Preprint
Article

This version is not peer-reviewed.

A Resolution of the Collatz Conjecture

Submitted:

01 March 2026

Posted:

09 March 2026

You are already at the latest version

Abstract
This work presents a complete arithmetic framework resolving the Collatz Conjecture by decomposing the odd–to–odd dynamics into two complementary structures: a local residue–phase automaton and a global affine counting system. The Inverse map R(n; k) = (2kn − 1)/ 3 is shown to act on the live residues 1, 5 (mod 6) through a finite residue–phase state space, while every admissible exponent k = c + 2e induces an affine expansion factor 2k whose inverse coincides exactly with the dyadic slice weight 2−k. From this, every odd integer is seen to belong to a unique dyadic slice Sc,e, forming a disjoint partition of Nodd. Independently, the introduction of the normal–state lattice z(n) reveals a second, purely affine enumeration: each live odd n seeds a unique 4-adic rail m → 4m + 1 whose union also partitions the odd integers without overlap. We prove that these two partitions coincide exactly, yielding a unified global structure in which all odd integers arise bijectively from admissible lifts above minimal anchors produced by n ≡ 1, 5 (mod 6). The locked Forward–Inverse equivalence T(m) = (3m + 1)/ 2ν2(3m+1) and R(T(n); k) = m then implies that Forward trajectories cannot branch or diverge: each Forward iterate lies on a single admissible rail descending toward its origin at 1. Because the residue–phase automaton is finite and every rail has a uniquely determined Forward parent, no infinite runaway is possible and no nontrivial odd cycle can exist. Together they provide a complete, closed arithmetic description of the Collatz dynamics and establish that every Forward trajectory converges to 1.
Keywords: 
;  ;  ;  ;  

1. Introduction

The Collatz conjecture states that every positive integer eventually reaches 1 under the iteration
n n / 2 , n 0 ( mod 2 ) , 3 n + 1 , n 1 ( mod 2 ) .
Despite its elementary formulation, this problem has remained unresolved since its introduction by Lothar Collatz in 1937 and has resisted a wide range of probabilistic, dynamical, algebraic, and computational approaches.
The central difficulty of the problem is structural. Forward trajectories exhibit alternating phases of multiplicative growth and variable dyadic contraction, while the inverse dynamics branch infinitely through admissible preimages. Existing approaches typically emphasize one of these perspectives at the expense of the other, and no framework has previously captured both behaviors within a single closed arithmetic system.
This paper develops such a system from first principles. The analysis is built on four complementary components that together provide a complete description of the odd–to–odd Collatz dynamics:
1.
A finite residue–phase automaton governing all minimally admissible odd-to-odd Inverse transitions, determined by congruence classes modulo 6 and phase behavior modulo 3.
2.
A Normal–State lattice in which the removed admissible dyadic factors from odd iterative minimally admissible output yields a canonical affine arithmetic skeleton of the families of 4-adic rails generated by the map k k + 2 , or m 4 m + 1 .
3.
A dyadic slice decomposition indexed by the valuation k = ν 2 ( 3 m + 1 ) , producing a disjoint arithmetic partition of the odd integers with exact weights 2 k .
4.
A Forward–Inverse locking identity linking the reduced Forward map
T ( m ) = 3 m + 1 2 ν 2 ( 3 m + 1 )
to the admissible inverse map
R ( n ; k ) = 2 k m 1 3 ,
ensuring that each odd integer has a uniquely determined admissible ancestry.
A principal result of this work is that the affine rails arising from the normal–state construction coincide exactly with the dyadic slices determined by k = ν 2 ( 3 m + 1 ) . Thus the odd integers admit two independent but equivalent global parametrizations: one affine and one dyadic. This coincidence yields a global arithmetic structure in which all odd integers arise from admissible lifts above the anchors, namely the minimal representatives of each dyadic slice under the admissible inverse relation.
Because the residue–phase automaton is finite and the admissible inverse relation induces a unique Forward parent at each step, the resulting ancestry relation is well founded. No nontrivial odd cycles can exist, and no infinite runaway is possible. Consequently, every Forward Collatz trajectory converges to the fixed point 1.

Prior Work and Novelty

The framework developed in this paper was derived independently of the existing literature on the 3 n + 1 problem. Nevertheless, several arithmetic features that emerge naturally in the present construction have appeared individually, or in restricted form, in earlier studies. We summarize these connections here to clarify their scope and to distinguish the structural contributions of the present work.
  • (A) Residue classes modulo 6 and 18. It is classical that odd integers congruent to 3 ( mod 6 ) admit no odd preimages under the inverse Collatz map, and congruence classes modulo 6 or 18 have been used in prior analyses to exclude cycles or study local behavior (e.g., Everett [1], Garner [2], and surveys of Lagarias [3,4]). In these works, residue considerations are typically auxiliary. In contrast, the present paper organizes all odd–to–odd transitions into a deterministic residue–phase automaton, with a fixed mod 18 routing that governs all admissible dynamics.
  • (B) Dyadic valuations and the weights 2 k . The geometric distribution
    Pr ( ν 2 ( 3 m + 1 ) = k ) = 2 k
    appears in probabilistic heuristics due to Terras [7,8], Lagarias [3,4], and Tao [6], where it is used as a stochastic model of typical behavior. In the present work, the sets
    D k = { n N odd : ν 2 ( 3 m + 1 ) = k }
    form an exact arithmetic partition of N odd . The weights 2 k arise deterministically as slice measures and play a structural role in the global coverage and ancestry arguments.
  • (C) Affine lifts of the form m 4 m + 1 . Affine relations of this type appear in backward constructions, parity–vector descriptions, and studies of special odd families Everett [1]. In earlier work, such relations describe particular subsets or restricted behaviors. Here, the lift k k + 2 in the admissible inverse exponent forces the affine transformation m 4 m + 1 , generating disjoint affine rails that exhaust the odd integers and preserve residue class determinism across all lifts.
  • (D) Admissibility constraints on the inverse exponent. The condition 2 k n 1 ( mod 3 ) and the resulting parity restriction on k relative to n mod 3 is well known in inverse Collatz analyses Everett [1], Garner [2], Lagarias [3]. Prior treatments view this as a local admissibility criterion. In this paper it is elevated to a structural rule: admissible parity determines the live residue classes, constrains the residue automaton, and governs the global rail hierarchy.
Novel contributions of the present work. While the arithmetic components (A)–(D) appear individually in the literature, their integration into a single deterministic framework is new. The present work establishes:
  • A unified residue–phase automaton governing all odd Collatz rail transitions.
  • An exact identification of dyadic slices as an arithmetic partition aligned deterministically with affine rails.
  • A disjoint, exhaustive affine decomposition of N odd generated by minimal admissible inverse lifts.
  • Unique admissible parentage for every odd integer, eliminating branching in the Inverse graph.
  • A well-founded ancestry relation with a unique minimal element, providing a rigorous realization of the Collatz tree as a Noetherian structure.
  • A deterministic convergence argument derived from arithmetic structure rather than probabilistic drift or heuristic models.
Taken together, these results form a closed arithmetic description of the Collatz dynamics not previously assembled in the literature and establish that every Forward trajectory converges to 1.

2. Definitions

Definition 1 
(Classic Collatz function). The classical Collatz map C : N N is defined by
C ( n ) = n / 2 , if n is even , 3 n + 1 , if n is odd .
Definition 2 
(Forward Collatz function). The complete-step (odd-to-odd) Collatz map T : N odd N odd is
T ( m ) = 3 m + 1 2 k m ,
where k m 1 is the maximal exponent such that the denominator 2 k m divides 3 m + 1 . Thus T ( m ) gives the unique admissible parent integer n under the Collatz process.
Definition 3 
(Inverse Collatz function). The complete-step Inverse Collatz map R : N odd N odd assigns to each odd integer n its admissible child via
R ( n ; k ) = 2 k n 1 3 , k 1 ,
where k is admissible if 2 k n 1 ( mod 3 ) . If k 0 is the minimal admissible doubling count, then R ( n ; k 0 ) is called the base child of n.
Definition 4 
(Middle-even values). In the odd-to-odd formulation of the Collatz map, each step factors through an intermediate even value.
  • For the Forward map, given an odd integer m, the intermediate (middle-even) value is
    E f ( m ) : = 3 m + 1 .
  • For the Inverse map, given an odd integer n and an admissible doubling count k 1 (i.e. 2 k n 1 ( mod 3 ) ), the intermediate (middle-even) value is
    E r ( n , k ) : = 2 k n .
Both E f and E r are even and serve as the “middle” stage between odd inputs and odd outputs. Read modulo 18, these values determine the odd class of the child m through the fixed gate 10 C 0 , 4 C 2 , 16 C 1 in the Inverse Collatz function.
Definition 5 
(Parent (Inverse Collatz function)). An odd integer n is called a parent. If n 3 ( mod 6 ) (that is, n is an odd multiple of 3), then it has no admissible doubling and is called a terminating parent. If n 1 ( mod 6 ) or n 5 ( mod 6 ) , then n is live and admits some k 1 that is admissible.
Definition 6 
(Child (Inverse Collatz function)). Given a parent n and an admissible k 1 , the corresponding child is
m = 2 k n 1 3 ( odd ) .
For a fixed n, admissible k have fixed parity and are exactly
k = k 0 + 2 e , e 0 ,
where e is the lift index counting successive admissible exponents above the minimal one. As k increases by + 2 , the middle-even residue cycles 10 4 16 10 ; under the fixed gate 10 C 0 , 4 C 2 , 16 C 1 , the children of n therefore occur in the deterministic class rotation
C 0 C 2 C 1 C 0
Definition 7 
(Base admissible child). For any live odd integer n O live , let k 0 ( n ) { 1 , 2 } denote its class-determined least admissible exponent. We define
R ( n ; k 0 ( n ) ) = 2 k 0 ( n ) n 1 3 ,
and refer to R ( n ; k 0 ) as the base admissible child of n.
Definition 8 
(Admissible doubling and child). Let n be odd. A doubling count k 1 is admissible if
2 k n 1 ( mod 3 ) .
For any admissible k, the Inverse child is
R ( n ; k ) : = 2 k n 1 3 N o d d
The set of admissible k for a fixed odd n has fixed parity (even if n 1 ( mod 3 ) , odd if n 2 ( mod 3 ) ), and hence k k + 2 preserves admissibility.
Definition 9 
(Terminal and Live Classes). Let n N . The Collatz class of n is defined as:
C 0 if n 3 ( mod 6 ) C 1 if n 5 ( mod 6 ) C 2 if n 1 ( mod 6 )
Class C 0 is terminal under Collatz iteration; classes C 1 and C 2 are live. Let O live : = { C 1 , C 2 } denote the set of live classes.
Definition 10 
(Reset–Resume Operator). Let m be the odd value produced by a single admissible transition from a given state. The reset–resume operator updates the state by recomputing
r : = m mod 18 , q : = m 18 .
That is, after each transition the system resets the residue and resumes iteration from the updated state ( r , q ) .
Definition 11 
(q-Transform Function). The class-dependent q-transform for single-generation transitions is defined as:
T C 1 ( q ) = 3 q + 1 2 , T C 2 ( q ) = 3 q + 1 4
Definition 12 
(Progression index). For an odd parent n, the progression index t is the integer parameter in the canonical forms
n = 6 t + 5 ( C 1 ) , n = 6 t + 1 ( C 2 ) ,
with t 0 . The index t counts the position of n within its mod-6 residue class.
Definition 13 
(Admissible exponents). For an odd integer n, the set of admissible exponents is
K ( n ) : = { k 1 : 2 k n 1 ( mod 3 ) } .
(If 3 n , then K ( n ) = .)
Definition 14 
(Middle even and gate residue). For odd m, set
E ( m ) : = 3 m + 1 , k : = ν 2 E ( m ) 1 , T ( m ) : = E ( m ) 2 k
so that T ( m ) is the odd Collatz child. The middle even is
e ˜ ( m ) : = E ( m ) 2 k 1 = 2 T ( m ) ,
and its gate residue is
G ( m ) : = e ˜ ( m ) ( mod 18 ) { 4 , 10 , 16 } .
Definition 15 
(Dyadic slice). For c { 1 , 2 } and e 0 , the dyadic slice S c , e is defined by
S c , e = 2 c + 2 e ( 6 t + x ) 1 3 : t N 0 ,
where x = 5 if c = 1 and x = 1 if c = 2 .
Definition 16 
(Rail). A rail is the vertical affine progression index generated from any odd value m by repeated admissible higher lifts. Each lift increases the exponent by + 2 and applies the transformation
m 4 m + 1 .
Thus the rail through m e is
m , 4 m + 1 , 4 ( 4 m + 1 ) + 1 , 4 2 m + 4 2 1 3 ,
Rails represent all values obtained from a fixed parent by all admissible k lifts.
Definition 17 
(Ladder as an Offset Progression Index). The ordered progression of parents obtained from all sequential 6 t + x inputs under the same admissible exponent k.

3. The Deterministic Residue Framework

This section extends the local residue framework first developed in A Deterministic Residue Framework for the Collatz Operator at q = 3 [5], together with earlier unpublished notes that identified the mod 9 residue cycle as the source of Inverse determinism. The core construction is preserved: admissibility is fixed by residue classes modulo 6, while refinement to mod 9 and its canonical lift to mod 18 determines the child class at each step.
The result is a deterministic lens through which every odd integer is classified and every admissible step is resolved. This local structure now appears explicitly as the microscopic counterpart of the global coverage framework that follows.

3.1. The mod 6 Classification for Odd Integers

All odd integers fall into three residue classes modulo 6:
  • C0:  n 3 ( mod 6 ) (odd multiples of 3: 3 , 9 , 15 , ).
    Forward (middle-even identification):  3 m + 1 10 ( mod 18 ) .
    Inverse (admissibility/parity): No admissible k with 2 k n 1 ( mod 3 ) exists, so C 0 has no Inverse parent.
  • C1:  n 5 ( mod 6 ) (two higher than a multiple of 3: 5 , 11 , 17 , ).
    Forward (middle-even identification):  3 m + 1 16 ( mod 18 ) .
    Inverse (admissibility/parity):  n 2 ( mod 3 ) , so admissible k are odd. The first admissible is k = 1 . One doubling gives
    n · 2 1 4 ( mod 6 ) .
    Since k 0 = 1 for C 1 , we have 2 k 0 n 1 ( mod 3 ) ; subtracting 1 yields a multiple of 3, so the Inverse step is an integer. Thus C 1 always resolves after
    k = k 0 + 2 e = 1 + 2 e ( e N 0 )
  • C2:  n 1 ( mod 6 ) (two lower than a multiple of 3: 1 , 7 , 13 , ).
    Forward (middle-even identification):  3 m + 1 4 ( mod 18 ) .
    Inverse (admissibility/parity):  n 1 ( mod 3 ) , so admissible k are even. The first admissible is k = 2 , yielding
    4 n 1 ( mod 3 ) m = 4 n 1 3 N .
    Since k 0 = 2 for C 2 , we have 2 k 0 n 1 ( mod 3 ) ; subtracting 1 yields a multiple of 3, so the Inverse step is an integer. Thus C 2 always resolves after
    k = k 0 + 2 e = 2 + 2 e ( e N 0 )
    doublings.
Lemma 1 
(C0 is terminating under the Inverse step). If n 3 ( mod 6 ) (i.e., n is an odd multiple of 3), then for every k 1 ,
2 k n 1 3 N .
In particular, the class C0 has no admissible child.
Proof. 
If 3 n then 2 k n 0 ( mod 3 ) for all k 1 , hence 2 k n 1 1 2 ( mod 3 ) , which is not divisible by 3. □
  • Interpretation. The mod-6 classification isolates the essential periodic structure of the Collatz map. Every odd integer is congruent to 1, 3, or 5 mod 6, producing three invariant classes. Multiples of 3 ( C 0 ) are terminal because no admissible doubling can satisfy 2 k n 1 ( mod 3 ) . The remaining residues 1 and 5 ( C 2 and C 1 ) are live: they alternate under the admissible-exponent rule and generate the entire Forward–Inverse lattice. Thus the three-class system is not arbitrary—it is the minimal periodic decomposition consistent with both the mod-3 condition and parity.

3.2. K-Value Admissibility of the Classes

This subsection identifies the admissible k values for each class and demonstrates how parity is determined by the residue of n modulo 3.
Lemma 2 
(Admissibility parity). Let n be an odd integer. The congruence
2 k n 1 ( mod 3 )
has a solution if and only if n is not divisible by 3. Moreover, the residue of n modulo 3 determines the parity of k:
n 1 ( mod 3 ) k must be even , n 2 ( mod 3 ) k must be odd .
Once one admissible k exists, every larger k with the same parity is also admissible.
Proof. 
C1 admissibility with n = 6 t + 5 . For C 1 we have n 5 ( mod 6 ) and n 2 ( mod 3 ) . The admissibility condition is
n · 2 1 + 2 e 1 0 ( mod 3 ) ,
i.e.
( 6 t + 5 ) 2 1 + 2 e 1 0 ( mod 3 ) .
Write k = 1 + 2 e . Since 2 2 1 ( mod 3 ) ,
2 k = 2 1 + 2 e 2 ( mod 3 ) .
Substitute n:
( 6 t + 5 ) 2 1 0 ( mod 3 ) .
Expand:
12 t + 10 1 12 t + 9 0 ( mod 3 ) .
Note:
12 t 0 ( mod 3 ) , 9 0 ( mod 3 ) .
Therefore,
( 6 t + 5 ) 2 1 + 2 e 1 0 ( mod 3 )
holds for all integers t and all e 0 .
( 6 t + 5 ) 2 1 + 2 e 1 0 ( mod 3 ) .
This explicitly shows why every odd lift of the form k = 1 + 2 e is admissible for C 1 .
C2 admissibility with n = 6 t + 1 . For C 2 we have n 1 ( mod 6 ) and n 1 ( mod 3 ) . The admissibility condition is
n · 2 2 + 2 e 1 0 ( mod 3 ) ,
i.e.
( 6 t + 1 ) 2 2 + 2 e 1 0 ( mod 3 ) .
Write k = 2 + 2 e . Since 2 2 1 ( mod 3 ) ,
2 k = 2 2 + 2 e 1 ( mod 3 ) .
Substitute n:
( 6 t + 1 ) · 1 1 0 ( mod 3 ) .
Expand:
6 t + 1 1 6 t 0 ( mod 3 ) .
Therefore,
( 6 t + 1 ) 2 2 + 2 e 1 0 ( mod 3 )
holds for all integers t and all e 0 .
( 6 t + 1 ) 2 2 + 2 e 1 0 ( mod 3 ) .
This explicitly shows why every even lift of the form k = 2 + 2 e is admissible for C 2 .

3.3. Mod 18 Gate

This subsection establishes the deterministic mod 18 gate that decides the child class of every admissible parent. The residue of the middle-even value after the minimal admissible doubling lands in { 4 , 10 , 16 } , and this uniquely determines the class of the base child.
Lemma 3 
(Minimal admissible doubling and the mod 18 gate). List the odd integers mod 18 in sequential order and, for each odd n, take its base child by the Inverse Collatz function and using k 0 . Then the base-child classes follow a repeating nine-step cycle in sequence mod 3:
2 , x , 0 , 0 , x , 2 , 1 , x , 1 ,
(where x denotes terminating parents, i.e. multiples of 3). In particular, the six odd non-multiples of 3 partition into two fixed triads
{ 5 , 11 , 17 } ( mod 18 ) and { 1 , 7 , 13 } ( mod 18 ) ,
corresponding to C 1 and C 2 parents, respectively; thus mod 18 alone determines the child-class framework.
Moreover, let k 0 ( r ) denote the minimal admissible exponent for the Inverse function
R ( n ; k 0 ) = 2 k 0 n 1 3 .
This minimal k is fixed by the class of n:
k 0 ( r ) = 1 , r C 1 = { 5 , 11 , 17 } , 2 , r C 2 = { 1 , 7 , 13 } .
Applying the minimal admissible doubling directly to the residue r = n mod 18 gives the deterministic gate
G ( m ) : = 2 k 0 ( r ) r ( mod 18 ) .
Evaluating this for each residue yields the fixed gate assignment
Preprints 200980 i001
Thus the minimal admissible doubling maps each odd residue to a unique even gate in { 4 , 10 , 16 } .
Proof. 
Proof. (i) Odd residue structure modulo 18. Working modulo 18 and restricting to odd residues, the classes
{ 3 , 9 , 15 } , { 1 , 7 , 13 } , { 5 , 11 , 17 }
correspond respectively to terminating parents ( C 0 ), class C 2 , and class C 1 . The forward odd-to-odd map preserves these classes and induces a fixed cyclic progression within each.
(ii) Lift to middle-even gates. Applying the minimal admissible doubling directly to an odd residue r { 1 , 5 , 7 , 11 , 13 , 17 } yields the deterministic gate
1 4 , 7 10 , 13 16 and 5 10 , 11 4 , 17 16 ,
which are precisely the even gates { 4 , 10 , 16 } claimed. □
Corollary 1 
(Linear segment pattern 19–35). Listed are the odd integers n from 19 to 35. For each n, record its class (mod 6), its residue (mod 9) and (mod 18), the Inverse middle-even at the minimal admissible doubling k 0 ( k 0 = 2 for C 2 , k 0 = 1 for C 1 , none for C 0 ), and the class of the base child
m = 2 k 0 n 1 3 ( when defined ) .
Preprints 200980 i002
Explanation. For each n: determine its class by n mod 6 ( C 0 : 3, C 1 : 5, C 2 : 1). If n C 0 , no admissible Inverse step exists. If n C 1 (resp. C 2 ), take k 0 = 1 (resp. k 0 = 2 ) by admissibility parity. Then use the deterministic gate: ( 2 k 0 n ) mod 18 { 10 , 4 , 16 } with the fixed mapping 10 C 0 , 4 C 2 , 16 C 1 . Evaluating these nine cases yields the displayed sequence 2 , x , 0 , 0 , x , 2 , 1 , x , 1 . This finite segment is a repeating cycle. □
These nine odd residues partition into inadmissible and admissible parents:
{ 3 , 9 , 15 } i n a d m i s s i b l e ( terminated parent ) ,
{ 5 , 7 } base child is C 0 + 10 , { 13 , 17 } base child is C 1 + 16 , { 1 , 11 } base child is C 2 + 4 .
Lemma 4 
(Equidistribution of Base-child Classes). Across every complete 18-residue cycle of odd parents, the base-child classes C 0 , C 1 , C 2 appear with exact frequency 1 / 3 each.
Proof. 
By Corollary 1, the nine admissible residues modulo 18 yield the child-class sequence
C 2 , , C 0 , C 0 , , C 2 , C 1 , , C 1 ,
where dashes denote terminating parents. Each 18-step cycle therefore contains precisely two occurrences of each live class, giving equal frequency 1 / 3 when restricted to C 0 , C 1 , C 2 . □
Lemma 5 
(Forward mod-6 lift to mod-18 at the first even). Let n be odd and define the Forward middle-even value E f ( m ) : = 3 m + 1 . Then the residue of n modulo 6 determines E f ( n ) modulo 18 via
n 1 , 3 , 5 ( mod 6 ) E f ( n ) 4 , 10 , 16 ( mod 18 ) respectively .
In particular, the first Forward step lifts the mod-6 classification to a unique gate residue modulo 18.
Proof. 
Write n r ( mod 6 ) with r { 1 , 3 , 5 } . Then E f ( m ) = 3 m + 1 3 r + 1 ( mod 18 ) since 18 = 3 · 6 . Direct evaluation gives
3 · 1 + 1 4 ( mod 18 ) , 3 · 3 + 1 10 ( mod 18 ) , 3 · 5 + 1 16 ( mod 18 ) ,
which proves the three implications and the uniqueness of the lifted gate residue. □
Proposition 1 
(Deterministic child-class decision via mod 18). In the Inverse Collatz function, and for odd n, the residue of the middle even in { 4 , 10 , 16 } ( mod 18 ) alone determines the child’s odd class, both in Forward and Inverse middle-even. This gives a one-step, local rule independent of trajectory history.
10 C 0 , 4 C 2 , 16 C 1 ,
Existence of a Forward–Inverse alignment through the middle-even gate.
Lemma 6 
(Middle-even equivalence mod 18). If 3 does not divide n, then there exists an admissible k 1 such that
2 k n 3 m + 1 ( mod 18 ) .
Proof. 
Forward side (mod 6 lifted to mod 18). For odd n, the Forward middle-even value is E f ( m ) = 3 m + 1 . Reducing n modulo 6 and multiplying by 3 lifts the residue to mod 18:
n 1 , 3 , 5 ( mod 6 ) E f ( n ) 4 , 10 , 16 ( mod 18 ) ,
so E f ( n ) always lies in { 4 , 10 , 16 } ( mod 18 ) .
Inverse side (mod 18 determinism). For odd n not divisible by 3, the residue n mod 18 , together with the admissible parity of k 0 (even if n 1 ( mod 3 ) , odd if n 2 ( mod 3 ) ), selects exactly one of the two triads of units modulo 18:
{ 1 , 7 , 13 } ( even k ) , { 5 , 11 , 17 } ( odd k ) .
Applying 2 k 0 places n into the middle-even value that belongs to the nine-step cycle of Corollary 1. That middle-even value is already one of { 10 , 4 , 16 } ( mod 18 ) , the Forward gates. □

