤ℓ are
fixed, and those with 𝑗 >ℓ
equal 1. For 𝑁 ≥ℓ and each 𝑗 ≤ℓ, the remaining factors satisfy
𝑁∏𝑘=ℓ+11−𝑞𝑘−𝑗+𝜇𝑗1−𝑞𝑘−𝑗=(𝑞𝑁+1−𝑗;𝑞)𝜇𝑗(𝑞ℓ+1−𝑗;𝑞)𝜇𝑗⟶1(𝑞ℓ+1−𝑗;𝑞)𝜇𝑗.(20)
Thus each 𝑊𝑁(𝜇) has the same limit as for
constant weights.
To pass this limit through the sum over partitions, we need a bound
independent of 𝑁 that remains
summable as both the number and size of the parts grow. Only factors
with 𝑗 ≤ℓ can differ from 1. For each such 𝑗, the denominator product in the
Vandermonde quotient is at least 𝑃,
and its numerator product is at most 1. Together with the polynomial shift
bound, this gives
𝑊𝑁(𝜇)≤(𝐶𝑃−2)ℓℓ∏𝑗=1(1+𝜇𝑗)𝜅𝑞(2𝑗−1)𝜇𝑗.
Let 𝐴 =∑𝑢≥1(1 +𝑢)𝜅𝑞𝑢−1 <∞. Dropping the ordering of the positive parts,
we obtain
∑ℓ(𝜇)=ℓsup𝑁𝑊𝑁(𝜇)≤(𝐶𝑃−2)ℓℓ∏𝑗=1∑𝑢≥1(1+𝑢)𝜅𝑞(2𝑗−1)𝑢≤(𝐶𝑃−2𝐴)ℓ𝑞ℓ2.
Here 𝑞(2𝑗−1)𝑢 ≤𝑞2𝑗−1𝑞𝑢−1 and 1 +3 +⋯ +(2ℓ −1) =ℓ2. Since 𝑞 <1, the bound (𝐶𝑃−2𝐴)ℓ𝑞ℓ2 is summable
over ℓ, independently of 𝑁.
Dominated convergence gives the same limiting partition sum as for
𝑎𝑘 =1. By (15), this
sum tends to M(𝑞), the
reciprocal of the limiting Cauchy denominator. Together with Δ𝑁/𝑃2𝑁 →M(𝑞)2, it
accounts for all three copies of M(𝑞). Restoring the principal tuple gives
𝐷𝑁𝐷(0)𝑁∏𝑘<𝑁𝑎𝑘⟶1.
The model asymptotic (16)
now proves the theorem. The comparison explains why the normalised limit
retains the geometric spacing of the nodes but loses the individual
weights. ◻
We now return to 𝑎𝑘 =𝑃4𝛾𝑘. A factorisation into two
finite Gaussian multinomial sums supplies both the shift hypotheses and
the first correction to 𝑎𝑘/𝑐𝑘.
The shift hypotheses allow application of the determinant theorem; the
correction determines the product ∏𝑘<𝑁𝑎𝑘.
Proposition 3.7 (the moment weights as a product of
two finite sums). For 𝑟 ≥1
and 𝑘 ≥0 set
𝑅(𝑟)𝑘(𝑞)=∑𝑛1+⋯+𝑛𝑟=𝑘(𝑞;𝑞)𝑘∏𝑗≤𝑟(𝑞;𝑞)𝑛𝑗,
the sum being over
compositions into 𝑟 nonnegative
parts, so that 𝑅(𝑟)𝑘 is the sum
of all 𝑞-multinomial coefficients
of degree 𝑘 and length 𝑟, equivalently the multivariate
Rogers–Szegő polynomial at unit arguments [42]. These are polynomial identities in the
indeterminate 𝑞; at a prime power,
𝑟 =2 gives the Galois number
counting the subspaces of a 𝑘-dimensional space over the field of
that order, and 𝑟 =3 counts the
flags 𝑉1 ⊆𝑉2 in that
space. The source is cited for those identifications; the factorisation
below is proved here. Then
𝛾𝑘(𝑞)=𝑅(2)𝑘(𝑞)𝑅(3)𝑘(𝑞)(𝑞;𝑞)𝑘.
The product 𝑅(2)𝑘𝑅(3)𝑘 lies
in ℤ≥0[𝑞], has degree ⌊𝑘2/4⌋ +⌊𝑘2/3⌋, and has coefficient sum 6𝑘. Consequently (𝑞;𝑞)𝑘𝛾𝑘 ∈ℤ[𝑞], and the weights
𝑎𝑘 =𝑃4𝛾𝑘 satisfy
𝑃5𝑐𝑘≤𝑎𝑘≤𝑃−1𝑐𝑘(𝑘≥0),
together with 𝑎𝑘+ℎ/𝑎𝑘 ≤𝑃−6(1 +ℎ)3, so the
hypotheses of Theorem 3.6
hold with 𝜅 =3.
Proof. Write E(𝑧) =(𝑧;𝑞)−1∞. Euler’s expansion gives E(𝑧)𝑟 =∑𝑛≥0𝑅(𝑟)𝑛𝑧𝑛/(𝑞;𝑞)𝑛. We seek the product
𝑅(2)𝑘𝑅(3)𝑘 at a common
index 𝑘. Splitting 𝑘 =𝑛 +𝑗 keeps 𝑅(3)𝑘 fixed while the sum over ((𝑞;𝑞)𝑛(𝑞;𝑞)𝑗)−1 supplies 𝑅(2)𝑘/(𝑞;𝑞)𝑘. The operator 𝜕𝑞𝑓(𝑧) =(𝑓(𝑧) −𝑓(𝑞𝑧))/𝑧 produces
the needed index shift: 𝜕𝑞𝑧𝑗 =(1 −𝑞𝑗)𝑧𝑗−1 cancels the
last factor of (𝑞;𝑞)𝑗. Thus
𝜕𝑞E=E,𝜕𝑛𝑞E(𝑧)3=∑𝑗≥0𝑅(3)𝑛+𝑗(𝑞;𝑞)𝑗𝑧𝑗.
The 𝑞-Leibniz rule, obtained by induction
from the product rule, is
𝜕𝑛𝑞(𝑓𝑔)(𝑧)=𝑛∑𝑗=0[𝑛𝑗]𝑞(𝜕𝑗𝑞𝑓)(𝑞𝑛−𝑗𝑧)(𝜕𝑛−𝑗𝑞𝑔)(𝑧).
Write ℎ𝑘(𝑧) =∑𝑘𝑗=0[𝑘𝑗]𝑞(𝑧;𝑞)𝑗.
Applying the rule to E ⋅E and using E(𝑞𝑚𝑧) =(𝑧;𝑞)𝑚E(𝑧) gives 𝜕𝑘𝑞E(𝑧)2 =E(𝑧)2ℎ𝑘(𝑧); at 𝑘 =1 both
sides are E(𝑧)2(2 −𝑧).
Applying it once more, to E ⋅E2, gives
𝜕𝑛𝑞E(𝑧)3=E(𝑧)3𝑛∑𝑘=0[𝑛𝑘]𝑞(𝑧;𝑞)𝑘ℎ𝑘(𝑧),
Hence
∑𝑛≥0𝑤𝑛(𝑞;𝑞)𝑛𝜕𝑛𝑞E(𝑧)3=E(𝑤)E(𝑧)3∑𝑘≥0𝑤𝑘(𝑧;𝑞)𝑘(𝑞;𝑞)𝑘ℎ𝑘(𝑧).
The left-hand
side is ∑𝑛,𝑗≥0𝑅(3)𝑛+𝑗𝑤𝑛𝑧𝑗/((𝑞;𝑞)𝑛(𝑞;𝑞)𝑗).
On setting 𝑧 =𝑤, all pairs with the
same sum contribute to a single coefficient. Thus the coefficient of
𝑤𝑘 is 𝑅(3)𝑘∑𝑗≤𝑘((𝑞;𝑞)𝑗(𝑞;𝑞)𝑘−𝑗)−1 =𝑅(2)𝑘𝑅(3)𝑘/(𝑞;𝑞)𝑘. On the right-hand side, put 𝑧 =𝑤, expand ℎ𝑘, and write 𝑘 =𝑗 +𝑡. The identity (𝑤;𝑞)𝑗+𝑡 =(𝑤;𝑞)𝑗(𝑤𝑞𝑗;𝑞)𝑡 gives
E(𝑤)4∑𝑗≥0𝑤𝑗(𝑤;𝑞)2𝑗(𝑞;𝑞)𝑗∑𝑡≥0(𝑤𝑞𝑗;𝑞)𝑡(𝑞;𝑞)𝑡𝑤𝑡.
The inner sum
is evaluated by the 𝑞-binomial
theorem:
∑𝑡≥0(𝑤𝑞𝑗;𝑞)𝑡(𝑞;𝑞)𝑡𝑤𝑡=(𝑤2𝑞𝑗;𝑞)∞(𝑤;𝑞)∞.
Finally, (𝑤;𝑞)𝑗 =(𝑤;𝑞)∞/(𝑤𝑞𝑗;𝑞)∞
cancels two of the five factors E(𝑤), leaving
E(𝑤)3∑𝑗≥0𝑤𝑗(𝑞;𝑞)𝑗(𝑤2𝑞𝑗;𝑞)∞(𝑤𝑞𝑗;𝑞)2∞=𝐺𝑞(𝑤).
Every step holds coefficientwise, and absolutely for
|𝑤| small.
A 𝑞-multinomial coefficient has
nonnegative integral coefficients and degree ∑𝑖<𝑗𝑛𝑖𝑛𝑗. At 𝑞 =1 it equals the corresponding ordinary
multinomial coefficient. Summing over compositions gives coefficient sum
𝑟𝑘 for 𝑅(𝑟)𝑘 and hence 6𝑘 for the product. The degree is
maximised by balanced parts, which gives ⌊𝑘2/4⌋ for 𝑟 =2 and ⌊𝑘2/3⌋ for 𝑟 =3; no leading cancellation occurs
because all coefficients are nonnegative.
For the bounds, write 𝑏(𝑟)𝑘 =[𝑧𝑘](𝑧;𝑞)−𝑟∞, so that
𝑅(𝑟)𝑘 =(𝑞;𝑞)𝑘𝑏(𝑟)𝑘 and
𝛾𝑘 =(𝑞;𝑞)𝑘𝑏(2)𝑘𝑏(3)𝑘.
Euler’s expansion exhibits 𝑏(𝑟)𝑘 as an 𝑟-fold convolution of the sequence 1/(𝑞;𝑞)𝑛, whose terms lie in [1,𝑃−1]; the number of compositions of
𝑘 into 𝑟 nonnegative parts is (𝑘+𝑟−1𝑟−1), so
(𝑘+𝑟−1𝑟−1)≤𝑏(𝑟)𝑘≤𝑃−𝑟(𝑘+𝑟−1𝑟−1).
Combining these at 𝑟 =2,3 with 𝑃 ≤(𝑞;𝑞)𝑘 ≤1 and 𝑐𝑘 =(𝑘 +1)(𝑘+22) gives 𝑃5𝑐𝑘 ≤𝑎𝑘 ≤𝑃−1𝑐𝑘. The shift
bound follows from 𝑐𝑘+ℎ/𝑐𝑘 ≤(1 +ℎ)3.
It remains to show that 𝑎𝑘+ℎ/𝑎𝑘 →1 for each fixed ℎ. The two convolutions grow at least
linearly and quadratically; it suffices to bound their increments by a
constant and a linear function, respectively. Put 𝑒𝑛 =1/(𝑞;𝑞)𝑛. Since (𝑞;𝑞)𝑛+1 =(1 −𝑞𝑛+1)(𝑞;𝑞)𝑛, these
terms satisfy 1 =𝑒0 ≤𝑒1 ≤⋯ ≤𝑃−1, and the convolutions read 𝑏(2)𝑘 =∑𝑖≤𝑘𝑒𝑖𝑒𝑘−𝑖 and
𝑏(3)𝑘 =∑𝑖≤𝑘𝑒𝑖𝑏(2)𝑘−𝑖. Hence
𝑏(2)𝑘+1−𝑏(2)𝑘=∑𝑖≤𝑘𝑒𝑖(𝑒𝑘+1−𝑖−𝑒𝑘−𝑖)+𝑒𝑘+1,𝑏(3)𝑘+1−𝑏(3)𝑘=∑𝑖≤𝑘𝑒𝑖(𝑏(2)𝑘+1−𝑖−𝑏(2)𝑘−𝑖)+𝑒𝑘+1.
Every bracket is nonnegative. In the first line
the brackets add up to 𝑒𝑘+1 −1 <𝑃−1 and each 𝑒𝑖 ≤𝑃−1, so 0 ≤𝑏(2)𝑘+1 −𝑏(2)𝑘 ≤𝑃−2 +𝑃−1 ≤2𝑃−2. Inserting this bound into the 𝑘 +1 terms of the second line gives 0 ≤𝑏(3)𝑘+1 −𝑏(3)𝑘 ≤2(𝑘 +1)𝑃−3 +𝑃−1 ≤3(𝑘 +1)𝑃−3.
Against the lower bounds 𝑏(2)𝑘 ≥𝑘 +1 and 𝑏(3)𝑘 ≥(𝑘 +1)(𝑘 +2)/2 displayed above,
the ratio 𝑏(𝑟)𝑘+1/𝑏(𝑟)𝑘
lies in [1,1 +2𝑃−2/(𝑘 +1)] for
𝑟 =2 and in [1,1 +6𝑃−3/(𝑘 +2)] for 𝑟 =3. Both ratios tend to 1, and therefore so does 𝑏(𝑟)𝑘+ℎ/𝑏(𝑟)𝑘, a product of
ℎ consecutive ratios. Finally (𝑞;𝑞)𝑘+ℎ/(𝑞;𝑞)𝑘 =∏ℎ𝑗=1(1 −𝑞𝑘+𝑗) →1,
and 𝑎𝑘+ℎ/𝑎𝑘 =𝛾𝑘+ℎ/𝛾𝑘 is the
product of these three ratios. The Lean proof obtains the fixed-shift
limit by the same steps. ◻
The factorisation proves positivity at each fixed real 𝑞, not coefficientwise positivity in
𝑞: for example, 𝑎0 =𝑃4 has 𝑞-coefficient −4. The cubic factors 𝑐𝑘 multiply to 𝐶𝑁, but 𝑎𝑘/𝑐𝑘 →1 alone would not determine the
product of 𝑁 weights. The first
relative correction has order 1/𝑘
and accumulates as a harmonic sum; the remaining 𝑂𝑞(𝑘−2) terms determine a finite
constant. The two convolutions supply this first correction
explicitly.
Theorem 3.8 (the size of 𝑉∗𝑁 at a fixed base). Let 𝛾𝐸 be Euler’s constant. The
product
A(𝑞)=𝑒−8𝛾𝐸𝐿∏𝑘≥0(𝑎𝑘𝑐𝑘𝑒8𝐿/(𝑘+1))
converges to a positive finite value. With 𝐾(𝑞) =A(𝑞)M(𝑞)3,
𝑉∗𝑁(𝑞)∼𝐾(𝑞)𝐶𝑁𝑞𝐵𝑁𝑃2𝑁𝑁−8𝐿,
equivalently
log𝑉∗𝑁(𝑞)=𝐵𝑁log𝑞+log𝐶𝑁+2𝑁log𝑃−8𝐿log𝑁+log𝐾(𝑞)+𝑜(1).
Proof of Theorem 3.8.
Put 𝐿 =𝐹(1/𝑞), 𝑒𝑘 =(𝑞;𝑞)−1𝑘 and 𝐸 =𝑃−1. Replacing every 𝑒𝑘 by 𝐸 in the two convolution sums gives 𝐸2(𝑘 +1) and 𝐸3(𝑘+22). The factors 𝑘 +1 and (𝑘+22) count the nonnegative
pairs and triples with sum 𝑘,
respectively. For a fixed index 𝑖,
there is one pair (𝑖,𝑘 −𝑖) and there
are 𝑘 −𝑖 +1 triples whose first
coordinate is 𝑖. Thus a summable
deficit in the sequence 𝑒𝑖
produces a constant correction in the two-fold sum and a linear
correction in the three-fold sum. We calculate that deficit and bound
terms with two or more deficits.
Writing 𝑑𝑘 =𝐸 −𝑒𝑘, the identity
𝑒𝑘+1 −𝑒𝑘 =𝑞𝑘+1𝑒𝑘+1 gives
𝑑𝑘=∑𝑗>𝑘𝑞𝑗𝑒𝑗,0≤𝑑𝑘≤𝐸𝑞𝑘+11−𝑞.
Thus ∑𝑑𝑘 and ∑𝑘𝑑𝑘 converge. To evaluate the
former, use Euler’s identity E(𝑧) =∑𝑘≥0𝑒𝑘𝑧𝑘 =(𝑧;𝑞)−1∞ for |𝑧| <1. Tonelli’s theorem and
logarithmic differentiation at 𝑧 =𝑞
give
𝑆:=∑𝑘≥0𝑑𝑘=∑𝑗≥1𝑗𝑞𝑗𝑒𝑗=𝑞E′(𝑞)=𝐸∑𝑟≥1𝑞𝑟1−𝑞𝑟=𝐸𝐿.
