The result
The Collatz conjecture asks for termination of every orbit. This paper
asks a different quantitative question: how far down can one force the
orbit for most starting integers, where “most” is measured by ordinary
counting? A natural-density-one result permits exceptions, but requires
their proportion among the first \(X\) integers to vanish as \(X\)
grows. That distinction turns typical descent into a precise asymptotic
statement without pretending to settle any exceptional orbit. Here the
certified landing scale is prescribed in advance and is eventually
smaller than every fixed power of the starting value, with both an
exceptional-count rate and a logarithmic witnessing time.
Work with the shortcut map, which halves even numbers and takes one
combined step on odd ones:
\[
T(n)=\begin{cases} n/2, & n\equiv 0 \pmod 2,\\[2pt]
(3n+1)/2, & n\equiv 1 \pmod 2,\end{cases}
\qquad T_{\min}(n)=\min_{k\ge 0}T^k(n).
\]
Theorem 1.1 — main theorem
Put
\(\delta_0=\log(1/a_0)/\log(2/a_0)
=0.251245530155874\ldots\), where
\(a_0=(\log_2 3)/2\). For every fixed
\(0<\delta<\delta_0\),
\[ T_{\min}(n)\;\le\;\exp\!\left((\log n)^{1-\delta}\right) \]
on a set of natural density one.
The endpoint \(\delta_0\) is a supremum of the strict parameter ranges
used in the proof; equality at \(\delta=\delta_0\) is not claimed.
Theorem 1.1, part 1 — exceptional count
For every fixed \(0<\delta<\delta_0\) and every
\(0<\sigma<1-\delta/\delta_0\),
\[ \#\left\{n\le X: T_{\min}(n)>\exp\!\left((\log n)^{1-\delta}\right)\right\}
\;\le\; 5X\exp\!\left(-c_{\delta,\sigma}(\log X)^{\sigma}\right) \]
for all sufficiently large \(X\).
Theorem 1.1, part 2 — logarithmic-time witness
There is a natural-density-one set on which every sufficiently large
\(n\) reaches the threshold at some step
\[ 0\le k < 6.953\log n, \]
with \(T^k(n)\le\exp((\log n)^{1-\delta})\).
What this does not do. These are almost-all statements
in natural density. They do not prove the Collatz conjecture, do not
establish descent for every initial value, and do not exclude
exceptional cycles or divergent trajectories. They are compatible with
arbitrarily long individual exceptional orbits.