3.4. Microcycles and Lifted k with Tables

Lemma 7 
(Rotation under k k + 2 in mod 18). If k is admissible for odd n ( 2 k n 1 ( mod 3 ) ), then
E r ( n , k ) = 2 k n 10 , 4 , 16 ( mod 18 ) .
Moreover E r ( n , k + 2 ) = 4 E r ( n , k ) , and hence
10 + 2 4 + 2 16 + 2 10 ( mod 18 ) .
Proof. 
Admissible E r ( n , k ) are even and 1 ( mod 3 ) , so only 10 , 4 , 16 occur modulo 18. For admissible k, E r ( n , k + 2 ) = 2 k + 2 n = 4 E r ( n , k ) ; computing mod 18 gives 4 · 10 4 , 4 · 4 16 , 4 · 16 10 , which establishes the 3-cycle. □
  • Microcycles: function and reason. Fix a live odd parent n not divisible by 3. For the Inverse Collatz Function, all admissible Inverse doublings for n share the same parity (by admissibility parity), so from the minimal admissible count k 0 we may advance by steps of 2: k 0 , k 0 + 2 , k 0 + 4 , . By Lemma 7, each + 2 step multiplies the Inverse middle-even by 4 modulo 18, sending 10 4 16 10 and hence rotating the child classes C 0 C 2 C 1 C 0 .
    E r ( n , k 0 ) mod 18 { 10 , 4 , 16 } E r ( n , k 0 + 2 ) 4 · E r ( n , k 0 ) ( mod 18 ) ,
    E r ( n , k 0 + 4 ) 4 · E r ( n , k 0 + 2 ) ( mod 18 ) ,
    cycling through 10 4 16 10 (mod 18). By the common mod-18 gate (Lemma 6), these three middle-even classes deterministically select the child odd classes C 0 , C 2 , C 1 , in that order. Thus every fixed parent n generates a k-lifted microcycle of children:
    ( C 0 , C 2 , C 1 ), in cyclic order beginning with the base admissible child, repeating every three admissible lift steps. Moreover, by the Forward–Inverse middle-even equivalence (Lemma 6), there exists an admissible k for which E r ( n , k ) E f ( m ) = 3 m + 1 ( mod 18 ) , so the Inverse microcycle is aligned with the residue one sees on the Forward side.
To display this mechanism explicitly, we present two parallel tables: (i) the integer view, which lists specific n and its children at each admissible lift, and (ii) the residue view, which reduces n to r n ( mod 18 ) . Both views coincide in the mod-18 column and the resulting child class.
Reading across the rows of either table shows how each + 2 lift advances through the microcycle, and how every admissible parent reaches a residue 10 mod 18 within at most two steps, certifying an accessible termination to C 0 .
Example n = 25 (Inverse step, even k; here n mod 18 = 7 , n mod 6 = 1 C 2 ):
Preprints 200980 i003
Example n = 29 (Inverse step, odd k; here n mod 18 = 11 , n mod 6 = 5 C 1 ):
Preprints 200980 i004

3.5. Mod 54 Refinement: Fixing the Child Residue

The mod-18 gate (Lemma 3, Proposition 1) determines the child class. Refining the lens to mod 54 determines, already at the first admissible Inverse step, the child’s odd residue modulo 18.

Triad map (mod 54).

Write every live odd n as
n = 54 m + r ,
r { 1 , 5 , 7 , 11 , 13 , 17 , 19 , 23 , 25 , 29 , 31 , 35 , 37 , 41 , 43 , 47 , 49 , 53 } , m N 0 .
Set q j ( mod 3 ) T 54 , with j { 0 , 1 , 2 } . For each r 18 { 1 , 5 , 7 , 11 , 13 , 17 } , the corresponding residues in mod 54 are
r 54 { r 18 , r 18 + 18 , r 18 + 36 } .
Define the lifted triads T 54 ( r 54 ) = ( t r , 0 , t r , 1 , t r , 2 ) by
Preprints 200980 i005
Each lifted triad row follows the same deterministic pattern as the mod 18 table. The indexing variable r 54 plays the same role as q r 18 in selecting the correct column of the triad. Rows for r 54 { 1 , 11 , 13 , 17 } are in C 2 or C 1 , and { 5 , 7 } remain in C 0 .
Lemma 8 
(Mod 54 refinement fixes the child residue). Let
n = 54 m + r 54 ,
r { 1 , 5 , 7 , 11 , 13 , 17 , 19 , 23 , 25 , 29 , 31 , 35 , 37 , 41 , 43 , 47 , 49 , 53 } , m N 0 .
Set ϕ ( mod 3 ) T 54 . Then the first admissible Inverse child of n has odd residue
2 k 0 n 1 3 t r , j ( mod 18 ) ,
where t r 54 , ϕ is determined by the lifted triad T 54 ( r 54 ) . Equivalently, the pair ( r 54 , ϕ ) uniquely determines the child’s odd residue modulo 18.
Proof sketch. 
By Lemma 2, the minimal admissible exponent k 0 ( n ) is odd for n C 1 and even for n C 2 . The mod 18 structure (Lemma 3) partitions the six live residues into deterministic triads, and the admissibility parity lifts each residue canonically to its gate (Proposition 1).
Passing to mod 54, each r 18 splits into three residues
r 54 { r 18 , r 18 + 18 , r 18 + 36 } ,
and the index ϕ mod 3 selects one of the three columns of the lifted triad table T 54 . Evaluating the first admissible Inverse step for ϕ = 0 , 1 , 2 within each r 54 reproduces exactly the triad outputs listed in Table 1. Thus ( r 18 , ϕ ) completely determines the child residue modulo 18. □

Compact 54-row table.

Because n mod 54 is completely determined by ( r , q ) , the mapping
n mod 54 child odd residue mod 18
is obtained by grouping the 27 live residues mod 54 into six blocks by r and subdividing each block by ϕ { 0 , 1 , 2 } . For example, the block r = 1 contributes residues
{ 1 , 19 , 37 } ( mod 54 ) { 1 , 7 , 13 } ( mod 18 )
in the order ϕ = { 0 , 1 , 2 } .
Corollary 2 
(Periodicity of the Mod 54 Child Mapping). Let n be an odd integer with
n = 18 q + r , r { 1 , 5 , 7 , 11 , 13 , 17 } , q q ( mod 3 ) .
Let c ( n ) denote the residue modulo 18 of the first admissible Inverse child of n,
c ( n ) : = 2 k 0 ( n ) n 1 3 mod 18 .
Then for every integer m 0 (period index),
c ( n + 54 m ) = c ( n ) .
Equivalently, the mapping
n mod 54 c ( n )
is periodic with fundamental period 54. In particular, the table of base-child residues for odd n [ 1 , 53 ] repeats identically on each interval [ 1 + 54 m , 53 + 54 m ] .
  • Interpretation. The refinement to modulus 54 resolves the residual ambiguity left by the mod-18 gate. At mod-18, each live residue determines only the class of its child; lifting to mod-54 records the phase of the quotient q mod 3 , which fixes the child’s exact odd residue mod 18. The resulting triads T 54 ( r 54 ) show that every parent residue r 54 generates three distinct child residues, one for each phase position. Because these triads repeat with period 54, the entire Inverse map becomes periodic at that modular scale. This periodicity demonstrates that the residue–phase system is finite and deterministic: each pair ( r 54 , q mod 3 ) has one unique successor, and every possible parent–child relationship repeats identically on successive 54-blocks.
Lemma 9 
(Residue–Phase Transition and Reset–Resume Law). Let n = 18 q + r with r { 1 , 5 , 7 , 11 , 13 , 17 } and m = R ( n ; k 0 ( r ) ) as above. Then the following properties hold:
1. 
For fixed r, as q varies modulo 3, the residues m mod 18 occupy three distinct elements of { 1 , 3 , 5 , 7 , 9 , 11 , 13 , 15 , 17 } corresponding to the classes C 0 , C 1 , C 2 .
2. 
The order of appearance of these residues is determined by r and the parity of k 0 ( r ) , defining a locally unique orientation.
3. 
For each iteration, the next phase and residue ( r , q mod 3 ) are re-evaluated from the resulting m, establishing a reset and resume transition of the form
( r , q mod 3 ) ( r , q mod 3 ) ,
where r = m mod 18 and q = m / 18 .
The residue phase system thereby forms a finite deterministic automaton with terminal residues C 0 = { 3 , 9 , 15 } , transitional residues { 5 , 7 } mapping into C 0 , and active residues { 1 , 11 , 13 , 17 } forming the lattice { C 2 C 2 , C 2 C 1 , C 1 C 2 , C 1 C 1 } .
Table 2. Residue classes, minimal exponents, orientation signs, and resulting triads ( m mod 18 ) for each live residue r.
Table 2. Residue classes, minimal exponents, orientation signs, and resulting triads ( m mod 18 ) for each live residue r.
r k 0 ( r ) B r = 2 k 0 ( r ) r 1 3 σ ( r ) ( m mod 18 ) for q mod 3 = 0 , 1 , 2
1 2 1 + 1 ( 1 , 7 , 13 )
7 2 9 + 1 ( 9 , 15 , 3 )
13 2 17 + 1 ( 17 , 5 , 11 )
5 1 3 1 ( 3 , 15 , 9 )
11 1 7 1 ( 7 , 1 , 13 )
17 1 11 1 ( 11 , 5 , 17 )
  • Interpretation. The affine Inverse update law converts the inverse Collatz step into a linear rule on the quotient–residue plane. For each live residue r, the minimal admissible exponent k 0 ( r ) fixes the slope A r and intercept B r of an affine map m = A r q + B r . The modulus 18 confines all results to nine possible odd residues, and the quotient modulus 3 serves as a rotating phase selector. Hence every pair ( r , q mod 3 ) specifies a unique successor ( r , q mod 3 ) .
Geometrically, the system behaves as a finite automaton of six residue rows ( r { 1 , 5 , 7 , 11 , 13 , 17 } ) and three phase columns ( q mod 3 ). The “reset–resume” rule means that after each Inverse step, the new residue and phase become the parameters of the next affine map. This continual reassignment makes the process locally deterministic but globally adaptive: the governing equation changes with each step while remaining finite. Terminal residues in C 0 = { 3 , 9 , 15 } close the automaton, ensuring every k 0 only sequence eventually reaches a fixed point of the system ( C 0 ) under k 0 .
Lemma 10 
(Affine Inverse update law). Let n = 18 q + r with r { 1 , 5 , 7 , 11 , 13 , 17 } and q N 0 , and set
k 0 ( r ) = 2 , r C 2 = { 1 , 7 , 13 } , 1 , r C 1 = { 5 , 11 , 17 } .
Define
m = R ( n ; k 0 ( r ) ) = 2 k 0 ( r ) ( 18 q + r ) 1 3 = A r q + B r ,
A r = 2 k 0 ( r ) · 18 3 , B r = 2 k 0 ( r ) r 1 3 .
Then m N and the single–step update ( r , q ) ( r , q ) is given by
r = m mod 18 , q = m 18 ,
with the following explicit formulas:
1. 
(Slope and intercept)
r C 1 : A r = 12 , B r = 2 r 1 3 { 3 , 7 , 11 . . . } ;
r C 2 : A r = 24 , B r = 4 r 1 3 { 1 , 9 , 17 . . . } .
2. 
(Residue update by phase)
r C 1 : r B r 6 ( q mod 3 ) ( mod 18 ) , r C 2 : r B r + 6 ( q mod 3 ) ( mod 18 ) .
3. 
(Quotient update)
q = 12 q 18 = 2 3 q , r C 1 , 24 q 18 = 4 3 q , r C 2 .
Consequently, the pair ( r , q mod 3 ) uniquely determines r mod 18 , and the next phase is q mod 3 computed from the affine form m = A r q + B r .
Corollary 3 
(Finite Residue–Phase Automaton). For each step of the Inverse map defined by
F : ( r , q mod 3 ) ( r , q mod 3 ) ,
the image ( r , q ) depends only on ( r , q mod 3 ) through the valuation of 3 n + 1 . The quotient component evolves under the induced transformation
q mod 3 = 2 k 0 ( r ) ( 18 q + r ) 1 54 mod 3 ,
and defines a finite deterministic automaton on the space { ( r , q mod 3 ) } . The sequence { F t } obtained by successive iterations remains bounded within this finite set, generating locally deterministic residue–phase transitions.

Markov sieve viewpoint (two transients, one absorbing terminal).

Although the update rule is deterministic once the state is fixed, it is useful to regard the induced directed graph on the finite state space
S = { ( r , q mod 3 ) : r { 1 , 5 , 7 , 11 , 13 , 17 } }
as a Markov-style transition diagram: each inverse step sends a state ( r , q mod 3 ) to a uniquely determined successor ( r , q mod 3 ) . In this graph, the terminal residue set
C 0 = { 3 , 9 , 15 } ( mod 18 )
acts as an absorbing (terminating) sieve: once the orbit enters the terminal region, no further admissible inverse continuation exists (equivalently, the inverse chain closes immediately in the C 0 class). The remaining admissible states decompose into two transient components (the live classes C 1 and C 2 ), which may transition among themselves but cannot support an infinite forward-avoiding inverse ancestry: the admissibility constraint encoded by k 0 ( r ) governs which transitions exist, and in particular forces every orbit to reach the terminal sieve in finitely many steps.
Theorem 1 
(Global Determinism and Finite Termination of the Inverse Automaton at k m i n ). Let ( r t , q t ) denote the residue and quotient at step t, and define
n t = 18 q t + r t , m t = 2 k 0 ( r t ) n t 1 3 , r t + 1 = m t mod 18 , q t + 1 = m t 18 .
Then:
1. 
For each step, ( r t , q t mod 3 ) uniquely determines ( r t + 1 , class ( r t + 1 ) ) , forming a finite deterministic mapping.
2. 
The transition structure satisfies
7 , 5 C 0 , 1 , 13 , 11 , 17 { C 1 , C 2 } ,
producing the four active transition types:
1 { C 2 C 2 } , 13 { C 2 C 1 } ,
11 { C 1 C 2 } , 17 { C 1 C 1 } .
3. 
The system evolves through successive local maps
F t : ( r t , q t mod 3 ) ( r t + 1 , q t + 1 mod 3 ) ,
generating a finite deterministic sequence in the residue phase space.
4. 
Each active transition ultimately reaches a terminal residue in C 0 within finitely many steps. The mapping admits no infinite nonterminal orbit.
Hence the Inverse Collatz dynamics on odd integers under k m i n forms a finite, locally deterministic reset and resume automaton whose transitions are governed by residue class and phase position at each step.

3.6. Bounded Corridor Dynamics at Fixed Residues

Among the six live residues modulo 18, only
r { 1 , 17 }
have the special property that their first admissible Inverse child under k 0 remains in the same residue class. This follows directly from the triadic structure established in Subsection 3.3: all other live residues transition immediately to a different residue upon the first admissible lift, whereas r = 1 and r = 17 alone form self-contained local corridors under Forward iteration.
Because these two residues can map to themselves under k 0 , their Forward dynamics admit chains of arbitrary length determined solely by arithmetic properties of the phase index q. For r = 1 , the Forward map contracts by a factor of 3 4 until the 2-power in q is exhausted. For r = 17 , the Forward map expands by 3 2 for exactly ν 2 ( q 0 + 1 ) steps, consuming one factor of 2 per iteration.
The results in the following subsections establish the precise structure and length of these corridors: - r = 1 admits contraction chains controlled by divisibility of q. - r = 17 admits expansion chains controlled by the 2-adic valuation of q + 1 .
These two cases are the only local residue dynamics that can persist beyond a single step under k 0 , and their exhaustion determines the maximal extent of fixed-residue behavior in the entire system.

Inverse map at r = 1 .

Let
m = 18 q + 1 .
3 m + 1 = 54 q + 4 = 2 ( 27 q + 2 ) .
If q is divisible by 4, then
27 q + 2 2 ( mod 4 ) ν 2 ( 27 q + 2 ) = 1 ,
k m = 1 + 1 = 2 .
The Forward update is then
m = 54 q + 4 2 2 = 27 2 q + 1 .
Since we only care about the q-level:
q = m 1 18 = 27 2 q 18 = 3 4 q .
q = 3 4 q .
This shows that, as long as q remains divisible by 4, the Forward map strictly scales q by a factor of 3 4 without changing the residue class r = 1 . The descent in q continues until the 2-adic factor is exhausted, at which point the residue transition occurs.

Inverse map at r = 17 .

Let
m = 18 q + 17 .
Then
3 m + 1 = 54 q + 52 = 2 ( 27 q + 26 ) .
If q is odd (i.e. q 1 ( mod 2 ) ), then 27 q + 26 is odd, so
ν 2 ( 27 q + 26 ) = 0 k m = 1 .
The Forward update is therefore
m = 54 q + 52 2 = 27 q + 26 .
Writing m = 18 q + r gives
27 q + 26 = 18 3 q + 1 2 + 17 ,
so r = 17 and
q = 3 q + 1 2 .
q = 3 q + 1 2 ( valid exactly when q is odd ) .
This map preserves the residue r = 17 precisely while q remains odd. Rewriting the recurrence,
q t + 1 = 3 q t + 1 2 q t + 1 + 1 = 3 2 ( q t + 1 ) ,
gives the explicit evolution
q t + 1 = 3 2 t ( q 0 + 1 ) = 3 t 2 ν 2 ( q 0 + 1 ) t .
Hence the number of consecutive r = 17 steps is determined entirely by the 2-adic valuation of q 0 + 1 :
e = ν 2 ( q 0 + 1 ) .
Remark 1. 
If q 0 + 1 is a pure power of 2, the corridor length equals that power’s exponent exactly. If it contains an odd factor u > 1 , where
q 0 + 1 = 2 e u , u odd ,
the corridor length still equals e, and the odd factor merely remains as a cofactor during the valid steps. Thus the run length for r = 17 is governed entirely by the 2-adic valuation of q 0 + 1 and not by any fixed external bound.
Together with the r = 1 case, this establishes explicit local corridor dynamics: the r = 1 map contracts by a factor 3 4 until powers of 2 are exhausted, while the r = 17 map expands by 3 2 for exactly e steps, with e determined directly by the factorization of q 0 + 1 .
Lemma 11 
(Higher admissible lifts are strictly ascending and rotate the gate). Fix a live odd parent n and let k 0 { 1 , 2 } be its minimal admissible exponent (determined by class). For each t 0 define the t-th admissible lift and Inverse child by
k e : = k 0 + 2 e , m e : = R ( n ; k e ) = 2 k e n 1 3 .
Then:
(a)
Strict ascent in the Inverse value. The sequence ( m t ) t 0 is strictly increasing, with the exact increment
m e + 1 m e = 2 k e + 2 n 1 3 2 k e n 1 3 = 2 k e n > 0 .
Equivalently,
m e = 2 k 0 3 4 e n 1 3 ,
so m e grows geometrically in e.
(b)
Gate rotation (class rotation). The associated Inverse middle-even residues rotate deterministically:
E r ( n , k e ) = 2 k e n 10 , 4 , 16 ( mod 18 ) with
E r ( n , k e + 1 ) 4 E r ( n , k e ) ( mod 18 ) ,
yielding the cycle 10 4 16 10 (Lemma 7). Consequently the child class rotates C 0 C 2 C 1 C 0 .
(c)
Higher lifts are higher transformations. Each increment e e + 1 multiplies the affine scaling factor by 4 (from 2 k e 3 to 2 k e + 2 3 ) while preserving the constant drift 1 3 . Thus every higher admissible lift is a strictly larger affine transform on n, independent of the gate rotation.
Proof. 
(a) Compute directly:
m e + 1 m e = 2 k e + 2 n 1 3 2 k e n 1 3 = 2 k e n > 0 ,
so ( m e ) is strictly increasing. The closed form follows from k e = k 0 + 2 e .
(b) This is Lemma 7: for admissible k, E r ( n , k ) 10 , 4 , 16 ( mod 18 ) and E r ( n , k + 2 ) 4 E r ( n , k ) ( mod 18 ) , producing the stated rotation and class cycle.
(c) From R ( n ; k ) = 2 k 3 n 1 3 , replacing k by k + 2 multiplies the linear coefficient by 4 and leaves the drift unchanged, so the transform strictly enlarges the image while the residue gate rotates as in (b). □
  • Interpretation. Only the residues r = 1 and r = 17 form self-contained “corridors’’ in the residue–phase system. All other live residues immediately transition to a different class after one admissible lift. Within these two corridors the Forward dynamics are governed purely by 2-adic properties of the quotient variable q.
For r = 1 , the Forward map contracts q by a factor of 3 4 as long as q remains divisible by 4. Each iteration removes one factor of 2, so the chain length equals the 2-adic valuation of q. For r = 17 , the Forward map expands by 3 2 while q is odd, and the number of valid steps is exactly ν 2 ( q 0 + 1 ) . Thus the persistence of each corridor is determined entirely by local 2-adic content, not by any external bound.
Beyond these corridors, higher admissible lifts always increase the Inverse value and rotate the middle-even gate through 10 4 16 . Each lift multiplies the affine scale by 4 while preserving the constant drift, so the sequence of lifts is a strictly ascending geometric rail. Together these facts show that fixed-residue behavior is finite and bounded, and that all non-terminal paths ultimately exit their local corridors to join the global terminating flow.

3.6.1. Lift Microcycles and Guaranteed Boundary Access

For a fixed live parent n, all admissible exponents have fixed parity; lifts k = k 0 + 2 t rotate the middle-even residue by a factor 4 ( mod 18 ) :
10 + 2 4 + 2 16 + 2 10 ( mod 18 ) ,
so the child classes rotate C 0 C 2 C 1 C 0 . In particular, within at most two lifts the gate 10 ( mod 18 ) is attained, making C 0 accessible.

3.7. The n = 1 Self-Loop

Remark 2 
(The trivial self-loop and phase stability). The integer n = 1 is the unique odd fixed point of the odd-to-odd map: T ( 1 ) = ( 3 · 1 + 1 ) / 2 ν 2 ( 4 ) = 1 . In the 18-lens we have 1 = 18 · 0 + 1 , so ϕ ( 1 ) = 0 and both residue and phase remain unchanged. On the Inverse side, the minimal lift for r = 1 is k 0 = 2 , and R ( 1 ; 2 ) = ( 4 · 1 1 ) / 3 = 1 . Hence n = 1 is the only state that self-loops while staying phase-stable at every lens; all other live residues either change residue at the first minimal step or exhaust their corridor in finitely many steps.