In the double sum, 𝑞𝑗𝑒𝑗 occurs once for each 𝑘 =0,…,𝑗 −1, which explains the factor
𝑗. Logarithmic differentiation is
justified by locally uniform convergence on |𝑧| <1.
Let 𝑏(𝑟)𝑘 =[𝑧𝑘]E(𝑧)𝑟. The finite-sum formula in Proposition 3.7
becomes
𝑎𝑘=𝑃4(𝑞;𝑞)𝑘𝑏(2)𝑘𝑏(3)𝑘.
We expand each finite convolution using
𝑒𝑘 =𝐸 −𝑑𝑘. For two factors,
𝑏(2)𝑘=𝐸2(𝑘+1)−2𝐸𝑘∑𝑖=0𝑑𝑖+𝑘∑𝑖=0𝑑𝑖𝑑𝑘−𝑖=𝐸2(𝑘+1−2𝐿)+𝑂𝑞((𝑘+1)𝑞𝑘).
For three factors, the terms with
one 𝑑𝑖 contribute −3𝐸2∑𝑘𝑖=0(𝑘 −𝑖 +1)𝑑𝑖. Here the sum
equals (𝑘 +1)𝑆 +𝑂𝑞(1) because ∑𝑖𝑑𝑖 <∞. Terms with two
𝑑𝑖 are bounded by 3𝐸𝑆2, and the term with three is 𝑂𝑞((𝑘 +1)2𝑞𝑘). It follows that
𝑏(3)𝑘=𝐸3((𝑘+22)−3𝐿(𝑘+1))+𝑂𝑞(1).
Dividing the correction −3𝐿(𝑘 +1) by
the leading term (𝑘+22)
gives the relative correction −6𝐿/(𝑘 +2). The two-fold convolution
contributes −2𝐿/(𝑘 +1) in the same
way. Since (𝑞;𝑞)𝑘 =𝑃(1 +𝑂𝑞(𝑞𝑘)),
the leading constants in 𝑎𝑘 =𝑃4(𝑞;𝑞)𝑘𝑏(2)𝑘𝑏(3)𝑘 multiply to 𝑃5𝐸5 =1. Replacing (𝑘 +2)−1 by (𝑘 +1)−1 changes only the 𝑂𝑞((𝑘 +1)−2) error. Thus the
coefficients 2𝐿 and 6𝐿 add, and with 𝑐𝑘 =(𝑘 +1)2(𝑘 +2)/2 we obtain
𝑎𝑘𝑐𝑘=(1−2𝐿𝑘+1+𝑂𝑞(𝑞𝑘))(1−6𝐿𝑘+2+𝑂𝑞((𝑘+1)−2))(1+𝑂𝑞(𝑞𝑘))=1−8𝐿𝑘+1+𝑂𝑞((𝑘+1)−2).
In particular 𝑎𝑘+1/𝑎𝑘 →1, and multiplication of
finitely many adjacent ratios gives 𝑎𝑘+ℎ/𝑎𝑘 →1 for each fixed ℎ. The uniform shift bound follows from
Proposition 3.7,
so Theorem 3.6
applies.
For large 𝑘, taking logarithms
preserves the first-order term and leaves the summable error log(𝑎𝑘/𝑐𝑘) +8𝐿/(𝑘 +1) =𝑂𝑞((𝑘 +1)−2).
The finitely many earlier factors are positive, so the regularised
product also has a positive finite limit: 0 <A(𝑞) <∞. Since ∏𝑘<𝑁𝑐𝑘 =𝐶𝑁, the harmonic
contribution separates as
log∏𝑘<𝑁𝑎𝑘𝐶𝑁=−8𝐿∑𝑘<𝑁1𝑘+1+∑𝑘<𝑁(log𝑎𝑘𝑐𝑘+8𝐿𝑘+1).
The second sum tends to logA(𝑞) +8𝛾𝐸𝐿. Using ∑𝑘<𝑁(𝑘 +1)−1 =log𝑁 +𝛾𝐸 +𝑜(1), the Euler-constant terms cancel, giving
∏𝑘<𝑁𝑎𝑘 ∼A(𝑞)𝐶𝑁𝑁−8𝐿. Theorem 3.6
now gives the stated determinant asymptotic. Taking logarithms yields
log𝑉∗𝑁=𝐵𝑁log𝑞+log𝐶𝑁+2𝑁log𝑃−8𝐿log𝑁+log𝐾(𝑞)+𝑜(1).
◻
The convolution proof explains 8𝐿 as 2𝐿 +6𝐿, one contribution from each finite
sum. An alternative reads the same correction from the generating
function near 𝑤 =1. Its pole of
order four accounts for the cubic growth of 𝑎𝑘; the next principal-part coefficient
accounts for the relative term of order 1/𝑘.
An alternative coefficient calculation. Write Π(𝑤) =(𝑞𝑤;𝑞)∞, so that (𝑤;𝑞)∞ =(1 −𝑤)Π(𝑤), and for 𝑡 ≥1 put
𝑓𝑡(𝑤)=(𝑞𝑡𝑤2;𝑞)∞(𝑞;𝑞)𝑡(𝑞𝑡𝑤;𝑞)2∞,S(𝑤)=∑𝑡≥1𝑤𝑡(𝑓𝑡(𝑤)−𝑃−1).
On each
compact subset of |𝑤| <𝑞−1 the
bracket is 𝑂𝑞(𝑞𝑡) uniformly, so
S is analytic there.
Separating the summand 𝑡 =0, whose
denominator carries the factor (1 −𝑤)2, and subtracting the constant
part of the remaining summands gives
D(𝑤):=𝑃4(1−𝑤)4𝐺𝑞(𝑤)=𝑃4Π(𝑤)3((1+𝑤)(𝑞𝑤2;𝑞)∞Π(𝑤)2+𝑤𝑃+(1−𝑤)S(𝑤)).
Hence D is analytic on a disc of
radius greater than 1.
At 𝑤 =1 one has Π(1) =𝑃 and Π′(1)/Π(1) = −𝐿, since Π′/Π = −∑𝑗≥1𝑞𝑗/(1 −𝑞𝑗𝑤).
Also (𝑞𝑤2;𝑞)∞ equals 𝑃 at 𝑤 =1, and the logarithmic derivative of
(𝑞𝑤2;𝑞)∞/Π(𝑤)2 at 𝑤 =1 is −2𝐿 +2𝐿 =0. Therefore the bracket has value
3/𝑃 and derivative (2 −𝐿)/𝑃 at 𝑤 =1; here S(1) =𝐿/𝑃, because 𝑓𝑡(1) =(𝑃(1 −𝑞𝑡))−1 and
∑𝑡≥1((1 −𝑞𝑡)−1 −1) =𝐿.
Combining with the factor 𝑃4Π−3, whose logarithmic derivative
at 1 is 3𝐿, gives
D(1)=3,D′(1)=3(3𝐿+2−𝐿3)=2+8𝐿.
The first
two principal-part terms are determined by D(1) and D′(1). The terms from its
second and third derivatives have coefficients of order at most 𝑘; after the full principal part is
subtracted, the remainder is analytic on a larger disc and has
exponentially decreasing coefficients. Keeping only the first two terms
therefore gives
𝑎𝑘=3(𝑘+33)−(2+8𝐿)(𝑘+22)+𝑂𝑞(𝑘),𝑎𝑘𝑐𝑘=1−8𝐿𝑘+1+𝑂𝑞((𝑘+1)−2),
the
second line because 3(𝑘+33) =𝑐𝑘(𝑘 +3)/(𝑘 +1) and (𝑘+22) =𝑐𝑘/(𝑘 +1).
The logarithmic error is again summable. The product argument in the
first proof therefore gives 0 <A(𝑞) <∞ and, using ∑𝑘<𝑁(𝑘 +1)−1 =log𝑁 +𝛾𝐸 +𝑜(1),
∏𝑘<𝑁𝑎𝑘∼A(𝑞)𝐶𝑁𝑁−8𝐿.
Proposition 3.7
supplies the uniform shift bound and the fixed-shift limit, so
Theorem 3.6
applies to (𝑎𝑘) and gives 𝑉∗𝑁 ∼M(𝑞)3𝑞𝐵𝑁𝑃2𝑁∏𝑘<𝑁𝑎𝑘. Substituting the product
asymptotic proves both displays. ◻
Comparison with the cubic bound.
The estimate identifies the terms 2𝑁log𝑃, −8𝐹(1/𝑞)log𝑁 and
log𝐾(𝑞) within the previous 𝑂𝑞(𝑁) error. It leaves the cubic
coefficient unchanged and has no effect on prime-power valuations. For
the denominator estimate at 3/2,
the difference of the relevant exponents is
3941(4𝑁3−3𝑁2)−(2𝑁3−𝑁)=𝑁(74𝑁2−117𝑁+41)41>0(𝑁≥2),
the positivity
being immediate from 74𝑁2 −117𝑁 +41 =74(𝑁 −2)2 +179(𝑁 −2) +103. Its
leading size is (74/41)𝑁3. A
logarithmic correction cannot offset this cubic gap in the stated
denominator model. The factorisation refines the moment weights, not the
denominator of an irrationality form; any such form still needs an
estimate for its own rational coefficients.
An extension with limiting weight ratio
For 0 <𝜌 <𝑞−1 set
M(𝜌;𝑞)=∏𝑑≥1(1−𝜌𝑞𝑑)−𝑑,M(1;𝑞)=M(𝑞).
A limiting
adjacent-weight ratio supplies an exponential shift bound, replacing the
polynomial bound above. The condition 𝜌𝑞 <1 makes that bound summable and changes one copy of the
product constant from M(1;𝑞) to M(𝜌;𝑞). The ordinary proof below has no Lean proof in the
supplied record; this unformalised remark is not used in the checked
fixed-base argument.
Ordinary argument for the ratio-limit remark. Choose ˆ𝜌 with 𝜌 <ˆ𝜌 <𝑞−1. There is
a 𝐾 such that 𝑎𝑗+1/𝑎𝑗 ≤ˆ𝜌 for 𝑗 ≥𝐾. With
𝐶=∏𝑗<𝐾max(1,𝑎𝑗+1ˆ𝜌𝑎𝑗),
we obtain, by multiplying adjacent ratios,
𝑎𝑘+ℎ𝑎𝑘≤𝐶ˆ𝜌ℎ(𝑘,ℎ≥0).(22)
This also gives 𝑎ℎ ≤𝐶𝑎0ˆ𝜌ℎ, so every
moment converges because 𝑞ˆ𝜌 <1. For finitely many
nodes, Cauchy–Binet expands their moment determinant as a sum of squared
Vandermonde products. We let the number of nodes tend to infinity.
Entrywise convergence gives the limit of the determinant, while
positivity gives the limit of the sum. Hence
𝐷𝑁=∑0≤𝑘0<⋯<𝑘𝑁−1∏𝑖<𝑁𝑎𝑘𝑖𝑞𝑘𝑖∏𝑖<𝑗<𝑁(𝑞𝑘𝑖−𝑞𝑘𝑗)2.(23)
The tuple 𝑘𝑖 =𝑖 contributes
𝑞𝐵𝑁Δ𝑁∏𝑖<𝑁𝑎𝑖,Δ𝑁=𝑁−1∏𝑑=1(1−𝑞𝑑)2(𝑁−𝑑).
Write 𝑘𝑖 =𝑖 +𝜆𝑖 and reverse the
displacements: 𝜇𝑗 =𝜆𝑁−𝑗
for 1 ≤𝑗 ≤𝑁. Then 𝜇1 ≥⋯ ≥𝜇𝑁 ≥0. After
division by the least-tuple contribution, the summand becomes
𝑊𝑁(𝜇)=𝑞∑𝑗≤𝑁(2𝑗−1)𝜇𝑗∏𝑗≤𝑁𝑎𝑁−𝑗+𝜇𝑗𝑎𝑁−𝑗⋅∏1≤𝑗<𝑘≤𝑁(1−𝑞𝑘−𝑗+𝜇𝑗−𝜇𝑘1−𝑞𝑘−𝑗)2.(24)
For partitions of length greater than 𝑁, set 𝑊𝑁(𝜇) =0. All the sums now have the
same countable index set.
Suppose that 𝜇 has ℓ positive parts. Only the factors
with 𝑗 ≤ℓ can differ from 1. For a fixed such 𝑗, the denominators in the Vandermonde
quotient multiply to at least 𝑃,
and its numerators are at most 1.
We therefore have a bound independent of 𝑁
𝑊𝑁(𝜇)≤(𝐶𝑃−2)ℓℓ∏𝑗=1ˆ𝜌𝜇𝑗𝑞(2𝑗−1)𝜇𝑗.
We sum
this majorant by first fixing ℓ
and then dropping the ordering condition on the positive parts. This
gives
∑ℓ(𝜇)=ℓsup𝑁𝑊𝑁(𝜇)≤(𝐶𝑃−2)ℓℓ∏𝑗=1∑𝑢≥1ˆ𝜌𝑢𝑞(2𝑗−1)𝑢≤𝐶ℓ∗𝑞ℓ2,𝐶∗=𝐶ˆ𝜌𝑃−21−ˆ𝜌𝑞.
Here ∑𝑗≤ℓ(2𝑗 −1) =ℓ2 and 1 −ˆ𝜌𝑞2𝑗−1 ≥1 −ˆ𝜌𝑞 >0. The series ∑ℓ≥0𝐶ℓ∗𝑞ℓ2
converges.
For fixed ℎ, telescoping the
adjacent ratios shows that 𝑎𝑘+ℎ/𝑎𝑘 →𝜌ℎ. Thus, for each fixed partition, the weight ratios in
(24)
have the same limit as for 𝑎𝑘 =𝜌𝑘. The Vandermonde quotient is
independent of the weights, and its convergence follows from the same
finite identity (20).
Dominated convergence therefore reduces the limit of ∑𝜇𝑊𝑁(𝜇) to the case 𝑎𝑘 =𝜌𝑘.
In that case 𝑀𝑚 =(1 −𝜌𝑞𝑚+1)−1, and Cauchy’s determinant gives
𝐷𝑁=𝜌𝑁(𝑁−1)/2𝑞𝐵𝑁Δ𝑁∏0≤𝑖,𝑗<𝑁(1−𝜌𝑞𝑖+𝑗+1).
The multiplicity of
1 −𝜌𝑞𝑑 in the denominator
increases to 𝑑, so the normalised
sum tends to M(𝜌;𝑞).
Finally,
Δ𝑁𝑃2𝑁=∏𝑑<𝑁(1−𝑞𝑑)−2𝑑∏𝑑≥𝑁(1−𝑞𝑑)−2𝑁⟶M(1;𝑞)2,
since the logarithm of the
second product is 𝑂𝑞(𝑁𝑞𝑁).
Combining the two limits proves (21). ◻
For example, 𝑎𝑘 =𝜌𝑘(𝑘 +1)𝑠,
with 𝑠 ∈ℝ, satisfies the
ratio hypothesis, and ∏𝑘<𝑁𝑎𝑘 =𝜌𝑁(𝑁−1)/2(𝑁!)𝑠.
For 𝑠 =1 the moments are (1 −𝜌𝑞𝑚+1)−2, giving
det((1−𝜌𝑞𝑖+𝑗+1)−2)𝑖,𝑗<𝑁∼M(𝑞)2M(𝜌;𝑞)𝑞𝐵𝑁𝑃2𝑁𝜌𝑁(𝑁−1)/2𝑁!.
The choice 𝑎𝑘 =𝜌𝑘exp(√𝑘) also satisfies
the ratio hypothesis, since √𝑘+1 −√𝑘 →0. For 𝜌 =1, its relative growth at 𝑘 =0 exceeds every polynomial in the
shift. Thus this argument extends beyond the polynomial-bound hypotheses
of Theorem 3.6.
Positive Hankel determinants and a rational special value
We construct a generating function with the rational special value
1, although its moment determinants
have the same formal orders, leading coefficients and type of fixed-base
power correction as Zudilin’s. This shows why those determinant
properties alone do not establish irrationality. The construction uses
neither Zudilin’s recurrence nor his polynomial factorisation or
cyclotomic divisors, and gives no conclusion about 𝐹(3/2). The arguments below have ordinary
proofs only and are stated as unformalised remarks.
We choose the tail of the weight sequence to obtain the determinant
asymptotic, and its first terms to fix the special value. A telescoping
difference of the moments will then give the value 1. The cut-off below separates these two
choices while leaving room to keep every weight positive.
Put
𝑐𝑘=(𝑘+1)2(𝑘+2)2,𝑑𝑘=(𝑘+1)(𝑘+2)2,𝑅(𝑤)=∑𝑘≥0𝑐𝑘𝑤𝑘=1+2𝑤(1−𝑤)4.
