Petty's Notebook
ArticlesPapersnfieldAbout
Get notified when new posts are published. No spam, just math.
Alexander S. Petty  |  ©2009-2026
← Back
collision

The Collision Transform and the Critical Strip

January 13, 202413 min read
Companion paper: The Collision Transform and the Critical Strip →
Blue and gold points converge toward a bright vertical line against a dark field.
Give the large primes more weight, and the zeros of the selected L-functions become possible barriers to convergence.

Take the prime 111111. Its centered collision weight in base three is 4/34/34/3. Divide by 111111 and its contribution to the prime sum is about 0.12120.12120.1212. Divide by the square root of 111111 and the contribution becomes about 0.40200.40200.4020.

The digits and the collision count stay put. Only the divisor changes.

Do this at every prime. A prime near a million receives roughly a thousand times as much weight when the divisor changes from the prime to its square root. The positive and negative terms now have more to cancel.

The Centered Collision Sum proves convergence with the divisor ppp. How much more weight can the large primes carry before the sum fails to converge?

Six numbers to start with

In base three, compare the first two digits of every fraction r/pr/pr/p. Count the matches, subtract the bin scale ⌊(p−1)/3⌋\lfloor(p-1)/3\rfloor⌊(p−1)/3⌋, then subtract the mean for the prime’s family modulo three. Beyond nine, the answer depends only on the remainder modulo nine. The whole centered table fits on one row.

Remainder modulo 9 1 2 4 5 7 8
Centered weight 2/32/32/3 4/34/34/3 2/32/32/3 −2/3-2/3−2/3 −4/3-4/3−4/3 −2/3-2/3−2/3

Eleven takes 4/34/34/3. Thirteen takes 2/32/32/3. Seventeen takes −2/3-2/3−2/3. Every larger prime consults the same six entries.

Write f(p)f(p)f(p) for that weight. The sum is

F(s)=∑p>9f(p)ps,F(s)=\sum_{p>9}\frac{f(p)}{p^s},F(s)=p>9∑​psf(p)​,

with primes added in increasing order. At s=1s=1s=1, convergence is proved. Decrease the real exponent sss and more of each large prime’s contribution remains.

The six entries sum to zero. That alone will not settle the question. The primes visit these entries in their own order, and convergence depends on the imbalance left by those visits.

The next nine million

Take every prime in 106<p≤10710^6<p\leq10^7106<p≤107. There are 586,081586{,}081586,081. Start a fresh total at zero and add their contributions one at a time.

Four running paths compare base three and base ten at exponents one and one half. The paths repeatedly rise and fall before their final endpoints. Four running paths compare base three and base ten at exponents one and one half. The paths repeatedly rise and fall before their final endpoints.
Each path adds every prime from one million through ten million, starting at zero just above one million. Teal uses the base-three table; gold uses the base-ten table. The vertical scales differ and are marked. Select the figure to inspect the fluctuations.

At s=1s=1s=1, the base-three path ends near +0.000042+0.000042+0.000042. At s=1/2s=1/2s=1/2, it ends near +0.077496+0.077496+0.077496. Base ten ends near +0.000065+0.000065+0.000065 and −0.366499-0.366499−0.366499, respectively. Each base uses its own centered table. Within a base, the same primes and the same table entries produce both paths.

The endpoint conceals a fair amount of travel. A window can finish near zero after substantial excursions on either side. Increasing the weights can also reverse the sign of its final contribution, as it does here in base ten.

These are finite sums. A small contribution from this window does not prove convergence. A larger one does not disprove it. The next window is not obliged to resemble this one.

Five bases, three exponents, every prime in the window
Fifteen full-resolution running paths compare five bases at exponents one, three quarters and one half across the same prime window. Fifteen full-resolution running paths compare five bases at exponents one, three quarters and one half across the same prime window.
Rows use bases three, five, seven, ten and twelve. Columns use exponents one, three quarters and one half. Every one of the 586,081 primes contributes to each path. The vertical scales are individual, the endpoints are labelled, and none of the panels represents an infinite sum.

The full-size plate uses bases 3,5,7,10,123,5,7,10,123,5,7,10,12 and exponents 1,3/4,1/21,3/4,1/21,3/4,1/2. Every prime contributes to every path. Each panel has its own marked vertical scale. Enlarging a nearly flat path changes its display, not the size of the underlying sum.

The decimal window can also be split by the prime’s actual remainder modulo three. At s=1s=1s=1, its 292,963292{,}963292,963 primes congruent to one contribute about +0.0002534203+0.0002534203+0.0002534203. The 293,118293{,}118293,118 congruent to two contribute about −0.0001883766-0.0001883766−0.0001883766. Together they give +0.0000650437+0.0000650437+0.0000650437. The signs oppose each other at all six exponents checked in the companion paper. This is an observation about the declared window, not a theorem about an enduring bias.

Two turns around nine

Multiply repeatedly by two modulo nine. The remainders run through

1, 2, 4, 8, 7, 5, 1.1,\ 2,\ 4,\ 8,\ 7,\ 5,\ 1.1, 2, 4, 8, 7, 5, 1.