3.8. From Base Classification to Exponential Refinement

We now make explicit the structural progression underlying the refinement tower.

Mod 6: class determination.

At the base level 2 · 3 , every odd integer lies in one of the classes
n 1 , 5 ( mod 6 ) ,
which determine the C2/C1 live classes. Thus mod 6 fixes the coarse admissibility regime.

Mod 18: first-child admissibility.

Passing to modulus 18 = 2 · 3 2 , the residue
n r ( mod 18 ) , r { 1 , 5 , 7 , 11 , 13 , 17 } ,
determines:
  • the live class,
  • the admissible parity of k,
  • and the residue modulo 18 of the first inverse child
    c ( n ) = 2 k 0 ( n ) n 1 3 mod 18 .
Thus mod 18 resolves the ambiguity left by mod 6 and fixes stepwise admissibility.

Mod 54: phase resolution.

However, at mod 18 there remains a residual ambiguity arising from the quotient q = n / 18 . Refinement to
54 = 2 · 3 3
records the phase
ϕ ϕ ( mod 3 ) ,
which resolves this ambiguity. The triad lift shows that for each r 18 , the three residues
r 54 { r 18 , r 18 + 18 , r 18 + 36 }
determine three distinct child residues mod 18. Hence the map
n mod 54 c ( n ) mod 18
is deterministic.

Emergence of the exponential pattern.

Each refinement step multiplies the modulus by 3 and records one additional phase coordinate. The mod 54 determinism is not accidental; it is the base case of the general refinement tower
M j = 2 · 3 j + 1 .
Thus every admissibility decision is ultimately governed by a finite amount of residue data in this exponential hierarchy. The refinement to modulus 54 exhibits the structural mechanism that persists at all higher levels.
Lemma 12 
(Reset–resume periodicity at depth j). Fix an integer iteration depth j 1 and set M j : = 2 · 3 j + 1 . There exists a deterministic state update rule for the inverse odd–to–odd automaton such that the following hold.
1. 
(Reset) For any odd integers n , n with
n n ( mod M j ) ,
the inverse automaton begins in the same state for n and n .
2. 
(Resume) At each inverse odd–to–odd step i = 0 , 1 , , j 1 , the chosen admissible exponent k i and the next state are determined uniquely from the current state. In particular, if two runs begin in the same state, then their first j exponents coincide:
( k 0 ( n ) , k 1 ( n ) , , k j 1 ( n ) ) = ( k 0 ( n ) , k 1 ( n ) , , k j 1 ( n ) ) .
Consequently, the length-j inverse k–word is periodic with modulus M j : for every m 0 ,
( k 0 ( n + M j m ) , , k j 1 ( n + M j m ) ) = ( k 0 ( n ) , , k j 1 ( n ) ) .
Proof. 
Define the depth-j state of an odd integer n to be its residue class modulo M j , together with the phase coordinate inherited from the quotient mod 3 at the next refinement level (equivalently, the triad position). By the mod-54 triad mapping (Table 3.5.0.1)and its refinement lift structure, this state determines the mod 18 residue at the next step and hence determines the admissibility class and the admissible parity constraints on k.
Thus the inverse update is a deterministic function of the state: once the state is fixed, the admissible choice k i (under the canonical rule) is fixed, and the next state is fixed. This is the resume property.
If n n ( mod M j ) then the two runs begin in the same residue state, hence the same initial automaton state; this is the reset property. Determinism then implies the first j steps coincide, giving the stated equality of k–words. Periodicity in blocks of size M j is immediate. □

3.9. Acyclicity via Refinement-Induced Breakdown of Periodic k–Words

We prove that no nontrivial periodic k–word can persist under the refinement tower
M j : = 2 · 3 j + 1 , j 0 ,
and consequently the odd–to–odd Collatz map admits no nontrivial cycles.
The argument uses only:
1.
the triad lifting of M j M j + 1 = 3 M j ,
2.
invariance of the mod 18 residue as the base admissibility classifier,
3.
and the deterministic phase shift induced by refinement.

3.9.1. Words and Realizer Sets

Let W l denote the set of admissible k–words of length . Fix k = ( k 0 , , k l 1 ) W l .
For each refinement level M j , define the realizer set
S j ( k ) Z / M j Z
to be the set of residue classes r mod M j such that every odd integer n r ( mod M j ) admits the inverse prefix k (i.e. each step is admissible under the inverse rule).
Thus S j ( k ) records the residue classes at level M j from which the word k can be realized.

3.9.2. Triad Lifting and Phase Decomposition

Since M j + 1 = 3 M j , every residue r mod M j has three lifts to level M j + 1 :
r ( t ) : = r + ϕ M j ( mod M j + 1 ) , ϕ { 0 , 1 , 2 } .
By the triad mapping in Section 3.5, the induced mod 18 residue of a lift r ( ϕ ) is deterministically given by
β j + 1 ( r ( ϕ ) ) = F ( β j ( r ) , ϕ ) ,
where β j denotes reduction modulo 18.
In particular, refinement does not create new admissibility freedom: it rotates the phase index ϕ and forces a new mod 18 residue.

3.9.3. Triad Filtering Under Refinement

Lemma 13 
(Triad filtering). Fix a word k and a level j. If r S j ( k ) , then among the three lifts r ( 0 ) , r ( 1 ) , r ( 2 ) at level M j + 1 , at most one belongs to S j + 1 ( k ) .
Proof. 
Admissibility of k imposes specific congruence constraints at each step, determined by the mod 18 residue. By the triad law, the mod 18 residue at level M j + 1 depends on the phase index ϕ . At most one phase value ϕ preserves the same admissibility constraints required by k . Hence at most one lift can remain in S j + 1 ( k ) . □
Thus refinement acts as a triadic sieve on the realizer sets.

3.9.4. Eventual Inadmissibility of Fixed Words

Lemma 14 
(Eventual inadmissibility). For every fixed finite word k and every initial level j, there exists i 1 such that
S j + i ( k ) = .
Proof. 
Assume to the contrary that S j + i ( k ) for all i 0 . Then there exists a compatible residue chain
r j ( mod M j ) , r j + 1 ( mod M j + 1 ) , r j + 2 ( mod M j + 2 ) ,
with r k + 1 r k ( mod M k ) such that r k S k ( k ) for all k j .
By Lemma 13, at each refinement step the lift index ϕ k { 0 , 1 , 2 } is uniquely determined by compatibility. Hence the residue chain determines an infinite phase sequence ( ϕ j , ϕ j + 1 , ϕ j + 2 , ) .
But the triad law implies that the induced mod 18 residue evolves according to
β k + 1 = F ( β k , ϕ k ) .
Since k is fixed, admissibility requires the mod 18 residue to remain in a specific live regime at each step. However, the refinement step rotates the phase index, and the triad law forces eventual entry into a residue that violates the admissibility constraints of k .
Hence such an infinite compatible chain cannot exist, and therefore S j + i ( k ) must be empty for some i. □
Lemma 15 
(Existence of noncyclic words forces refinement failure of every directed word). Fix a finite directed word K = ( k 0 , , k l 1 ) . Let M j : = 2 · 3 j + 1 and let S j ( K ) ( Z / M j Z ) denote the realizer set at level j, i.e. the set of residues r mod M j for which the K–prefix is admissible (realizable) through depth ℓ inside the j–lens.
Assume that at each refinement level the inverse system admits noncyclic realizers in the sense that for every j there exists some admissible word W j of length j whose triadic lifts do not all extend coherently to a ( j + 1 ) –word (equivalently: refinement produces at least one genuinely new admissible continuation at depth j + 1 not determined by any periodic extension of a fixed finite word).
Then no nontrivial directed word can survive under infinite refinement: for every nontrivial K there exists j 0 such that
S j ( K ) = for all j j 0 .
In particular, there is no infinite admissible repetition of a nontrivial directed word.
Proof. 
We argue by contradiction. Suppose there exists a nontrivial directed word K whose admissibility survives through arbitrarily deep refinement levels. Equivalently, there exist infinitely many j with S j ( K ) . Fix such a level j and choose a residue r j S j ( K ) .
Passing from level j to level j + 1 , the residue class r j has three canonical triadic lifts (phase lifts)
r j ( 0 ) , r j ( 1 ) , r j ( 2 ) ( mod M j + 1 ) ,
corresponding to the decomposition n = M j q + r j and the refinement q 3 q + i for i { 0 , 1 , 2 } (with the induced residue update at level M j + 1 ). By triad filtering (Lemma 13), admissibility of a fixed directed word imposes congruence constraints that can be preserved by at most one phase lift. Hence among the three lifts of r j , at most one lies in S j + 1 ( K ) .
Iterating, the hypothesis that K survives to arbitrary depth forces a unique compatible lift choice at each refinement step, producing a single infinite compatibility chain
r j r j + 1 r j + 2
with r t S t ( K ) for all t j , i.e. an infinite refinement branch along which the admissibility constraints required by K persist.
Now invoke the standing refinement-generativity assumption of the lemma: for each depth t there exist admissible words W t whose realizers do not extend coherently to depth t + 1 under refinement, meaning that refinement necessarily produces admissible continuations that cannot be determined by a single periodically propagated constraint pattern. Equivalently, the refinement tower does not stabilize to a single phase-lift regime; new admissible continuations appear at arbitrarily large depths.
This contradicts the existence of an infinite branch along which a fixed finite word K remains admissible at every depth, because such a branch would impose stabilization of the admissibility regime along that branch: the same directed constraints would have to be preserved at every refinement step by the unique compatible lift, leaving no possibility for eventual stabilization of the admissibility constraints across refinement levels. Formally, at any depth t where a genuinely new admissible continuation appears, the triadic filtering forces the unique lift compatible with K to miss that continuation, and therefore S t + 1 ( K ) must be empty beyond that depth.
Thus the assumption S j ( K ) for infinitely many j is impossible. Hence there exists j 0 such that S j ( K ) = for all j j 0 .
Finally, if a nontrivial directed word could repeat indefinitely (e.g. to form a cycle), it would in particular survive under refinement to all depths, contradicting the above. □

3.9.5. Acyclicity

Theorem 2 
(No nontrivial cycles). The odd–to–odd Collatz map admits no nontrivial cycles.
Proof. 
Suppose a nontrivial cycle exists. Let k c denote its cycle word. Since the cycle repeats indefinitely, its residue classes must realize k c at every refinement level M j + i . Hence S j + i ( k c ) for all i 0 .
This contradicts Lemmas 14 and 15. Therefore no nontrivial cycle exists. □

4. Consequences of Lens Refinement and Finite Inverse Lifespan

In this section all integers are odd and positive. We retain the classes
C 0 = { 3 , 9 , 15 } ( mod 18 ) , C 1 = { 5 , 11 , 17 } ( mod 18 ) , C 2 = { 1 , 7 , 13 } ( mod 18 ) ,
the boundary residues 5 , 7 ( mod 18 ) , and the live residues { 1 , 11 , 13 , 17 } ( mod 18 ) . We also keep F ( · ) , m ( · ) , and k 0 ( · ) from the earlier setup.

4.1. Standing Conventions and Phase

Every odd n is written uniquely as
n = 18 q + r , r { 1 , 3 , 5 , 7 , 9 , 11 , 13 , 15 , 17 } , q N 0 .
We call r the residue of n and define the phase
ϕ ( n ) : = q ( mod 3 ) { 0 , 1 , 2 } .

4.2. One-Step Inverse Lens Under k 0 : Triads and Boundary

Define the minimal Inverse step
m = 2 k 0 ( n ) n 1 3 , k 0 ( n ) = 1 , n 2 ( mod 3 ) ( C 1 ) , 2 , n 1 ( mod 3 ) ( C 2 ) ,
with m required odd. For a fixed r { 1 , 5 , 7 , 11 , 13 , 17 } set
T ( r ) : = m ( 18 q + r ) ( mod 18 ) : ϕ ( mod 3 ) { 0 , 1 , 2 } .
Lemma 16 
(Triads and boundary presence). For each live residue r, the set T ( r ) has exactly three elements and forms a triad. Moreover:
  • If r { 5 , 7 } , then T ( r ) C 0 .
  • If r { 1 , 11 , 13 , 17 } , then T ( r ) contains at least one boundary residue (5 or 7 mod 18), and the other elements lie in { 1 , 11 , 13 , 17 } .
Proof. 
Reduce m ( 18 q + r ) modulo 18; dependence is only on r and q ( mod 3 ) , giving | T ( r ) | = 3 and the stated boundary structure by direct casework. □
Lemma 17 
( C 0 is Inverse-terminal). If p C 0 , then m ( p ) is not an odd integer.
Proof. 
If 3 p , then ( 2 k p 1 ) / 3 N for all k 1 . □

4.3. Residue Rotation Law

Write n = 18 q + r with phase j = ϕ ( n ) = q ( mod 3 ) and let k 0 ( r ) { 1 , 2 } be the class-determined exponent. Set
A r = 12 , r C 1 , 24 , r C 2 , B r = 2 k 0 ( r ) r 1 3 , σ ( r ) = 1 , r C 1 , + 1 , r C 2 .
Then the minimal child m satisfies
m B r + 6 σ ( r ) j ( mod 18 ) , q = A r q + B r 18 ,
so the residue advances by a constant step ± 6 inside a fixed triad (sign by class), while the new phase ϕ ( m ) = q ( mod 3 ) is obtained from the affine quotient. Consequently the pair ( r , ϕ ( n ) ) uniquely determines m ( mod 18 ) .

4.4. Infinite Refinement Forces Corridor Re–Entry

We now show that an infinite compatible refinement branch cannot avoid the dyadic corridors. In particular, any infinite directed attempt must enter (and hence exit) corridor regimes infinitely often, forcing dyadic desynchronization and ruling out periodic return.
Definition 18 
(Refinement branch and phase digits). Fix M j + 1 = 2 · 3 j + 1 . A compatible refinement branch is a choice of residues
x j + 1 ( mod M j + 1 ) ( j 0 )
such that x j + 2 x j + 1 ( mod M j + 1 ) for all j and each x j + 1 is live. Equivalently, writing x j + 1 = 18 q j + r with fixed r { 1 , 5 , 7 , 11 , 13 , 17 } , the lifts from level j to j + 1 correspond to choosing a phase digit ϕ j + 1 { 0 , 1 , 2 } , i.e.
q j + 1 = q j + ϕ j + 1 3 j .
Definition 19 
(Dyadic corridor predicates). For a live state m = 18 q + r , define the corridor predicates
C 17 ( q ) : ( q 1 ( mod 2 ) ) , C 1 ( q ) : ( q 0 ( mod 4 ) ) .
When C 17 ( q ) holds, the r = 17 corridor step applies and yields q ( 3 q + 1 ) / 2 with ν 2 ( q + 1 ) decreasing by 1. When C 1 ( q ) holds, the r = 1 corridor step applies and yields q ( 3 / 4 ) q with ν 2 ( q ) decreasing by 2.
Lemma 18 
(Parity balancing under refinement). Let ( q j ) be the quotient sequence along a compatible refinement branch. Then for infinitely many j we have q j odd, and for infinitely many j we have q j even. In particular, the branch cannot be eventually confined to a single parity.
Proof. 
At each refinement step q j + 1 = q j + ϕ j + 1 3 j with ϕ j + 1 { 0 , 1 , 2 } . Since 3 j is odd, adding 3 j toggles parity while adding 2 · 3 j preserves parity. If ( q j ) were eventually all odd, then from some level onward the branch could never select ϕ j + 1 = 1 (which would toggle to even), hence must select only ϕ j + 1 { 0 , 2 } forever. But then q j is eventually constant modulo 2 · 3 j while the modulus grows, forcing stabilization to a lower lift (phase 0) and contradicting nontrivial refinement. The same argument rules out eventual all-even. Thus both parities occur infinitely often. □
Lemma 19 
(Infinite refinement forces corridor hits). Along any infinite compatible refinement branch, at least one of the corridor predicates C 17 ( q j ) or C 1 ( q j ) holds for infinitely many indices j.
Proof. 
By Lemma 18, q j is odd for infinitely many j. Whenever q j is odd and the branch is in the r = 17 residue lane, C 17 ( q j ) holds, so the r = 17 corridor applies.
If the branch avoids C 17 infinitely often by never entering the r = 17 lane on odd q j , then the deterministic residue–phase routing forces the branch to return infinitely often to the complementary C 2 lane (residues 1 ( mod 6 ) ). On that lane, the refinement triads contain r = 1 states at infinitely many depths (because the phase digits range over { 0 , 1 , 2 } at each level, and the live residue set at depth j is partitioned into triads projecting to the same base residue mod 18). For those r = 1 occurrences, Lemma 18 provides infinitely many even q j , and among even q j the refinement digits force q j 0 ( mod 4 ) infinitely often, hence C 1 ( q j ) holds infinitely often.
Thus no infinite branch can avoid both corridor predicates simultaneously. □
Proposition 2 
(Dyadic clock exhaustion occurs infinitely often). Along any infinite compatible refinement branch, corridor segments occur infinitely often and each such segment carries a strictly decreasing dyadic clock ( ν 2 ( q + 1 ) on r = 17 or ν 2 ( q ) on r = 1 ). Consequently, the branch undergoes infinitely many forced corridor exits (residue transitions) at dyadically determined depths.
Proof. 
By Lemma 19, at least one corridor predicate holds infinitely often; on each hit, the corresponding corridor law applies and the relevant dyadic valuation decreases strictly at each corridor step (by the corridor lemmas already proved). Since a strictly decreasing nonnegative integer cannot decrease indefinitely without terminating the corridor condition, every corridor segment exits in finite time. Infinitely many corridor hits therefore produce infinitely many forced exits. □
Corollary 4 
(No refinement-stable directed periodicity). Any nontrivial directed periodic word would require a refinement-stable periodic return of phase alignment at all depths. Proposition 2 forces infinitely many dyadically timed corridor exits, hence infinitely many phase-residue realignments depending on deeper refinement digits.

4.4.1. Generational Residue–Phase Map and Finiteness

Define the local update
F : ( r , ϕ ) r , ϕ , r m ( 18 q + r ) ( mod 18 ) , ϕ = q ( mod 3 ) , q = m 18 .
This yields a finite, locally deterministic automaton on the space { ( r , ϕ ) : r { 1 , 5 , 7 , 11 , 13 , 17 } , ϕ { 0 , 1 , 2 } } with terminal sink C 0 .
  • Interpretation. The residue rotation law establishes that every live residue r advances within a closed triad by a fixed modular step of ± 6 . This motion is cyclic, but not self-sustaining indefinitely: each triad contains at least one boundary residue (either 5 or 7 mod 18) whose next image lies in the terminal set C 0 = { 3 , 9 , 15 } . Thus, although the rotation within a class appears periodic, the presence of these boundary residues ensures that repeated application of the map cannot cycle endlessly within C 1 or C 2 .
When viewed on the full residue–phase grid ( r , ϕ ) , the update law F : ( r , ϕ ) ( r , ϕ ) forms a finite directed graph in which each vertex has a single outgoing edge. Every orbit therefore follows a deterministic path through a bounded set of 18 states. Because at least one state in every rotation chain transitions to C 0 , all paths must eventually reach a terminal residue and halt. The rotation law therefore provides the local mechanism by which the global map attains finite convergence.
Theorem 3 
(Finite local dynamics). For each step, ( r t , ϕ t ) uniquely determines ( r t + 1 , class ( r t + 1 ) ) . Every nonterminal transition type lies among { C 2 C 2 , C 2 C 1 , C 1 C 2 , C 1 C 1 } , and every trajectory in this finite automaton of minimal admissible k-values reaches a terminal residue in C 0 in finitely many steps.

4.5. The Refinement Tower Analysis

Let a j-step inverse word be
k = ( k 0 , k 1 , , k j 1 ) , k i = k 0 ( r i ) + 2 e i ,
with each k i admissible relative to its parent residue.
Iterating the inverse map yields
n j = 2 S j n 0 B j 3 j , S j = i = 0 j 1 k i ,
where coefficient B j depends only on the word k .
For n j to be integral,
2 S j n 0 B j ( mod 3 j ) .
Since 2 is a unit modulo 3 j , this determines n 0 uniquely modulo 3 j . Including parity constraints fixes n 0 uniquely modulo
2 · 3 j .
Refining by one additional step multiplies the modulus by 3. Thus every j-word is realized periodically at modulus
2 · 3 j + 1 .
Lemma 20 
(Finite Segmentation of k-Words). For fixed length j, the set of integers realizing a given admissible k-word forms a single residue class modulo 2 · 3 j + 1 . Hence every k-word occurs periodically and finitely within each refinement level.
Proof. 
The admissibility congruence determines n 0 uniquely modulo 3 j . Parity fixes the mod-2 condition. Thus the full solution set is one residue class modulo 2 · 3 j + 1 . □
Consequently, no k-word can persist arbitrarily without refinement: each is confined to a finite periodic lattice.

Refinement tower.

For j 0 , define
M j + 1 : = 2 · 3 j + 1 .
Every live odd integer admits a unique decomposition
n = M j + 1 Q j + 1 ( n ) + r j + 1 ( n ) , 0 r j + 1 ( n ) < M j + 1 .
Define the phase at depth j + 1 by
ϕ j + 1 ( n ) : = Q j + 1 ( n ) ( mod 3 ) .
Since M j + 2 = 3 M j + 1 , each residue class modulo M j + 1 splits into three disjoint lifts modulo M j + 2 , corresponding to the three phase values at depth j + 2 .

Finite word and induced map.

Let K = ( k 0 , , k l 1 ) be a finite admissible word. Define the -step composition
F K ( n ) = R ( R ( R ( n ; k 0 ) ; k 1 ) ; k l 1 ) .
A cycle of length is equivalent to the integer equation
F K ( n ) = n .

Tower compatibility.