For 0 <𝑞 ≤2/3 define, with a single fixed
cut-off 32,
𝑎𝑘(𝑞)={𝑐𝑘(1−𝑞)32,1≤𝑘<32,𝑐𝑘−12𝑞𝑑𝑘,𝑘≥32,𝑎0(𝑞)=1−∑𝑘≥1𝑎𝑘(𝑞)𝑞𝑘.(25)
The weight generating function 𝐴𝑞(𝑤) =∑𝑘≥0𝑎𝑘(𝑞)𝑤𝑘 is rational
in 𝑤. The value 𝐺𝑞(𝑞) concerns a different generating
function, formed from the moments below. To obtain 𝐴𝑞, put
𝑇𝑞(𝑤)=𝑅(𝑤)−12𝑞(1−𝑤)3−31∑𝑘=0(𝑐𝑘−12𝑞𝑑𝑘)𝑤𝑘,
so that 𝐴𝑞(𝑤) equals
𝑎0(𝑞)+(1−𝑞)3231∑𝑘=1𝑐𝑘𝑤𝑘+𝑇𝑞(𝑤),𝑎0(𝑞)=1−(1−𝑞)3231∑𝑘=1𝑐𝑘𝑞𝑘−𝑇𝑞(𝑞).
Set 𝜇𝑚(𝑞) =𝐴𝑞(𝑞𝑚+1), 𝜈𝑚(𝑞) =𝜇𝑚(𝑞) −𝑞𝜇𝑚+1(𝑞), and
𝐺𝑞(𝑧) =∑𝑚≥0𝜈𝑚(𝑞)𝑧𝑚. The
choice of 𝑎0 makes 𝜇0 =1, while the factor 𝑞 in 𝜈𝑚 makes the sum defining 𝐺𝑞(𝑞) telescope. Independently, for
𝑘 ≥32 the tail satisfies 𝑎𝑘/𝑐𝑘 =1 −12𝑞/(𝑘 +1); at 𝑞 =2/3 this becomes 1 −8/(𝑘 +1), which produces the required
power 𝑁−8 in the product of the
weights. The proof below checks positivity, convergence and both
determinant claims.
This countermodel and its denominator calculation have ordinary
proofs below; they have not been Lean-checked or externally peer
reviewed.
Proof. For 𝑘 ≥32 we
have 𝑎𝑘(𝑞) =𝑑𝑘(𝑘 +1 −12𝑞) >0, and
the smaller-index weights are plainly positive. Write 𝑀(𝑞) =(1 −𝑞)32∑31𝑘=1𝑐𝑘𝑞𝑘. The
generating function for the 𝑐𝑘
gives 𝑅(𝑞) −1 ≤6𝑞(1 −𝑞)−4, whence
𝑀(𝑞) ≤6𝑞(1 −𝑞)28 ≤6/29 <1/4.
For 𝑘 ≥32,
𝑑𝑑𝑞(𝑑𝑘(𝑘+1−12𝑞)𝑞𝑘)=𝑑𝑘(𝑘+1)𝑞𝑘−1(𝑘−12𝑞)>0.
Direct substitution into the
rational expression for 𝑇𝑞 gives
𝑇2/3(2/3)=24794846199808205891132094649<14.
Therefore 1/2 <𝑎0(𝑞) =1 −𝑀(𝑞) −𝑇𝑞(𝑞) <1.
The moments have positive atomic representations
𝜇𝑚=∑𝑘≥0𝑎𝑘𝑞𝑘(𝑞𝑘)𝑚,𝜈𝑚=∑𝑘≥0𝑎𝑘𝑞𝑘(1−𝑞𝑘+1)(𝑞𝑘)𝑚.
Infinitely many
distinct atoms have positive mass. The Gram quadratic form of a nonzero
polynomial of degree below 𝑁 is
strictly positive for either measure, proving positive definiteness of
every 𝑁-by-𝑁 Hankel matrix. Summing the geometric
series in 𝑚 gives
𝐺𝑞(𝑧)=∑𝑘≥0𝑎𝑘𝑞𝑘(1−𝑞𝑘+1)1−𝑧𝑞𝑘.
Each 𝑧 =𝑞−𝑘 is a genuine pole:
its residue is nonzero and the other terms are analytic there. Hence
𝐺𝑞 is not rational. Telescoping
shows 𝐺𝑞(𝑞) =𝜇0(𝑞) =𝐴𝑞(𝑞) =1 and,
for 𝑆𝑛−1 =∑𝑚<𝑛𝑞𝑚𝜈𝑚,
gives
1−𝑆𝑛−1=𝑞𝑛𝜇𝑛∈(0,𝑞𝑛](𝑛≥0).
Every 𝑎𝑘(𝑞) belongs to ℤ[[𝑞]] and has constant term 𝑐𝑘, including 𝑎0, for which the defining sum is
coefficientwise finite. The moments 𝜇𝑚 and 𝜈𝑚 also lie in ℤ[[𝑞]], but their constant terms are
1: only 𝑎0 contributes at 𝑞 =0. Their rational expressions have no
poles for |𝑞| <1, so these formal
series converge at 𝑞0. For 𝐻𝑁(𝑞) =det(𝜇𝑖+𝑗(𝑞))𝑖,𝑗<𝑁, the
Gram determinant expansion is
𝐻𝑁(𝑞)=∑0≤𝑘0<⋯<𝑘𝑁−1(∏𝑖<𝑁𝑎𝑘𝑖(𝑞)𝑞𝑘𝑖)∏𝑖<𝑗(𝑞𝑘𝑖−𝑞𝑘𝑗)2.
It holds first for
finitely many atoms and then coefficientwise. The lowest possible degree
of one summand is ∑𝑖<𝑁(2𝑁 −1 −2𝑖)𝑘𝑖. Its unique
minimum is attained at 𝑘𝑖 =𝑖 and
equals 𝐵𝑁; the coefficient is
∏𝑖<𝑁𝑐𝑖 =𝐶𝑁. Replacing
𝑎𝑘 by 𝑎𝑘(1 −𝑞𝑘+1) proves the same leading
term for (𝜈𝑚).
At 𝑞0 set 𝜀 =3−32 and 𝑏0 =𝑎0(𝑞0) >0. For 𝑘 ≥32, 𝑎𝑘(𝑞0)/𝑐𝑘 =(𝑘 −7)/(𝑘 +1); all these
ratios lie in [𝜀,1].
Hence for fixed ℎ, 𝑎𝑘+ℎ/𝑎𝑘 →1 as 𝑘 →∞, and uniformly 𝑎𝑘+ℎ/𝑎𝑘 ≤332(1 +ℎ)3. These are
precisely the weight hypotheses of Theorem 3.6,
whose conclusion is
𝐻𝑁(𝑞0)∼M(𝑞0)3𝑞𝐵𝑁0𝑃(𝑞0)2𝑁∏𝑘<𝑁𝑎𝑘(𝑞0).
The finite product
has the exact form, for 𝑁 ≥32,
∏𝑘<𝑁𝑎𝑘(𝑞0)𝐶𝑁=𝑏0𝜀3132!24!(𝑁−8)!𝑁!.
Thus
A =𝑏0𝜀3132!/24!, and 𝑁8(𝑁 −8)!/𝑁! →1. The displayed exponent
is exactly −8𝜉 because 𝜉 =1; it is asserted at this one fixed
base, not as a uniform special-value formula for this family. ◻
The following calculation is retained with its ordinary proof. It has
no Lean proof in the supplied record.
Proof. At 𝑞0, split
the rational seed into a pole part and a polynomial:
𝐴𝑞0(𝑤)=−7+10𝑤(1−𝑤)4+𝑄(𝑤),𝑄(𝑤)=𝑝0+31∑𝑘=1𝑝𝑘𝑤𝑘,
where 𝑝0 =𝑏0 +7 and 𝑝𝑘 =(3−32 −1)𝑐𝑘 +8𝑑𝑘. These
coefficients have only powers of three in their denominators. The finite
formulas give 𝑣3(𝑝0) ≥ −63, 𝑣3(𝑝𝑘) ≥ −32 for 1 ≤𝑘 ≤30, and 𝑣3(𝑝31) = −31: in the last calculation
𝑐31 =16896 has 𝑣3(𝑐31) =1 and the other numerator
terms are multiples of 332. At
𝑤 =(2/3)𝑛+1, 𝑛 ≥1, the term 𝑝31𝑤31 has valuation −31𝑛 −62, uniquely lower than all other
terms of 𝑄(𝑤). The pole part equals
33𝑛+3(−7⋅3𝑛+1+10⋅2𝑛+1)𝛿4𝑛
and has positive 3-adic valuation.
Hence 𝑣3(𝜇𝑛) = −31𝑛 −62.
Every prime ℓ ∣𝛿𝑛
differs from 2,3. Its numerator in
the displayed pole part is congruent to 3 ⋅2𝑛+1(mod𝛿𝑛) and is
coprime to 𝛿𝑛. The polynomial
part is ℓ-integral, so it cannot
cancel the pole part’s ℓ-denominator of order 4𝑣ℓ(𝛿𝑛). There are no other
denominator primes. Multiplying by 𝑞𝑛0 =2𝑛/3𝑛 adds exactly 𝑛 factors of three, proving the second
formula. In the affine error, 𝑞−𝑛0 =3𝑛/2𝑛 has denominator 2𝑛, coprime to the odd denominator of
𝜇𝑛. Subtraction does not reduce
either negative valuation, proving the stated least common
denominator. ◻
Each individual 𝜇𝑛 has
logarithmic height linear in 𝑛:
logden𝜇𝑛 =(35𝑛 +66)log3 +𝑜(1).
The determinant has a different scale.
The following calculation is retained with its ordinary proof. It has
no Lean proof in the supplied record.
Proof. The positive Heine expansion above gives a bound
independent of the asymptotic theorem. Since 0 <𝑎𝑘(𝑞0) ≤𝑐𝑘, write 𝑘𝑖 =𝑖 +𝑠𝑖. Dropping the ordering
restriction and bounding 𝑐𝑖+𝑠𝑖/𝑐𝑖 ≤(1 +𝑠𝑖)3 and each
residual Vandermonde factor by one gives
0<𝐻𝑁(𝑞0)≤𝐶𝑁𝑞𝐵𝑁0∏𝑗≥0∑𝑠≥0(𝑠+1)3𝑞(2𝑗+1)𝑠0.
For 𝐴(𝑡) =∑𝑠≥0(𝑠 +1)3𝑡𝑠 =(1 +4𝑡 +𝑡2)/(1 −𝑡)4,
log𝐴(𝑡) ≤𝐴(𝑡) −1 ≤8𝑡/(1 −𝑡)4.
The product is therefore at most exp(3888/5). Since 𝐷𝑁𝐻𝑁 is a positive integer,
log𝐷𝑁≥𝐵𝑁log(3/2)−log𝐶𝑁−3888/5.
Here 𝐵𝑁 ∼𝑁3/3 and log𝐶𝑁 =𝑂(𝑁log𝑁). Conversely,
𝐸𝑁=331𝑁(𝑁−1)+62𝑁∏0≤𝑖,𝑗<𝑁𝛿4𝑖+𝑗
clears every term in the determinant
expansion, by the preceding denominator formula. Thus 𝐷𝑁 ∣𝐸𝑁; using log𝛿𝑚 ≤(𝑚 +1)log3 and ∑𝑖,𝑗<𝑁(𝑖 +𝑗 +1) =𝑁3 gives the
asserted cubic upper bound.
For the assertion about 𝐻2,
den𝜇1 =39354
and den𝜇2 =3124194. At
five, 𝑣5(𝜇2) =0 and 𝑣5(𝜇21) = −8, while the proposed
product contributes only 54. At
three and nineteen that product clears the denominator, and no other
prime occurs. The remaining denominator is therefore 54 =625. ◻
Zudilin’s determinantal criterion retains a divisibility condition on
its successive clearing integers [11]; the calculation for 𝐻2 rules out replacing it with their
numerical ordering, not the criterion itself. The usual
integer-polynomial height criterion likewise needs a common coefficient
denominator for the same polynomial being evaluated. The
model’s exact partial errors alone cannot supply one cheaply. In fact,
with 𝛼𝑚 =𝑞−𝑚0 and 𝛽𝑚 =𝛼𝑚 −𝜇𝑚(𝑞0), the pencil
det(𝛼𝑖+𝑗𝑋 −𝛽𝑖+𝑗)𝑖,𝑗<𝑁
is affine in 𝑋 because (𝛼𝑖+𝑗) has rank one. At 𝑋 =1 it is the positive rational 𝐻𝑁(𝑞0); after primitive integral
clearing its value is a positive integer. Matching Hankel order,
positivity, fixed-base asymptotic and a small rational value
thus leaves the rational-base denominator problem exactly where it was.
The Christoffel-type reweighting 𝑎𝑘𝑞𝑘 ↦𝑎𝑘𝑞𝑘(1 −𝑞𝑘+1) is
standard moment machinery, not a new transform [31]; this example’s claim is the
explicit combination and its arithmetic obstruction.
Coefficient moments and cyclotomic content
We now study the coefficient sequence, not the remainder sequence.
The identity 𝑣∗𝑚 =𝛼𝑚𝐹(𝑝) −𝛽𝑚 does not
transfer a representing measure from (𝑣∗𝑚) to (𝛼𝑚): subtraction mixes two
coefficient sequences. Their positivity, spectral properties and
cyclotomic factors therefore require separate calculations. Fix 𝑝 >1 and define, using Gaussian
binomial polynomials,
𝑅𝑚(𝑝)=𝑚∑𝑘=0(−1)𝑚+𝑘𝑝𝑘(𝑘+1)/2[𝑚𝑘]𝑝[𝑚+𝑘𝑘]𝑝,𝑠𝑚(𝑝)=([𝑚]𝑝!)3𝑅𝑚(𝑝),
where [𝑚]𝑝! =∏𝑚𝑗=1(1 +𝑝 +⋯ +𝑝𝑗−1).
Each 𝑅𝑚 is the signed value at
𝑥 =𝑝𝑚+1 of the little 𝑞-Legendre polynomial of degree 𝑚, with 𝑞 =𝑝−1; this identification is
discussed in the related-work section. The polynomial normalisation
of [9], at 𝑥 =𝑧 =1, gives
𝛼𝑚=𝑝[𝑝(𝑝−1)3]𝑚𝑠𝑚(𝑝),𝛽𝑚=[𝛼𝑚∑𝑗≥1𝜏(𝑗)𝑝−𝑗]+−1,𝑣∗𝑚=𝛼𝑚𝐹(𝑝)−𝛽𝑚.
The brackets mean the polynomial part at
infinity. Thus 𝛼0 =𝑝 and 𝛽0 =0. This fixes the normalisation
before any content or positivity test.
A positive expansion is not a moment representation.
Substituting 𝑥 =𝑝𝑚+1 into Van
Assche’s alternative expansion [18] gives the identity
𝑅𝑚(𝑝)=𝑚∑𝑘=0[𝑚𝑘]𝑝[𝑚+𝑘𝑘]𝑝𝑝(𝑚−𝑘)(𝑚−𝑘+1)/2𝑚∏𝑗=𝑚−𝑘+1(𝑝𝑗−1).
Indeed (𝑞𝑥;𝑞)𝑘 =( −1)𝑘∏𝑚𝑗=𝑚−𝑘+1(𝑝𝑗 −1),
so the two signs cancel. This proves 𝑅𝑚(𝑝) >0 for 𝑝 >1, and nonnegative coefficients in
the variable 𝑡 =𝑝 −1; it does not
prove Hankel positivity. In fact,
det(𝑅𝑖+𝑗(𝑝))𝑖,𝑗<3=−36(𝑝−1)2+𝑂((𝑝−1)3)(𝑝↓1).
A geometric factor 𝑐𝜌𝑚 with 𝑐,𝜌 >0 would change a Hankel matrix
only by a positive scalar and an invertible diagonal congruence, so it
would preserve positive definiteness. The factor ([𝑚]𝑝!)3 is not geometric: its values
at 𝑚 =0,1,2 are 1,1,(1 +𝑝)3. It cannot be discarded in
testing the moment condition. Nor does its positivity alone prove that
multiplication by it repairs the failed condition for 𝑅𝑚. At 𝑝 =1, 𝑠𝑚(1) =(𝑚!)3 is the moment sequence of a
product of three independent unit exponential variables, since their
𝑚th moments multiply. This is only
the polynomial endpoint; 𝐹(1)
diverges. Berg’s Theorem 5.1 states that (𝑚!)𝑐 is Stieltjes indeterminate for
𝑐 >2 [36]. Thus a measure exists at the endpoint but
is not unique. Neither uniqueness nor a canonical deformation is a
premise of the question at 𝑝 >1.
Finite certificates and an all-rank degree check.
Put 𝐷𝑁,ℎ(𝑝) =det(𝑠𝑖+𝑗+ℎ(𝑝))0≤𝑖,𝑗<𝑁, with 𝐷0,ℎ =1.
Exact polynomial calculations give strictly positive coefficients in
𝑡 =𝑝 −1 for 𝐷𝑁,ℎ(1 +𝑡) when ℎ =0,1 and 1 ≤𝑁 ≤8. Thus sixteen determinant
polynomials are positive for every real 𝑝 ≥1. Their degrees, in increasing rank,
are
ℎ=00105415634063010501624ℎ=12269623647082213161976.
