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Erdős 699: further effective prime-pair estimates


This is a retained earlier research note. The current reading guide gives the latest status and distinguishes completed proofs from remaining cases.

P699 research · Small-index bounds · The first effective index-24 bound

The general Padé theorem of Bennett, Filaseta, and Trifonov (BFT) gives additional useful prime-pair estimates. The twelve choices below are certified by directed interval arithmetic. They include improvements to the published weights for (2,11)(2,11) and (3,5)(3,5).

The source is the BFT paper, Theorem 2.2. No assertion of optimality is made for these parameters.

The additional estimates

For each pair in the table, and every fixed positive integer DD, there is an effectively computable threshold such that

∣pau−qbv∣≤D⟹max⁡(u,v)>min⁡(pau,qbv)λ.(1)|p^a u-q^b v|\le D \quad\Longrightarrow\quad \max(u,v)>\min(p^a u,q^b v)^{\lambda}. \tag{1}

Both quantities in the minimum must exceed the threshold. The cofactors are positive integers and a,ba,b are nonnegative integers.

In the seed column, PP and QQ are powers of the two indicated primes, in whichever order makes a0P−b0Qa_0P-b_0Q positive.

PairCertified λ\lambdaSeed a0P−b0Qa_0P-b_0Qs=c/ds=c/d
2,112,11.1399.139921⋅215−47⋅114=121\cdot2^{15}-47\cdot11^4=113/613/6
3,53,5.2543.25437⋅54−2⋅37=17\cdot5^4-2\cdot3^7=113/813/8
2,172,17.3560.356017−24=117-2^4=134/2534/25
3,173,17.1190.11902⋅32−17=12\cdot3^2-17=131/1831/18
5,175,17.0093.00933⋅17−2⋅52=13\cdot17-2\cdot5^2=157/2657/26
3,193,19.1268.126836−2⋅192=73^6-2\cdot19^2=735/2735/27
7,197,19.1588.158820⋅73−193=120\cdot7^3-19^3=167/4067/40
11,1911,19.2077.20773⋅112−192=23\cdot11^2-19^2=253/3753/37
17,1917,19.2176.21765⋅172−4⋅192=15\cdot17^2-4\cdot19^2=132/1732/17
2,232,23.0245.0245232−29=1723^2-2^9=1745/3845/38
5,235,23.2144.214452−23=25^2-23=241/3141/31
11,2311,23.1478.147823−2⋅11=123-2\cdot11=15/35/3

For (17,19)(17,19) take ϵ=10−6\epsilon=10^{-6} in BFT Theorem 2.2; for every other row take ϵ=10−5\epsilon=10^{-5}. The parameter certificate checks Ω1>1\Omega_1>1, Ω2>1\Omega_2>1, and λ1>λ+ϵ\lambda_1>\lambda+\epsilon for every row. Its lower bounds for the digamma differences use the positive series and integral tails proved in the earlier index-24 note, rather than unbounded floating-point evaluations. Thus (1) follows directly from BFT Theorem 2.2.

For example, the two improved old pairs have certified intervals

{p,q}log⁡Ω1log⁡Ω2λ1{2,11}(.00658244,.00658249)(3.66503731,3.66503736)(.139927933,.139927936){3,5}(.04739944,.04739948)(4.26327874,4.26327879)(.254372338,.254372341).\begin{array}{c|c|c|c} \{p,q\}&\log\Omega_1&\log\Omega_2&\lambda_1\\\hline \{2,11\}&(.00658244,.00658249)&(3.66503731,3.66503736)&(.139927933,.139927936)\\ \{3,5\}&(.04739944,.04739948)&(4.26327874,4.26327879)&(.254372338,.254372341). \end{array}

Their weights in the prime-pair table are .0698.0698 and .2238.2238, respectively.

Combining all available pairs

Choose the maximal positions rpr_p and cofactors upu_p as in the small-index note, and set

zp=log⁡uplog⁡(n−i+1).z_p=\frac{\log u_p}{\log(n-i+1)}.