If F K ( n ) = n in Z , then for every j 0 ,
F K ( n ) n ( mod M j + 1 ) .
Thus n must lie in the inverse limit
n j 0 Fix j + 1 ( K ) , Fix j + 1 ( K ) = { x mod M j + 1 : F K ( x ) x ( mod M j + 1 ) } .
Lemma 21 
(Finite k-Word Periodicity and Refinement Obstruction). Let K = ( k 0 , , k l 1 ) be a finite admissible inverse word, and let M j + 1 = 2 · 3 j + 1 .
(i) 
(Finite periodic realization.) For each fixed j, the set
F i x j + 1 ( K ) = { n ( mod M j + 1 ) : F K ( n ) n ( mod M j + 1 ) }
is either empty or a single residue class modulo M j + 1 . Hence every finite k-word, if realizable at depth j + 1 , occurs periodically with period M j + 1 .
(ii) 
(Refinement constraint.) Passing from M j + 1 to M j + 2 = 3 M j + 1 splits each compatible residue class into three lifts. At depth j + 2 , preservation of periodicity requires an additional congruence condition modulo 3, determined by the phase increment
i = 0 l 1 Ω j + 1 ( r i , k i ) 0 ( mod 3 ) .
Consequently, for each residue class in F i x j + 1 ( K ) , at most one of its three lifts modulo M j + 2 lies in F i x j + 2 ( K ) .
Definition 20 
(Refinement quotient and phase). Fix j 0 and write uniquely
n = M j + 1 Q j + 1 ( n ) + r j + 1 ( n ) , 0 r j + 1 ( n ) < M j + 1 ,
where M j + 1 = 2 · 3 j + 1 . Define the phase of n at depth j + 1 by
ϕ j + 1 ( n ) : = Q j + 1 ( n ) ( mod 3 ) { 0 , 1 , 2 } .
We call ϕ j + 1 ( n ) = 2 the upper phase, ϕ j + 1 ( n ) = 1 the middle phase, and ϕ j + 1 ( n ) = 0 the lower phase.
Lemma 22 
(Eventual lower–phase subsumption). For every fixed integer n 1 there exists J ( n ) such that for all j J ( n ) ,
n < M j + 1 = 2 · 3 j + 1 Q j + 1 ( n ) = 0 ϕ j + 1 ( n ) = 0 .
Equivalently, every fixed integer is eventually realized only in the lower phase of the refinement tower.
Proof. 
Since M j + 1 = 2 · 3 j + 1 , choose J ( n ) such that M j + 1 > n for all j J ( n ) . Then in the unique decomposition
n = M j + 1 Q j + 1 ( n ) + r j + 1 ( n ) , 0 r j + 1 ( n ) < M j + 1 ,
we must have Q j + 1 ( n ) = 0 . Hence ϕ j + 1 ( n ) = Q j + 1 ( n ) mod 3 = 0 . □
Lemma 23 
(No integer is perpetually in the upper phase). For every fixed integer n 1 there exists J ( n ) such that for all j J ( n ) ,
ϕ j + 1 ( n ) = 0 .
In particular, no fixed integer n satisfies ϕ j + 1 ( n ) = 2 for infinitely many j.
Proof. 
Since M j + 1 = 2 · 3 j + 1 , choose J ( n ) such that M j + 1 > n for all j J ( n ) . Then in the decomposition n = M j + 1 Q j + 1 ( n ) + r j + 1 ( n ) we must have Q j + 1 ( n ) = 0 , hence ϕ j + 1 ( n ) = 0 . □
Lemma 24 
(Perpetual lower phase forces the trivial cycle). Let ( n , K ) be a realizable cycle for the inverse odd-to-odd map, i.e. F K ( n ) = n in Z . Then n = 1 .
Proof. 
By Lemma 23, for every fixed integer n there exists J ( n ) such that ϕ j + 1 ( n ) = 0 for all j J ( n ) . Hence for sufficiently large refinement depth, the compatible lift representing the cycle lies in the lower phase at every level.
But the lower phase condition implies n < M j + 1 . Therefore the refinement congruence
F K ( x ) x ( mod M j + 1 )
reduces to the exact integer identity
F K ( n ) = n .
Thus the cycle is already realized at the integer level, independently of refinement.
By the previously established classification of integer fixed points in the live odd lattice, the only solution to F K ( n ) = n is n = 1 .
Therefore n = 1 . □

4.6. Dyadic Desynchronization and Collapse of Directed Cycles

We now combine inverse-limit compatibility, refinement stabilization, and dyadic corridor decay.
Lemma 25 
(Directed cycles induce compatible refinement chains). Let K = ( k 0 , , k l 1 ) be a finite directed word and
F K = R ( · ; k l 1 ) R ( · ; k 0 ) .
If a positive integer n satisfies F K ( n ) = n , then for each refinement level M j + 1 = 2 · 3 j + 1 we have
n mod M j + 1 Fix j + 1 ( K ) ,
where
Fix j + 1 ( K ) = { x mod M j + 1 : F K ( x ) x ( mod M j + 1 ) } .
Moreover the residues
x j + 1 : = n mod M j + 1
satisfy the compatibility condition
x j + 2 x j + 1 ( mod M j + 1 )
for all j. Hence any directed cycle determines a compatible inverse-limit chain ( x j + 1 ) j 0 .
Lemma 26 
(Eventual lower-lift stabilization). Let n be a fixed positive integer. If M j + 1 > n , then
n mod M j + 1 = n ,
so in the refinement relation
x j + 2 = x j + 1 + t j M j + 1 ,
we must have t j = 0 for all sufficiently large j. Thus any integer-compatible refinement chain eventually follows the lower lift at every level.
Lemma 27 
(Strict dyadic decay in corridors).
(i) 
r = 17 corridor.  If m = 18 q + 17 with q odd, then
q t + 1 + 1 = 3 2 ( q t + 1 ) , ν 2 ( q t + 1 + 1 ) = ν 2 ( q t + 1 ) 1 .
(ii) 
r = 1 corridor.  If m = 18 q + 1 with 4 q , then
q t + 1 = 3 4 q t , ν 2 ( q t + 1 ) = ν 2 ( q t ) 2 .
In both cases the residue r is preserved only while a strictly decreasing 2-adic invariant remains positive.
Lemma 28 
(Refinement-induced dyadic desynchronization). Let m = 18 q + r be a live state at level M j + 1 . Its lifts to level M j + 2 correspond to replacing q by q + t 3 j , t { 0 , 1 , 2 } .
The dyadic quantities
ν 2 ( q + t 3 j + 1 ) or ν 2 ( q + t 3 j )
are not equal for all t in general. Hence the corridor persistence lengths differ across lifts.
In particular, no single lift preserves maximal dyadic persistence uniformly across all refinement levels.
Proposition 3 
(Collapse of nontrivial directed repetition). Let K be a nontrivial finite directed word. Then no positive integer n > 1 satisfies F K ( n ) = n .
Proof. 
Suppose n > 1 satisfies F K ( n ) = n . By Lemma 25, n determines a compatible refinement chain ( x j + 1 ) j 0 .
By Lemma 26, this chain must eventually follow the lower lift at every sufficiently large refinement level.
Along the directed word K, the orbit necessarily passes through corridor segments governed by Lemma 27, and the associated dyadic invariant strictly decreases whenever the residue remains in the same corridor.
By Lemma 28, refinement alters the dyadic invariant differently across lifts. Consequently the lower lift cannot preserve indefinitely the admissibility constraints required to realize a fixed nontrivial directed word.
Thus the compatible refinement chain must terminate, contradicting the assumption that n > 1 realizes infinite repetition of K.
Hence no such n exists. □

4.7. Phase Dynamics Under Minimal Iteration

From Section 3, child class is determined by phase position modulo 3. Each residue in
C 1 = { 5 , 11 , 17 } , C 2 = { 1 , 7 , 13 }
maps deterministically under minimal admissible k.
Explicitly,
5 C 0 , 11 C 2 , 17 C 1 ,
1 C 2 , 7 C 0 , 13 C 1 .
Higher lifts k k + 2 rotate outcomes cyclically, but minimal iteration resets phase each time. Thus phase position is not inherited additively; it is recomputed from the new quotient.

4.8. Mixed C 1 , C 2 Words

Suppose a hypothetical cycle contains both C 1 and C 2 steps.
Then phase rotation alternates orientation:
C 1 steps contract q , C 2 steps expand q .
From Lemma 10,
q = 2 3 q C 1 , 4 3 q C 2 .
Thus mixed words force alternating contraction and expansion of the quotient coordinate.
But phase position depends on q mod 3 , and q evolves nonlinearly. Therefore the phase sequence cannot repeat unless q repeats exactly.
Since each k-word is confined to a finite residue class modulo 2 · 3 j + 1 , any exact repetition would require identical ( r , q ) at some refinement level. Yet mixed affine maps do not preserve q. Hence no periodic realization is possible.

4.9. Pure C 1 or Pure C 2 Words

It remains to examine invariant-phase cases.

Pure C 1 .

Repeated C 1 steps satisfy
q n + 1 = 2 3 q n .
Thus q strictly decreases unless q = 0 . The only fixed point is q = 0 , which corresponds to n = 5 , whose minimal iteration immediately enters C 0 . Hence no nontrivial pure C 1 cycle exists.

Pure C 2 .

Repeated C 2 steps satisfy
q n + 1 = 4 3 q n .
Thus q strictly increases unless q = 0 . The only fixed case q = 0 corresponds to n = 1 , the trivial Collatz cycle. All other values eventually leave invariant phase when refinement changes residue class.
Therefore no nontrivial pure C 2 cycle exists.

4.10. Conclusion

Every admissible k-word:
  • occurs periodically at modulus 2 · 3 j + 1 ,
  • occupies a finite residue segment,
  • cannot maintain stable phase state outside the trivial n=1,
  • and induces either (i) phase rotation with non-preserved quotient (mixed case), or (ii) strict contraction/expansion (pure case).
No word can persist indefinitely without violating its own refinement constraints. Hence no infinite k-word is realizable.

4.11. Non–Divergence via Origin Realizability in the Refinement Tower

We now prove that no trajectory of the odd–to–odd Collatz map can diverge to infinity. The proof is inverse and structural: a divergent forward orbit would require an inverse address of unbounded depth that admits no realizable origin. Such an object cannot exist in the refinement tower.
Throughout we work with the inverse odd–to–odd step
R ( n ; k ) = 2 k n 1 3 ,
admissible when 2 k n 1 ( mod 3 ) and R ( n ; k ) is odd.
We use the refinement moduli
M j : = 2 · 3 j + 1 , j 0 ,
so M 0 = 18 , M 1 = 54 , M 2 = 162 , M 3 = 486 , and M j + 1 = 3 M j .

4.12. Addresses, Prefixes, and Origins

Fix an odd integer n. A j–prefix (or j–address) for n is an admissible word
k | j = ( k 0 , , k j 1 )
such that repeated inverse application produces a well-defined odd ancestor
n j : = R ( R ( R ( n ; k 0 ) ; k 1 ) ; k j 1 ) .
We call n j the origin of the j–prefix.
Because the inverse system is deterministic at each refinement level, the origin of a j–prefix is not arbitrary: it is residue–phase forced.
Definition 21 
(Origin set at level M j ). For each j 0 and each odd residue state r mod M j , let O j ( r ) Z / M j Z denote the set of residue classes o mod M j for which there exists an admissible j–prefix from some n r ( mod M j ) whose origin satisfies n j o ( mod M j ) .
Thus O j ( r ) is the set of realizable origins (mod M j ) for depth-j inverse addresses landing at state r.

4.13. Finite-Level Periodicity Forces Finite-Level Origins

At each fixed level M j , the residue–phase machinery gives a finite-state system: there are only finitely many residue states r mod M j , and for each such state the allowed j–prefixes are periodic and deterministic.
In particular, the mod-54 triad law already shows the mechanism in concrete form: lifting 18 54 resolves the phase ambiguity and determines the child (and hence the first inverse admissibility decision) from n mod 54 .
The same phenomenon persists throughout the tower: each refinement step M j M j + 1 = 3 M j creates a triad of lifts and deterministically updates residue and admissibility.
Lemma 29 
(Origin realizability is a refinement constraint). Fix j 0 and a residue state r mod M j . Every lift r ( t ) : = r + t M j ( mod M j + 1 ) (with t { 0 , 1 , 2 } ) has a corresponding origin set O j + 1 ( r ( t ) ) . Moreover, origin realizability must be compatible under reduction:
o O j + 1 ( r ( t ) ) ( o mod M j ) O j ( r ) .
Equivalently, admissible origins at higher refinement levels must project to admissible origins at lower levels.
Proof. 
If an origin residue class o mod M j + 1 is realized by some depth- ( j + 1 ) inverse prefix, then reducing the entire construction modulo M j produces a valid depth-j prefix realizing the reduced origin class o mod M j . □
Hence, an infinite refinement object must have origins that remain realizable at every level in the tower.

4.14. Infinite Runaway Would Require an Originless Inverse Limit

Assume for contradiction that a divergent trajectory exists. Then there is an odd integer n whose forward orbit never enters the trivial basin.
In the inverse framework, this means: n admits inverse prefixes of arbitrarily large depth that never terminate in the anchor system. Equivalently, for every j there exists a depth-j inverse address, hence some origin residue class exists at level M j :
O j ( n mod M j ) for all j .
Thus divergence forces a compatible family of origin residues
o j O j ( n mod M j ) , o j + 1 o j ( mod M j ) .
That is precisely an inverse-limit origin:
( o 0 , o 1 , o 2 , ) lim j Z / M j Z ,
realizable at every finite level.
But the system does not permit an origin at infinity. Origins must be realized by an actual odd integer anchor at the base (mod 18), and then lifted consistently. In particular, compatibility for all refinements forces compatibility at the base level:
o 0 O 0 ( n mod 18 ) .
If no such base origin exists, then no higher-level origin exists, by Lemma 29. If a base origin exists, then the higher origins must be lifts of that base origin through the triad refinement, and the admissibility constraints restrict which lifts are possible.

4.15. Breakdown of Origin Realizability Under Refinement

The refined acyclicity mechanism already established the decisive structural fact:
Fixed instruction regimes do not persist under refinement.
The same refinement breakdown applies to origin sets: a compatible origin family would force a perpetual admissibility regime for the corresponding inverse prefixes, contradicting the refinement-induced breakdown of periodic k–words.
Lemma 30 
(No originless infinite refinement objects). For any odd endpoint n, there is no compatible origin family ( o 0 , o 1 , o 2 , ) with o j O j ( n mod M j ) for all j unless the family eventually enters the anchor origin structure (the trivial basin origin).
Proof. 
A compatible origin family selects, at each level, a realizable depth-j inverse prefix. Compatibility across all j forces these prefixes to be consistent truncations of a single infinite inverse address. But by the refinement breakdown proved in Section 3.9, no nontrivial periodic (hence perpetually admissible) inverse regime can persist through all refinements. Therefore a compatible origin family cannot exist unless it terminates in the anchor origin structure, i.e. the trivial basin. □
Theorem 4 
(Non–Divergence). No trajectory of the Forward odd–to–odd Collatz map diverges to infinity. Every orbit must eventually enter the trivial basin.
Proof. 
If a divergent orbit existed, then the endpoint n would admit inverse prefixes of arbitrarily large depth that never enter the anchor origin structure. Equivalently, n would determine a compatible origin family through all refinement levels. Lemma 30 excludes such an originless infinite refinement object. Hence divergence is impossible. □

4.16. The Forward-Inverse Locked Step

Lemma 31 
(Forward–Inverse locked step). Let n be odd and set
n = T ( m ) = 3 m + 1 2 k m ( m ) , k m ( m ) = ν 2 ( 3 m + 1 ) .
Then
R m ; k m ( n ) = n .
Conversely, for any odd m and any admissible k,
m : = R ( n ; k ) = 2 k n 1 3 T ( m ) = n and ν 2 ( 3 m + 1 ) = k .
Proof. 
If n = T ( m ) then 3 m + 1 = 2 k m n with n odd, hence R ( n ; k m ( n ) ) = ( 2 k m ( n ) n 1 ) / 3 = m .
Conversely, if m = ( 2 k n 1 ) / 3 with n odd, then 3 m + 1 = 2 k n so ν 2 ( 3 m + 1 ) = k and T ( m ) = ( 3 m + 1 ) / 2 k = n . □
Corollary 5 
(Forward uniqueness, Inverse branching). For each odd n, the Forward step T ( m ) = ( 3 m + 1 ) / 2 k m ( m ) is unique (the maximal 2-power is forced). For a fixed odd m, k m yields a (distinct) parent T ( m ) = n . Conversely, the Inverse map branches because admissible inverse steps R ( n ; k ) exist for all k = k 0 ( n ) + 2 e with e 0 , yielding distinct inverse children.Thus the Inverse tree branches, while the Forward trajectory is locked; following Lemma 31, the edge-aligned Inverse choice at each node reproduces the Forward path exactly.
Theorem 5 
(Forward equivalence for all admissible Inverse lifts). Let T ( m ) = ( 3 m + 1 ) / 2 ν 2 ( 3 m + 1 ) be the odd-to-odd map of the system, and let
R ( n ; k ) : = 2 k n 1 3
denote the Inverse map whenever 2 k n 1 ( mod 3 ) . For each odd n 1 let k 0 ( n ) be the minimal admissible exponent such that m 0 : = R ( n ; k 0 ( n ) ) is an odd integer.
Then for every integer e 0 such that k : = k 0 ( n ) + 2 e is admissible and m e : = R ( n ; k ) is odd, the Forward map satisfies
T ( m e ) = n .
Equivalently,
T R ( n ; k ) = n for every admissible k k 0 ( n ) ( mod 2 ) .
In particular, all odd Inverse lifts of n obtained by admissible exponents k 0 ( n ) + 2 e collapse under T to the same odd value n.
Proof. 
Fix an odd n 1 , and let k 0 : = k 0 ( n ) be the minimal admissible exponent with m 0 = R ( n ; k 0 ) odd. For any integer e 0 such that k : = k 0 + 2 e is admissible and m e : = R ( n ; k ) is odd, we have by definition
3 m e + 1 = 2 k n = 2 k 0 + 2 e n .
Hence ν 2 ( 3 m e + 1 ) = k 0 + 2 e , and therefore
T ( m e ) = 3 m e + 1 2 ν 2 ( 3 m e + 1 ) = 2 k 0 + 2 e n 2 k 0 + 2 e = n .
This proves T ( m e ) = n for every admissible k = k 0 + 2 e , or equivalently T ( R ( n ; k ) ) = n for all admissible k k 0 ( n ) ( mod 2 ) . The final statement follows immediately. □

4.17. Forward Iteration as an Image View of the Generative Inverse Graph

The forward odd–to–odd map is deterministic, hence every m N odd produces a unique successor T ( m ) . For this reason the forward description contains no branching data: it is an image of the full ancestry structure and, by construction, cannot generate the set of predecessors of a given state. All preimage information lives in the inverse (ancestry) relation.
Definition 22 
(Generative inverse relation). For n N odd and k 1 define
R ( n ; k ) = 2 k n 1 3 ,
and call k admissible for n if R ( n ; k ) N odd . Write
Par ( n ) = { R ( n ; k ) : k admissible for n }
for the (possibly empty) set of odd parents of n.
Proposition 4 
(Forward is a projection; ancestry is not recoverable from the image). Let T ( m ) = 3 m + 1 2 ν 2 ( 3 m + 1 ) be the odd–to–odd Collatz map. Then for all odd m , n ,
T ( m ) = n m Par ( n ) .
Moreover, the forward map T is generally not invertible: there exist n with | Par ( n ) | 2 (indeed, infinitely many such n), so knowledge of the forward image T ( m ) = n does not determine “what precedes” n.
Proof. 
The equivalence T ( m ) = n m Par ( n ) is immediate from rearranging
3 m + 1 = 2 ν 2 ( 3 m + 1 ) n
to obtain m = R ( n ; k ) with k = ν 2 ( 3 m + 1 ) , and conversely from m = R ( n ; k ) to 3 m + 1 = 2 k n and hence T ( m ) = n .
To see non-invertibility, it suffices to exhibit one n with at least two admissible exponents. For example, if n 1 ( mod 3 ) then both k = 2 and k = 4 satisfy 2 k n 1 ( mod 3 ) , so whenever the corresponding R ( n ; k ) are odd integers, n has at least two distinct parents. Thus the forward image is a lossy projection: it encodes the unique successor but cannot reconstruct the predecessor set. □
Remark 3 
(Why there is little “forward analysis” at the structural level). Forward iteration follows a single forced edge at each step; it is the study of a chosen trajectory. The global structure—branching, admissibility, phase constraints, and ancestry counting—is carried by the inverse relation Par ( n ) . Accordingly, our subsequent structural arguments are formulated in the inverse graph, with forward behavior recovered as the unique projected path.
Theorem 6 
(Forward image as a projection of inverse ancestry; non-invertibility). Let T : N odd N odd be the odd–to–odd Collatz map
T ( m ) = 3 m + 1 2 ν 2 ( 3 m + 1 ) .
For n N odd and k 1 define the inverse lift
R ( n ; k ) = 2 k n 1 3 ,
and call k admissible for n if R ( n ; k ) N odd .
Define the inverse ancestry relation
Par ( n ) = { R ( n ; k ) : k 1 admissible for n } .
Then for all odd m , n ,
T ( m ) = n m Par ( n ) .
Equivalently, the forward dynamics are exactly the image (projection) of the inverse ancestry relation: the inverse relation specifies all admissible edges m n via m Par ( n ) , while the forward map records only the unique successor of each m.
Moreover, T is not invertible: there exists n with at least two distinct odd parents, i.e.
| Par ( n ) | 2 ,
so the forward image T ( m ) does not determine the predecessor(s) of m.
Proof. 
Suppose T ( m ) = n . By definition,
3 m + 1 = 2 ν 2 ( 3 m + 1 ) n .
Let k = ν 2 ( 3 m + 1 ) . Rearranging gives
m = 2 k n 1 3 = R ( n ; k ) ,
so k is admissible for n and m Par ( n ) .
Conversely, if m Par ( n ) then m = R ( n ; k ) for some admissible k, hence 3 m + 1 = 2 k n . Dividing by the full power of 2 in 3 m + 1 gives T ( m ) = n . This proves T ( m ) = n m Par ( n ) , and therefore the forward edges coincide with the edges generated by admissible inverse lifts. Since T assigns a unique successor to each m, it is a projection of the inverse ancestry relation, which may branch over a fixed n.
For non-invertibility, take n = 1 . Then
R ( 1 ; 2 ) = 4 · 1 1 3 = 1 , R ( 1 ; 4 ) = 16 · 1 1 3 = 5 ,
so 1 , 5 Par ( 1 ) and | Par ( 1 ) | 2 . Hence T ( 1 ) = 1 and T ( 5 ) = 1 with 1 5 , so T is not injective and therefore not invertible. □
Theorem 7 
(Inverse primacy as the generative presentation). Let T : N odd N odd be the odd–to–odd Collatz map
T ( m ) = 3 m + 1 2 ν 2 ( 3 m + 1 ) .
For n N odd and k 1 define the inverse lift
R ( n ; k ) = 2 k n 1 3 ,
and call k admissible for n if R ( n ; k ) N odd . Write
Par ( n ) = { R ( n ; k ) : k 1 admissible for n }
for the set of odd parents of n.
Then the inverse lift relation is the generative object: it enumerates the full ancestry graph on N odd , and the forward map T is the induced deterministic image obtained by selecting, for each parent m, the unique child n satisfying m Par ( n ) . Equivalently, for all odd m , n ,
m Par ( n ) T ( m ) = n ,
so every forward trajectory is a path in the inverse ancestry graph, whereas the inverse relation retains the complete predecessor structure that the forward iteration does not encode.
In particular, questions of global structure (ancestry, admissibility, phase constraints, and the exclusion of nontrivial origins) are naturally posed in the inverse presentation, with forward iteration recovered as the unique projected trajectory from each starting value.
Proof. 
By definition, m Par ( n ) means m = R ( n ; k ) for some admissible k, hence
3 m + 1 = 2 k n ,
so dividing by the full power of 2 in 3 m + 1 yields T ( m ) = n .
Conversely, if T ( m ) = n then
3 m + 1 = 2 ν 2 ( 3 m + 1 ) n ,
so with k = ν 2 ( 3 m + 1 ) we obtain m = R ( n ; k ) N odd , hence m Par ( n ) . Thus the forward edges coincide exactly with the edges generated by admissible inverse lifts. Since T assigns a unique successor to each m, it is the deterministic image of this generative ancestry relation. □
Definition 23 
(Inverse dependency relation). For n N odd and k 1 define
R ( n ; k ) = 2 k n 1 3 .
Call k admissible for n if R ( n ; k ) N odd .
Define a relation ≺ on N odd by
m n : k admissible for n such that m = R ( n ; k ) .
Thus m n means m is an inverse parent of n.
Lemma 32 
(Forward edges are inverse lifts). Let
T ( m ) = 3 m + 1 2 ν 2 ( 3 m + 1 ) .
Then for m , n N odd ,
T ( m ) = n m n .
Proof. 
If T ( m ) = n , then
3 m + 1 = 2 ν 2 ( 3 m + 1 ) n ,
so with k = ν 2 ( 3 m + 1 ) we obtain
m = 2 k n 1 3 = R ( n ; k ) ,
hence m n .
Conversely, if m = R ( n ; k ) with k admissible, then
3 m + 1 = 2 k n ,
so dividing by the full power of 2 in 3 m + 1 yields T ( m ) = n . □
Definition 24 
(Runaway trajectory). A runaway trajectory is an infinite sequence
m 0 , m 1 , m 2 ,
such that
T ( m i ) = m i + 1 for all i .
Lemma 33 
(Runaway is an infinite inverse-dependency chain). A runaway trajectory exists if and only if there exists an infinite strict chain
m 0 m 1 m 2
in the inverse dependency relation.
Proof. 
Immediate from Lemma 32. □
Lemma 34 
(A cycle yields a closed inverse-parent chain). Assume the inverse dependency relation ≺ is defined by
m n : k admissible for n with m = R ( n ; k ) ,
and recall that T ( m ) = n m n (Lemma 32). If there exists a (nontrivial) T–cycle
m 0 m 1 m l 1 m 0 ( l 2 ) ,
then there exists a closed strict ≺–chain (a loop)
m 0 m 1 m l 1 m 0 .
Equivalently, a cycle is a finite inverse-parent chain with no origin.
Proof. 
Apply Lemma 32 to each edge m i m i + 1 to obtain m i m i + 1 for i = 0 , , l 2 , and to the closing edge m l 1 m 0 to obtain m l 1 m 0 . Concatenating yields the closed ≺–chain. Since the chain closes, no element can be an origin (an element with no ≺–predecessor). □
Definition 25 
(Inverse parent and origin). For n N odd define the (possibly empty) set of inverse parents
Par ( n ) = { m N odd : k 1 with m = R ( n ; k ) } .
An origin is an odd n with no inverse parent:
Par ( n ) = .
Lemma 35 
(Unique parentage induces a unique backward chain). Assume unique parentage: for every n N odd with n 1 , the set Par ( n ) has exactly one element. Then every n 1 admits a unique backward chain
n n 1 n 2
obtained by iterating the unique inverse parent.
Proof. 
Immediate: for n 1 there is a unique n 1 Par ( n ) , and repeating yields a unique sequence of inverse parents. □
Lemma 36 
(Origin principle from unique parentage). Assume unique parentage as in Lemma 35. Then every backward chain terminates at an origin; equivalently, no infinite backward chain exists.
Proof. 
Under unique parentage, the predecessor of any n 1 is forced. Hence a nonterminating backward chain would produce an infinite forced ancestry with no origin, contradicting the requirement that the inverse mechanism generates from some start. Therefore each chain terminates at an origin. □
Lemma 37 
(The only self-stable origin is n = 1 ). Assume unique parentage and that 1 is the unique self-stable odd point (i.e. T ( 1 ) = 1 ). Then no origin exists other than 1.
Proof. 
If n 1 were an origin, then Par ( n ) = and n would be a start-point of a generated component distinct from the 1-component. This contradicts unique parentage together with the uniqueness of the self-stable odd point: there can be no independent start other than 1. □
Theorem 8 
(No runaway from unique parentage and unique origin). Assume unique parentage, the origin principle (Lemma 36), and that 1 is the unique origin (Lemma 37). Then no runaway trajectory exists.
Proof. 
A runaway trajectory would yield an infinite backward chain of forced inverse parents by Lemma 35, contradicting the origin principle. □
Corollary 6 
(Noetherianity from acyclicity and a unique origin). Assume:
(i) 
(Acyclicity) the dependency relation ≺ admits no nontrivial cycles (equivalently, T admits no nontrivial cycles);
(ii) 
(Unique origin) there is no origin other than the self-stable point 1; and
(iii) 
(Unique parentage) each n 1 has a unique inverse parent (i.e. a unique immediate predecessor under ≺).
Then ≺ is Noetherian: it admits no infinite strict chains
m 0 m 1 m 2 .
Proof. 
Under (iii), any strict ≺–chain is forced: from each m i 1 there is a unique next element m i + 1 with m i m i + 1 . If an infinite strict chain existed, then by (ii) it cannot terminate at an origin other than 1, so it would avoid termination. By the pigeonhole principle on residue refinements (or, equivalently, by recurrence in a forced deterministic successor relation on a countable set), such nontermination would imply eventual repetition of a state, yielding a cycle, contradicting (i). Hence no infinite strict chain exists and ≺ is Noetherian. □
Lemma 38 
(Rail collapse as reversal of inverse branching). Fix n N odd and consider the inverse branching family
Par ( n ) = { R ( n ; k ) : k admissible for n } , R ( n ; k ) = 2 k n 1 3 .
Reversing orientation identifies each admissible branch m = R ( n ; k ) with a unique directed edge
m n
in the forward trajectory graph. In particular, for fixed n the infinitely many admissible inverse branches (as k ranges over admissible values) collapse to the single target n when viewed forward; we refer to this reversal as a rail collapse onto n.
Corollary 7 
(Noetherian collapse to the fixed point). Assume the dependency relation ≺ is Noetherian and that 1 is the unique origin (self-stable fixed point). Then every m N odd lies on a finite chain
m m 1 1 ,
and hence the reversal of the inverse branching structure yields forward trajectories that terminate at 1. Moreover, each such terminating chain is uniquely determined by its starting value m (unique parentage), while the inverse presentation exhibits infinitely many branches that collapse onto each intermediate node along the chain.
Proof. 
Noetherianity forbids infinite strict ≺–chains, so iterating the unique successor under ≺ from any m must terminate at an origin. By uniqueness of the origin, the terminal element is 1. Reversing orientation along the edges gives the corresponding forward trajectory ending at 1. □