The calculation uses exact arithmetic in ℤ[𝑝]. Starting from 𝐷0,ℎ =1 and 𝐷1,ℎ =𝑠ℎ, the Desnanot–Jacobi identity
gives
𝐷𝑁,ℎ=𝐷𝑁−1,ℎ𝐷𝑁−1,ℎ+2−𝐷2𝑁−1,ℎ+1𝐷𝑁−2,ℎ+2(𝑁≥2).
The degree argument below shows that each
denominator is nonzero. The computation checks that every division has
zero remainder, then substitutes 𝑝 =1 +𝑡 and tests every coefficient. All
8824 coefficients in the sixteen
polynomials are strictly positive. A program
computes the full
lists. An independent
checker evaluates each stored polynomial at more integer bases than
its degree and compares the values with fraction-free determinants of
the integer Hankel matrices, which identifies the stored list with 𝐷𝑁,ℎ(1 +𝑡) in ℤ[𝑡]. As a separate check of the
normalisation, direct integer determinants at 𝑝 =1,2,3,5,11 agree with evaluations of
all sixteen polynomials. Those evaluations are checks, not the proof of
polynomial positivity. This is a finite computer-algebra calculation and
gives no all-rank result.
For the eight unshifted determinants, positivity is also a Lean
theorem, proved by a different certificate. Put 𝑇 =22929. An explicit bound shows that
every coefficient of 𝐷𝑁,0(1 +𝑡),
𝑁 ≤8, has absolute value less than
𝑇/2. An integer polynomial with
this property is determined by its value at 𝑡 =𝑇, and its coefficients are the
base-𝑇 digits of that value
whenever every digit is less than 𝑇/2. The Lean kernel computes the eight
integers 𝐷𝑁,0(1 +𝑇) exactly and
checks this digit condition and that the lowest digit is nonzero. Every
coefficient of 𝐷𝑁,0(1 +𝑡) is
therefore nonnegative and the constant term is positive, so 𝐷𝑁,0(𝑝) >0 for every real 𝑝 ≥1. This is the positivity used in
Proposition 3.9. The
strict positivity of every coefficient, and the shifted determinants
𝐷𝑁,1, rest on the computation
above. Neither the finite computation nor the Lean proof yields an
all-rank coefficient-positivity theorem.
The degrees admit a separate all-rank proof. The Gaussian binomial
[𝑢𝑣]𝑝 is
monic of degree 𝑣(𝑢 −𝑣). In the
signed sum for 𝑅𝑚, the degree
increases by 2𝑚 −𝑘 from the 𝑘th to the (𝑘 +1)st term. The unique maximal term is
𝑘 =𝑚, with positive leading
coefficient. Hence 𝑅𝑚 is monic of
degree (3𝑚2 +𝑚)/2, and 𝑠𝑚 is monic of degree 3𝑚2 −𝑚. In the determinant, the only
permutation-dependent part of the degree is 6∑𝑖𝑖𝜎(𝑖); strict rearrangement
makes the identity its unique maximum. Therefore
deg𝐷𝑁,ℎ=𝑁−1∑𝑖=0(3(2𝑖+ℎ)2−(2𝑖+ℎ)),lc𝐷𝑁,ℎ=1.
More generally the same
argument works for a fixed minor with distinct increasing row and column
indices. Each such minor is positive for all sufficiently large 𝑝, with a threshold that may depend on
the minor. At 𝑝 =1, both leading
Hankel families are positive definite by the infinite-support product
measure, so each fixed rank is also positive in some neighbourhood of
1. Neither argument provides a
neighbourhood or large-base threshold uniform over every rank.
A Stieltjes moment representation requires positive semidefiniteness
of both Hankel families at all ranks. The positive-definite formulation
for nondegenerate sequences is stated in [33]; finite support requires allowing
semidefinite matrices. The necessity of both conditions is visible from
their quadratic forms: if a positive measure 𝜇 on [0,∞) satisfies 𝑠𝑚 =∫∞0𝑥𝑚 𝑑𝜇(𝑥), and 𝑃(𝑥) =∑𝑁−1𝑖=0𝑐𝑖𝑥𝑖 has real
coefficients, then
𝑁−1∑𝑖,𝑗=0𝑐𝑖𝑐𝑗𝑠𝑖+𝑗+ℎ=∫∞0𝑥ℎ𝑃(𝑥)2𝑑𝜇(𝑥)≥0,ℎ=0,1.
The shifted test records nonnegative support, not
merely positivity of the measure. For example, the positive point mass
at −1 has moments ( −1)𝑚. Its unshifted quadratic form is
𝑃( −1)2, whereas its shifted form
is −𝑃( −1)2. Thus a Hamburger
moment sequence, which permits support anywhere on ℝ, need not be a Stieltjes moment
sequence. The two tests above do not assert a measure for the entire
coefficient sequence considered here. Coefficientwise total positivity
would be stronger than the sixteen certificates above. Positive
production matrices and path constructions can supply such a mechanism
in other families [38][39]; no such matrix for this moving-degree
sequence has been established here.
A finite spectral consequence.
Write 𝐴𝑁 =(𝛼𝑖+𝑗)0≤𝑖,𝑗<𝑁 and 𝐵𝑁 =(𝛽𝑖+𝑗)0≤𝑖,𝑗<𝑁. We
study the matrix pencil 𝑌𝐴𝑁 −𝐵𝑁,
where 𝑌 is a scalar variable,
through the roots of its determinant. Let 𝐷 =diag(1,𝑝(𝑝 −1)3,…,[𝑝(𝑝 −1)3]𝑁−1).
Then 𝐴𝑁 =𝑝𝐷(𝑠𝑖+𝑗)𝐷. For 𝑝 >1 this is an invertible positive
diagonal congruence. The remainder representation already proves 𝐹(𝑝)𝐴𝑁 −𝐵𝑁 =(𝑣∗𝑖+𝑗) >0 at every
rank.
Proposition 3.9 (finite coefficient positivity and
pencil roots). For every real 𝑝 >1 and 1 ≤𝑁 ≤8, 𝐴𝑁 is positive definite and all roots of
det(𝑌𝐴𝑁 −𝐵𝑁) are real and
strictly less than 𝐹(𝑝). The roots
at consecutive ranks 𝑁,𝑁 +1 ≤8
interlace non-strictly.
Proof. The leading principal minors of (𝑠𝑖+𝑗)𝑖,𝑗<𝑁 are exactly 𝐷𝑘,0(𝑝) for 1 ≤𝑘 ≤𝑁; their coefficient positivity
proved above, together with Sylvester’s criterion, gives positive
definiteness. The diagonal congruence gives 𝐴𝑁 >0. The real symmetric matrix 𝐴−1/2𝑁𝐵𝑁𝐴−1/2𝑁 has these pencil
roots as eigenvalues, and 𝐹(𝑝)𝐼 −𝐴−1/2𝑁𝐵𝑁𝐴−1/2𝑁 >0 puts
them strictly below 𝐹(𝑝). The
minimum–maximum principle for 𝑥𝖳𝐵𝑁𝑥/(𝑥𝖳𝐴𝑁𝑥) on nested coordinate subspaces gives
non-strict interlacing. These are subspaces for the original pencils;
the separately conjugated symmetric matrices need not be principal
submatrices of one another. ◻
Proposition 3.9 uses
only the eight unshifted certificates 𝐷𝑘,0, not an all-rank coefficient
measure. The shifted certificates 𝐷𝑘,1 are used below for a truncated
Stieltjes moment representation and the first fifteen continued-fraction
coefficients, not for this application of Sylvester’s criterion. An
infinite-support coefficient measure would extend the pencil argument to
all ranks. At the certified ranks, the largest root is a nondecreasing
lower bound for 𝐹(𝑝); convergence
to 𝐹(𝑝), simple roots, strict
interlacing and denominator control are not established. At 𝑝 =1 the congruence degenerates and 𝐹 diverges, so the proposition excludes
that endpoint.
The pencil is different from the Jacobi matrix of the coefficient
moments. This is already visible at rank two. The defining formulas give
𝛽0=0,𝛽1=𝑝3(𝑝−1)2(𝑝+2)>0(𝑝>1).
Consequently det𝐵2 = −𝛽21 <0. Since 𝐴2 >0, the product of the two real
pencil roots is det𝐵2/det𝐴2 <0: one root is negative and the other positive. In
contrast, the finite Stieltjes construction below has only positive
nodes. Positivity of the coefficient Hankel matrix therefore does not
identify these two spectral constructions.
Formal continued fractions and finite quadrature.
Write 𝐷𝑛 =𝐷𝑛,0, 𝐸𝑛 =𝐷𝑛,1, with 𝐷0 =𝐸0 =1. All these determinant
polynomials are nonzero by the all-rank degree calculation above. The
classical Stieltjes continued fraction is thus defined over the
rational-function field ℚ(𝑝), with
the convention
∑𝑚≥0𝑠𝑚(𝑝)𝑧𝑚=11−𝜆1𝑧1−𝜆2𝑧1−⋯,
𝜆2𝑛−1=𝐸𝑛𝐷𝑛−1𝐷𝑛𝐸𝑛−1,𝜆2𝑛=𝐷𝑛+1𝐸𝑛−1𝐸𝑛𝐷𝑛(𝑛≥1).
Here
𝑠0 =1, and the identity is in ℚ(𝑝)[[𝑧]]. The classical moment
correspondence is recalled in [37]. Specialising a ratio at a fixed real 𝑝 requires its displayed denominators to
be nonzero. The sixteen certificates ensure this and 𝜆1,…,𝜆15 >0 for
every 𝑝 ≥1; they do not ensure it
at all indices. Seeking positive formulas for all these ratios is
therefore a specific version of the coefficient-moment question. The
generating series has radius of convergence zero for every 𝑝 ≥1, so the displayed identity must be
read formally. At 𝑝 =1 this follows
from 𝑠𝑚(1) =(𝑚!)3. For 𝑝 >1, the 𝑘 =0 term of the positive expansion for
𝑅𝑚 and the inequality [𝑚]𝑝! ≥𝑝𝑚(𝑚−1)/2 give
𝑠𝑚(𝑝)≥𝑝2𝑚2−𝑚.
Thus 𝑠𝑚(𝑝)1/𝑚 →∞. This concerns the
moment power series; it does not decide convergence of the continued
fraction at an individual nonzero value of 𝑧.
The same certificates also give a finite representing measure: for
each fixed 𝑝 ≥1, eight positive
atoms reproduce exactly 𝑠0,…,𝑠15. The construction uses
only the two certified 8 ×8
matrices, not positivity at higher ranks. Set
𝐻0=(𝑠𝑖+𝑗)𝑖,𝑗<8,𝐻1=(𝑠𝑖+𝑗+1)𝑖,𝑗<8,𝑇=𝐻−10𝐻1,
and give ℝ8 the inner product ⟨𝑢,𝑣⟩ =𝑢𝖳𝐻0𝑣. The
operator 𝑇 is self-adjoint and
positive definite because 𝐻0𝑇 =𝐻1
is symmetric and positive definite. If 𝑒0,…,𝑒7 are the coordinate
vectors, the Hankel identities give 𝑇𝑒𝑗 =𝑒𝑗+1 for 0 ≤𝑗 <7. Hence 𝑒0 is cyclic: its first eight iterates
form a basis. The spectral theorem now gives eight distinct positive
eigenvalues and a positive weight at each, namely the squared norm of
the corresponding projection of 𝑒0. Cyclicity ensures that no projection
vanishes and that no eigenspace has dimension greater than one.
Let 𝜈 be the resulting atomic
measure. For 0 ≤𝑚 ≤14, choose
𝑖,𝑗 ≤7 with 𝑖 +𝑗 =𝑚. Self-adjointness gives
∫𝑥𝑚𝑑𝜈(𝑥)=⟨𝑇𝑚𝑒0,𝑒0⟩=⟨𝑒𝑖,𝑒𝑗⟩=𝑠𝑚.
For the last moment,
∫𝑥15𝑑𝜈(𝑥)=⟨𝑇7𝑒0,𝑇𝑇7𝑒0⟩=𝑒𝖳7𝐻1𝑒7=𝑠15.
The weights sum to 𝑠0 =1. Hence the measure agrees with the
moment functional on every polynomial of degree at most 15; this is the degree range certified
for the eight-node quadrature obtained here. In an orthonormal
polynomial basis it is the classical Jacobi construction; Golub and
Welsch describe the computation of its nodes and weights [41]. Nothing here
identifies the subsequent moments of 𝜈 with 𝑠16,𝑠17,…. This finite
construction must also be distinguished from the coefficient pencil
(𝐴𝑁,𝐵𝑁). For rational
modifications of an already known moment functional, see Krattenthaler
[32]; such a
modification producing the entire sequence 𝑠𝑚 has not been identified.
Testing for additional cyclotomic factors.
Independently of the moment question, let 𝑣Φ𝑑 denote the multiplicity of the
cyclotomic factor Φ𝑑 in a
nonzero polynomial in ℚ[𝑝], and
set 𝑣Φ𝑑(0) =∞. For a
2 ×2 matrix with entry
valuations 0,2,2,5, the two
determinant products have valuations 5 and 4. The lower one is unique, so the
determinant has valuation 4. A tie
is different: all four entries of (1111+Φ𝑑)
have valuation zero, but its determinant is Φ𝑑. At general rank, we must find the
least total valuation and then test whether the terms attaining it
cancel. For 𝑁,𝑑 ≥1, define
H𝑁(𝑌;𝑝)=det(𝛼𝑖+𝑗𝑌−𝛽𝑖+𝑗)𝑖,𝑗<𝑁,𝑡𝑚,𝑑=min(𝑣Φ𝑑(𝛼𝑚),𝑣Φ𝑑(𝛽𝑚)),𝑒𝑁,𝑑=min𝜎∈𝑆𝑁𝑁−1∑𝑖=0𝑡𝑖+𝜎(𝑖),𝑑.
The last expression is a minimum-cost assignment:
row 𝑖 is matched to column 𝜎(𝑖) at cost 𝑡𝑖+𝜎(𝑖),𝑑. The valuation of a
polynomial in 𝑌 means the minimum
valuation of its coefficients in ℚ[𝑝]. Each determinant term is divisible
by Φ𝑒𝑁,𝑑𝑑. Set
Γ𝑁,𝑑(𝑌)=∑𝜎∈𝑆𝑁∑𝑖𝑡𝑖+𝜎(𝑖),𝑑=𝑒𝑁,𝑑sgn(𝜎)∏𝑖――――――――――――――Φ−𝑡𝑖+𝜎(𝑖),𝑑𝑑(𝛼𝑖+𝜎(𝑖)𝑌−𝛽𝑖+𝜎(𝑖)),
where the
bar is reduction in (ℚ[𝑝]/(Φ𝑑))[𝑌]. Then 𝑣Φ𝑑H𝑁 =𝑒𝑁,𝑑 exactly
when Γ𝑁,𝑑 ≠0. This
isolates the cancellation that a genuine additional factor would
require. The assignment bound records the smallest valuation available
among the determinant terms. Excess divisibility is possible only if
their leading residues cancel. To test that cancellation by one
determinant, we distribute the minimum valuation between rows and
columns. The integer costs are finite, since every 𝛼𝑚 is nonzero. Minimum-cost
assignment duality gives integer row and column potentials with
𝑢𝑖+𝑣𝑗≤𝑡𝑖+𝑗,𝑑,∑𝑖𝑢𝑖+∑𝑗𝑣𝑗=𝑒𝑁,𝑑.
Here is a direct construction, so
their existence is not an additional hypothesis. Choose a minimum-cost
permutation 𝜎. On the column
indices put a directed edge from 𝜎(𝑖) to 𝑗 of length 𝑡𝑖+𝑗,𝑑 −𝑡𝑖+𝜎(𝑖),𝑑. A negative
directed cycle would improve 𝜎
by reassigning the corresponding rows along that cycle; there is
therefore no such cycle. Add a new vertex with an edge of length zero to
every column. The shortest-path distances 𝑣𝑗 are finite integers and satisfy
𝑣𝑗−𝑣𝜎(𝑖)≤𝑡𝑖+𝑗,𝑑−𝑡𝑖+𝜎(𝑖),𝑑.
Putting 𝑢𝑖 =𝑡𝑖+𝜎(𝑖),𝑑 −𝑣𝜎(𝑖) gives
the inequalities above, with equality on the chosen assignment and hence
equality of totals.
Divide row 𝑖 by Φ𝑢𝑖𝑑 and column 𝑗 by Φ𝑣𝑗𝑑 over ℚ(𝑝). The inequalities ensure that every
resulting entry is in ℚ[𝑝,𝑌], even
if some potentials are negative. Reduce these entries modulo Φ𝑑. Only those with 𝑢𝑖 +𝑣𝑗 =𝑡𝑖+𝑗,𝑑 survive. The
determinant of the reduced matrix is Γ𝑁,𝑑, because every non-minimal
permutation vanishes on reduction. Thus the valuation exceeds 𝑒𝑁,𝑑 exactly when the reduced matrix
is singular over (ℚ[𝑝]/(Φ𝑑))(𝑌). A kernel relation
valid at just one value of 𝑌 is
insufficient: the determinant must vanish as a polynomial in 𝑌. Conversely, one nonzero value Γ𝑁,𝑑(𝑌0) proves equality with
the assignment bound. Neither assignment duality nor the existence of
the potentials forces the reduced determinant to vanish.