A Dirichlet character assigns complex weights that multiply as the remainders do. Choose χ(2)=eπi/3\chi(2)=e^{\pi i/3}χ(2)=eπi/3. Each multiplication by two then turns its arrow through sixty degrees. Six turns bring it home. The conjugate character turns the other way.

Of the six characters on this cycle, only these two occur in the centered table. Reflection eliminates the even characters. Family centering eliminates the remaining odd character that depends only on the remainder modulo three. The exact expansion is

f(a)=cχ(a)+c‾ χ‾(a),f(a)=c\chi(a)+\overline c\,\overline\chi(a),f(a)=cχ(a)+cχ​(a),

where

c=1−i33.c=\frac{1-i\sqrt3}{3}.c=31−i3​​.

Six pairs of conjugate arrows rotate through the remainders one, two, four, eight, seven and five. Their imaginary parts cancel and their real parts reconstruct the centered weights. Six pairs of conjugate arrows rotate through the remainders one, two, four, eight, seven and five. Their imaginary parts cancel and their real parts reconstruct the centered weights.
Follow the six panels in reading order. Each step multiplies the remainder by two modulo nine. Teal gives c times the character; gold gives its conjugate. Their horizontal projections add to the fraction below the circle. At remainders two and seven the arrows coincide.

At remainder one, the arrows are ccc and c‾\overline cc. Their vertical parts cancel and their horizontal parts add to 2/32/32/3. At remainder two, both arrows point along the positive real axis. Their sum is 4/34/34/3. Continuing around the cycle recovers all six fractions exactly.

We can therefore split F(s)F(s)F(s) into two prime sums, one weighted by χ\chiχ, the other by χ‾\overline\chiχ​. In another base, or at another lag, a different finite table may select different characters. A character with a nonzero coefficient is called active.

The prime sum inside the logarithm

Each character has a Dirichlet LLL-function. Its Euler product has one factor for each prime. Take the logarithm and expand each factor using −log⁡(1−z)=z+z2/2+z3/3+⋯-\log(1-z)=z+z^2/2+z^3/3+\cdots−log(1−z)=z+z2/2+z3/3+⋯.

log⁡L(s,χ)=∑pχ(p)ps+∑p∑k≥2χ(p)kkpks.\begin{aligned} &\log L(s,\chi)\\ &\quad=\sum_p\frac{\chi(p)}{p^s} +\sum_p\sum_{k\ge2}\frac{\chi(p)^k}{k p^{ks}}. \end{aligned}​logL(s,χ)=p∑​psχ(p)​+p∑​k≥2∑​kpksχ(p)k​.​

The first sum is the one we need. The second brings along the squares, cubes and higher powers of each prime. Initially this identity holds for Re⁡(s)>1\operatorname{Re}(s)>1Re(s)>1, where the sums converge absolutely.

Subtract the higher powers and the finitely many small primes excluded from the collision sum. For any fixed base and lag, we obtain

F(s)=∑χcχlog⁡L(s,χ)−R(s).F(s)=\sum_\chi c_\chi\log L(s,\chi)-R(s).F(s)=χ∑​cχ​logL(s,χ)−R(s).

Here RRR collects those corrections. The digit table supplies the coefficients cχc_\chicχ​.

The higher powers start at p−2sp^{-2s}p−2s. Their absolute convergence requires 2Re⁡(s)>12\operatorname{Re}(s)>12Re(s)>1. Thus RRR is analytic throughout Re⁡(s)>1/2\operatorname{Re}(s)>1/2Re(s)>1/2, with no singularity to contribute there. Any singularity of the continued expression in this region must come from the selected logarithms.

On suitable zero-free domains, we can choose logarithms and continue the formula. That does not yet prove that adding the original prime terms converges there. Analytic continuation and ordinary convergence are different claims.

Moving the line left

Let sss be complex. Its real part gives the horizontal coordinate. The critical strip lies between real parts zero and one; the critical line passes through 1/21/21/2.

The Generalized Riemann Hypothesis places the nontrivial zeros of primitive Dirichlet LLL-functions on that line. Assume GRH for the primitive LLL-functions selected by our table. Then the ordinary collision series converges, locally uniformly, throughout

Re⁡(s)>12.\operatorname{Re}(s)>\frac12.Re(s)>21​.

This conditional theorem concerns the original prime sum, not just a continuation of its formula. It does not include the line itself.

Under the hypothesis, the accumulated character values along the primes have square-root bounds, with logarithmic factors. Partial summation combines that cancellation with the divisor psp^sps. For a real exponent s=1/2+εs=1/2+\varepsilons=1/2+ε, the resulting tail is bounded by an integral of the form

∫X∞(log⁡t)At1+ε dt,\int_X^\infty\frac{(\log t)^A}{t^{1+\varepsilon}}\,dt,∫X∞​t1+ε(logt)A​dt,

for a fixed logarithmic exponent AAA. Every positive ε\varepsilonε makes this integral finite and its tail tend to zero. At ε=0\varepsilon=0ε=0, the same bound no longer works. The companion paper gives the explicit-formula estimate and the partial-summation argument.