Once the source thresholds hold, every pair gives max⁡(zp,zq)≥λpq\max(z_p,z_q)\ge\lambda_{pq}. Combining the new table with BFT Corollary 2.3 gives the exact minimum sums below:

Available primesMinimum sum of the zpz_p
2,3,5,7,11,132,3,5,7,11,131.01201.0120
The preceding primes and 17171.09231.0923
The preceding primes and 19191.30991.3099
The preceding primes and 23231.45771.4577

The recorded certificate contains all componentwise minimal vectors, not just their minimum sums. They can therefore also be used in estimates that keep the individual cofactor exponents.

The finite verification is elementary. Start with the zero vector. For each edge of weight ww, leave a vector unchanged if an endpoint is already at least ww; otherwise make the two possible extensions by raising one endpoint to ww. Remove any vector componentwise larger than another retained vector. Every feasible real vector dominates a retained vector at every stage, by induction on the edges. Thus the minimum sum in the final list is the exact minimum for the original maximum inequalities. This verifies a finite system of inequalities; it does not search through binomial rows.

Algebraic bounds after the source thresholds

If γ\gamma is the relevant minimum, the earlier argument gives

Ui(n)≤2γ[i]Sinsi−γ(n≥2(i−1)).U_i(n)\le\frac{2^\gamma}{[i]_{S_i}}n^{s_i-\gamma} \quad(n\ge2(i-1)).

Together with the retained fat-point lower bound, this implies

nηi<2γii[i]Si,ηi=i−ρi−si+γ.n^{\eta_i}<\frac{2^\gamma i^i}{[i]_{S_i}},\qquad \eta_i=i-\rho_i-s_i+\gamma.

The certificate checks the following powers of ten by clearing the rational exponent denominators and comparing integer powers:

iiγ\gammaηi\eta_iBound once all source thresholds hold
19191.09231.0923.0923.0923n<10267n<10^{267}
22221.30991.3099.3099.3099n<1093n<10^{93}
24241.45771.4577.1377.1377n<10234n<10^{234}
25251.45771.4577.4577.4577n<1075n<10^{75}

These improve the algebraic part of the stopping argument. They are not complete numerical last-row bounds: the additional BFT thresholds must also be included, and stronger exponents can require larger thresholds.

An evaluator for the fully explicit theorem

The separate explicit-threshold evaluator implements BFT Theorem 2.4. It accepts a certified value of log⁡L1\log L_1 and a threshold m0m_0 proving BFT (2.8), together with the seed, c,d,D,ϵc,d,D,\epsilon.

Both integrals defining C1,δC_{1,\delta} and C2,δC_{2,\delta} are polynomial integrals with rational coefficients. The evaluator computes them exactly using

∫01ta(1−t)b(1−zt)k dt=∑r=0k(kr)(−z)r(a+r)!b!(a+b+r+1)!.\int_0^1 t^a(1-t)^b(1-zt)^k\,dt =\sum_{r=0}^k\binom kr(-z)^r \frac{(a+r)!b!}{(a+b+r+1)!}.

It then encloses κ1,κ2,M,log⁡x0\kappa_1,\kappa_2,M,\log x_0 by directed interval arithmetic and certifies an integer KK for which x0<10Kx_0<10^K. The value of log⁡L1\log L_1 and its m0m_0 remain explicit inputs; the evaluator does not assume an effective asymptotic estimate is already a numerical bound.

Fully numerical bounds at 22, 24, and 25

Using the published entries of BFT Proposition 5.1, the evaluator certifies these deliberately less sharp exponents with useful numerical thresholds. Here D=100D=100 throughout.

PairSeedc/dc/dL1L_1m0m_0ϵ\epsilonCertified weightRow threshold
2,172,1717−16=117-16=17/57/51.41351.41357474.012.012.3259.32591097610^{976}
17,1917,195⋅289−4⋅361=15\cdot289-4\cdot361=1221.93771.9377150150.007.007.1855.18551095710^{957}
11,2311,2323−2⋅11=123-2\cdot11=17/47/41.62191.62196060.011.011.1068.10681094010^{940}

The recorded intervals give respectively

log⁡x0<2246.800,log⁡x0<2202.645,log⁡x0<2163.632.\begin{aligned} \log x_0&<2246.800,\\ \log x_0&<2202.645,\\ \log x_0&<2163.632. \end{aligned}

Each row threshold already absorbs all maximal-position shifts through 3333: the checker verifies x0<10K−33x_0<10^K-33 for the displayed exponent KK. Thus the estimates hold at every binomial row n≥10Kn\ge10^K for the indices at most 3434 considered here.