An exact calculation outside Lean gives the following monic contents.
Here cont𝑌 means
the monic gcd in ℚ[𝑝] of the
coefficients in 𝑌:
𝑁cont𝑌H𝑁1𝑝2𝑝5(𝑝−1)43𝑝14(𝑝−1)15(𝑝+1)44𝑝30(𝑝−1)32(𝑝+1)8(𝑝2+𝑝+1)45𝑝55(𝑝−1)55(𝑝+1)19(𝑝2+1)4(𝑝2+𝑝+1)8.
These factorisations attain the assignment bound
for every 𝑑 at these five ranks.
The residue certificates verify equality for 𝑑 ≤8; the displayed complete
factorisations contain no other cyclotomic factors, so the nonnegative
assignment bound is zero at all remaining 𝑑. The power of 𝑝 is not cyclotomic content.
For the table, an exact program
computes the full polynomials H𝑁(𝑌0;𝑝) at 𝑌0 =0,…,𝑁 by fraction-free
elimination, checking every polynomial division. Their monic gcd in
ℚ[𝑝] is cont𝑌H𝑁. A
divisor of all coefficients divides every evaluated polynomial;
conversely, the 𝑁 +1 values recover
those coefficients by rational interpolation in 𝑌. This proves the reverse divisibility
over ℚ[𝑝], where the interpolation
denominators are units. The calculation includes every factor, not just
a prescribed list of cyclotomic candidates.
The same program produces a nonzero residue witness for every pair
1≤𝑁≤8,1≤𝑑≤max(8,2𝑁−2).
There are 76 such pairs. For each, the certificate
gives an optimal assignment, integer dual potentials, an integer 𝑌0 ∈{0,…,𝑁} and the nonzero
residue Γ𝑁,𝑑(𝑌0). The
signed minimum-cost subset recurrence and the determinant of the reduced
matrix give the same residue. A separate check computes the full
polynomial H𝑁(𝑌0;𝑝) and
verifies directly that division by Φ𝑒𝑁,𝑑𝑑 leaves exactly this
nonzero residue. At 𝑁 =2,𝑑 =1, for
example, the entry valuations are (0225),
𝑒2,1 =4, and Γ2,1(0) = −9.
The source coefficients, determinant-value polynomials and witnesses
are computed by that program, which also repeats the direct determinant
checks; its recorded
result lists every witness. At ranks six to eight these certificates
cover only the stated cyclotomic-index window; complete coefficient
contents are computed only through rank five.
These computations distinguish systematic common factors from
cancellation beyond entry valuations, a distinction also important in
fraction-free matrix decompositions [40]. In particular the gcd argument at the
points 0,…,𝑁 is over ℚ[𝑝]: the rational Vandermonde inverse
is not generally integral, so it must not be used to assert the
corresponding coefficient gcd in ℤ[𝑝].
Proposition 4 of Krattenthaler–Rochev–Väänänen–Zudilin [13] obtains cyclotomic
factors through root-of-unity annihilation for a different first-order
tail recurrence. No corresponding recurrence has been established for
this moving-diagonal pencil. The finite witnesses prove equality with
the assignment bound at these 76
pairs. They do not exclude excess at larger ranks or, at ranks six to
eight, cyclotomic indices outside the stated window. Whether
minimum-valuation residues ever cancel systematically, and whether 𝑠𝑚 is a Stieltjes sequence, remain
separate questions. The remainder measure answers neither.
Rescaling integer rows
For a single irrationality form, the essential conditions are
integral coefficients and a nonzero remainder tending to zero. Dividing
a nonzero integer row (𝑈,𝑉) by
gcd(|𝑈|,|𝑉|) preserves integrality
and divides its remainder by the same amount; the resulting row is
primitive. A useful content division removes a factor already shared by
the two entries. Multiplying a row first merely introduces a factor that
also multiplies its remainder. For two rows, the same factors multiply
their determinant. The identities below separate this rescaling from
genuine cancellation. A height estimate is needed for an irrationality
measure, not for the elementary single-form criterion. For a real target
𝑆, put
𝐿𝑆(𝑈,𝑉)=𝑈𝑆−𝑉,Δ((𝑈𝑛,𝑉𝑛),(𝑈𝑚,𝑉𝑚))=𝑈𝑛𝑉𝑚−𝑈𝑚𝑉𝑛.
Here 𝐿𝑆(𝑈,𝑉) is the error of the
integer linear form, not the rational approximation error |𝑆 −𝑉/𝑈| when 𝑈 ≠0. The determinant eliminates 𝑆 exactly:
Δ=𝑈𝑚𝐿𝑆(𝑈𝑛,𝑉𝑛)−𝑈𝑛𝐿𝑆(𝑈𝑚,𝑉𝑚).
If this integer determinant does not vanish, then
1≤|Δ|≤|𝑈𝑚||
|
|𝐿𝑆(𝑈𝑛,𝑉𝑛)|
|
|+|𝑈𝑛||
|
|𝐿𝑆(𝑈𝑚,𝑉𝑚)|
|
|,
and the two errors cannot both be smaller than 1/(|𝑈𝑛| +|𝑈𝑚|). The next theorem
compares the divisor introduced by rescaling with the resulting change
in the determinant’s absolute value.
Theorem 4.1 (rescaling rows and their determinant).
Let 𝑆 be real, let (𝑈𝑛,𝑉𝑛) and (𝑈𝑚,𝑉𝑚) be pairs of integers, and let
𝑐𝑛,𝑐𝑚 be integers. Then
𝐿𝑆(𝑐𝑛𝑈𝑛,𝑐𝑛𝑉𝑛)=𝑐𝑛𝐿𝑆(𝑈𝑛,𝑉𝑛),
Δ(𝑐𝑛(𝑈𝑛,𝑉𝑛),𝑐𝑚(𝑈𝑚,𝑉𝑚))=𝑐𝑛𝑐𝑚Δ((𝑈𝑛,𝑉𝑛),(𝑈𝑚,𝑉𝑚)),
and consequently
|Δ(𝑐𝑛(𝑈𝑛,𝑉𝑛),𝑐𝑚(𝑈𝑚,𝑉𝑚))|=|𝑐𝑛||𝑐𝑚||Δ((𝑈𝑛,𝑉𝑛),(𝑈𝑚,𝑉𝑚))|.
In
particular 𝑐𝑛𝑐𝑚 divides the
scaled determinant. Multiplication by these scalars therefore introduces
a divisor whose absolute value is exactly the factor multiplying the
determinant’s absolute value.
Proof. Expand the linear form and use the bilinearity of the
determinant. The original integer determinant is the quotient witnessing
divisibility; it need not be primitive. ◻
Example 4.2. Take (𝑈𝑛,𝑉𝑛) =(1,2) and (𝑈𝑚,𝑉𝑚) =(3,5), so that Δ =1 ⋅5 −3 ⋅2 = −1. Multiplying
the first row by 𝑐𝑛 =6 and the
second by 𝑐𝑚 =10 gives the rows
(6,12) and (30,50), whose determinant is 6 ⋅50 −30 ⋅12 = −60. That determinant
is now divisible by 60, which looks
like a local gain of 60; and its
absolute value has risen from 1 to
60, which is a cost of exactly the
same size.
Lean checks the error identity in error
scaling, the determinant identity in content
factorisation, the exact absolute-height identity in absolute
determinant scaling, the divisor statement in content-product
divisibility, and the elimination identity in exterior
determinant identity.
The identities allow zero scalars, but cancelling the scalar factors
requires them to be nonzero. Multiplication alone gives no improvement
in the comparison between a divisor and the determinant’s absolute
value. The theorem neither asserts that the determinant is nonzero nor
estimates the original approximation error. Cancelling polynomial
factors before evaluation, finding factors common to several minors, and
adding different rows remain separate operations.
Congruences after evaluation at 3/2
We use congruences modulo powers of 2 and 3 to find combinations of evaluated
polynomials with prescribed divisibility. The argument applies to
arbitrary integral polynomials, including the forms of [8]. The
denominator-clearing map must be the same for every row that will be
added. We therefore fix a common truncation index 𝑊 ≥0 and, for 𝑃(𝑋) =∑𝑖𝑝𝑖𝑋𝑖 ∈ℤ[𝑋], put
𝐻𝑊(𝑃)=𝑊∑𝑖=0𝑝𝑖3𝑖2𝑊−𝑖.
This is the denominator-cleared
evaluation at 3/2. Each term
𝑝𝑖𝑋𝑖 with 𝑖 ≤𝑊 contributes 𝑝𝑖3𝑖2𝑊−𝑖. Keep the index 𝑊 fixed when polynomials are added. When
𝑊 ≥deg𝑃, this is exactly the
cleared numerator, since
𝑊∑𝑖=0𝑝𝑖3𝑖2𝑊−𝑖=2𝑊𝑊∑𝑖=0𝑝𝑖(32)𝑖=2𝑊𝑃(32).
Here a unit coefficient in ℤ
means 1 or −1. Thus a monic polynomial of degree
𝑊 with constant term ±1 satisfies both unit conditions
below. Those conditions are sufficient, not necessary: the congruences
themselves only require that the relevant coefficient not be divisible
by the relevant prime.
Theorem 5.1 (endpoint residues). Let 𝑃 =∑𝑖𝑝𝑖𝑋𝑖 ∈ℤ[𝑋] and let 𝑊 ≥0. Then
𝐻𝑊(𝑃)≡𝑝02𝑊(mod3),𝐻𝑊(𝑃)≡𝑝𝑊3𝑊(mod2).
Consequently a unit constant
coefficient prevents divisibility by 3, and a unit coefficient at index 𝑊 prevents divisibility by 2.
Proof. Modulo 3, every
summand with 𝑖 >0 vanishes;
modulo 2, every summand with 𝑖 <𝑊 vanishes. The remaining powers are
units in the corresponding residue fields. ◻
Since 2𝑊 is invertible modulo
3 and 3𝑊 is invertible modulo 2, the two congruences say more than the
stated consequence: divisibility of 𝐻𝑊(𝑃) by 3 is decided by 𝑝0 alone, and divisibility by 2 by 𝑝𝑊 alone. The rest of the coefficient
vector is invisible to both primes. The coefficient 𝑝𝑊 is the top coefficient of 𝑃 exactly when deg𝑃 =𝑊, and is zero when deg𝑃 <𝑊. The identity 𝐻𝑊(𝑃) =2𝑊𝑃(3/2) is guaranteed when
deg𝑃 ≤𝑊. Without a degree
bound, increasing the truncation index gives
𝐻𝑊+1(𝑃)=2𝐻𝑊(𝑃)+𝑝𝑊+13𝑊+1,
so
the truncated sum doubles precisely when the extra coefficient is
zero.
Example 5.2. Take 𝑊 =2. The three polynomials below differ
only at an endpoint.
𝑃 |
𝐻2(𝑃) |
3 ∣𝐻2(𝑃) |
2 ∣𝐻2(𝑃) |
| 𝑋2 +1 |
1 ⋅4 +0 ⋅6 +1 ⋅9 =13 |
no |
no |
| 𝑋2 +3 |
3 ⋅4 +0 ⋅6 +1 ⋅9 =21 |
yes |
no |
| 2𝑋2 +1 |
1 ⋅4 +0 ⋅6 +2 ⋅9 =22 |
no |
yes |
The first has both endpoints equal to 1 and its evaluation, 13, is divisible by neither prime; as a
check, 22((3/2)2 +1) =13. The second
and third show that each hypothesis is used: spoiling the constant
endpoint admits 3, and spoiling the
top endpoint admits 2.
Formal proofs cover the congruences modulo
3 and modulo
2, together with the
consequences for a unit
constant coefficient and a unit
coefficient of 𝑋𝑊.
In the following proposition, a unit top endpoint means that the
coefficient at index 𝑊 is 1 or −1, with no degree bound imposed. The two
conditions apply to different entries of the polynomial pair.
Proposition 5.3 (common divisor). Let 𝑈,𝑉 ∈ℤ[𝑋] and let 𝑊 ≥0. If 𝑈 has unit top endpoint, 𝑉 has unit constant endpoint, and an
integer 𝑐 divides both 𝐻𝑊(𝑈) and 𝐻𝑊(𝑉), then
2∤𝑐and3∤𝑐.
Proof. If 2 ∣𝑐, then
2 ∣𝐻𝑊(𝑈), contrary to the unit
coefficient at index 𝑊 and
Theorem 5.1. Similarly,
3 ∣𝑐 would imply 3 ∣𝐻𝑊(𝑉), contrary to the unit
constant coefficient. ◻
Lean checks this common-divisor
exclusion. The proposition does not say that the two evaluations are
coprime; it says only that every common divisor is coprime to 6. It gives no restriction on the other
prime factors of that divisor.
Example 5.4. Take 𝑊 =2, 𝑈 =𝑋2 +3 and 𝑉 =5𝑋2 +1. The top endpoint of 𝑈 and the constant endpoint of 𝑉 are both 1, and
𝐻2(𝑈)=3⋅4+1⋅9=21,𝐻2(𝑉)=1⋅4+5⋅9=49.
Here gcd(21,49) =7. The endpoint assumptions
therefore allow a nontrivial common divisor, but that divisor is coprime
to 6.
Corollary 5.5 (limits of rescaling and common-divisor
cancellation at 3/2). Under
the endpoint hypotheses of Proposition 5.3, every
common divisor of the unscaled evaluations 𝐻𝑊(𝑈) and 𝐻𝑊(𝑉) is coprime to 6. Multiplying two integer rows by
nonzero integers 𝑐𝑛,𝑐𝑚 multiplies
their determinant by 𝑐𝑛𝑐𝑚 and its
absolute value by |𝑐𝑛𝑐𝑚|.
Cancelling this introduced scalar factor therefore leaves the original
comparison between divisor and determinant size unchanged.
Proof. The common-divisor assertion is Proposition 5.3. By
Theorem 4.1,
rescaling the two rows by 𝑐𝑛,𝑐𝑚
multiplies their errors by 𝑐𝑛,𝑐𝑚,
respectively, and their 2 ×2
determinant by 𝑐𝑛𝑐𝑚. For nonzero
scalars, the introduced divisor has the same absolute value as the
introduced factor in that determinant. Dividing out that factor restores
the original determinant, including its original divisor-to-size
comparison. ◻
One further consequence of Theorem 5.1 is worth
stating, because it bears on the most natural way one might hope to
import an existing denominator reduction. Write Φ𝑚 for the 𝑚th cyclotomic polynomial and, for
coprime 𝑎 >𝑏 ≥1, put Φ𝑚(𝑎,𝑏) =𝑏𝜑(𝑚)Φ𝑚(𝑎/𝑏) for
its homogenisation, with exponent 𝜑(𝑚) =degΦ𝑚.
Proposition 5.6 (coprimality of homogenised
cyclotomic values). Let 𝑎 >𝑏 ≥1 with gcd(𝑎,𝑏) =1 and let 𝑚 ≥1. Then gcd(Φ𝑚(𝑎,𝑏),𝑎𝑏) =1. In particular
gcd(Φ𝑚(3,2),6) =1 for every
𝑚.
Proof. The polynomial Φ𝑚 is monic and Φ𝑚(0) = ±1. The endpoint argument in
Theorem 5.1 also works
at (𝑎,𝑏): modulo a prime dividing
𝑏, only 𝑎𝜑(𝑚) survives, and modulo a
prime dividing 𝑎, only Φ𝑚(0)𝑏𝜑(𝑚) survives.
Coprimality of 𝑎 and 𝑏 makes each surviving term
nonzero. ◻
Rhin and Viola’s factorial-coset quotients [17] reduce denominators of rational forms
in 𝜁(2). Zudilin’s 𝑞-analogue has an order-twelve symmetry
group for the normalised series; its denominator cancellation uses the
order-six subgroup preserving the required sign condition [8]. Proposition 5.6 applies to
these cyclotomic factors: each homogenised value at (3,2), and hence any product of them, is
divisible by neither 2 nor 3. It makes no such assertion about an
arbitrary integer or factorial factor, which can contain both primes.
Cancelling a common cyclotomic factor can still reduce the real absolute
values. That reduction is distinct from producing the powers of 2 or 3 sought in Section 10.
Scalar multiplication can introduce powers of 2 and 3, but does not improve this comparison.
Under the endpoint hypotheses, the unscaled pair has no common factor at
either prime. Neither observation shows that a gain at these primes is
necessary for a proof by linear forms at 3/2.
The operation studied next is different: take an integer combination
of several rows and ask that the combination be divisible where the
individual rows are not. The proposed divisor must come from
cancellation between rows, not from multiplying a row by that divisor.
The endpoint congruences are the first case of a divisibility condition
that can be imposed to any depth, and it is that condition, read
additively, which is counted below.
