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Bit Destruction ​

A way of measuring how big a drop is, in bits. It is an explainer: the fact that β(s)>0\beta(s) > 0 is just a restatement of "a drop is a decrease", and it is not a step toward proving convergence.

Statement ​

Identity. A drop of kk steps, ss of them odd, has contraction ratio 3s/2k−s3^s/2^{k-s}, which removes (k−s)−slog⁡23(k-s) - s \log_2 3 bits. The ratio has to be below 1, so k−s≥⌊slog⁡23⌋+1k - s \geq \lfloor s \log_2 3 \rfloor + 1, and with exactly that many halvings it removes

β(s)=⌊s⋅log⁡23⌋+1−s⋅log⁡23=1−{s⋅log⁡23}\beta(s) = \lfloor s \cdot \log_2 3 \rfloor + 1 - s \cdot \log_2 3 = 1 - \{s \cdot \log_2 3\}

bits, where {x}\{x\} is the fractional part. So β(s)\beta(s) is positive and at most 1, and it equals 1 only at s=0s = 0, because log⁡23\log_2 3 is irrational.

Every dropping set with k≤39k \le 39, and every n≤107n \le 10^7, uses exactly this smallest number of halvings. It is not proved that every nn does (see Affine Orbit Structure).

Why it is interesting ​

A drop through a set with small β(s)\beta(s) barely shrinks the number. How small β(s)\beta(s) can get is governed by how well log⁡23\log_2 3 can be approximated by rationals, which ties the size of drops to Diophantine approximation.

The Bit Destruction Landscape ​

Table of β(s)\beta(s) for s=0s = 0 through 2929:

sss⋅log⁡23s \cdot \log_2 3β(s)\beta(s)Setk_kStatus
00.0001.0001
11.5850.4153
23.1700.8306
34.7550.2458
46.3400.66011
57.9250.07513slow
69.5100.49016
711.0950.90519
812.6800.32021
914.2650.73524
1015.8500.15026slow
1117.4350.56529
1219.0200.98032
1320.6050.39534
1422.1890.81137
1523.7740.22639
1625.3590.64142
1726.9440.05644slow
1828.5290.47147
1930.1140.88650
2031.6990.30152
2133.2840.71655
2234.8690.13157slow
2336.4540.54660
2438.0390.96163
2539.6240.37665
2641.2090.79168
2742.7940.20670
2844.3790.62173
2945.9640.03675slow

Pattern: slow sets occur when s⋅log⁡23s \cdot \log_2 3 approaches an integer from below.

Proof ​

The contraction ratio for a drop of kk steps with ss odd steps is 3s/2k−s3^s / 2^{k-s}. With the smallest number of halvings that brings the ratio below 1, k−s=⌊s⋅log⁡23⌋+1k - s = \lfloor s \cdot \log_2 3 \rfloor + 1 (these values of kk are OEIS A122437).

The bits destroyed equal the negative log of the contraction ratio:

β(s)=−log⁡2 ⁣(3s2k−s)=(k−s)−s⋅log⁡23=⌊s⋅log⁡23⌋+1−s⋅log⁡23\beta(s) = -\log_2\!\left(\frac{3^s}{2^{k-s} }\right) = (k-s) - s \cdot \log_2 3 = \lfloor s \cdot \log_2 3 \rfloor + 1 - s \cdot \log_2 3

A fractional part is always below 1, so β(s)=1−{s⋅log⁡23}>0\beta(s) = 1 - \{s \cdot \log_2 3\} > 0 always.

How small can β(s)\beta(s) get? ​

The slowest sets come from rational approximations p/sp/s to log⁡23\log_2 3 that lie just above it, so that slog⁡23s \log_2 3 falls just short of the integer pp:

ppssp/sp/sβ(s)\beta(s)
851.6000.075
65411.5850.017
4853061.5850.0015

(Convergents that lie just below log⁡23\log_2 3, such as 19/1219/12 and 84/5384/53, give β(s)\beta(s) close to 1 instead.)

Since log⁡23\log_2 3 is transcendental, the lower bounds that are proved come from Baker's theory of linear forms in logarithms: ∣E−Slog⁡23∣>S−κ|E - S \log_2 3| > S^{-\kappa} for an effective constant κ\kappa (Rhin: κ≈13\kappa \approx 13). So β(s)\beta(s) can shrink as ss grows, but not faster than a power of ss.

What this does not say ​

Knowing that every drop removes a positive number of bits says nothing about how many times an orbit drops, or whether it grows without bound between drops. It is a convenient scale for measuring drops, not an ingredient of a proof.