For i=22,25i=22,25, the pair (17,19)(17,19) is disjoint from the six primes in the original explicit table. Its saving .1855.1855 therefore adds directly to the published-table saving .913.913, giving

γ=1.0985,η22=η25=.0985.\gamma=1.0985,\qquad\eta_{22}=\eta_{25}=.0985.

Exact integer comparisons in the pair checker give algebraic caps 1029010^{290} and 1034410^{344}, respectively. The source threshold dominates both. Hence

n<10957for every bad triple with i=22 or 25.\boxed{n<10^{957}\quad\text{for every bad triple with }i=22\text{ or }25.}

For i=24i=24, retain the individual cofactor exponents in the weighted-ramp argument. The original explicit BFT table together with the three weights above gives gain 983/1250=.7864983/1250=.7864 at k=16k=16, including every possible collision of maximal positions. The exact weighted certificate gives the algebraic cap 1063510^{635} and elementary threshold 11 132 00011\,132\,000. Again the source threshold dominates, proving

n<10976for every bad triple with i=24.\boxed{n<10^{976}\quad\text{for every bad triple with }i=24.}

These three are complete numerical row bounds. The intervals below them have not been excluded by these arguments.

Retaining different exponents at the two endpoints

The asymmetric cofactor lemma improves the estimates further. For an oriented seed with prime powers P,QP,Q, put

K=log⁡max⁡(P,Q)+log⁡Ω4s.K=\log\max(P,Q)+\frac{\log\Omega_4}{s}.

Any strict endpoint targets

tP<1−log⁡PK,tQ<1−log⁡QKt_P<1-\frac{\log P}{K},\qquad t_Q<1-\frac{\log Q}{K}

give the disjunction u>xtPu>x^{t_P} or v>xtQv>x^{t_Q} for sufficiently large bounded-gap inputs, where xx is the smaller input. The two targets need not be equal. The cited lemma supplies an explicit threshold when L1,m0L_1,m_0 are explicit, and an effective threshold for a strict rational lower bound on log⁡L(s)\log L(s).

The larger table checker verifies 23 numerical and 24 effective parameter choices. It checks every seed's prime-power labels, the published L1,m0L_1,m_0 entries, and strict interval margins for both endpoint targets. For the effective entries it also verifies the rational inequality log⁡L1<log⁡L(c/d)\log L_1<\log L(c/d) by the finite series bounds above. These disjunctions supplement the old symmetric table; replacing a symmetric constraint by an asymmetric one can lose an independently useful restriction.

Two of the numerical entries are

u5>x.3613oru7>x.2277,u7>x.0987oru13>x.2080.\begin{aligned} u_5>x^{.3613}&\quad\text{or}\quad u_7>x^{.2277},\\ u_7>x^{.0987}&\quad\text{or}\quad u_{13}>x^{.2080}. \end{aligned}

They use respectively the published GCD parameters (c,d,L1,m0)=(8,5,1.5407,53)(c,d,L_1,m_0)=(8,5,1.5407,53) and (7,5,1.4135,74)(7,5,1.4135,74). For input gaps at most 100100, the direct threshold checker gives x≥102 405 782x\ge10^{2\,405\,782} and x≥10484 367x\ge10^{484\,367}, respectively. Together with the earlier effective pair constraints, these are the additional inputs to the positive whole-index i=18i=18 weighted certificate: k=12k=12, degree 156156, and gain 186/625186/625 over every cofactor vector and every collision pattern. The complete index-18 certificate checks all 65 minimal vectors and 5707 collision capacity lists. Its algebraic term is 1081410^{814}, and its full bound is n<max⁡{X18,102 405 782}+17n<\max\{X_{18},10^{2\,405\,782}\}+17, where X18X_{18} is the maximum of the effective symmetric source thresholds for gap 1717.