We first raise the two congruences to prime powers. Fix depths 𝑅,𝑆 ≥0. For 𝑃 ∈ℤ[𝑋], let 𝐽3,𝑅(𝑃) and 𝐽2,𝑆(𝑃) be the residues of 𝐻𝑊(𝑃) modulo 3𝑅 and 2𝑆, respectively. Theorem 5.1 computes the
depth-one residues. At depth 𝑅,
terms with 𝑖 ≥𝑅 are invisible
modulo 3𝑅; at depth 𝑆, terms with 𝑊 −𝑖 ≥𝑆 are invisible modulo 2𝑆. Thus deeper congruences inspect
longer segments of the two ends of the coefficient list, always at the
same fixed 𝑊.
Lemma 5.7 (a residue and divisibility by 3𝑅). Vanishing of the residue
modulo 3𝑅 is exactly
divisibility by the corresponding power of three: 𝐽3,𝑅(𝑃) =0 if and only if 3𝑅 ∣𝐻𝑊(𝑃).
Proof. By definition 𝐽3,𝑅(𝑃) is the image of the integer
𝐻𝑊(𝑃) in ℤ/3𝑅ℤ. The kernel of
this quotient map is 3𝑅ℤ,
which proves the equivalence, including 𝑅 =0. ◻
The same argument gives 𝐽2,𝑆(𝑃) =0 ⟺ 2𝑆 ∣𝐻𝑊(𝑃) for 𝑆 ≥0.
The vector of four residues of a coefficient pair (𝑈,𝑉) is then the quadruple
(𝐽3,𝑅(𝑈),𝐽3,𝑅(𝑉),𝐽2,𝑆(𝑈),𝐽2,𝑆(𝑉))∈(ℤ/3𝑅ℤ)2×(ℤ/2𝑆ℤ)2,
two residues for each of
the two primes, one from each entry of the pair. By the displayed
criteria it vanishes exactly when 3𝑅 divides both specialised entries and
2𝑆 divides both.
Instead of requiring each input row to have a common divisor, we seek
a small integer combination whose two entries are both divisible by
3𝑅2𝑆. Since 𝐻𝑊 is additive, the four residues of the
combination are the corresponding sums of the input residues. This
allows a pigeonhole argument on subset sums.
Theorem 5.8 (equal residues for two subset sums).
Fix a truncation index 𝑊 and
depths 𝑅,𝑆, and let (𝑈𝑗,𝑉𝑗)𝑗<𝑀 be any 𝑀 pairs of integral polynomials.
Represent each subset of {0,…,𝑀 −1} by its indicator vector
in {0,1}𝑀. If the 2𝑀 subsets outnumber the possible
residue vectors in
(ℤ/3𝑅ℤ)2×(ℤ/2𝑆ℤ)2,
then two
distinct subsets have the same residue vector. Subtracting their
indicator vectors gives a nonzero coefficient vector in { −1,0,1}𝑀 cancelling all four
residues. The target has exact cardinality
(3𝑅)2(2𝑆)2.
In particular, if 𝑅 >0 and 4𝑅 +2𝑆 ≤𝑀, such a collision
exists.
Proof. Send each subset to the sum of the residue vectors of
its members. The pigeonhole principle gives two distinct subsets with
the same residue vector. The number of possible vectors is the product
of the four moduli. For 𝑅 >0,
(3𝑅)2(2𝑆)2<(4𝑅)2(2𝑆)2=24𝑅+2𝑆≤2𝑀,
which proves the stated sufficient threshold. ◻
The power bracket improves the generic coefficient 4𝑅 when the depth 𝑅 is a positive integer multiple of 41. All depths and row counts in the
following corollary, including 𝑇,
are integers.
Corollary 5.9 (the exact count at depth 41). Let 𝑇 >0. At modulus 3𝑅 with 𝑅 =41𝑇, any family of 𝑀 ≥130𝑇 +2𝑆 integral polynomial pairs has
two distinct binary vectors with the same residue vector. For 𝑇 =1 the coefficient 130 is exact for this counting argument:
2129+2𝑆<|
|
|(ℤ/341ℤ)2×(ℤ/2𝑆ℤ)2|
|
|.
No exact-optimality
assertion is made here for 𝑇 >1.
Proof. The upper power inequality gives
(341𝑇)2(2𝑆)2<(265)2𝑇(2𝑆)2=2130𝑇+2𝑆≤2𝑀,
so Theorem 5.8 applies. For
𝑇 =1, direct integer evaluation
gives 2129 <382;
multiplying by (2𝑆)2 gives the
displayed reverse count at 129 +2𝑆. ◻
The formal statements check the sufficient
count 130𝑇 +2𝑆 and, when 𝑇 =1, the failure
of the count at 129 +2𝑆.
For all depths at once the ambient-cardinality inequality 2𝑀 >32𝑅22𝑆 holds exactly when
𝑀 ≥ ⌊2𝑅log23+2𝑆⌋+1,
by the definition of
the floor function; irrationality of log23 is not needed for this strict-inequality reformulation. At
𝑅 =41 this is 130 +2𝑆, and at 𝑅 =41 ⋅31 it is 4029 +2𝑆, one below the uniform bound
4030 +2𝑆 of Corollary 5.9; the
corollary trades exactness for a certificate that is a single integer
comparison. Here 41 is the exponent
of 3 in the modulus, not the number
of input rows; at that depth the counting bound is 130 +2𝑆 rows.
The count produces two distinct subsets, not necessarily two distinct
row sums or remainder values. Repeated rows already illustrate the first
failure. To prevent the second, we bound how many subsets can have any
specified remainder. The following finite-set statement isolates that
requirement.
Theorem 5.10 (equal residues with different values).
Let 𝐴 and 𝐵 be finite sets, let 𝑓 :𝐴 →𝐵, and let 𝑔 :𝐴 →𝐶 be any map into a set 𝐶. Suppose every fibre of 𝑔 has at most 𝑘 elements. If
|𝐵|𝑘<|𝐴|,
then there exist distinct
𝑥,𝑦 ∈𝐴 such that
𝑓(𝑥)=𝑓(𝑦)and𝑔(𝑥)≠𝑔(𝑦).
Thus, when 𝑓 records
the four residues and 𝑔 records the
real remainder, a bound on the multiplicities of equal remainders
guarantees a pair with equal residues and different remainders.
Proof. If every pair in a common 𝑓-fibre also had the same 𝑔-value, each 𝑓-fibre would lie in one 𝑔-fibre and hence have size at most 𝑘. Summing over the at most |𝐵| fibres of 𝑓 would give |𝐴| ≤|𝐵|𝑘, contrary to the
hypothesis. ◻
If 𝑔 is injective, the
hypothesis holds with 𝑘 =1. It need
not hold with a useful small 𝑘 for
subset sums: repeated rows produce many equal sums, even when every row
is primitive. The theorem assumes a bound on every fibre of 𝑔, not merely on the fibres of (𝑓,𝑔). It gives a nonzero difference but
no upper bound on its real size. To bound the size as well, we partition
the range of 𝑔 into small
intervals. The count now uses residue class, interval and multiplicity.
Only repetitions within one residue class matter, so the quantitative
version assumes a bound for fibres of (𝑓,𝑔) rather than for all fibres of 𝑔.
Theorem 5.11 (equal residues with close, distinct
values). Let 𝐴,𝐵,𝐽 be finite
sets and let 𝑓 :𝐴 →𝐵, 𝑔 :𝐴 →ℝ and 𝜄 :𝐴 →𝐽. Suppose that each
simultaneous fibre of (𝑓,𝑔) has at
most 𝑘 elements and that, for some
𝛿 >0,
𝜄(𝑥)=𝜄(𝑦)⟹|𝑔(𝑥)−𝑔(𝑦)|<𝛿.
If |𝐵||𝐽|𝑘 <|𝐴|, then some distinct 𝑥,𝑦 ∈𝐴 satisfy
𝑓(𝑥)=𝑓(𝑦),0<|𝑔(𝑥)−𝑔(𝑦)|<𝛿.
Proof. Suppose that no such pair exists. Two points in a
fibre of (𝑓,𝜄) have equal 𝑓-values and 𝑔-values less than 𝛿 apart, so their 𝑔-values must be equal. Thus each fibre
of (𝑓,𝜄) lies in a fibre of
(𝑓,𝑔) and contains at most 𝑘 points. Summing over its at most |𝐵||𝐽| fibres gives |𝐴| ≤|𝐵||𝐽|𝑘, a contradiction. ◻
For an application, let 𝑀
integral coefficient rows (𝐴𝑗,𝐵𝑗)
have real remainders 𝑒𝑗 at the
same target. Let 𝐷 be a positive
integer, and suppose that the coefficient-pair subset sums ∑𝑗∈𝐼(𝐴𝑗,𝐵𝑗) take 𝑄 values in (ℤ/𝐷ℤ)2. Put 𝑇 =∑𝑗|𝑒𝑗|. The least and greatest
subset remainders are respectively
∑𝑒𝑗<0𝑒𝑗and∑𝑒𝑗>0𝑒𝑗,
so the interval between them has length 𝑇. Divide it into half-open intervals of
width 𝐷/𝑛, using a final interval
for the right endpoint if necessary. At most ⌊𝑛𝑇/𝐷⌋ +1 intervals are
needed. If each simultaneous residue-and-remainder fibre has size at
most 𝑘, the inequality
2𝑀>𝑄𝑘(⌊𝑛𝑇/𝐷⌋+1)
therefore gives equal residues with
remainder difference strictly between 0 and 𝐷/𝑛 in absolute value. Subtracting the
two subset sums and dividing both coefficients by 𝐷 gives an integral form of nonzero
absolute value less than 1/𝑛. For a
prescribed family, the number 𝑄,
the width 𝑇 and the multiplicity
bound 𝑘 must all be justified. We
have no such bounds giving the required forms for the Zudilin family at
3/2.
The next improvement needs a much stronger hypothesis than
primitivity: adjacent determinants must vanish modulo the chosen
modulus. Unit multiples of one unimodular row satisfy it. Arbitrary
primitive rows do not; for example, (1,0) and (0,1) have determinant 1. Under this hypothesis the rows lie in
the free rank-one submodule generated by a unimodular row. A change of
coordinates makes their second coordinates zero, so only one residue
coordinate must be counted.
Theorem 5.12 (vanishing minors and a residue count).
Let 𝑅0 be a commutative ring
and let 𝑤𝑛 =(𝐴𝑛,𝐵𝑛) ∈𝑅20.
Suppose that each row is unimodular, meaning that 𝑢𝑛𝐴𝑛 +𝑣𝑛𝐵𝑛 =1 for some 𝑢𝑛,𝑣𝑛 ∈𝑅0, and that every adjacent
minor vanishes:
𝐴𝑛𝐵𝑛+1−𝐵𝑛𝐴𝑛+1=0(𝑛≥0).
Then every pairwise minor 𝐴𝑖𝐵𝑗 −𝐵𝑖𝐴𝑗 vanishes. In particular,
take 𝑅0 =ℤ/(2𝑆3𝑅)ℤ with 𝑅 >0. If 𝑆 +2𝑅 ≤𝑘, there are two distinct binary
vectors 𝑠,𝑡 ∈{0,1}𝑘 such that
∑𝑖<𝑘𝑠𝑖𝑤𝑖=∑𝑖<𝑘𝑡𝑖𝑤𝑖.
Thus 𝑆 +2𝑅 rows suffice. The ambient
two-coordinate argument gives the sufficient bound 2𝑆 +4𝑅.
Proof. If (𝑎,𝑏) is
unimodular, say 𝑢𝑎 +𝑣𝑏 =1, and 𝑎𝑦 −𝑏𝑥 =0, then
(𝑥,𝑦)=(𝑢𝑥+𝑣𝑦)(𝑎,𝑏).
Indeed, the first
coordinate follows by replacing 𝑎𝑦
with 𝑏𝑥, and the second by the
reverse substitution. Apply this identity to consecutive rows: each next
row is a scalar multiple of the current one. Induction places the entire
tail on the line through 𝑤0 and
proves the pairwise-minor assertion. Right multiplication by
(𝑢0−𝐵0𝑣0𝐴0)
has determinant 𝑢0𝐴0 +𝑣0𝐵0 =1 and
sends 𝑤0 to (1,0). All transformed subset sums
therefore have second coordinate zero and occupy at most 2𝑆3𝑅 values. Finally
2𝑆3𝑅<2𝑆4𝑅=2𝑆+2𝑅≤2𝑘,
so the
pigeonhole principle gives two distinct subsets with the same sum. ◻
No particular coordinate needs to be invertible: modulo six, (2,3) is unimodular because −2 +3 =1, although neither entry is a unit.
Some nondegeneracy is essential. The rows (1,0),(0,0),(0,1) have zero adjacent
minors but outer minor one. For the counting conclusion, vanishing is
required only in the quotient ring. The integer rows (1,0),(1,6) used in Section 10 are independent
over ℚ, with determinant 6, but coincide modulo 6. Thus dependence modulo the modulus
neither follows from primitivity nor implies dependence of the integer
rows.
This conditional theorem is stronger than the ambient count of
possible residue vectors only after its minor-vanishing hypothesis has
been established. No such all-tail hypothesis is proved here for an
actual 𝑞-Apéry or Zudilin family,
and the theorem says nothing about whether the difference of the subset
sums has nonzero analytic remainder.
The count in Corollary 5.9 is sharp
at 𝑇 =1 for comparison with the full
residue space. To obtain different remainders, Theorem 5.10
additionally needs a bound on how often the same real value occurs. Such
a bound is not proved here for the 𝑞-Apéry or Zudilin remainder family.
Lean checks the cardinality
of the residue space, the pigeonhole
argument for the residue map and the sufficient
row count for equal residues. The pigeonhole argument gives
divisibility without an independence hypothesis. Further information
about the family is needed to ensure that the nonzero difference of the
indicator vectors gives a nonzero polynomial pair and a nonzero analytic
remainder. None of these statements supplies such a family or proves
either nonvanishing conclusion.
Example 5.13. At depths 𝑅 =𝑆 =1 the space of four residue
coordinates is (ℤ/3ℤ)2 ×(ℤ/2ℤ)2, of
cardinality 9 ⋅4 =36, and the
threshold reads 𝑀 ≥4 ⋅1 +2 ⋅1 =6. With six pairs
there are 26 =64 subsets and only
36 possible residue vectors. Two
subsets therefore have equal residues. The difference of their indicator
vectors is a nonzero vector in { −1,0,1}6 whose sum vanishes in all
four coordinates.
The following elementary comparison concerns only the two scalar
exponents of Zudilin’s construction; it makes no assertion about the
coefficient polynomials or their real remainders.
Theorem 5.14 (a restriction on the two scalar
exponents). Let 𝐶1 >0. If
𝐶0 ≤0 or 2𝐶0 ≤𝐶1, then
𝐶0log3−𝐶1log2<0.
In the
positive branch 𝐶0 >0 and 2𝐶0 ≤𝐶1, the stronger estimate is
𝐶0log3−𝐶1log2<−1741𝐶0log2.
Proof. If 𝐶0 ≤0, then
𝐶0log3 −𝐶1log2 ≤ −𝐶1log2 <0.
If 𝐶0 >0 and 2𝐶0 ≤𝐶1, use 341 <265 to obtain
𝐶0log3−𝐶1log2≤𝐶0(log3−2log2)<−1741𝐶0log2<0.
◻
Written multiplicatively, the conclusion is 3𝐶0 <2𝐶1. Lean checks the inequality
and the 17/41 margin of the positive branch.
The scope of this elementary inequality matters. The primary Zudilin
theorem [8] supplies
an integer-base irrationality-exponent estimate on its parameter cone,
and the elementary inequality 𝜇 ≥2 then forces 2𝐶0 ≤𝐶1 whenever 𝐶0 >0; Lean checks that implication
separately. The primary 2004 theorem is stated for an integer inverse
base. The rational specialisation proved earlier in this record has
separate proofs for the constructed forms. The scalar statement in this
paragraph is only the displayed inequality; it neither constructs a new
family at 3/2 nor formalises a
universal exclusion of linear-form methods.
Complements and further questions
An unrestricted construction of small nonzero integer forms is
another formulation of irrationality, not yet a method of proving it.
The next problem remains equivalent to irrationality at 3/2 even with its quadratic degree
bounds, and even after imposing the exponential coefficient-height bound
discussed below. We prove the equivalence before asking what a specified
approximation family can supply.
Problem 10.1 (a divided linear form with small nonzero
remainder). Exhibit an integer constant 𝐶 ≥1 and, for every sufficiently large
positive integer 𝑛, positive
integers 𝑊𝑛,𝑅𝑛,𝑆𝑛,𝑀𝑛 such that
𝑛2≤𝑊𝑛,𝑅𝑛,𝑆𝑛≤𝐶𝑛2,4𝑅𝑛+2𝑆𝑛≤𝑀𝑛≤𝐶𝑛2,
together with polynomial pairs
(𝑈𝑛,𝑗,𝑉𝑛,𝑗) ∈ℤ[𝑋]2 for
0 ≤𝑗 <𝑀𝑛, each of degree at
most the common degree bound 𝑊𝑛,
whose specialised integer rows are primitive:
gcd(𝐻𝑊𝑛(𝑈𝑛,𝑗),𝐻𝑊𝑛(𝑉𝑛,𝑗))=1.
