# Next paper: the logarithmic change of variable for wide brackets Not part of the current paper. Recorded here so the reasoning that leads to it is not reconstructed from scratch. ## Why this is a separate paper and not a fix The current paper's method is *additive*: every step moves the iterate by an absolute amount, `|f|/|f'|`. On the Chandrupatla families `fun3.*`, `fun4.*`, `fun5.*` the bracket is up to 10^12 wide while the root sits at |x| ≤ 3, so the search must cross **twelve orders of magnitude**. An additive step cannot do that efficiently: it is sized by the local slope, which says nothing about how many decades remain. That is exactly what stage 7 measured. The cube-root similarity beats the proposed rule on all five members of `fun4` — 32/32/40/47/59 against 89/93/113/125/153, a factor of 2.6 — and it does so because its step is `(|f|/σ)^(1/3)·D` rather than `(|f|/σ)·D`, i.e. a fixed *fraction* of the bracket rather than an absolute distance. It marches geometrically. So the regime is not "a different similarity function". It is **multiplicative versus additive movement**, and that is a change of the space the method works in, not of a coefficient inside it. ## What was already tried and must not be repeated All of this is measured, in the repository, and pinned by tests. 1. **Use `cbrt` where it wins.** A switch chosen per benchmark set is *worse* than not switching: 6905 evaluations against 6026. `cbrt` wins the `fun` families and loses the rest of Chandrupatla (4099 against 3220 over that set). The regime is narrower than the set. 2. **Detect the regime from the value ratio.** `rho = 1 − |f_n|/|f_{n−1}|` destroys the order (2.000 → 0.904) and doubles the cost on the standard problems (84 → 161). Near the root both values are negligible and their ratio is noise. 3. **Detect it from the local order of `f`.** Dropping the linearity assumption from the contraction law *does* produce the march exponent, `p = L/(L − ln m)` with `L = ln(e/D)`, and it collapses to the multiplier `m = 1/(1 − θ)`, `θ = f·f''/(f')²`. The derivation is sound and the order survives (2.001), but the estimator is not sharp enough: on Alefeld–Potra–Shi, where almost every root is simple and the truth is `m = 1`, it reports `m > 1` on **27.9%** of steps with excursions to `m = 34.8`; on the flat families it fires on **35.8%**. 27.9 against 35.8 is not a separation, and the false positives cost 273 evaluations. 4. **Separate the regimes by anything the method can see before it commits.** Bracket width does not do it: the winners overlap completely, the proposed scale winning on widths from 10^0 to 10^12. ## The proposal Work in `u = sign(x − c)·log(1 + |x − c|/s)` rather than in `x`, with the origin `c` and the unit `s` read from the bracket rather than chosen. An additive step in `u` is a multiplicative step in `x`, so the same similarity rule, the same derived scale and the same projection safeguard become a geometric march without any new coefficient — and the march exponent, which `cbrt` fixed at 1/3 by accident, disappears as a free quantity. Two things must be established before this is a paper: - **The transform must be parameter-free.** `c` and `s` have to come from the bracket ends and the sign change, not from a choice. If they cannot, the line closes the same way the phase detector did. - **It must not cost anything on ordinary problems.** The transform has to be the identity, to within rounding, when the bracket is narrow — otherwise it buys the wide-bracket families at the price of the canonical set, which is exactly the trade every attempt so far has failed. ## What would settle it The same protocol as the current paper: the 154 Alefeld–Potra–Shi problems and the 45 Chandrupatla problems, evaluations of `f` as the cost, failures charged the full budget, the worst-case bound checked on every solved run, and the configuration fixed by the derivation before the ranking is consulted. Target to beat: **6026** evaluations over the two sets, 193 of 199 solved, with the `2⌈log₂(w/xtol)⌉ + 3` guarantee intact. On the Chandrupatla set alone the target is ITP's **2857**, which the current method does not reach (3220).