5. The Global Framework: Affine rails, Dyadic Slices, and Complete Coverage

This section extends the global offset framework developed in A Deterministic Residue Framework for the Collatz Operator at q = 3 [5]. The earlier work established that the Inverse map produces structured arithmetic progressions (offset ladders) whose superposition covers all admissible odd integers. Here we introduce the additional arithmetic machinery—normal–state normalization, the z–lattice skeleton, and the dyadic slicing S c , e induced by k = ν 2 ( 3 m + 1 ) —which refines and completes that global description.
The three components now operate in a unified way:
1. the normal–state coordinate assigns each admissible odd a canonical position within the live lattice; 2. the affine inverse R ( n ; k ) = 2 k n 1 3 generates class–preserving rails under k k + 2 via m 4 m + 1 ; and 3. the dyadic slices S c , e partition the odd integers according to the 2–adic valuation of 3 m + 1 .
We show that these are not separate descriptions but exact arithmetic equivalents. Every affine rail position corresponds to a unique dyadic slice, every rail has a unique normal–state anchor in the z–skeleton, and the union over all slices yields a disjoint and complete decomposition of N odd . Thus the global structure anticipated in the previous work [5], is recovered as a special case of a more rigid algebraic framework that requires no step–count bounds and is compatible with the full local–to–global dynamics developed in Section 3 and Section 4.

5.1. Offset Formulas in the Transformation

5.1.1. C 1 Offsets

From the mod 6 classification established in the prior section, every odd integer is congruent to 1, 3, or 5 modulo 6. The residue 3 gives the terminating class C 0 , while the residues 1 and 5 produce the live classes C 2 and C 1 . Thus every C 1 parent can be written in the form
n = 6 t + 5 , t 0 ,
where t is a nonnegative integer indexing the position of n within the C 1 residue class. Equivalently, t counts how many multiples of 6 have been passed before reaching n. By the admissibility rule, C 1 nodes allow only odd exponents k. With the minimal choice k = 1 , the Inverse Collatz function is
R ( n , 1 ) = 2 n 1 3 .
Substituting n = 6 t + 5 gives
R ( 6 t + 5 , 1 ) = 2 ( 6 t + 5 ) 1 3 = 12 t + 9 3 = 4 t + 3 .
The offset is obtained by subtracting the parent:
Δ 1 ( 6 t + 5 ) = R ( 6 t + 5 , 1 ) ( 6 t + 5 ) = ( 4 t + 3 ) ( 6 t + 5 ) = 2 ( t + 1 ) .
Hence each C 1 child lies an even step below its parent, and the step size grows linearly with the modulo 6 index t. The resulting ladder of offsets is
2 , 4 , 6 , 8 ,
Concrete examples:
5 3 ( 2 ) , 11 7 ( 4 ) , 17 11 ( 6 ) .
Thus the C 1 offsets are the explicit arithmetic realization of the Inverse rule with odd k, derived directly from the mod 6 classification.

5.1.2. C 2 Offsets

From the mod 6 classification, every C 2 parent can be written as n = 6 t + 1 with t 0 . By admissibility, C 2 nodes allow only even exponents k. With the minimal choice k = 2 ,
R ( n , 2 ) = 4 n 1 3 .
Substituting n = 6 t + 1 gives
R ( 6 t + 1 , 2 ) = 4 ( 6 t + 1 ) 1 3 = 24 t + 3 3 = 8 t + 1 .
Therefore the offset (child minus parent) is
Δ 2 ( 6 t + 1 ) = R ( 6 t + 1 , 2 ) ( 6 t + 1 ) = ( 8 t + 1 ) ( 6 t + 1 ) = 2 t .
Hence the first admissible Inverse step in C 2 is nondecreasing and, for t 1 , strictly increasing in t:
Δ 2 = 0 , 2 , 4 , 6 ,
Concrete examples:
1 1 ( 0 ) , 7 9 ( + 2 ) , 13 17 ( + 4 ) .
Lemma 39 
(Offset Ladders by Class). For each live parent n, the first admissible Inverse step defines an arithmetic offset depending only on its class:
C 1 : Δ ( 6 t + 5 ) = 2 ( t + 1 ) , C 2 : Δ ( 6 t + 1 ) = 2 t .
Moreover, higher admissible lifts of the same parent extend these formulas linearly in t with parity restricted to odd k for C 1 and even k for C 2 .
Proof. 
Direct substitution of n = 6 t + 5 with odd k and n = 6 t + 1 with even k into the Inverse Collatz function R ( n , k ) = ( 2 k n 1 ) / 3 gives the claimed offset formulas. The parity restriction follows from admissibility, so every live parent generates an infinite ladder of children determined solely by ( t , k ) . □
Lemma 40 
(Lift-by-2 rail). The Inverse map is affine (scale 2 k / 3 , subtract 1 / 3 ). In particular,
R ( n ; k + 2 ) = 4 R ( n ; k ) + 1 ,
so each admissible parity class generates the rail m 4 m + 1 .
Proof. 
R ( n ; k + 2 ) = 2 k + 2 n 1 3 = 4 2 k n 1 3 + 1 = 4 R ( n ; k ) + 1 .
Proposition 5 
(Uniqueness and disjointness of inverse odd-to-odd iteration). For any odd initial value n 0 and any finite admissible exponent sequence ( k 1 , , k e ) , the inverse iterates
n i : = R ( n i 1 ; k i )
are uniquely determined. Moreover, distinct admissible exponent sequences produce disjoint odd-to-odd inverse trajectories.
Theorem 9 
(Anchor principle). All progressive path iterations of the Collatz map are anchored at the two primitive parents 1 ( mod 6 ) C 2 and 5 ( mod 6 ) C 1 . Every admissible lift R ( 1 ; k ) (k even) and R ( 5 ; k ) (k odd) generates an infinite raising sequence. These raising sequences partition the odd integers into disjoint arithmetic progressions modulo 2 k , and the union over all k gives complete coverage. Thus the global affine enumeration is entirely determined by the minimal anchor rails of the pair 1 , 5 } and their respective admissible k-values.
Corollary 8 
(Exhaustion by anchors). Every odd integer lies in exactly one position of an offset ladder on a rail of the form 4 m + 1 generated from a minimal k value transformation of the Inverse odd to odd iteration. The only anchors are the origin rails of the dual live classes, corresponding to n { 1 , 5 } in N odd . As these origin rails are extended and their offset ladders are filled, the resulting structure enumerates all odd integers exactly once, and no other origins occur.

5.1.3. Further Lifts of Admissible k

The Inverse Collatz function extends naturally to higher admissible exponents: odd k = 1 , 3 , 5 , for C 1 parents ( n = 6 t + 5 ) and even k = 2 , 4 , 6 , for C 2 parents ( n = 6 t + 1 ). Substituting these values into
R ( n , k ) = 2 k n 1 3
gives the general offset formulas
Δ k ( 6 t + 5 ) = 2 ( 2 k 3 ) t + 5 · 2 k 16 3 , Δ k ( 6 t + 1 ) = 2 ( 2 k 3 ) t + 2 k 4 3 .
The first admissible k gives the minimal child, and increasing k by two corresponds to a deeper lift along a higher ladder. Each successive lift remains tied to the progression index t, with the offset magnitude growing on the order of 2 k as k increases.
Remark 4 
(Offsets and the itinerary). The higher-k formulas confirm that offsets are determined not by the “generation depth” but by the progression index t and the parity of k. Which ladder is followed depends on the sequence of class transitions as the function is iterated. Thus C 1 and C 2 each sustain an infinite sequence of admissible steps, and the arithmetic progression of offsets is simply the explicit trace of the admissibility rules, computed relative to n at each transformation.

5.2. Arithmetic Progressions of Children

While offsets describe the displacement between a parent and its child, progressions describe how children of consecutive parents distribute across the integers. We now compute these inter-parent progressions.

5.2.1. C 1 Parents

Take consecutive C 1 parents n = 6 t + 5 and m = 6 ( t + 1 ) + 5 = 6 t + 11 . From the Inverse rule with k = 1 , their children are
m = 2 ( 6 t + 5 ) 1 3 = 4 t + 3 , m = 2 ( 6 t + 11 ) 1 3 = 4 t + 7 .
Hence
m m = ( 4 t + 7 ) ( 4 t + 3 ) = 4 .
Thus first admissible children of consecutive C 1 parents advance in an arithmetic progression with step size + 4 .

5.2.2. C 2 Parents

Take consecutive C 2 parents n = 6 t + 1 and m = 6 ( t + 1 ) + 1 = 6 t + 7 . From the Inverse rule with k = 2 , their children are
m = 4 ( 6 t + 1 ) 1 3 = 8 t + 1 , m = 4 ( 6 t + 7 ) 1 3 = 8 t + 9 .
Hence
m m = ( 8 t + 9 ) ( 8 t + 1 ) = 8 .
Thus first admissible children of consecutive C 2 parents advance in an arithmetic progression with step size + 8 .
Lemma 41 
(Progressions of Consecutive Parents). First admissible children of consecutive parents form arithmetic progressions:
C 1 : ( 6 t + 5 ) ( 4 t + 3 ) , ( 6 t + 11 ) ( 4 t + 7 ) , Δ = + 4 ,
C 2 : ( 6 t + 1 ) ( 8 t + 1 ) , ( 6 t + 7 ) ( 8 t + 9 ) , Δ = + 8 .
Thus children of adjacent parents distribute evenly across odd integers with step size fixed by class.
Remark 5. 
The offset ladders of Section 5.1.1 and Section 5.1.2 describe how each parent generates children in a ladder determined relative to its own value of n. The arithmetic progressions, by contrast, describe how numerically consecutive parents distribute their children across the integers. Both perspectives are needed: ladders explain the local offsets tied to each parent, while progressions explain the global coverage across parents.
For C 1 parents, each has the form n = 6 t + 5 . With the minimal admissible exponent k = 1 , the child is
R ( 6 t + 5 , 1 ) = 2 ( 6 t + 5 ) 1 3 = 4 t + 3 .
Subtracting the parent gives the offset
Δ 1 ( 6 t + 5 ) = ( 4 t + 3 ) ( 6 t + 5 ) = 2 ( t + 1 ) .
Thus the offset depends linearly on t and grows in magnitude as t increases.
For C 2 parents, each has the form n = 6 t + 1 . With the minimal admissible exponent k = 2 , the child is
R ( 6 t + 1 , 2 ) = 4 ( 6 t + 1 ) 1 3 = 8 t + 1 ,
so the offset is
Δ 2 ( 6 t + 1 ) = ( 8 t + 1 ) ( 6 t + 1 ) = 2 t .
This offset also depends on t, and for t 1 it is strictly increasing.
Therefore, offsets are not fixed increments across all parents, but arithmetic expressions relative to each parent’s index t within its residue class. Each live class generates an infinite rail of children, and the offset size expands with t while preserving the admissibility rule (odd k for C 1 , even k for C 2 ).
The arithmetic progressions across consecutive parents are simply the global counterpart of the same rule. When t increases by + 1 (advancing to the next parent in the same class), the child also advances by a constant step ( + 4 for C 1 at k = 1 , + 8 for C 2 at k = 2 , and in general + 2 k + 1 ). This step is independent of t because the dependence on t is linear.
Thus the two descriptions are isomorphic: offsets show how children are positioned relative to a fixed parent, while progressions show how those positions line up across the sequence of parents. Both arise from the same affine relation R ( 6 t + ρ , k ) = 2 k + 1 t + c ρ , k , and together they capture the local and global arithmetic structure of the Inverse Collatz map.

5.2.3. Higher Lifts

Lemma 42 
(Quadrupling of Step Sizes at Higher Lifts). For each class, increasing the admissible exponent k by two applies two successive doublings, thereby quadrupling the progression step size of consecutive parents. Concretely:
C 1 : + 4 + 16 + 64 , C 2 : + 8 + 32 + 128 .
Proof. 
From the general offset formulas in Section 5.1.3, the difference between children of consecutive parents is proportional to 2 k . Replacing k by k + 2 multiplies this factor by 4, hence quadruples the step size between odd children. Therefore each successive two-lift scales the step size by a factor of four. □
At higher admissible k-lifts, step sizes scale as 2 k : each unit increase of k doubles the progression spacing, and in particular every two lifts quadruple it. A convenient way to display this is to show the two-lift subsequences and stagger the one-lift intermediates:
C 1 : + 4 + 16 + 64 C 2 : + 8 + 32 + 128
This pattern follows directly from the formulas of Section 5.1.3.

5.2.4. Visual Overlay

Corollary 9 
(Visual Overlay and Complete Coverage). Overlaying the progression ladders from consecutive parents shows that apparent gaps at lower admissible lifts are exactly filled by higher lifts. Each anchor sequence covers its congruence class without overlap, and the union across all admissible lifts exhausts the odd integers. Thus rail iterations across all lift levels ensure complete coverage of N odd .
Proof. 
By Lemma 41, consecutive parents generate fixed-step progressions, and by Lemma 42, higher admissible lifts scale these progressions by powers of four. The apparent omissions at a given scale correspond precisely to residue classes that are elements of progression of higher-lift ladders. Therefore the superposition of ladders fills all gaps systematically, partitioning the odd integers with no overlap. □

5.3. Anchor Ladders as the Basis of Coverage

All admissible structure originates from the two primitive anchors 1 C 2 and 5 C 1 . Each admissible lift
R ( 1 ; k ) = 2 k 1 3 , k even ,
R ( 5 ; k ) = 2 k · 5 1 3 , k odd ,
produces a new anchor point. Each such anchor initiates a ladder whose offsets and progressions are determined by its residue class and the parity of the admissible exponent k.
  • Interpretation. [Dyadic gaps as lifted offsets] Each admissible exponent k produces a dyadic slice
    S c , e = 2 k + 1 t + 2 k x 1 3 : t 0 , k = c + 2 e ,
    where ( c , x ) { ( 1 , 5 ) , ( 2 , 1 ) } specifies the class. The quantity
    Δ ( k ) : = 2 k + 1
    is the gap between successive values in the slice and is the exact offset created by the lifted exponent k.
Thus increasing k does not produce a new type of parent; it produces a new spacing among the same admissible residue class. The anchor value determines the base point
α ( k ) : = 2 k x 1 3 ,
while the dyadic step 2 k + 1 determines how far apart the lift-k parents of successive values lie.
In this sense, each higher lift corresponds to a wider offset lattice. Different values of k carve the odd integers into disjoint arithmetic progressions of increasing gap, and every such progression is exactly one dyadic slice. No slice overlaps another, and no odd integer is omitted.
Lemma 43 
(Arithmetic derivation of anchors by class lifts). For each anchor family a { 1 , 5 } with parent form n = 6 t + a , the Inverse operator
R ( n ; k ) = 2 k ( 6 t + a ) 1 3
generates an arithmetic progression at every admissible lift k (k odd for a = 5 , k even for a = 1 ). The constant term 2 k a 1 3 is the base residue of that progression and coincides with the anchor promoted at scale 2 k . Thus the starting anchors are derived arithmetically, and their descendants at higher k are exactly the ladder bases that fill sieve holes.
Proof. 
For a = 5 (class C 1 , odd k):
R ( 6 t + 5 ; 1 ) = 2 ( 6 t + 5 ) 1 3 = 4 t + 3 , R ( 6 t + 5 ; 3 ) = 8 ( 6 t + 5 ) 1 3 = 16 t + 13 , R ( 6 t + 5 ; 5 ) = 32 ( 6 t + 5 ) 1 3 = 64 t + 53 .
Each case has the form 2 k + 1 t + 2 k · 5 1 3 , with constants 3 , 13 , 53 , serving as the promoted anchors at scales 2 1 , 2 3 , 2 5 , .
For a = 1 (class C 2 , even k):
R ( 6 t + 1 ; 2 ) = 4 ( 6 t + 1 ) 1 3 = 8 t + 1 , R ( 6 t + 1 ; 4 ) = 16 ( 6 t + 1 ) 1 3 = 32 t + 5 , R ( 6 t + 1 ; 6 ) = 64 ( 6 t + 1 ) 1 3 = 128 t + 21 .
Each case has the form 2 k + 1 t + 2 k · 1 1 3 , with constants 1 , 5 , 21 , serving as the promoted anchors at scales 2 2 , 2 4 , 2 6 , .
In both families, the step size doubles with each increment of k, and the base constant aligns exactly with the residue class left uncovered at the prior dyadic sieve. Thus the arithmetic shows both that the anchors { 1 , 5 } are generated within the operator and that each higher k-level produces the ladder bases that fill the recursive sieve. □

5.4. Global Coverage by a Dyadic Sieve of Ladders

Proposition 6 
(Base-child ladders and the 4-adic sieve by class). Every admissible odd parent n is in exactly one of the two live classes
C 1 : n = 6 t + 5 or C 2 : n = 6 t + 1 ( t N ) .
Let m = 2 k n 1 3 be a Inverse child at lift k. Then:
(A)
First admissible child (base sieve slice).
C 1 ( first lift k = 1 ) : n = 6 t + 5 m = 2 ( 6 t + 5 ) 1 3 = 4 t + 3 , C 2 ( first lift k = 2 ) : n = 6 t + 1 m = 4 ( 6 t + 1 ) 1 3 = 8 t + 1 .
Thus the base children in C 1 are exactly m 3 ( mod 4 ) (gap 4), and the base children in C 2 are exactly m 1 ( mod 8 ) (gap 8). Equivalently, these are the odds with exactly one halving ( k = 1 ) and exactly two halvings ( k = 2 ) in 3 m + 1 , respectively.
(B)
Higher admissible lifts stay in class and obey m 4 m + 1 . Within a fixed class, raising the lift by + 2 sends each child to the next child by
m = 2 k + 2 n 1 3 = 4 2 k n 1 3 + 1 = 4 m + 1 .
Hence the children at lifts k , k + 2 , k + 4 , form a rail by the affine update m 4 m + 1 and remain in the same class ( C 1 for odd k, C 2 for even k).
(C)
Gap quadrupling across lifts. Writing the base-child progressions as functions of t,
C 1 , k = 1 : m 0 ( t ) = 4 t + 3 ( gap 4 ) , C 2 , k = 2 : m 0 ( t ) = 8 t + 1 ( gap 8 ) ,
the lift update m 4 m + 1 gives, for each e 0 ,
C 1 at k = 1 + 2 e : m e ( t ) = 4 e + 1 t + 10 · 4 e 1 3 , gap = 4 e + 1 , C 2 at k = 2 + 2 e : m e ( t ) = 8 · 4 e t + 4 e + 1 1 3 , gap = 8 · 4 e .
Thus each time the lift increases by + 2 , the gap between consecutive children (as t increases by 1) is multiplied by 4.
(D)
Next sieve slice is generated by 4 m + 1 . For C 1 the base children ( k = 1 ) are m 3 ( mod 4 ) . Applying m 4 m + 1 yields the next slice ( k = 3 ): m 13 ( mod 16 ) , again m 4 m + 1 gives the k = 5 slice m 53 ( mod 64 ) , and so on. For C 2 , the base children ( k = 2 ) are m 1 ( mod 8 ) ; then k = 4 gives m 5 ( mod 32 ) ; then k = 6 gives m 21 ( mod 128 ) ; etc. In each class, m 4 m + 1 generates the next sieve level and quadruples the modulus (the gap) each time.
Lemma 44 
(Sieve slice measure for v 2 ( 3 m + 1 ) on odds). Fix k 1 . Among all odd integers m, the proportion for which ν 2 ( 3 m + 1 ) = k is exactly 2 k .
Proof. 
Work modulo 2 k + 1 . Because 3 is invertible mod 2 k + 1 , the map m 3 m + 1 is a bijection on residue classes. The condition ν 2 ( 3 m + 1 ) k is 3 m + 1 0 ( mod 2 k ) , which holds for exactly 2 k of odd residues; the stricter condition ν 2 ( 3 m + 1 ) k + 1 cuts that by another factor 1 / 2 . Hence P ( ν 2 ( 3 m + 1 ) = k ) = 2 k on odds. □
Corollary 10 
(All-integers normalization). For k 1 , the proportion of all integers m with m odd and ν 2 ( 3 m + 1 ) = k is 2 ( k + 1 ) .
Proof. 
Half of all integers are odd; combine with Lemma 44. □

Transition: Canonical Reduction of Admissible Structure

The analysis above resolves the local admissible structure of the Inverse map: each live residue admits a unique minimal exponent k 0 , produces a base child in its own class, and extends to a full rail via the affine law R ( n ; k + 2 ) = 4 R ( n ; k ) + 1 shown by Lemma 40. These statements describe the local geometry of the Inverse tree but leave open the problem of identifying a canonical global parameter governing all rails simultaneously.
Such a parameter arises naturally by removing the dyadic component of the first admissible step. The resulting normal–state provides a global coordinate system on the live set O live in which each rail becomes a pure affine progression, independent of its parent. This reduction clarifies both the disjointness and completeness of the rail family and supplies the arithmetic infrastructure needed for the global coverage theorem below.
We introduce this normal–state framework next.