Find a nonzero vector 𝜆(𝑛) ∈{ −1,0,1}𝑀𝑛 for
which, on putting
𝑈𝑛=∑𝑗<𝑀𝑛𝜆(𝑛)𝑗𝑈𝑛,𝑗,𝑉𝑛=∑𝑗<𝑀𝑛𝜆(𝑛)𝑗𝑉𝑛,𝑗,
the pair
(𝑈𝑛,𝑉𝑛) is not (0,0), all four residues vanish,
𝐽3,𝑅𝑛(𝑈𝑛)=𝐽3,𝑅𝑛(𝑉𝑛)=0,𝐽2,𝑆𝑛(𝑈𝑛)=𝐽2,𝑆𝑛(𝑉𝑛)=0,
where every residue in
this display is formed using the common degree bound 𝑊𝑛, and the resulting divided integer
linear form
𝐴𝑛=𝐻𝑊𝑛(𝑈𝑛)3𝑅𝑛2𝑆𝑛,𝐵𝑛=𝐻𝑊𝑛(𝑉𝑛)3𝑅𝑛2𝑆𝑛,𝜌𝑛=𝐴𝑛𝐹(3/2)−𝐵𝑛
satisfies the explicit analytic condition
0<|𝜌𝑛|<1𝑛.
The residue equations make 𝐴𝑛,𝐵𝑛 integers. A solution would prove
irrationality: if 𝐹(3/2) =𝑎/𝑏 in
lowest terms, every nonzero 𝜌𝑛
has absolute value at least 1/𝑏,
contradicting the displayed bound for 𝑛 >𝑏. Theorem 5.8 supplies
only a nonzero signed relation with the four residue equations once the
pairs and size inequality are present; it does not supply primitive
input rows, a nonzero combined polynomial pair, or the nonvanishing and
decay of 𝜌𝑛.
Why the choice of family matters.
The converse can start from an arbitrary small integer form and build
the polynomial rows afterwards. Pigeonhole approximation supplies the
small form; Bézout’s identity lifts its coordinates to polynomial
evaluations. Thus the degree and residue conditions do not constrain how
the approximation was obtained. Let 𝜉 be any irrational real number.
Comparing the fractional parts of 0,𝜉,…,(𝑛 +1)𝜉 in 𝑛 +1 equal half-open intervals gives
integers 𝐴 ≥1 and 𝐵 with
𝐴≤𝑛+1,0<|𝐴𝜉−𝐵|<1𝑛+1<1𝑛.
Set 𝑤 =𝑛2, 𝑊𝑛 =𝑅𝑛 =𝑆𝑛 =𝑤, 𝑀𝑛 =6𝑤, and 𝐷 =6𝑤. The three integer rows
(𝐷𝐴,1),(1,𝐷𝐵−1),(−1,0)
are
primitive and sum to (𝐷𝐴,𝐷𝐵). Pad
them to 𝑀𝑛 rows with (1,0), and use the coefficient vector
(1,1,1,0,…,0).
To realise every coordinate as a polynomial evaluation of degree at
most 𝑤, choose integers 𝑢,𝑣 such that 𝑢2𝑤 +𝑣3𝑤 =1. For any integer ℎ, the polynomial ℎ(𝑢 +𝑣𝑋𝑤) satisfies 𝐻𝑤(ℎ(𝑢 +𝑣𝑋𝑤)) =ℎ. Lift all row
coordinates this way. The combined polynomial pair is nonzero because
its first evaluation is 𝐷𝐴 ≠0. Its
two evaluations are divisible by 3𝑤2𝑤, and its divided remainder is
𝐴𝜉 −𝐵. All the conditions of
Problem 10.1,
with 𝐹(3/2) replaced by 𝜉, hold with 𝐶 =6.
Even a coefficient-height bound of the form exp(𝑂𝜉(𝑛2)) would not exclude these
lifts. Choose 0 ≤𝑣 <2𝑤, which
gives |𝑢| <3𝑤. Since |𝐵| ≤(𝑛 +1)|𝜉| +1, every lifted
coefficient has absolute value at most (|𝜉| +2)(𝑛 +1)18𝑤. Together with the
preceding rationality contradiction, this proves that the unrestricted
construction problem for a real target 𝜉 is equivalent to the irrationality of
𝜉. It does not establish either
assertion for 𝐹(3/2).
The short paper refers to this formulation and to its equivalence
with irrationality. To pose a more specific question, one must replace
the free choice of polynomial pairs by an actual set given by
coefficient formulas, admissible parameters and permitted
normalisations. The restriction must exclude the freedom to choose the
rows from an already good approximation. Merely giving the resulting
family a name, an explicit formula or an exponential height bound does
not do so: the lifts above have all three. For a fixed indexed family,
the distinction between all sufficiently large indices and a sparse
subsequence can matter. Arbitrary padding and reindexing remove it in
the unrestricted problem.
Corollary 5.5 gives no
improvement from integer rescaling and, under its endpoint hypotheses,
no common factor 2 or 3 in the unscaled evaluations. It makes
no general assertion about polynomial cancellation before
specialisation, combinations of rows, determinant-specific divisibility
or other approximation families.
A prescribed family must supply nonvanishing and decay for the same
signed combinations. A residue collision alone supplies neither;
separate examples of the two properties would not suffice either. A
coefficient-height estimate is needed when the approximation argument
calls for it, not as an extra hypothesis of the elementary irrationality
criterion above.
A congruence relation with nonzero remainder
Fixing the approximation family is not enough: the residue map must
also use a fixed normalisation. Polynomial coefficient content, content
of an evaluated row, and content of a combined row are three different
quantities. We keep them separate as follows. For each 𝑛, let 𝑊𝑛 be a common degree bound and let
(𝑈𝑛,𝑗,𝑉𝑛,𝑗,R𝑛,𝑗)𝑗<𝑀𝑛
be the chosen forms, with 𝑈𝑛,𝑗,𝑉𝑛,𝑗 ∈ℤ[𝑋] of degree at most
𝑊𝑛 and
R𝑛,𝑗(𝑡)=𝑈𝑛,𝑗(𝑡)𝐹(𝑡)−𝑉𝑛,𝑗(𝑡)(𝑡>1).
This
identity uses the same normalisation as the evaluated rows and all
subsequent residue equations. Fix all divisions before forming the
residue map. Require each polynomial pair to have coefficient gcd 1, by dividing its common integer
coefficient factor if necessary. This is different from making the two
evaluated integers coprime, as required in Problem 10.1. The two
operations need not preserve the same polynomial family. Coefficient
content 1 alone gives no
coprimality with 6 after
evaluation: at 𝑊 =1, the pairs (𝑋,3) and (2𝑋 −1,2) have coefficient content 1 but give the integer rows (3,6) and (4,4), respectively.
The gcd
gcd(𝐻𝑊𝑛(𝑈𝑛,𝑗),𝐻𝑊𝑛(𝑉𝑛,𝑗))
of one evaluated row can differ from the gcd of the final sum. Neither
is divided out without also dividing the corresponding remainder and
measuring the height after that division. If, in addition, the
coefficient of 𝑋𝑊𝑛 in 𝑈𝑛,𝑗 and the constant coefficient of
𝑉𝑛,𝑗 are both units,
Proposition 5.3 makes this
row gcd coprime to 6. These
endpoint assumptions are extra conditions, not consequences of
coefficient primitivity. Dividing by such a gcd preserves divisibility
by every power of 2 and 3 for that individual row. It need not
preserve a relation with a fixed coefficient vector when different rows
are divided by different contents. For example, at 𝑊 =1 the pairs (𝑋 −1,𝑋 −1) and (𝑋 +1,𝑋 +1) give rows (1,1) and (5,5). Their sum is zero modulo 6, whereas the sum of their primitive
normalisations is (2,2), not zero
modulo 6. Both pairs satisfy the
two unit conditions just stated. Each division is invertible modulo
6, but different rows are
multiplied by different units, so their sum need not stay zero. The
residue map must therefore be formed again after row-by-row
normalisation.
Dividing a specialised row by its content need not preserve the
chosen polynomial family, and lifting the divided row back is a
constrained problem. For fixed 𝑊,
the map 𝑃 ↦𝐻𝑊(𝑃) on integer
polynomials of degree at most 𝑊 is
surjective onto ℤ, since 3𝑊 and 2𝑊 are coprime, so a lift always
exists. The issue is not an arbitrary exponential height bound, as the
construction above shows. It is whether the lift belongs to the chosen
approximation family and satisfies that family’s remainder identity and
quantitative height estimate. With 𝑊 =1, for instance, (𝑋 +1,𝑋 +1) specialises to (5,5), whose primitive normalisation
(1,1) lifts to (𝑋 −1,𝑋 −1), but not to an integer scalar
multiple of the original pair. Any lift used below is therefore supplied
together with its degree bound, its height bound and its exact
remainder.
For target depths 𝑅𝑛,𝑆𝑛, let
𝐽𝑛(𝜆) be the vector of four
residues of the pair ∑𝑗𝜆𝑗(𝑈𝑛,𝑗,𝑉𝑛,𝑗), and
define
C𝑛={𝜆∈{−1,0,1}𝑀𝑛\{0}:𝐽𝑛(𝜆)=0},
𝐾poly𝑛={𝜆∈{−1,0,1}𝑀𝑛:∑𝑗𝜆𝑗𝑈𝑛,𝑗=0, ∑𝑗𝜆𝑗𝑉𝑛,𝑗=0},𝐾rem𝑛={𝜆∈{−1,0,1}𝑀𝑛:∑𝑗𝜆𝑗R𝑛,𝑗(3/2)=0}.
The second set consists of signed relations whose
remainder vanishes at 3/2. It also
contains every relation with an identically zero remainder function.
These are sets of restricted coefficient vectors, not assertions that
the signed cube is a vector space.
The exact pigeonhole condition is
2𝑀𝑛>32𝑅𝑛22𝑆𝑛,equivalently𝑀𝑛>2𝑅𝑛log23+2𝑆𝑛.(26)
Thus the least integer number of rows satisfying
this counting test is
⌊2𝑅log23+2𝑆⌋+1.
The checked condition 𝑀 ≥4𝑅 +2𝑆 for 𝑅 >0 is a convenient sufficient
corollary, not the exact threshold. Applying Cauchy–Schwarz to the sizes
of the residue classes shows that there are at least
12(22𝑀𝑛32𝑅𝑛22𝑆𝑛−2𝑀𝑛)(27)
unordered pairs of distinct subsets with equal
residues. It would therefore suffice to prove that fewer than this many
pairs give a zero polynomial combination or a zero remainder at 3/2.
Theorem 5.8 supplies
only C𝑛 ≠∅; it
does not rule out zero polynomial pairs or zero real remainders. For a
useful approximation family, bounding the multiplicities in (27)
remains a possible way to obtain nonvanishing. Without restrictions on
the family, however, nonvanishing alone is elementary.
Example 10.2 (nonvanishing without decay). For
𝑛 ≥1, set 𝑊𝑛 =𝑅𝑛 =𝑆𝑛 =𝑛2 and 𝑀𝑛 =6𝑛2. Take
(𝑈𝑛,0,𝑉𝑛,0)=((1+2𝑊𝑛)𝑋𝑊𝑛,1),(𝑈𝑛,𝑗,𝑉𝑛,𝑗)=(𝑋𝑊𝑛,1)(1≤𝑗<𝑀𝑛),
and define R𝑛,𝑗(𝑡) =𝑈𝑛,𝑗(𝑡)𝐹(𝑡) −𝑉𝑛,𝑗(𝑡) for 𝑡 >1. All pairs have coefficient gcd
1 and primitive evaluated rows. The
coefficient vector (1, −1,0,…,0) belongs to C𝑛\(𝐾poly𝑛 ∪𝐾rem𝑛), but the divided
integer form equals 𝐹(3/2) for
every 𝑛.
Indeed, the evaluated rows are (3𝑊𝑛 +6𝑊𝑛,2𝑊𝑛) and (3𝑊𝑛,2𝑊𝑛); their first
coordinates are odd, so both rows are primitive. Their difference is
(6𝑊𝑛,0), while the polynomial
difference is (2𝑊𝑛𝑋𝑊𝑛,0).
Thus all four residues vanish. The unscaled remainder difference is
3𝑊𝑛𝐹(3/2) >0. Clearing the
evaluation denominators multiplies it by 2𝑊𝑛, giving 6𝑊𝑛𝐹(3/2). Dividing this cleared
integer form by 3𝑅𝑛2𝑆𝑛 =6𝑊𝑛 leaves the same
positive constant 𝐹(3/2). The
counting condition (26)
holds because log23 <2.
Example 10.2 meets the two
nonvanishing requirements in Problem 10.1 without any
irrationality assumption. What it fails is the smallness condition. The
useful question is therefore to obtain nonvanishing and decay in the
same prescribed approximation family, not merely to exhibit some family
with a nonzero congruence relation.
The range of subset sums.
The residue condition and the real-error condition can be counted
together. Within each residue class, subdivide the range of subset
remainders into intervals of width 𝐷/𝑛; a bound on repeated remainder values
then forces a nonzero small difference. Fix a positive integer 𝑛. For 𝑀 integer rows (𝐴𝑗,𝐵𝑗) and a modulus 𝐷 ≥1, set 𝑒𝑗 =𝐴𝑗𝐹(3/2) −𝐵𝑗. For each attained
residue vector 𝑏, let 𝑇𝑏 be the difference between the largest
and smallest remainders ∑𝑗𝜀𝑗𝑒𝑗 with 𝜀𝑗 ∈{0,1} and ∑𝑗𝜀𝑗(𝐴𝑗,𝐵𝑗) ≡𝑏(mod𝐷). Let the integer 𝑘𝑏
bound the number of subsets attaining any one remainder value in that
residue class. Then
2𝑀>∑𝑏𝑘𝑏(⌊𝑛𝑇𝑏𝐷⌋+1)
produces two subsets with equal residues and distinct remainders less
than 𝐷/𝑛 apart. Within each residue
fibre, subtract the least remainder, multiply by 𝑛/𝐷, and take floors. These integer
indices range from 0 to ⌊𝑛𝑇𝑏/𝐷⌋, including a
separate final index when 𝑇𝑏 is a
positive integral multiple of 𝐷/𝑛.
Equal indices give a remainder difference strictly less than 𝐷/𝑛. If each index corresponded to only
one remainder value, it would account for at most 𝑘𝑏 subsets, contradicting the displayed
inequality. Subtracting the two subset sums and dividing their
coefficients by 𝐷 gives an integer
form with nonzero absolute value less than 1/𝑛. The common width bound 𝑇 =∑𝑗|𝑒𝑗| and a common multiplicity
bound 𝑘 give the coarser count
𝑄𝑘(⌊𝑛𝑇/𝐷⌋ +1), where
𝑄 is the number of attained residue
vectors. All rows must have the same normalisation. Primitive rows can
still have repeated subset sums, and positivity need not survive
subtraction.
The lattice after evaluation.
For example, (1,0),(1,6)
generate ℤ ⊕6ℤ. They give two
residues modulo 2. Within that
lattice, the vectors whose two coordinates are even form 2ℤ ⊕6ℤ; dividing them by 2 gives ℤ ⊕3ℤ, of index 3. These are two different counts: the
number of attainable residues before division, and the index of the
lattice left after division. Smith normal form computes both for any
rank-two lattice. The first count describes congruences available before
division; the second describes the integrality restriction that survives
it. Neither count estimates the real remainders of the rows.
Let primitive integer rows 𝑢𝑗 ∈ℤ2 span a rank-two lattice 𝐿, and let 𝑔 be the gcd of their 2 ×2 minors. Since at least one row
is primitive, the Smith invariants are 1,𝑔 [34]. Hence, for 𝐷 ≥1,
|im(𝐿⟶(ℤ/𝐷ℤ)2)|=𝐷2gcd(𝑔,𝐷),[ℤ2:(𝐿∩𝐷ℤ2)/𝐷]=𝑔gcd(𝑔,𝐷).
Indeed an integral
unimodular change of coordinates takes 𝐿 to ℤ ×𝑔ℤ; reduction modulo 𝐷
and intersection with 𝐷ℤ2 give
the two formulas. This is Smith normal form over ℤ, not over ℤ[𝑝]. It measures the actual image,
rather than the ambient residue space. If two independent divided rows
have coordinate height at most 𝐻
and remainders of absolute value at most 𝜀, their nonzero integer
determinant gives the necessary inequality 2𝐻𝜀 ≥𝑔/gcd(𝑔,𝐷). That is not
a necessary condition for producing a single nonzero form. If the
specialised rows are not primitive, let 𝑑1 ∣𝑑2 be the positive Smith
invariants instead. For 𝐷 ≥1 the
corresponding formulas are
|im(𝐿mod𝐷)|=𝐷2gcd(𝑑1,𝐷)gcd(𝑑2,𝐷),[ℤ2:(𝐿∩𝐷ℤ2)/𝐷]=𝑑1𝑑2gcd(𝑑1,𝐷)gcd(𝑑2,𝐷).