Two complex-plane diagrams show the conditional open half-plane to the right of one half and a hypothetical zero to the right of an assumed convergence point at zero point seven. Two complex-plane diagrams show the conditional open half-plane to the right of one half and a hypothetical zero to the right of an assumed convergence point at zero point seven.
Above, GRH for the selected primitive functions gives ordinary convergence in the shaded open half-plane. Below, convergence at zero point seven requires every weighted zero multiplicity to vanish farther right. The marked zero is hypothetical; its height is arbitrary.

For a nonzero centered table, let σc(F)\sigma_c(F)σc​(F) denote the boundary of ordinary convergence. The conjecture is

σc(F)=12.\boxed{\sigma_c(F)=\frac12.}σc​(F)=21​.​

There are two inequalities to prove. GRH for the selected functions gives σc(F)≤1/2\sigma_c(F)\leq1/2σc​(F)≤1/2. Showing that the boundary cannot lie farther left is a separate problem. Even equality would leave the behavior on the boundary line undecided. Neither the finite paths above nor the conditional convergence theorem supplies that missing lower bound.

A zero that cannot hide

Now suppose we could prove ordinary convergence at s=0.7s=0.7s=0.7. General Dirichlet-series theory would make the sum analytic everywhere to the right of that line.

Put a hypothetical zero of an active LLL-function at ρ=0.8+iγ\rho=0.8+i\gammaρ=0.8+iγ. Its logarithm has a singularity inside the supposed region of analyticity. The correction RRR cannot remove it. Cancellation would have to come from other active LLL-functions vanishing at that same point.

Let mχm_\chimχ​ be the multiplicity of each such zero, or zero if that function does not vanish at ρ\rhoρ. The necessary condition is

∑χcχmχ=0.\sum_\chi c_\chi m_\chi=0.χ∑​cχ​mχ​=0.

One way to see the condition is to differentiate the logarithms. A zero of multiplicity mmm contributes m/(s−ρ)m/(s-\rho)m/(s−ρ) to L′/LL'/LL′/L, plus a regular term. An analytic sum cannot retain that pole, so its total coefficient must be zero.

A zero belonging to just one active primitive LLL-function cannot cancel. In larger active sets, shared zeros could cancel only with exactly the required weights. This is a restriction on possible zeros, not a theorem locating them or proving GRH.

The finite window, character powers and theorem domains
The five-base endpoint comparison at all six tested exponents. Each point is a complete finite-window sum, with the exponent decreasing from left to right.
The five-base endpoint comparison at all six tested exponents. Each point is a complete finite-window sum, with the exponent decreasing from left to right.
The six centered weights in multiplication order and the powers of all six character coefficients. Only modes one and five have nonzero power, each exactly four ninths.
The six centered weights in multiplication order and the powers of all six character coefficients. Only modes one and five have nonzero power, each exactly four ninths.
The two directions of the theorem. The upper domain assumes GRH for the selected functions. The lower marked zero is hypothetical and would require cancellation at that same point.
The two directions of the theorem. The upper domain assumes GRH for the selected functions. The lower marked zero is hypothetical and would require cancellation at that same point.

These views place the six tested exponents, all six character powers and the two theorem directions side by side with the running paths and coefficient geometry above.

In base three we can go further. There are only two active functions. At a fixed point ρ\rhoρ, let their multiplicities be mmm and nnn. Their weighted sum is

mc+nc‾=m+n3+i3(n−m)3.\begin{aligned} mc+n\overline c &=\frac{m+n}{3}\\ &\quad+i\frac{\sqrt3(n-m)}{3}. \end{aligned}mc+nc​=3m+n​+i33​(n−m)​.​

Its real part is (m+n)/3(m+n)/3(m+n)/3. Multiplicities are nonnegative integers. If either function vanishes, that real part is positive. Even a shared zero cannot cancel in this example.

Conjugating the character reflects a zero across the real axis. It does not automatically put a second zero at the original point. The calculation above allows either possibility. It needs no assumption that the two functions have different zeros.

A triangular lattice plots weighted multiplicities for two base-three characters. Every nonempty choice lies strictly to the right of the origin. A triangular lattice plots weighted multiplicities for two base-three characters. Every nonempty choice lies strictly to the right of the origin.
This is the plane of coefficient sums, not the plane of possible zero locations. A label gives the two multiplicities at one fixed zero. Each teal or gold step adds one third to the real part. Points up to total multiplicity six are shown; the same rule applies without a bound.

At a shared simple zero, the vertical parts cancel and the horizontal parts give 2/32/32/3. Making either zero multiple only pushes the point farther to the right. The cancellation equation asks for the origin.

Companion paper: The Collision Transform and the Critical Strip →
Share

Discussion

Sign in to join the discussion.

← All articlesRead the paper →
← Previous: The Collision Periodic Table
Next: The Neutrality Theorem →