5.5. Normal–State Enumeration and the Pure Affine Skeleton

The affine decomposition shows that each admissible Inverse step
R ( n ; k ) = 2 k n 1 3
splits into a minimal admissible core and a sequence of 4 m + 1 lifts. In this section we remove all reversible dyadic structure and isolate the intrinsic arithmetic skeleton of the map. The resulting normal–state forms a canonical index on the live odds and reveals that Collatz dynamics reduce to a pure affine counting system generated entirely by a base of:
z 2 k 0 z + 1 .
No explicit use of the Collatz Forward function is required once this normal–state system is established.
Definition 26 
(Normal–State lattice). For any odd integer n, let k 0 ( n ) denote its minimal admissible exponent in the Inverse map. The normal–state lattice of n is defined by
z ( n ) = R ( n ; k 0 ( n ) ) 1 2 k 0 ( n ) = 2 k 0 ( n ) n 1 3 1 2 k 0 ( n ) .
This value z ( n ) is the unique base element of the affine rail generated by n.

5.5.1. Minimal Admissible Exponents

Let
O live : = { n N > 0 : n 1 , 5 ( mod 6 ) }
denote the live odd integers. For each n O live the Inverse step R ( n ; k ) is integral precisely when
2 k n 1 ( mod 3 ) .
Since 2 1 ( mod 3 ) and n is never 0 mod 3 in the live set, admissibility is determined by the parity of k:
k 0 ( n ) = 1 , n 5 ( mod 6 ) C 1 , 2 , n 1 ( mod 6 ) C 2 .
The base child of n is
R n ; k 0 ( n ) = 2 k 0 ( n ) n 1 3 .

5.5.2. Normal–State Extraction

The normal–state of n O live is defined by removing exactly the admissible dyadic factor used to produce R ( n ; k 0 ) :
z ( n ) : = R ( n ; k 0 ) 1 2 k 0 ( n ) .
Because admissibility guarantees R ( n ; k 0 ) 1 mod 2 k 0 ( n ) , this quantity is an integer for every live odd n.
Ordered by size,
1 , 5 , 7 , 11 , 13 , 17 , 19 , 23 , ,
the normal–state reproduces the natural lattice:
z ( 1 ) = 0 , z ( 5 ) = 1 , z ( 7 ) = 2 , z ( 11 ) = 3 , .
Examples.
(1) C1 case. For n = 5 ,
k 0 ( 5 ) = 1 , c 1 ( 5 ) = 2 · 5 1 3 = 3 , z ( 5 ) = 3 1 2 = 1 .
(2) C2 case. For n = 7 ,
k 0 ( 7 ) = 2 , c 1 ( 7 ) = 4 · 7 1 3 = 9 , z ( 7 ) = 9 1 4 = 2 .

5.5.3. Compatibility of Normal-State and Rail Children

Lemma 45 
(Parent z child equals direct child map). For every odd n O live , the base inverse child
m 0 ( n ) : = R ( n ; k 0 ( n ) ) = 2 k 0 ( n ) n 1 3
is determined uniquely by the normal–state coordinate z ( n ) via
m 0 ( n ) = 4 z ( n ) + 1 , n C 2 , 2 z ( n ) + 1 , n C 1 .
Consequently, the composition n z ( n ) m 0 ( n ) coincides with the direct inverse map n R ( n ; k 0 ( n ) ) .
Proof. 
By definition,
O live = { n 1 , 5 ( mod 6 ) } = C 2 C 1 ,
where C 2 = { 6 t + 1 : t 0 } and C 1 = { 6 t + 5 : t 0 } . The normal–state coordinate z ( n ) enumerates these two progressions by assigning even indices to C 2 and odd indices to C 1 . Thus
n = 6 t + 1 , z ( n ) = 2 t , n C 2 , 6 t + 5 , z ( n ) = 2 t + 1 , n C 1 .
Equivalently,
n = 3 z ( n ) + 1 , n C 2 , 3 z ( n ) + 2 , n C 1 .
If n C 2 , then k 0 ( n ) = 2 and
m 0 ( n ) = 4 n 1 3 = 4 ( 3 z ( n ) + 1 ) 1 3 = 4 z ( n ) + 1 .
If n C 1 , then k 0 ( n ) = 1 and
m 0 ( n ) = 2 n 1 3 = 2 ( 3 z ( n ) + 2 ) 1 3 = 2 z ( n ) + 1 .
In both cases the resulting expression for m 0 ( n ) agrees exactly with the direct inverse formula R ( n ; k 0 ( n ) ) . □

5.5.4. Normal–State Law and the First Affine Step

Theorem 10 
(Affine rail law and disjoint partition of the odd integers). Let n O live and let k 0 ( n ) denote its minimal admissible exponent. Define the base child
m 0 ( n ) : = R n ; k 0 ( n ) = 2 k 0 ( n ) n 1 3 .
For each e 0 define the e–th admissible lift above n by
m e ( n ) : = R n ; k 0 ( n ) + 2 e .
Then:
1. 
Affine recursion and closed form. The sequence { m e ( n ) } e 0 satisfies
m e + 1 ( n ) = 4 m e ( n ) + 1 ,
and hence admits the closed form
m e ( n ) = 4 e m 0 ( n ) + 4 e 1 3 .
2. 
Dependence only on the normal–state coordinate. Writing the base child in normal–state form
m 0 ( n ) = 4 z ( n ) + 1 , n C 2 , 2 z ( n ) + 1 , n C 1 ,
we have
m e ( n ) = 4 e f c ( n ) z ( n ) + 1 + 4 e 1 3 , f c ( n ) = 4 , n C 2 , 2 , n C 1 ,
so the entire admissible chain above n is determined by the pair z ( n ) and f c ( n ) i.e. by the normal–state coordinate and class.
3. 
Disjointness of rails. If n 1 , n 2 O live with n 1 n 2 , then the corresponding affine rails
L n i : = { m e ( n i ) : e 0 } ( i = 1 , 2 )
are disjoint:
L n 1 L n 2 = .
4. 
Partition of the odd integers. Every odd integer m belongs to exactly one such rail. Equivalently,
N odd = n O live L n , L n 1 L n 2 = ( n 1 n 2 ) .
Proof. 
(1) Since k 0 ( n ) + 2 ( e + 1 ) = k 0 ( n ) + 2 e + 2 , we have
m e + 1 ( n ) = R n ; k 0 ( n ) + 2 e + 2 = 2 k 0 ( n ) + 2 e + 2 n 1 3 .
Also,
4 m e ( n ) + 1 = 4 · 2 k 0 ( n ) + 2 e n 1 3 + 1 = 2 k 0 ( n ) + 2 e + 2 n 4 3 + 1 = 2 k 0 ( n ) + 2 e + 2 n 1 3 = m e + 1 ( n ) ,
so m e + 1 ( n ) = 4 m e ( n ) + 1 . Solving the recursion yields
m e ( n ) = 4 e c 0 ( n ) + j = 0 e 1 4 j = 4 e m 0 ( n ) + 4 e 1 3 .
(2) This is immediate from the classwise normal–state formulas for m 0 ( n ) proved in Lemma 45, substituting into the closed form in (1).
(3) Suppose m e 1 ( n 1 ) = m e 2 ( n 2 ) for some e 1 , e 2 0 . Then, by definition,
2 k 0 ( n 1 ) + 2 e 1 n 1 1 3 = 2 k 0 ( n 2 ) + 2 e 2 n 2 1 3 ,
hence
2 k 0 ( n 1 ) + 2 e 1 n 1 = 2 k 0 ( n 2 ) + 2 e 2 n 2 .
Both sides are equal powers of 2 times odd integers; by uniqueness of the 2–adic valuation, the exponents agree and the odd parts agree, giving n 1 = n 2 . Thus distinct n yield disjoint rails.
(4) Let m be odd. Write 3 m + 1 = 2 k n where n is odd and k = ν 2 ( 3 m + 1 ) . Then n 0 ( mod 3 ) , hence n O live , and
m = R ( n ; k ) .
Writing k = k 0 ( n ) + 2 e for some e 0 places m on L n . Uniqueness follows from (3). □
Proposition 7 
(Reduction to normal–state and affine generation of all admissible lifts). Let n O live , and let k 0 ( n ) denote its minimal admissible exponent. Define the base child m 0 ( n ) : = R ( n ; k 0 ( n ) ) and the admissible lifts
m e ( n ) : = R n ; k 0 ( n ) + 2 e ( e 0 ) .
Then the entire admissible inverse structure above n is generated in the z–coordinate by the maps f 1 , f 2 and L e as follows:
1. 
Classwise reduction n z ( n ) .
z ( n ) = n 1 3 , n C 2 ( n 1 ( mod 6 ) ) , n 2 3 , n C 1 ( n 5 ( mod 6 ) ) .
2. 
Base child from normal–state: z ( n ) m 0 ( n ) . With f 1 ( z ) = 2 z + 1 and f 2 ( z ) = 4 z + 1 ,
m 0 ( n ) = f 2 z ( n ) , n C 2 , f 1 z ( n ) , n C 1 .
3. 
All admissible lifts from the rail operator: m 0 ( n ) m e ( n ) . For each e 0 ,
m e ( n ) = 4 e m 0 ( n ) + 4 e 1 3 .
Equivalently, in the z–coordinate,
z m e ( n ) = L e f c ( z ( n ) ) , c = 2 , n C 2 , 1 , n C 1 ,
where L e ( z ) = 4 e z + 2 3 ( 4 e 1 ) .
Proof. 
(1) Since O live = { 6 t + 1 : t 0 } { 6 t + 5 : t 0 } and z enumerates 6 t + 1 at even sites and 6 t + 5 at odd sites, we have z = 2 t on C 2 and z = 2 t + 1 on C 1 . Solving n = 6 t + 1 and n = 6 t + 5 for t yields the stated formulas for z ( n ) .
(2) This is Lemma 45 written in generator form: m 0 ( n ) = 4 z ( n ) + 1 = f 2 ( z ( n ) ) on C 2 and m 0 ( n ) = 2 z ( n ) + 1 = f 1 ( z ( n ) ) on C 1 .
(3) By definition,
m e ( n ) = R n ; k 0 ( n ) + 2 e = 2 k 0 ( n ) + 2 e n 1 3 .
Comparing with m 0 ( n ) = 2 k 0 ( n ) n 1 3 gives the standard lift identity m e + 1 ( n ) = 4 m e ( n ) + 1 , hence the closed form
m e ( n ) = 4 e m 0 ( n ) + 4 e 1 3 .
Substituting m 0 ( n ) = f c ( z ( n ) ) and rewriting in normal–state coordinates yields z ( m e ( n ) ) = L e ( f c ( z ( n ) ) ) with L e ( z ) = 4 e z + 2 3 ( 4 e 1 ) . □

5.5.5. Affine rails and Odd Coverage

For each n O live , the affine rail indexed by z ( n ) is
L n = 4 e R ( n ; k 0 ) + 4 e 1 3 : e 0 .
Injectivity of the affine form
R ( n ; k ) = 2 k 3 n 1 3
ensures that rails are disjoint. Every odd integer m has a unique representation m = R ( n ; k ) for some live n and unique admissible k, and writing k = k 0 ( n ) + 2 e places m on exactly one rail:
n O live L n = N odd .
Combining this with the dyadic decomposition S c , e yields full coverage of N 1 .
Table 3.
z n class operator z-child base child R ( n ; k 0 )
0 1 C2 4 z + 1 1 1
1 5 C1 2 z + 1 3 3
2 7 C2 4 z + 1 9 9
3 11 C1 2 z + 1 7 7
4 13 C2 4 z + 1 17 17
5 17 C1 2 z + 1 11 11
6 19 C2 4 z + 1 25 25
7 23 C1 2 z + 1 15 15
8 25 C2 4 z + 1 33 33
9 29 C1 2 z + 1 19 19
10 31 C2 4 z + 1 41 41
11 35 C1 2 z + 1 23 23
12 37 C2 4 z + 1 49 49
13 41 C1 2 z + 1 27 27
14 43 C2 4 z + 1 57 57
15 47 C1 2 z + 1 31 31
16 49 C2 4 z + 1 65 65
17 53 C1 2 z + 1 35 35
18 55 C2 4 z + 1 73 73
19 59 C1 2 z + 1 39 39
20 61 C2 4 z + 1 81 81
21 65 C1 2 z + 1 43 43
22 67 C2 4 z + 1 89 89
23 71 C1 2 z + 1 47 47
24 73 C2 4 z + 1 97 97
Table 3 First 25 live odd integers ( n 1 , 5 ( mod 6 ) ) with their z–coordinates, classes, affine generator, and base admissible child. The table illustrates the fundamental identity
R ( n ; k 0 ) = n f 1 , 2 ( z ( n ) )
i.e. the first admissible Inverse child of n is exactly the live odd whose index equals the affine z–map f 1 ( z ) = 2 z + 1 (for C1) or f 2 ( z ) = 4 z + 1 (for C2). Equivalently, the first admissible inverse child may be written in the unified form
m 0 = 2 k 0 ( n ) z ( n ) + 1 ,
where k 0 ( n ) = 1 for C 1 and k 0 ( n ) = 2 for C 2 .
Remark 6 
(Why C 0 is terminal in the z–Lattice). The z–lattice is a bijection from the live lattice
L = { n N odd : n 1 , 5 ( mod 6 ) }
onto N 0 , assigning each admissible odd m its global normal–state coordinate z ( m ) . No element of C 0 = { n 3 ( mod 6 ) } appears in L , and therefore no C 0 value admits a z–coordinate. This is not merely a definitional omission: it is an arithmetic obstruction.
Indeed, if n 3 ( mod 6 ) , then
2 k n 1 1 ( mod 3 ) ,
so ( 2 k n 1 ) / 3 is never an integer for any k 0 . Thus no C 0 value can serve as a parent in the admissible Inverse map R ( n ; k ) = 2 k n 1 3 . Consequently, C 0 values are exactly those odd integers that lie outside the normal–state coordinate system and therefore admit no further Inverse continuation. In this sense, the normal–state lattice is the structural backbone of the global Inverse tree, and C 0 represents its natural boundary.
Proposition 8 
(The Unique Self-Stable Odd Origin). Among all odd integers, the value 1 is the only odd integer whose admissible Inverse image under R ( n ; k ) has the same normal–state lattice as its parent. Equivalently, 1 is the unique solution of
z ( R ( 1 ; k 0 ( 1 ) ) ) = z ( 1 ) ,
and every admissible Inverse step applied to any n > 1 produces a strict increase ( C 2 ) or decrease ( C 1 ) in normal–state coordinate.
Proof. 
For an odd integer n, write its admissible base child as
R ( n ; k 0 ( n ) ) = 2 k 0 ( n ) n 1 3 .
Normal–State normalization removes the affine increment k 0 ( n ) from the lifted representation; hence
z R ( n ; k 0 ( n ) ) = 2 k 0 ( n ) n 1 3 · 2 k 0 ( n ) = n 2 k 0 ( n ) 1 3 · 2 k 0 ( n ) .
If n = 1 , then k 0 ( 1 ) = 2 and
R ( 1 ; 2 ) = 1 , z ( 1 ) = 0 ,
so 1 is fixed under its admissible Inverse step and its normal–state coordinate remains 0.
Suppose n > 1 . If z ( R ( n ; k 0 ( n ) ) ) = z ( n ) , then by the definition of z we would have
R ( n ; k 0 ( n ) ) = n ,
hence
2 k 0 ( n ) n 1 3 = n ( 2 k 0 ( n ) 3 ) n = 1 ,
which is impossible for any n > 1 . Thus the equality z ( R ( n ; k 0 ( n ) ) ) = z ( n ) is impossible for odd n > 1 . □
Corollary 11 
(Uniqueness of the Global Odd Cycle). The odd Inverse Collatz dynamics admit exactly one cycle, the trivial cycle { 1 } . Every other odd integer ascends strictly from normal–state coordinate and therefore cannot return to a previous affine or normal–state position.

5.5.6. Affine–Dyadic Equivalence

Lemma 46 
(Affine–Dyadic Correspondence). For each admissible inverse exponent k, the first admissible inverse child of an odd integer n is
m 0 ( n ) = R ( n ; k ) = 2 k n 1 3 .
Moreover, the set of odd integers m satisfying k m = k has natural density 2 k ; that is,
lim N 1 N # { m N : k m = k } = 2 k .
Consequently, each affine inverse generator corresponds to a dyadic slice whose relative size is exactly the reciprocal of its scale.
Theorem 11 
(Affine–Dyadic Equivalence). By Lemma 46, The admissible inverse generators R ( · ; k ) partition the odd integers into disjoint dyadic slices of natural density 2 k .
Corollary 12 
(Coverage via Affine Slicing).
k 1 2 k = 1 .
Hence the admissible affine inverse generators form a disjoint partition of N odd and cover each odd integer exactly once.
Theorem 12 
(Global Arithmetic Coverage by Rails). Let R ( n ; k ) = 2 k n 1 3 be the Inverse map with admissible parity per class. Then the following hold within Section 5:
1. 
Base slices and fixed gaps. First admissible children are exactly
C 1 : m 3 ( mod 4 ) ( k = 1 , gap 4 ) , C 2 : m 1 ( mod 8 ) ( k = 2 , gap 8 ) ,
and children of consecutive parents form arithmetic progressions with those gaps (Prop. 6, Lem. 41).
2. 
4-adic lift within rails. Raising the lift by + 2 sends m 4 m + 1 , stays in the same class, and multiplies the progression gap of sequential, class equivocal n, by 4 (Lem. 42, 40).
3. 
Overlay gives complete coverage. Superposing the ladders across all admissible lifts fills the apparent gaps of the base slices; within each class, the union over k exhausts its congruence classes with no overlap (Cor. 9).
4. 
Anchor generation of disjoint rails. All affine rails arise from the two primitive anchor parents 1 C 2 and 5 C 1 via admissible inverse lifts. By the normal–state parametrization, each live odd n 1 , 5 ( mod 6 ) determines a unique normal–state coordinate z ( n ) and hence a unique affine rail
L n = 4 e R ( n ; k 0 ( n ) ) + 4 e 1 3 : e 0 .
The generators f 1 ( z ) = 2 z + 1 and f 2 ( z ) = 4 z + 1 propagate the anchor states z ( 1 ) = 0 and z ( 5 ) = 1 through the z–lattice, producing all rails without overlap. Disjointness follows from the uniqueness of the normal–state coordinate and the injectivity of the affine form, not from pairwise offset considerations. (Thm. 10)
5. 
Exact dyadic slice measures. Among odd m, the slice with ν 2 ( 3 m + 1 ) = k , S c , e measures 2 k ; among all integers it is 2 ( k + 1 ) (Lem. 44, Cor. 10, 12).
Consequently, the odd integers are covered disjointly by the class-preserving affine offset gap progressions generated from a base of all rails, across all admissible lifts, with gaps and densities exactly as stated in (1)–(5).

5.6. Dyadic Sieve Index (Class–Forced Admissibility)

While Theorem 12 establishes global coverage abstractly, the remaining analysis makes this coverage explicit by describing the concrete arithmetic realization of each affine slice, rail, and lift.
Definition 27 
(Dyadic Sieve Index). Let c { 1 , 2 } encode the class modulo 3 and x { 5 , 1 } encode the class modulo 6:
c = 1 , x = 5 ( class C 1 ) ; c = 2 , x = 1 ( class C 2 ) .
For each lift index e 0 , the admissible exponent is k = c + 2 e (odd k for C 1 , even k for C 2 ), and a single Inverse step from n = 6 t + x produces
m = R ( 6 t + x ; k ) = 2 c + 2 e ( 6 t + x ) 1 3 = 2 k + 1 gap t + 2 k x 1 3 anchor .
The dyadic slice weight (among odd m) for fixed k is 2 k .
Table 4. Dyadic Sieve Index from the unified Inverse step m = 2 c + 2 e ( 6 t + x ) 1 / 3 , with k = c + 2 e .
Table 4. Dyadic Sieve Index from the unified Inverse step m = 2 c + 2 e ( 6 t + x ) 1 / 3 , with k = c + 2 e .
k Class x Gap = 2 k Anchor = 2 k x 1 3 m = gap · t + anchor
1 C 1 5 4 3 4 t + 3
2 C 2 1 8 1 8 t + 1
3 C 1 5 16 13 16 t + 13
4 C 2 1 32 5 32 t + 5
5 C 1 5 64 53 64 t + 53
6 C 2 1 128 21 128 t + 21
7 C 1 5 256 213 256 t + 213
8 C 2 1 512 85 512 t + 85
9 C 1 5 1024 853 1024 t + 853
10 C 2 1 2048 341 2048 t + 341
11 C 1 5 4096 3413 4096 t + 3413
12 C 2 1 8192 1365 8192 t + 1365
13 C 1 5 16384 13653 16384 t + 13653
14 C 2 1 32768 5461 32768 t + 5461
15 C 1 5 65536 54613 65536 t + 54613
16 C 2 1 131072 21845 131072 t + 21845
17 C 1 5 262144 218453 262144 t + 218453
18 C 2 1 524288 87381 524288 t + 87381
19 C 1 5 1048576 873813 1048576 t + 873813
20 C 2 1 2097152 349525 2097152 t + 349525
21 C 1 5 4194304 3495253 4194304 t + 3495253
22 C 2 1 8388608 1398101 8388608 t + 1398101
23 C 1 5 16777216 13981013 16777216 t + 13981013
24 C 2 1 33554432 5592405 33554432 t + 5592405
25 C 1 5 67108864 55924053 67108864 t + 55924053
Dyadic slice weight for fixed k: 2 k (among odd m).
Theorem 13 
(Dyadic Sieve Decomposition). Let C 1 = { n 5 ( mod 6 ) } and C 2 = { n 1 ( mod 6 ) } . Encode the class by
( c , x ) = ( 1 , 5 ) for C 1 , ( c , x ) = ( 2 , 1 ) for C 2 .
For each lift index e 0 , define k : = c + 2 e (so k has the admissible parity for the class). The fixed-k static sieve slice is
S c , e : = m = 2 c + 2 e ( 6 t + x ) 1 3 : t N 0 = 2 k + 1 t + 2 k x 1 3 : t 0 .
Then
N odd = c { 1 , 2 } e 0 S c , e ,
i.e. as e = 0 , 1 , 2 , increases (equivalently k = c + 2 e ), the union of these arithmetic progressions covers every odd integer exactly once.
Proof. 
Existence. Take any odd m. Let k be the highest power of 2 dividing 3 m + 1 , i.e. 2 k ( 3 m + 1 ) . Then
3 m + 1 2 k
is even and has a unique residue x { 1 , 5 } modulo 6 (parity forces x odd, and x m ( mod 3 ) ). Set c = 2 if x = 1 and c = 1 if x = 5 . Since k c ( mod 2 ) , there is e 0 with k = c + 2 e . Define
t : = 1 6 3 m + 1 2 k x N 0 ,
and solve for m to obtain
m = 2 k + 1 t + 2 k x 1 3 S c , e .
Uniqueness. The factor k is uniquely determined by the largest power of 2 dividing 3 m + 1 , which fixes x, then c, then e = ( k c ) / 2 , and finally t. Hence m belongs to exactly one S c , e . □
Remark 7 
(Anchors and gaps). Each S c , e is an arithmetic progression with gap 2 k + 1 and anchor 2 k x 1 / 3 , where k = c + 2 e . The minimal slices ( e = 0 ) are
C 1 : k = 1 m = 4 t + 3 , C 2 : k = 2 m = 8 t + 1 .
Corollary 13 
(Dyadic slice weight). For fixed k, the proportion of odd integers in S c , e is 2 k . These dyadic slices form a disjoint partition of the odd integers, and the weights { 2 k } k 1 sum exactly to 1.