They follow by applying the one-dimensional
calculation to each summand 𝑑𝑖ℤ.
Polynomial coefficient content alone does not determine either integer
Smith invariant after specialisation.
The lattice spanned by the actual tails.
The formulas above apply to any rank-two lattice. For the rows that
the approximation problem actually supplies, the invariant can be
computed outright, and it is the smallest one compatible with the base.
Let 𝑎 >𝑏 ≥1 be coprime, write
the partial sum 𝑆𝑚(𝑏/𝑎) =∑𝑟≤𝑚(𝑏/𝑎)𝑟/(1 −(𝑏/𝑎)𝑟) in lowest terms as 𝑃𝑚/𝑄𝑚 with 𝑄𝑚 >0, and set 𝑃0 =0, 𝑄0 =1. The primitive integer row of the
𝑚th tail is (𝑄𝑚,𝑃𝑚), which represents 𝑄𝑚𝐹(𝑎/𝑏) −𝑃𝑚.
Proposition 10.3 (the prefix lattice of the tails).
Every 𝑄𝑚 is coprime to 𝑎𝑏, and 𝑏 divides every 𝑃𝑚. For every prefix containing 𝑚 =0 and 𝑚 =1,
spanℤ{(𝑄𝑚,𝑃𝑚):0≤𝑚<𝑀}=ℤ×𝑏ℤ(𝑀≥2),
so the Smith invariants are 1,𝑏, the gcd of the 2 ×2 minors is 𝑏, and the image modulo 𝐷 has cardinality 𝐷2/gcd(𝑏,𝐷). Multiplying an individual
tail by a nonzero rational weight leaves its primitive row unchanged up
to sign.
Proof. A common denominator of 𝑆𝑚(𝑏/𝑎) is a product of the integers
𝑎𝑟 −𝑏𝑟 for 𝑟 ≤𝑚, each coprime to 𝑎𝑏; over that denominator every summand
has numerator divisible by 𝑏𝑟.
Reduction to lowest terms removes no prime factor of 𝑏, which gives the first two assertions.
The rows at 𝑚 =0,1 are (1,0) and (𝑎 −𝑏,𝑏), and subtracting 𝑎 −𝑏 copies of the first from the second
gives (0,𝑏); every later row
already lies in ℤ ×𝑏ℤ by the
first assertions. The Smith and image statements are the specialisation
of the formulas above at 𝑔 =𝑏.
Finally the rational line through a primitive pair meets ℤ2 in exactly the multiples of that
pair, so clearing denominators in a nonzero rational multiple and
dividing by the coordinate gcd returns the same pair up to sign. ◻
At 3/2 the first three partial
sums are 0, 2 and 14/5, with rows (1,0), (1,2) and (5,14). Their span is already ℤ ×2ℤ. There is no three-adic
collapse, and the only local saving is the single factor of two that the
image formula displays. For a consecutive window containing 𝑚 =𝑠 and 𝑚 =𝑠 +1 and no earlier row, every pairwise
minor is divisible by 𝑏𝑠+1. The
gcd has valuation (𝑠 +1)𝑣𝑝(𝑏) at
each prime 𝑝 ∣𝑏 and valuation
zero at each prime 𝑝 ∣𝑎. The
adjacent-row identity
𝑄𝑠𝑃𝑠+1−𝑃𝑠𝑄𝑠+1=𝑄𝑠𝑄𝑠+1𝑏𝑠+1𝑎𝑠+1−𝑏𝑠+1
attains both, since
its denominator is a unit at every prime dividing 𝑎𝑏.
Rescaling an individual tail and then making its row primitive
returns the same row up to sign. Thus it preserves the lattice spanned
by the full family. Integer combinations remain in that lattice, but a
selected family of combinations need not span all of it and can have a
larger minor gcd. At 3/2, write
𝑢0 =(1,0) and 𝑢1 =(1,2). The primitive rows 𝑢0 and 3𝑢1 −2𝑢0 =(1,6) span ℤ ×6ℤ, with minor gcd 6, although 𝑢0,𝑢1 span ℤ ×2ℤ. The selection replaces the
original lattice by an index-three sublattice, accounting for the change
from 2 to 6. Containment therefore preserves
divisibility by the original gcd, not equality of gcds or endpoint
valuations. The prefix and window equalities above concern the full
indicated families.
Rational combinations can also leave the original lattice: the
half-sum of 𝑢0,𝑢1 is the
primitive row (1,1), whose minor
against 𝑢0 is 1. Coefficient denominators must then be
accounted for; likewise, primitive normalisation after taking
combinations requires a new lattice calculation. These operations may
change the minor gcd in either direction. None by itself controls the
real error: a useful selected family must still have nonzero remainders
small enough after the proposed division.
Estimating the divided remainder
Once a construction is fixed, let 𝐻𝑛 ≥1 be its height, 𝐿𝑛 ≠0 its undivided remainder, and
𝐷𝑛 =3𝑅𝑛2𝑆𝑛 its proved
divisor, counted once. We ask for the additional height and remainder
estimate below. With a different divisor, the two logarithmic terms
should be replaced by log𝐷𝑛. The
estimate must use the height of the objects that enter the comparison
with a nonzero integer; scalar and exterior-determinant heights cannot
be interchanged. For scalar forms, integral coefficients and 0 <|𝐿𝑛|/𝐷𝑛 →0 already suffice for
irrationality, without a height factor. The proposed estimate implies
that decay because 𝐻𝑛 ≥1,
although it is not necessary for the scalar criterion. Allowing
arbitrarily small positive heights would lose this implication.
Problem 10.4 (an additional height and remainder
estimate). Prove the explicit estimate
lim sup𝑛→∞log𝐻𝑛+log|𝐿𝑛|−𝑅𝑛log3−𝑆𝑛log2𝑛2<0.(28)
Every denominator, row content and
final-combination content must already be included in 𝐻𝑛 and 𝐿𝑛.
Nonvanishing alone does not address (28).
Conversely, a formal decay estimate cannot supply a nonzero form if
every combination with the required residues has zero remainder. A
proposed divisor saving must be compared with the height and remainder
of the same explicitly normalised objects.
A restriction on Mahler functional equations
For the divisor generating series L(𝑧) =∑𝑛≥1𝜏(𝑛)𝑧𝑛, the
classification of Bell and Smertnig excludes a 𝑘-Mahler equation for every 𝑘 ≥2 [27]. We first explain its application
to 𝜏. We then prove the weaker
simultaneous 2/3 statement by combining the
Adamczewski–Bell theorem with the functional nonrationality from
Section 2.1. The
cited 2026 works have the status of the identified preprints. These
functional statements leave the arithmetic nature of an individual
rational-base value undecided.
To apply the classification, note that 𝜏 is multiplicative: for coprime
integers 𝑚,𝑛, each divisor of 𝑚𝑛 has a unique factorisation into a
divisor of 𝑚 and a divisor of 𝑛. Suppose that L were 𝑘-Mahler. The classification would give a
prime 𝑝, an integer 𝑟 ≥0 and an eventually periodic function
𝜒 with 𝜏(𝑚) =𝑚𝑟𝜒(𝑚) whenever 𝑝 ∤𝑚. For a prime ℓ ≠𝑝, this forces
𝜒(ℓ𝑗)=𝑗+1ℓ𝑗𝑟(𝑗≥0).
If 𝑟 =0, these values are unbounded.
If 𝑟 >0, they are nonzero and
tend to zero. Both alternatives contradict the finite range of an
eventually periodic function.
Here the ambient space is ℚ((𝑧)), the field of formal Laurent
series, viewed as a vector space over ℚ(𝑧). Stability means that substituting
𝑧𝑘 for 𝑧 sends each member of the subspace back
into that subspace; this substitution is not a ℚ(𝑧)-linear map.
Proposition 10.5 (no finite simultaneous 2/3-system). Let
L(𝑧)=∑𝑛≥1𝑧𝑛1−𝑧𝑛.
There is no
finite-dimensional ℚ(𝑧)-vector
space that contains L and
is stable under both 𝑧 ↦𝑧2
and 𝑧 ↦𝑧3.
Proof. Suppose 𝑉 were
such a space, of dimension 𝑑.
Stability under 𝑧 ↦𝑧2 places
the 𝑑 +1 elements L(𝑧),L(𝑧2),…,L(𝑧2𝑑) in 𝑉, so they
are linearly dependent over ℚ(𝑧);
clearing denominators gives polynomials 𝑃0,…,𝑃𝑑, not all zero, with ∑𝑑𝑖=0𝑃𝑖(𝑧)L(𝑧2𝑖) =0.
Linear dependence need not give a nonzero coefficient of the
unshifted function, as a Mahler equation requires. One cannot simply
replace 𝑧 by 𝑧1/2𝑗, since the polynomial
coefficients need not have exponents divisible by 2𝑗. Instead, separate their exponent
classes. Let 𝑗 be the least index
with 𝑃𝑗 ≠0. Write each polynomial
uniquely as 𝑃𝑖(𝑧) =∑2𝑗−1𝑟=0𝑧𝑟𝑄𝑖,𝑟(𝑧2𝑗).
Every series L(𝑧2𝑖)
with 𝑖 ≥𝑗 has exponents divisible
by 2𝑗, so the relation splits by
exponent residues modulo 2𝑗.
Choose 𝑟 with 𝑄𝑗,𝑟 ≠0 and put 𝑢 =𝑧2𝑗. The corresponding relation is
𝑑∑𝑖=𝑗𝑄𝑖,𝑟(𝑢)L(𝑢2𝑖−𝑗)=0,
with a nonzero coefficient of L(𝑢). Thus L is 2-Mahler. The same argument with 3 in place of 2 makes it 3-Mahler. Since 2 and 3 are multiplicatively independent, a
theorem of Adamczewski and Bell [16] then forces L to be a rational function.
Since L(𝑧) =𝐹(1/𝑧) for
0 <𝑧 <1, this contradicts the
nonrationality of 𝐹 proved in
Section 2.1. Rivin’s
periodic-coefficient corollary [24] gives the same nonrationality
conclusion. ◻
Proposition 10.5 uses no
property of the point 2/3: the
obstruction is functional and appears before regularity at a particular
point is considered. For this scalar function, Bell and Smertnig’s
single-base classification already implies the proposition. The proof
above instead derives it from simultaneous closure and elementary
functional nonrationality, using the Adamczewski–Bell theorem. A
construction using additional functions or functional relations must
specify those functions and its closure conditions; the single-base
statement is not an obstruction to every approximation method. The
classification and the Adamczewski–Bell theorem are cited, not proved
here; the needed nonrationality has the elementary proof given
earlier.
The Lean proof of Proposition 10.5 (no
finite simultaneous 2/3-system)
uses neither cited theorem, and it uses only stability under 𝑧 ↦𝑧2. As in the first step of the
proof above, that stability gives polynomials 𝑃0,…,𝑃𝑑, not all zero, with ∑𝑑𝑖=0𝑃𝑖(𝑧)L(𝑧2𝑖) =0, and this relation also holds between the values
of these functions on the open unit disc. If 𝜁 is a primitive 𝑛th root of unity, then (1 −𝑟)L(𝑟𝜁)/log(1/(1 −𝑟)) →1/𝑛 as 𝑟 ↑1. These limits, taken at roots
of unity of suitable orders, force every 𝑃𝑖 to vanish. The same argument
excludes, for every 𝑘 ≥2, a
finite-dimensional space containing L and stable under 𝑧 ↦𝑧𝑘 alone (single-base
statement).
A limitation of the rectangular exponent model
We conclude the comparison of exponent models by bounding ΘHP, defined in
Section 3.
For 𝜌 ≥0 and 𝜎 ≥1 +𝜌 its denominator
(1+𝜌)22+𝜎(1+𝜌)+1+𝜌22+𝜎
is positive. Put 𝑢 =𝜎 −1 −𝜌 ≥0. Multiplying the
difference ΘHP(𝜌,𝜎) −(1/2 −1/𝜋2)
by 2𝜋2 times this denominator
gives exactly
−𝜋2𝜌2−𝜋2𝜌𝑢−2𝜋2𝜌−2𝜌2−10𝜌𝑢−4𝜌−6𝑢2−8𝑢.
Every term is nonpositive. The original
difference has the same sign, and it vanishes exactly when 𝜌 =0 and 𝜎 =1 (exact
expansion, nonpositivity,
equality
case). Equivalently, within that model the displayed threshold never
exceeds the classical one-function margin, with equality only at the
classical endpoint (bound,
equality).
This bounds only the displayed exponent model. Applying it to an
approximation family would require the polynomial construction,
integrality and asymptotic estimates connecting that family to ΘHP. The rational cutoff
81/200 discussed above satisfies
81200<log2log3.
For a sufficient criterion of the form log𝑏/log𝑎 <𝑇, including 3/2 requires 𝑇 >log2/log3, not merely an
improvement on 81/200. This
numerical target applies to that form of criterion, not to every
irrationality argument.
A concrete optimisation question is available within the 2004
construction itself. Write a source parameter direction as 𝛼 =(𝛼0,𝛼1,𝛼2;𝛽),
with positive integer entries satisfying
𝛼1≤𝛼2,𝛼1+𝛼2<𝛽≤𝛼0+𝛼2,gcd(𝛼0,𝛼1,𝛼2,𝛽)=1.
The source parameters
are 𝑎𝑗 =𝛼𝑗𝑛 +1 and 𝑏 =𝛽𝑛 +2; here 𝑏 is not a rational-base denominator. The
gcd condition is a normalisation of the parameter direction, not a
primitivity assertion about evaluated rows. Its invariance under
dilation is checked below. For these directions set
𝑐00=𝛼0+𝛼1+𝛼2−𝛽,𝑐01=𝛼0,𝑐11=𝛼1,𝑐21=𝛼2,𝑐12=𝛽−𝛼1,𝑐22=𝛽−𝛼2,𝑚=max(𝑐00,𝑐01,𝑐11,𝑐21,𝑐12,𝑐22),
and define the periodic step function
𝜔𝛼(𝑢)=max{0,⌊𝑐21𝑢⌋+⌊𝑐22𝑢⌋−⌊𝑐11𝑢⌋−⌊𝑐12𝑢⌋,⌊𝑐01𝑢⌋+⌊𝑐21𝑢⌋−⌊𝑐00𝑢⌋−⌊𝑐12𝑢⌋}.
Zudilin’s constants in (25) and (26),
already used in the finite direction scan, are
𝐶1(𝛼)=(𝛼0+𝛼1+𝛼2)𝛽−𝛼21+𝛼22+𝛽22,𝐶0(𝛼)=𝛼212+𝛼0𝛼1+(𝛽−𝛼2)(𝛼2−𝛼1)−3𝜋2(𝑚2−∫10𝜔𝛼(𝑢)𝑑(−𝜓1(𝑢))).
Here 𝜓1
is the trigamma function used earlier. The step function is bounded,
nonnegative, periodic with period 1, and zero near zero, so the integral is
finite.
The gcd normalisation does not change the ratio being optimised.
Indeed, periodicity and −𝜓′1(𝑢) =2∑𝑗≥0(𝑢 +𝑗)−3
give, by Tonelli’s theorem,
∫10𝜔𝛼(𝑢)𝑑(−𝜓1(𝑢))=∫∞02𝜔𝛼(𝑢)𝑢3𝑑𝑢.
For any
positive integer 𝑘, the floor
formulas give 𝜔𝑘𝛼(𝑢) =𝜔𝛼(𝑘𝑢).
Substitution in the last integral therefore multiplies it by 𝑘2. All other terms in 𝐶0 and 𝐶1 are quadratic in the direction,
including 𝑚2. Hence 𝐶𝑖(𝑘𝛼) =𝑘2𝐶𝑖(𝛼) for 𝑖 =0,1, so passing to a primitive
direction preserves both positivity and 𝐶0/𝐶1. Let A be exactly the displayed
primitive directions with 𝐶0(𝛼) >0 and 𝐶1(𝛼) >0.
Problem 10.6 (optimising the published parameter
directions). Determine
sup𝛼∈A𝐶0(𝛼)𝐶1(𝛼),
or improve its bounds. In
particular, does an admissible direction give a ratio strictly greater
than the value 𝜃∗ in
Theorem 2.2,
attained at (14,12,14;27)? A finite
numerical scan does not establish optimality over A.
The immediate bounds are 𝜃∗ ≤supA𝐶0/𝐶1 ≤1/2. Indeed, at any integer base 𝑝 ≥2 the source gives 𝜇irr(𝐹(𝑝)) ≤𝐶1(𝛼)/𝐶0(𝛼), whereas pigeonhole approximation gives
𝜇irr(𝐹(𝑝)) ≥2. Thus even
the optimal reciprocal criterion in this class cannot exceed 1/2, which is below log2/log3. Optimising these directions
cannot include 3/2 by that
criterion. For other noninteger bases, a new direction would still
require the polynomial degree and coefficient-height estimates used in
the rational-base transfer; the integer-base source alone does not
supply that application. The unrestricted question of which rational
bases give irrational values is not settled here and is not reduced to
any one of these problems.