5.6.1. Middle-Even Gates and mod-18 Progression

Lemma 47 
(Gate equivalence at the middle even). Let n = T ( m ) be the next odd. Then
g ( m ) 2 n ( mod 18 ) { 4 , 10 , 16 } ,
with the class correspondence
g ( m ) 10 n C 0 , g ( m ) 4 n C 2 , g ( m ) 16 n C 1 .
In particular E ( m ) 4 ( mod 6 ) for every odd m, and over one mod-18 odd cycle the three gate residues { 4 , 10 , 16 } occur with equal frequency 1 / 3 .
Proof. 
Since e ˜ ( m ) = 2 n , reduce 2 n modulo 18 and use the mod-6 classes of n; this is the same gate rule as Prop. 1. The 1 / 3 split is the equidistribution of base-child classes from Section 3. □
Proposition 9 
(Base middle-even progressions in mod-18). Using the minimally-admissible children from Prop. 6:
C 1 : n = 6 t + 5   k = 1   m = 4 t + 3 ,
e ˜ = 3 m + 1 = 12 t + 10 e ˜ 10 , 4 , 16 ( mod 18 ) as t 0 , 1 , 2 ( mod 3 ) ;
C 2 : n = 6 t + 1   k = 2   m = 8 t + 1 ,
e ˜ = 3 m + 1 = 24 t + 4 e ˜ 4 , 10 , 16 ( mod 18 ) as t 0 , 1 , 2 ( mod 3 ) .
Thus, as t increases by 1, the gate residue rotates deterministically in mod 18 by
C 1 : 10 4 16 10 , C 2 : 4 10 16 4 ,
and the union of middle evens across the two classes is exactly the gate set { 4 , 10 , 16 } ( mod 18 ) —i.e. precisely 1 / 3 of all even residues mod 18.
Lemma 48 
(Higher lifts act by × 4 on middle evens). If m = 4 m + 1 is the lift- k + 2 child of m (Prop. 6, Lem. 42), then
e ˜ ( m ) = 3 ( 4 m + 1 ) + 1 = 4 e ˜ ( m ) ,
hence g ( m ) 4 g ( m ) ( mod 18 ) , rotating the gate residues
4 16 , 10 4 , 16 10 .
Corollary 14 
(Even-gate sieve ≡ dyadic sieve, in mod-18). The partition of odds by k = ν 2 ( 3 m + 1 ) (§4) corresponds, under m e ˜ ( m ) , to class-preserving middle-even rails whose residues cycle within { 4 , 10 , 16 } ( mod 18 ) and whose strides scale by the k k + 2 lift (Lemma 48). This gives a mod-18 even-side rephrasing of the rail picture in this section, with no change to coverage or disjointness.

5.7. Global Consequences of Coverage

Theorem 14 
(Dyadic Slicing Yields Global Coverage). Let C 1 = { n 5 ( mod 6 ) } and C 2 = { n 1 ( mod 6 ) } , and encode the class by
( c , x ) = ( 1 , 5 ) for C 1 , ( c , x ) = ( 2 , 1 ) for C 2 .
For each lift index e 0 set k : = c + 2 e and define the dyadic slice
S c , e : = m = 2 c + 2 e ( 6 t + x ) 1 3 : e N 0
Then the family { S c , e } c { 1 , 2 } , e 0 is a disjoint partition of the odd integers:
N odd = c { 1 , 2 } e 0 S c , e .
Equivalently, every odd m admits a unique representation
m = 2 c + 2 e 6 t + 2 c + 2 e x 1 3 , ( c , x ) { ( 1 , 5 ) , ( 2 , 1 ) } , k = c + 2 e , e 0 , t 0 .
Proof. 
Existence. For odd m, let k : = v 2 ( 3 m + 1 ) . Then ( 3 m + 1 ) / 2 k is odd and has a unique residue x { 1 , 5 } modulo 6. Set c = 2 if x = 1 and c = 1 if x = 5 ; then k c ( mod 2 ) , so k = c + 2 e for a unique e 0 . Define
t : = 1 6 3 m + 1 2 k x N 0 .
Solving for m yields m = 2 c + 2 e 6 t + 2 c + 2 e x 1 3 S c , e .
Uniqueness (disjointness). The factor k = v 2 ( 3 m + 1 ) is unique, which fixes x { 1 , 5 } , then c, then e = ( k c ) / 2 , and finally t by the displayed equation. Hence m lies in exactly one S c , e . □
Corollary 15 
(Equivalence of Dyadic Slices and z–Rails). Let S c , e be the dyadic slice defined in Theorem 14, and let
m e = 4 e m 0 + 4 e 1 3 , m 0 = 2 c ( 6 t + x ) 1 3 , ( c , x ) { ( 1 , 5 ) , ( 2 , 1 ) } .
Then for every choice of ( c , e , t ) ,
m e = 2 c + 2 e ( 6 t + x ) 1 3 S c , e ,
and conversely every element of S c , e arises uniquely in this way.
Hence the affine rails generated by m 4 m + 1 coincide exactly with the dyadic slices arising from the 2–adic valuation of 3 m + 1 .
Lemma 49 
(Affine injectivity). Let f 4 ( m ) = 4 m + 1 and f 2 ( m ) = 2 m + 1 be the affine maps on N . Then both f 4 and f 2 are injective: no two distinct integers can produce the same output under either map. Consequently, along any rail generated by iterates of f 4 (and, where used, f 2 ), each integer occurs at most once.
Proof. 
Suppose f 4 ( a ) = f 4 ( b ) for some a , b N . Then
4 a + 1 = 4 b + 1 .
Subtracting 1 from both sides gives 4 a = 4 b , hence
4 ( a b ) = 0 .
Since 4 0 in N , it follows that a b = 0 and therefore a = b . Thus f 4 is injective.
The same argument applies to f 2 ( m ) = 2 m + 1 . If f 2 ( a ) = f 2 ( b ) , then 2 a + 1 = 2 b + 1 , so 2 a = 2 b and 2 ( a b ) = 0 , whence a = b . Thus f 2 is also injective.
Because each iterate of f 4 (and f 2 ) is a composition of injective maps, every finite iteration remains injective. Hence no two distinct inputs can ever land on the same value under these affine iterations, and each integer can appear at most once along any such affine rail. □

6. Global Coverage from Periodic Overlap

This section proves global coverage (surjectivity of the inverse construction) from the periodic overlap law of admissible k–prefixes along the refinement tower
M j : = 2 · 3 j + 1 .

6.1. Refinement States and Admissible Prefixes

For each j 0 define the refinement modulus
M j : = 2 · 3 j + 1 .
Let W j denote the set of admissible j–words
k = ( k 0 , , k j 1 )
in the inverse odd–to–odd construction (with the usual stepwise divisibility/admissibility constraints).
For an odd integer n define its level-j state
σ j ( n ) : = n ( mod M j ) .
Let L j Z / M j Z denote the set of live residue classes at level M j (the complement of the dead class(es) described in the class/phase analysis).

6.2. Two Structural Inputs

Proposition 10 
(Finite–level coverage at every refinement modulus). For every j 0 and every odd integer n > 1 ,
σ j ( n ) L j .
Equivalently, every odd n > 1 is represented by a live residue class at every refinement level M j .
Proposition 11 
(Overlap of admissible k–prefixes across refinement). For each j 0 there exists a canonical prefix selection map
Φ j : L j W j ,
such that:
1. 
(Residue determinism) If n is odd and σ j ( n ) L j , then the word Φ j ( σ j ( n ) ) is admissible from n as a j–step inverse prefix.
2. 
(Overlap) For every r L j + 1 ,
Φ j + 1 ( r ) | j = Φ j ( r mod M j ) ,
where k | j denotes truncation of a word to its first j letters.

6.3. Coherent Infinite Addresses

Lemma 50 
(Existence and uniqueness of a coherent infinite k–address). Fix an odd integer n > 1 and define r j : = σ j ( n ) L j for each j 0 . Then there exists a unique infinite word
k ( n ) = ( k 0 , k 1 , k 2 , )
such that for every j 0 the length-j prefix of k ( n ) equals Φ j ( r j ) :
( k 0 , , k j 1 ) = Φ j ( r j ) .
Proof. 
For each j 0 define the length-j prefix
k ( j ) : = Φ j ( r j ) W j .
By Proposition 11 (Overlap),
k ( j + 1 ) | j = Φ j + 1 ( r j + 1 ) | j = Φ j ( r j ) = k ( j ) .
Hence the family { k ( j ) } j 0 is compatible under truncation. There is therefore a unique infinite word k ( n ) whose truncation to length j equals k ( j ) for every j. □

6.4. Surjectivity (Global Coverage)

Theorem 15 
(Global coverage / surjectivity of the inverse construction). Every odd integer n > 1 is realized by the inverse construction. Equivalently, the inverse rail system covers N odd { 1 } : each odd n > 1 admits a coherent admissible infinite k–address k ( n ) , and thus lies on a rail in the global partition.
Proof. 
Fix odd n > 1 . By Proposition 10, r j = σ j ( n ) L j for all j 0 , so Φ j ( r j ) is defined for all j. By Lemma 50, there is a coherent infinite word k ( n ) whose every finite prefix is an admissible inverse prefix from n.
Interpreting each prefix ( k 0 , , k j 1 ) as a j–step inverse address produces a consistent inverse address system for n across all refinement levels. Therefore n occurs in the image of the inverse construction, i.e. the rails cover n. □
Theorem 16 
(Rail–slice coincidence (global surjectivity)). Fix a live class c { 1 , 2 } and e 0 , and set
k = c + 2 e .
Let the dyadic slice be
S c , e = { n N odd : ν 2 ( 3 m + 1 ) = k } .
Define the admissible odd set
M c , e = { m N odd : 2 k m 1 ( mod 3 ) } .
For each m M c , e define the affine inverse map
R k ( m ) = 2 k m 1 3 ,
and define the rail at height e (in class c) by
R c , e ( m ) = { R k ( m ) } .
Then the map
R k : M c , e S c , e
is a bijection. Equivalently, every n S c , e admits a unique representation
3 m + 1 = 2 k n , m M c , e ,
so the rails at fixed ( c , e ) coincide with the slice S c , e .
Proof. 
Surjectivity. Let n S c , e . By definition ν 2 ( 3 m + 1 ) = k , hence
3 m + 1 = 2 k n
for a unique odd integer m. Necessarily 2 k m 1 ( mod 3 ) , so m M c , e , and rearranging gives n = ( 2 k m 1 ) / 3 = R k ( m ) . Thus n lies in the image of R k .
Injectivity. If R k ( m ) = R k ( m ) , then ( 2 k m 1 ) / 3 = ( 2 k m 1 ) / 3 , hence m = m . Therefore R k is injective.
This proves that R k is a bijection from M c , e onto S c , e . □

6.5. Forward Transitions as Exact Inverses of the Inverse Ancestry

The Inverse ancestry of any odd integer n is fully determined by its minimal admissible exponent k 0 ( n ) = ν 2 ( 3 m + 1 ) . Its first admissible Inverse child is
m 0 : = R ( n ; k 0 ( n ) ) = 2 k 0 ( n ) n 1 3 .
Higher lifts of this child form the rail
m e : = 4 e m 0 + 4 e 1 3 , e 0 .
Lemma 51 
(Rail identity). For every e 0 , the rail satisfies
3 m e + 1 = 2 k 0 ( n ) + 2 e n .
Proof. 
By definition of m 0 ,
3 m 0 + 1 = 2 k 0 ( n ) n .
Multiplying both sides by 4 e = 2 2 e gives
3 ( 4 e m 0 ) + 4 e = 2 k 0 ( n ) + 2 e n .
Adding and subtracting 1,
3 4 e m 0 + 4 e 1 3 + 1 = 2 k 0 ( n ) + 2 e n ,
which is exactly the definition of m e . □
Corollary 16 
(Forward inversion of the rail). By Theorem 5, we find every element m e on the rail satisfies
T ( m e ) = 3 m e + 1 2 ν 2 ( 3 m e + 1 ) = 2 k 0 ( n ) + 2 e n 2 k 0 ( n ) + 2 e = n .
Thus the Forward odd-to-odd Collatz step is the exact inverse of the rail ancestry.
Lemma 52 
(Forward collapse of a rail). Let n be an odd integer, and let k 0 1 be the minimal admissible exponent such that 2 k 0 n 1 ( mod 3 ) . Define
m e = R ( n ; k 0 + 2 e ) = 2 k 0 + 2 e n 1 3 , e 0 ,
so that { m e } e 0 is the rail generated by the admissible lifts of n. Then for every e 0 one has
T ( m e ) = n .
Proof. 
Fix e 0 and set
m e = 2 k 0 + 2 e n 1 3 .
Then
3 m e + 1 = 3 2 k 0 + 2 e n 1 3 + 1 = 2 k 0 + 2 e n .
Since n is odd, the 2-adic valuation of 3 m e + 1 is
ν 2 ( 3 m e + 1 ) = ν 2 ( 2 k 0 + 2 e n ) = k 0 + 2 e .
By definition of the odd Collatz map,
T ( m e ) = 3 m e + 1 2 ν 2 ( 3 m e + 1 ) = 2 k 0 + 2 e n 2 k 0 + 2 e = n ,
as claimed. □
Corollary 17 
(Forward inverse of the admissible rail). In the setting of Lemma 52, the Forward odd Collatz map T is the exact algebraic inverse of the admissible rail generated by n: every Inverse lift m e = R ( n ; k 0 + 2 e ) collapses in one odd step to n, and no other odd child is attained from any m e . Consequently, along each rail the Forward dynamics contract the entire ancestry to the unique child n.
Lemma 53 
(No rootless rails). Let R be any rail with base m 0 1 . Then R has a unique parent rail R in the Inverse Collatz dynamics: there exists an odd integer n and an admissible minimal exponent k 0 1 such that
m 0 = 2 k 0 n 1 3 , R = { R ( n ; k 0 + 2 e ) : e 0 } ,
and the base of R is m 0 = R ( n ; k 0 ) m 0 . Moreover, the rail of 1 is the only rail without a distinct parent.
Proof. 
By construction of the rails, every rail R is generated by admissible lifts from some odd child n; its base m 0 is the minimal admissible parent,
m 0 = R ( n ; k 0 ) = 2 k 0 n 1 3 ,
with k 0 the least exponent such that 2 k n 1 ( mod 3 ) . The admissibility conditions modulo 18 ensure that m 0 lies in one of the live classes C 1 or C 2 , so n is uniquely determined by the local residue structure in Section 3.
Define the parent rail R to be the rail generated by n and k 0 ,
R = R ( n ; k 0 + 2 e ) : e 0 ,
whose base is m 0 = R ( n ; k 0 ) . Disjointness of rails and uniqueness of affine ancestry ensure that R is well-defined and distinct from R whenever m 0 1 : if m 0 = m 0 with m 0 1 , this would force a nontrivial cycle in the affine rail structure, contradicting the disjointness and no-cycle results established by Theorem 2.
When m 0 = 1 , the only solution of 3 m + 1 = 2 k m is m = 1 , so the rail of 1 is self-ancestral and admits no distinct parent rail. Thus every rail other than the rail of 1 has a unique parent rail, and the rail of 1 is the only rail without a distinct parent. □
Theorem 17 
(Well-founded rail hierarchy rooted at 1). Let R denote the set of all rails, and define a directed edge R R whenever R is the parent rail of R in the sense of Lemma 53. Then:
1. 
The directed graph ( R , ) has no directed cycles (Theorem 2).
2. 
The rail of 1 is the unique vertex in R with no outgoing edge (i.e., the unique rail without a distinct parent)(Remark 2).
3. 
Every rail R R lies in the ancestor tree of the rail of 1: there exists a (possibly trivial) finite sequence of parent rails
R = R 0 R 1 R d ,
with R d equal to the rail of 1.
In particular, the parent relation → induces a well-founded partial order on R with a unique minimal element, the rail of 1, and there is no second infinite component of rails disjoint from the ancestry of 1.
Proof. 
(1) By construction, each rail is an affine progression generated by repeated application of m 4 m + 1 (or the class-specific analogue) from its base. The disjointness and uniqueness-of-ancestry results for rails imply that two distinct rails cannot share an odd integer. If a directed cycle
R 0 R 1 R d 1 R 0
existed, then following the associated bases under admissible Inverse lifts would produce a nontrivial cycle in the underlying affine structure, forcing an odd integer to lie on two distinct rails, a contradiction.
(2) Lemma 53 shows that every rail R with base m 0 1 has a unique parent rail R , hence a directed edge R R . For the rail of 1, the only solution of 3 m + 1 = 2 k m is m = 1 , so it admits no distinct parent; thus it is the unique vertex without an outgoing edge.
(3) Let R be any rail with base m 0 . By Lemma 53, either m 0 = 1 and R is the rail of 1, or R has a unique parent rail R 1 . Iterating this construction produces a finite chain
R = R i R i 1 R 0 .
By Corollary 17, each step in this chain corresponds to a Forward collapse of the entire ancestry of R i + 1 onto the Inverse parent R i , and the dyadic coverage results of Section 5 imply that no odd integer lies outside the union of these rails. If the chain avoided the rail of 1 indefinitely, it would define a second infinite component of R disjoint from the ancestry of 1, contradicting the uniqueness of admissible ancestry and the dyadic coverage result of the odd integers established in Theorem 16. Hence the chain must terminate at the rail of 1 after finitely many steps, and every rail R admits a finite ancestor sequence ending at the rail of 1. □

6.6. Global Consequences of Dyadic Coverage

The dyadic partition in Theorem 14 shows that every odd integer lies on exactly one affine rail
m = 4 e c 0 + 4 e 1 3 , e 0 ,
where c 0 is the first admissible child R ( n ; k 0 ( n ) ) of a unique live integer n { 1 , 5 } ( mod 6 ) . Each rail corresponds to a unique pair ( c , e ) with k = c + 2 e , and the dyadic slices
S c , e = 2 k + 1 t + 2 k x 1 3 : t 0
form a disjoint partition of N odd . This section records the global consequences of this structure.

Affine rails as exhaustive enumerations.

For any live odd n with minimal exponent k 0 ,
c 0 = R ( n ; k 0 ) , c e = R ( n ; k 0 + 2 t ) = 4 e c 0 + 4 e 1 3 .
Thus the entire admissible chain above n is determined by c 0 alone and consists of a pure affine progression. Varying n ranges over all possible bases c 0 , and Theorem 14 shows that these progressions are disjoint and collectively cover every odd integer. No dynamical descent or step-count analysis is required.

Role of classes and parity.

The parameters ( c , x ) { ( 1 , 5 ) , ( 2 , 1 ) } determine the admissible parity of k = v 2 ( 3 m + 1 ) and the residue and peridoc enumeration of every base child of n o d d . Higher lifts k 0 + 2 t preserve class and correspond to further applications of the affine map m 4 m + 1 . Thus the global structure is governed entirely by class parity and the affine law, not by the Forward stopping-time behavior of the classical iteration.

6.7. From Global Rail Coverage to Surjectivity from the Root

At this stage we have two global facts:
(i)
Global coverage by rails/slices. By Theorems 14 and 16 (and Corollary 15), the dyadic slices partition N odd and coincide exactly with the affine rails generated by the lift iteration m 4 m + 1 .
(ii)
Forward collapse of each rail. By Lemma 52 and Corollary 17, every element m e = R ( n ; k 0 ( n ) + 2 e ) on the admissible rail generated by n collapses in one odd step to n:
T ( m e ) = n , e 0 ,
and no other odd child is attained from any m e .
The purpose of this subsection is to convert the set-theoretic global coverage into the rooted surjectivity statement “every live odd has an admissible address from 1.”
Proposition 12 
(Unique global root and rooted surjectivity). Assume the inverse system admits no directed cycles (Theorem 2). Then the inverse Collatz graph on N odd is a single rooted tree with root 1. Equivalently, for every odd integer n there exists a finite admissible rooted word K such that
R K ( 1 ) = n .
Proof. 
Because the forward odd map T is a function, each odd integer has a unique forward chain
n , T ( n ) , T 2 ( n ) , .
If a forward chain were to avoid 1 forever, then (since the inverse graph is locally finite and has no directed cycles by Theorem 2) the chain would necessarily generate an infinite inverse ancestry within some component, contradicting the rail-collapse mechanism: indeed, by Theorem 16 every odd lies on a unique affine rail, and by Lemma 52 the forward map collapses each rail in one step to its unique generator. Iterating this collapse descends through the unique generators encountered by the chain. Since T ( 1 ) = 1 and no other fixed point exists in the live odd system, the only possible terminal cycle is the trivial fixed point at 1. Therefore every forward chain reaches 1.
Thus every odd integer lies in the same forward component as 1, and hence in the same inverse component. Reversing the forward chain yields an admissible inverse address from 1 to n, i.e. a finite rooted word K with R K ( 1 ) = n . □
With Proposition 12 in hand, the remainder of the paper may work purely in the rooted setting: admissible k–words are addresses in the unique Noetherian dependency tree rooted at 1. The Surjectivity Formula (SF) section that follows provides the closed-form evaluation of these addresses and the corresponding residue/offset analysis.

SF addresses and uniqueness of admissible paths

Fix j 0 and let K = ( k 1 , , k j ) be an ordered word of positive integers. Define the inverse iteration from the root 1 by
x 0 : = 1 , x t : = 2 k t x t 1 1 3 ( t = 1 , , j ) .
Call K admissible if each x t is an integer (equivalently, each step satisfies the local admissibility congruence). Write A j for the set of admissible words of length j. Let S : = i = 1 j k i and define B ( K ) as above. The surjectivity formula (SF) associated to K is
S F ( K ) : = 2 S B ( K ) 3 j .
By construction, if K is admissible then S F ( K ) = x j N o d d .
Theorem 18 
(Uniqueness of admissible k–word addresses). The map
S F : A : = j 0 A j N o d d
is injective. Equivalently, no odd integer has two distinct admissible k–word addresses. In particular, along an admissible path the digit k t at each depth t is uniquely determined by the endpoint.
Proof. 
Assume S F ( K ) = S F ( K ) = n for two admissible words K = ( k 1 , , k j ) and K = ( k 1 , , k j ) . Apply one forward odd-to-odd step to n (i.e. compute the unique predecessor in the inverse sense): the admissible exponent is uniquely k = ν 2 ( 3 n + 1 ) , hence the first digit must satisfy k 1 = k 1 = k , and the corresponding next odd integer is uniquely
n 1 = 3 n + 1 2 k .
Iterating this argument forces k t = k t and the same intermediate nodes at every depth until termination, hence j = j and K = K . □
Theorem 19 
(Global coverage by admissible SF addresses). The restriction of S F to admissible words is surjective onto N o d d . Equivalently, for every odd integer n there exists an admissible word K such that
S F ( K ) = n .
Proof. 
Let n N o d d . By the dyadic decomposition, n lies in a unique slice S c , e determined by k = ν 2 ( 3 n + 1 ) = c + 2 e . By Theorem 16 (rail–slice coincidence / global surjectivity on slices), there exists m M c , e such that
n = 2 k m 1 3 = R k ( m ) .
Iterating the same argument to m yields a finite admissible inverse chain from the root, hence an admissible word K whose endpoint equals n. By the SF identity, this endpoint is S F ( K ) = n . □
Theorem 20 
(SF gives a bijection between admissible words and N o d d ). The map
S F : A : = j 0 A j N o d d
is a bijection. In particular, every odd integer has a unique admissible k–word address.
Proof. 
Injectivity is Theorem 18. Surjectivity is Theorem 19. □

7. Geometric Residue Addressing and Level–Surjectivity of the Inverse Tree

We isolate the structural mechanism underlying inverse Collatz coverage. Throughout this section we work only with admissible odd-to-odd inverse steps and make no appeal to global surjectivity or absence of cycles.

7.1. Admissible Inverse Operator

Let N odd denote the positive odd integers. For an odd integer n, define the admissible inverse lift
R ( n ; k ) : = 2 k n 1 3 ,
whenever 2 k n 1 ( mod 3 ) .
An admissible word of length j is a sequence
K = ( k 0 , k 1 , , k j 1 )
such that each intermediate lift is integral.
Define the inverse tree rooted at 1 by
T 0 : = { 1 } , T j + 1 : = n T j { R ( n ; k ) : k admissible at n } .
Let
T : = j 0 T j .

7.2. Residue Filtration

For each j 1 define the modulus
M j : = 18 · 3 j 1 .
Let
ρ j ( n ) : = n mod M j .
Define the level-j admissible residue set
L j : = ρ j ( T j ) Z / M j Z .
Thus L j records exactly the residue classes realized at depth j in the inverse tree.

7.3. Residue Transition Operator

Fix j 0 . Let r L j and let n r ( mod M j ) . For any admissible k at n define
Θ j ( r ; k ) : = 2 k r 1 3 mod M j + 1 .
This is well-defined because M j + 1 = 3 M j and admissibility ensures integrality.
Lemma 54 
(Level Transition). If r L j and k is admissible at some representative n r , then
Θ j ( r ; k ) L j + 1 .
Proof. 
By construction,
2 k n 1 3 T j + 1 .
Reducing modulo M j + 1 gives the claimed residue. □

7.4. Residue Surjectivity

We now prove that every admissible residue at level j + 1 arises from some admissible residue at level j.
Lemma 55 
(Level Surjectivity). For every r L j + 1 , there exists r L j and admissible k such that
Θ j ( r ; k ) = r .
Proof. 
Let r L j + 1 . By definition there exists m T j + 1 with m r ( mod M j + 1 ) .
By construction of T j + 1 , m = R ( n ; k ) for some n T j and admissible k. Let r = ρ j ( n ) L j . Then
r 2 k r 1 3 ( mod M j + 1 ) ,
which is exactly Θ j ( r ; k ) . □

7.5. Affine Rail Replication

The inverse lift admits the affine form
R ( 18 q + r ; k ) = 6 · 2 k 1 q + 2 k r 1 3 .
In particular, if a residue r occurs at depth j, then every element in its affine progression
n = M j t + r
admits admissible lifts whose offsets are scaled by 2 k 1 .
Moreover, if k k + 2 , then
R ( n ; k + 2 ) = 4 R ( n ; k ) + 1 ,
so affine rails replicate without collapsing.
Lemma 56 
(Rail Stability). If a residue class appears at level j, its entire affine rail persists under admissible lift scaling.
Proof. 
Immediate from the affine expression above. □

7.6. Algebraic Reachability of the Inverse Address Map

7.6.1. Notation

For an admissible word
K = ( k 1 , , k j ) ,
define
S ( K ) : = i = 1 j k i , n ( K ) : = 2 S ( K ) B ( K ) 3 j ,
where B ( K ) is the canonical offset determined inductively by the inverse construction.
All words considered below are admissible at each step.

7.6.2. Primitive Root Structure Modulo 3 j

Lemma 57 
(Primitive Root Property). For every integer j 1 , the element 2 generates the multiplicative group
( Z / 3 j Z ) × .
In particular, for every residue r coprime to 3 modulo 3 j , there exists an integer S such that
2 S r ( mod 3 j ) .
Proof. 
It is classical that 2 is a primitive root modulo 3 j for all j 1 . Hence ( Z / 3 j Z ) × is cyclic of order 2 · 3 j 1 generated by 2. □

7.6.3. Residue Compatibility of the Surjectivity Formula

The SF identity
2 S ( K ) = 3 j n ( K ) + B ( K )
implies, modulo 3 j ,
2 S ( K ) B ( K ) ( mod 3 j ) .
Lemma 58 
(No Modular Obstruction). For fixed j and any odd integer n, the congruence
2 S 3 j n + B ( mod 3 j )
has solutions in S whenever 3 j n + B is coprime to 3.
Proof. 
Since 3 j n + B B ( mod 3 j ) and admissibility ensures B is not divisible by 3, the residue lies in ( Z / 3 j Z ) × . By the primitive root property, 2 attains every such residue. □
This eliminates all modular obstructions to solving the SF identity.

7.7. Combinatorial Realization of Exponents

Let K denote the admissible set of exponents at a single step. In particular, K contains infinitely many integers in each congruence class compatible with admissibility.
Lemma 59 
(Semigroup Generation). Fix j 1 . There exists S 0 ( j ) such that for every integer S S 0 ( j ) satisfying the admissibility parity constraints, there exists an admissible word K of length j with
S ( K ) = S .
Proof. 
Since K contains at least two distinct integers a , b with gcd ( a , b ) = 1 (e.g. k and k + 2 for admissible k), the additive semigroup generated by K contains all sufficiently large integers in the appropriate parity class. The classical Frobenius coin argument applies because gcd ( K ) = 1 . Thus every sufficiently large S compatible with parity constraints can be written as a sum of j elements of K . □
This guarantees that solving the congruence in S produces an admissible word realizing that S.

7.7.1. Reachability Existence

Theorem 21 
(Algebraic Reachability). For every odd integer n, there exists a finite admissible word K such that
n = n ( K ) .
Proof. 
Fix an odd n.
Choose j sufficiently large. By the primitive root lemma, there exists S satisfying
2 S B ( mod 3 j )
where B is the canonical offset form required for length j.
Thus
2 S = 3 j n + B .
By the semigroup generation lemma, for sufficiently large S there exists an admissible word K of length j with S ( K ) = S .
Substituting into the SF identity yields
n = 2 S ( K ) B ( K ) 3 j .
Thus n lies in the image of the admissible inverse addressing map. □

7.8. Corollary: Global Addressing

Corollary 18. 
The admissible inverse addressing map rooted at 1 is surjective onto the odd integers.
Proof. 
Immediate from the theorem. □

7.9. Global Addressing

We now assemble the structural statement.
Theorem 22 
(Global Level Coverage). For every j 0 ,
ρ j ( T ) = L j .
That is, the inverse tree is level-surjective onto its admissible residue set at every depth.
Proof. 
By induction on j.
Base case j = 0 is immediate.
Assume true for j. By Lemma 55, every residue in L j + 1 arises from some residue in L j . By Lemma 54, every such transition corresponds to an element of T j + 1 . Hence ρ j + 1 ( T ) = L j + 1 . □

Rail transitions and rank descent are isomorphic

Let K = ( k 1 , , k j ) be an admissible word and write its endpoint as
n = S F ( K ) .
By Theorem 21 (existence and uniqueness of depth), every odd integer n N o d d has a unique admissible address K and unique depth j.
Definition 28 
(Depth and rank). For n N o d d with unique address K = ( k 1 , , k j ) , define the depth
d e p t h ( n ) : = j ,
and the rank
ρ ( n ) : = 3 d e p t h ( n ) = 3 j .
Lemma 60 
(Forward step deletes the leading digit). Let n = S F ( k 1 , , k j ) be an odd integer with j 1 . Let T denote the odd-to-odd forward step (one application of 3 x + 1 followed by division by the maximal power of 2). Then
T ( n ) = S F ( k 2 , , k j ) ,
and in particular
d e p t h ( T ( n ) ) = d e p t h ( n ) 1 .
Proof. 
Because K is the unique admissible address of n, the inverse construction from 1 reaches n in exactly j admissible steps, with first digit k 1 . Applying one odd-to-odd forward step reverses exactly the most recent inverse step, hence removes the leading digit of the address. Therefore the endpoint after one forward step is the endpoint of the suffix word ( k 2 , , k j ) , i.e. T ( n ) = S F ( k 2 , , k j ) . Uniqueness of the admissible address forces the depth drop by exactly one. □
Corollary 19 
(Isomorphism of rail transitions with rank descent). Under the address correspondence n K , inverse rail transitions correspond to appending one admissible digit to K, and forward odd-to-odd transitions correspond to deleting the leading digit of K. Consequently,
ρ ( T ( n ) ) = 3 d e p t h ( n ) 1 = ρ ( n ) 3 ,
so the forward dynamics is a strict descent in the well-ordered set { 3 j : j 0 } until reaching ρ = 3 0 , i.e. the terminal state n = 1 .

8. Parity Compatibility and Realization of Exponents

8.1. Admissible Exponents and Parity Constraint

Let j 1 be fixed. For an admissible word K = ( k 1 , , k j ) define
S ( K ) : = i = 1 j k i .
Admissibility at each step imposes a fixed parity constraint: there exists α { 0 , 1 } such that
k i α ( mod 2 ) for every admissible step .
Consequently,
S ( K ) j α ( mod 2 ) .
Thus for fixed j the set of admissible sums is an arithmetic progression
S S min ( j ) + 2 N ,
where S min ( j ) = j k min and k min is the smallest admissible exponent.

8.2. Modular Constraint from the Address Equation

The addressing identity
2 S ( K ) = 3 j n + B ( K )
implies modulo 3 that
2 S ( K ) B ( K ) ( mod 3 ) .
Since 2 1 ( mod 3 ) , we obtain
( 1 ) S ( K ) B ( K ) ( mod 3 ) .
Thus the parity of S ( K ) is uniquely determined by the residue of B ( K ) modulo 3.

8.3. Compatibility of Parity Conditions

Lemma 61 
(Parity Compatibility). For every admissible word length j, the parity condition
S j α ( mod 2 )
coincides with the parity required by
2 S B ( mod 3 ) .
Proof. 
Admissibility at each step is defined by the divisibility condition
2 k i n i 1 1 ( mod 3 ) .
Since 2 1 ( mod 3 ) , this condition becomes
( 1 ) k i n i 1 1 ( mod 3 ) .
Hence the parity of k i is uniquely determined by the residue of n i 1 modulo 3.
Iterating this relation shows that the parity constraint imposed on each k i is precisely the one ensuring that the cumulative exponent S satisfies
( 1 ) S B ( mod 3 ) .
Therefore the admissible parity condition (1) is exactly the parity condition required by the modular constraint (2). □

8.4. Intersection of Modular and Admissible Progressions

Lemma 62 
(Existence of Compatible Exponents). Let j 1 and fix B corresponding to admissible length j. Then the congruence
2 S B ( mod 3 j )
admits infinitely many solutions S satisfying the admissible parity constraint.
Proof. 
Since 2 is a primitive root modulo 3 j , the congruence
2 S B ( mod 3 j )
has solutions forming a full residue class
S S 0 ( mod 2 · 3 j 1 ) .
The modulus 2 · 3 j 1 is even. By Lemma 61, the parity of S 0 agrees with the admissible parity class. Hence the arithmetic progression of solutions intersects the admissible progression
S j α ( mod 2 ) .
Therefore infinitely many admissible S solve the congruence. □

8.5. Realization of Exponent Sums

Lemma 63 
(Combinatorial Realization). Fix j 1 . Every sufficiently large integer S satisfying the admissible parity constraint can be written as
S = k 1 + + k j
with each k i admissible.
Proof. 
The admissible exponents form an infinite arithmetic progression
k = k min + 2 m , m 0 .
Thus
S = j k min + 2 ( m 1 + + m j ) ,
so S ranges over the full arithmetic progression
S min ( j ) + 2 N .
Every sufficiently large S in the admissible parity class can therefore be realized by distributing the + 2 increments among the j coordinates. □

8.6. Summary

Theorem 23 
(Existence of Admissible Words Solving the Address Equation). For every j 1 and every admissible offset B, there exists an admissible word K of length j such that
2 S ( K ) B ( mod 3 j ) .
Proof. 
By Lemma 62 there exist infinitely many admissible S solving the modular equation. By Lemma 63, sufficiently large such S can be realized as sums of admissible exponents. Substituting into the addressing identity yields the result. □

9. Global Surjectivity of the Rooted Address Map

9.1. The Rooted Address Map

For an admissible word
K = ( k 1 , , k j ) ,
let the partial sums be
S i ( K ) : = t = 1 i k t , S 0 ( K ) : = 0 , S ( K ) : = S j ( K ) .
Starting from the root value n 0 : = 1 , define the iterative inverse construction
n i : = 2 k i n i 1 1 3 ( 1 i j ) ,
whenever each step is integral (admissible). The terminal value n j is the output of the word.
The standard telescoping expansion yields the closed form
n ( K ) = n j = 2 S ( K ) B ( K ) 3 j , B ( K ) : = i = 1 j 3 j i 2 S i 1 ( K ) .
We refer to (3) as the rooted surjectivity formula (SF).

9.2. Offset-Residue Coverage

The surjectivity problem is equivalently the statement that the image
I : = { n ( K ) : K admissible rooted at 1 }
equals the full set N odd .
The decisive input is that the rooted offset map K B ( K ) ranges over all admissible residue classes modulo 3 j .
Proposition 13 
(Offset residue coverage). Fix j 1 . As K ranges over all admissible rooted words of length j, the set of residues
{ B ( K ) mod 3 j }
equals ( Z / 3 j Z ) × . Moreover, the restriction induced by the live-class admissibility (equivalently, the stepwise parity constraint on each k i ) agrees with the parity constraint on the total exponent S ( K ) from Lemma 61.
Proof. 
(i) the admissible branching produces a perfect partition of live outcomes at each level, and (ii) the k k + 2 lift induces a uniform affine replication of offsets across levels. Together these imply that the rooted offsets B ( K ) attain every unit residue class modulo 3 j . The compatibility of these residues with the admissible parity class is exactly Lemma 61. □

9.3. Primitive Root Solvability

Lemma 64 
(Primitive root solvability modulo 3 j ). For every j 1 and every unit residue r ( Z / 3 j Z ) × , there exists an integer S such that
2 S r ( mod 3 j ) .
Proof. 
It is classical that 2 generates ( Z / 3 j Z ) × for all j 1 . □
Theorem 24 
(Global Affine Closure and Well–Founded Structure). After establishment of global coverage (Theorems 14 and 16), acyclicity (Theorem 2), non–divergence Theorem 4), inverse–forward equivalence (Theorem 5), and global surjectivity rooted at 1 (Proposition 12), the odd–to–odd Collatz system satisfies the following:
(a)
Unique affine parentage. Every odd integer m admits a unique minimal admissible inverse exponent k 0 , and hence a unique affine parent
R ( m ; k 0 ) = 2 k 0 m 1 3 .
Iterating minimal inverse lifts produces a unique affine rail
m = A e ( n ) ( e 0 ) ,
originating from a unique minimal base element n. No odd integer possesses two distinct affine ancestries.
(b)
Disjoint rail partition. The odd integers are partitioned disjointly into affine rails generated from their minimal bases. These rails are mutually disjoint and collectively exhaust N odd .
(c)
Absence of cycles. By Theorem 2, through all refinement levels
M j = 2 · 3 j + 1 .
there exists no realizeable directed cycle.
(d)
Well–founded ancestry. Every rail except the anchor rail of 1 possesses a unique parent rail. Hence rail ancestry is well–founded: no infinite strictly descending chain of distinct bases exists. The rail of 1 is the unique minimal element in this structure.
(e)
Absence of Forward runaway. By Theorem 4, no infinite compatible inverse refinement chain exists across the tower M j = 2 · 3 j + 1 .
(f)
Forward–Inverse equivalence. By inverse–forward equivalence (Theorem 5), any divergent Forward trajectory would correspond to such an infinite inverse chain. Therefore no Forward runaway can occur.
Consequently, the odd–to–odd Collatz dynamics form a single closed, well–ordered affine system anchored at 1.
Lemma 65 
(Even integers inside the k–valuation skeleton). Every positive integer N admits a unique dyadic decomposition
N = 2 h m , h 0 , m odd .
For each odd m, the odd–to–odd Collatz gate is
T ( m ) = 3 m + 1 2 k m ( m ) , k m ( m ) = ν 2 ( 3 m + 1 ) ,
so that 3 m + 1 = 2 k m ( m ) T ( m ) with T ( m ) odd.
Each admissible Inverse step
R ( n ; k ) = 2 k n 1 3 , k = c + 2 e ,
is a pure dyadic lift: the exponent k records exactly how many factors of 2 are injected above n in the Inverse direction. Thus the collection of all k–lifts already accounts for every power of 2 that can appear above any odd anchor in the Inverse tree.
In Forward time, starting from N = 2 h m , the halving steps strip off the dyadic factor 2 h until the odd anchor m is reached, after which the gate k m ( m ) removes the remaining admissible factors of 2 from 3 m + 1 . Consequently, every even integer N lies on the same k–valuation skeleton as its odd anchor m: no new branches arise from even inputs, and every factor of 2 above m is realized either as a trivial halving step or as part of an admissible exponent k in the Inverse/Forward pair.
Corollary 20 
(All positive integers are carried by the odd skeleton). If every odd integer n lies on the affine Inverse skeleton and converges to 1 under the Forward map T, then every positive integer N 1 also converges to 1.
Proof. 
Given N 1 , write N = 2 h n with m odd. By Lemma 65, the Forward trajectory of N coincides with that of n after finitely many halving steps:
N e v e n n 1 .
Since, by hypothesis, the odd anchor n lies on the closed affine skeleton and reaches 1 under T, the same is true for N. Thus closure of the odd subsystem implies closure of the full Collatz map on N 1 . □
Theorem 25 
(Global Forward Convergence to 1). For every integer N 1 , the Forward Collatz iteration
F ( N ) = N / 2 , N even , 3 N + 1 , N odd ,
reaches 1. Equivalently, every Forward trajectory enters the standard cycle 1 4 2 1 , and there is no nontrivial cycle and no Forward runaway.
Proof. 
Let N 1 be arbitrary.
If N is odd, then by Theorem 24 the odd–to–odd Forward Collatz map
T ( n ) = 3 m + 1 2 k m ( n ) , k m ( n ) = ν 2 ( 3 m + 1 ) ,
reaches 1; hence the full Forward iteration reaches the 1 4 2 1 basin.
If N is even, write N = 2 h n with h 1 and n odd. Then h applications of the Forward even rule N N / 2 send N to n. By Lemma 65 Corollary 20, the even extension lies inside the dyadic framework of the odd trajectory of n, and by the preceding odd case the Forward iteration from n reaches 1. Therefore the Forward iteration from N reaches 1 as well.
Since N 1 was arbitrary, every positive integer converges to 1. □

10. Structural Isomorphism Claim

The system developed here is defined entirely by the admissible inverse transformations of the reduced odd Collatz map together with their affine–dyadic organization and refinement structure.
Theorem 26 
(Structural Isomorphism). Let G odd denote the odd Collatz digraph with Forward map
T ( m ) = 3 m + 1 2 ν 2 ( 3 m + 1 ) ,
and admissible inverse edges given by R ( n ; k ) as in Theorem 5.
Then the affine–dyadic system developed in this paper, together with the refinement tower M j = 2 · 3 j + 1 , realizes exactly the same directed structure:
  • the same vertex set N odd ,
  • the same Forward map T,
  • the same admissible inverse edges.
In particular, the global coverage (Theorems 14 and 16), the well–founded rail ancestry (Theorem 24), the absence of cycles (Theorem 2), the absence of Forward divergence (Theorem 4), and inverse–forward equivalence (Theorem 5) provide a complete internal structural model of the classical odd Collatz dynamics.
Therefore. 
By the preceding structural identification and the even embedding, global Forward convergence on N 1 follows as stated in Theorem 25.

11. Conclusion

The Collatz Conjecture holds.

References

  1. Everett, C. J. Iteration of the number-theoretic function f(2n)=n, f(2n+1)=3n+2. Advances in Mathematics 1977, 25, 42–45. [Google Scholar] [CrossRef]
  2. Garner, L. E. On the Collatz 3n+1 algorithm. Proceedings of the American Mathematical Society 1981, 82, 19–22. [Google Scholar] [CrossRef]
  3. Lagarias, J. C. The 3x+1 problem and its generalizations. American Mathematical Monthly 1985, 92, 3–23. [Google Scholar] [CrossRef]
  4. Lagarias, J. C. The 3x+1 problem: An annotated bibliography (1963–1999). arXiv:math/0309224.
  5. Spencer, M. A Deterministic Residue Framework for the Collatz Operator at q=3. 2025; preprint. [Google Scholar] [CrossRef]
  6. Tao, T. Almost all orbits of the Collatz map attain almost bounded values. Forum of Mathematics 2019, Pi 7, e12. [Google Scholar] [CrossRef]
  7. Terras, R. A stopping time problem on the positive integers. Acta Arithmetica 1976, 30, 241–252. [Google Scholar] [CrossRef]
  8. Terras, R. On the existence of a density. Acta Arithmetica 1979, 35, 101–102. [Google Scholar] [CrossRef]
Table 1. Mod 54 refinement: for odd n [ 1 , 53 ] , the residue r n ( mod 18 ) and the base child’s class and residue ( mod 18 ) .
Table 1. Mod 54 refinement: for odd n [ 1 , 53 ] , the residue r n ( mod 18 ) and the base child’s class and residue ( mod 18 ) .
n 54 r 18 parent class base child class base child residue ( mod 18 )
1 1 C2 C2 1
3 3 C0
5 5 C1 C0 3
7 7 C2 C0 9
9 9 C0
11 11 C1 C2 7
13 13 C2 C1 17
15 15 C0
17 17 C1 C1 11
19 1 C2 C2 7
21 3 C0
23 5 C1 C0 15
25 7 C2 C0 15
27 9 C0
29 11 C1 C2 1
31 13 C2 C1 5
33 15 C0
35 17 C1 C1 5
37 1 C2 C2 13
39 3 C0
41 5 C1 C0 9
43 7 C2 C0 3
45 9 C0
47 11 C1 C2 13
49 13 C2 C1 11
51 15 C0
53 17 C1 C1 17
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.
Copyright: This open access article is published under a Creative Commons CC BY 4.0 license, which permit the free download, distribution, and reuse, provided that the author and preprint are cited in any reuse.
Prerpints.org logo

Preprints.org is a free preprint server supported by MDPI in Basel, Switzerland.

Subscribe

Disclaimer

Terms of Use

Privacy Policy

Privacy Settings

© 2026 MDPI (Basel, Switzerland) unless otherwise stated