# 490d — C552–C571: sequential research record

Research begun27 September2026 in the user’s local timezone; packet dated28 September UTC. Working continuation of C531. No canonical source is changed; second-order inversion and quarantined primers remain deferred.

Each step records a question before its calculation, frozen inputs, exact result, finding, and reassessment. Preparatory source extraction and review were delegated; the numbered sequence was evaluated in order. These are bounded research actions, not independent discoveries.

## C552 — Generate the cumulative root family

**Question.** Does one affine rule reconstruct all six source rails?

**Sources.** File62 §§1.2–1.4; File61 §§7.3A–7.6

**Inputs**

```json
{
  "base": [
    2435,
    2260,
    2080,
    1933,
    1796,
    1663,
    1526
  ],
  "phases": [
    0,
    "7/2"
  ],
  "clutch": [
    0,
    7,
    14
  ]
}
```

**Results**

```json
{
  "rails": [
    [
      2435,
      2260,
      2080,
      1933,
      1796,
      1663,
      1526
    ],
    [
      2428,
      2253,
      2073,
      1926,
      1789,
      1656,
      1519
    ],
    [
      2421,
      2246,
      2066,
      1919,
      1782,
      1649,
      1512
    ],
    [
      "4877/2",
      "4527/2",
      "4167/2",
      "3873/2",
      "3599/2",
      "3333/2",
      "3059/2"
    ],
    [
      "4863/2",
      "4513/2",
      "4153/2",
      "3859/2",
      "3585/2",
      "3319/2",
      "3045/2"
    ],
    [
      "4849/2",
      "4499/2",
      "4139/2",
      "3845/2",
      "3571/2",
      "3305/2",
      "3031/2"
    ]
  ],
  "coordinate_matches": 42
}
```

**Finding.** C(p,d)=C0+p−d reconstructs all42 source coordinates. This is one family generated from seven inputs and two local state parameters, not42 independent successes.

**Reassessment.** Establish why the source clutch is14 and whether its three envelopes are independent.

## C553 — Recover one clutch from nested envelopes

**Question.** Are487/473,444/430 and350/336 independent compression measurements?

**Sources.** File61 §§6.3–6.6

**Inputs**

```json
{
  "envelopes": [
    [
      487,
      473
    ],
    [
      444,
      430
    ],
    [
      350,
      336
    ]
  ]
}
```

**Results**

```json
{
  "compressions": [
    14,
    14,
    14
  ],
  "removed_prefixes": [
    [
      43,
      43
    ],
    [
      94,
      94
    ]
  ]
}
```

**Finding.** All three envelopes express the same14-year compression after equal prefixes43 and94 are removed. The maximum nonoverlap envelope is a source model, not a literal succession of biographies.

**Reassessment.** Distinguish translating the whole root from moving a single boundary.

## C554 — Separate endpoint and whole-rail translation

**Question.** Which spans contract when the clutch moves only a parent boundary?

**Sources.** File61 §7.4; §§17.2–17.3

**Inputs**

```json
{
  "lifespans": [
    175,
    180,
    147,
    137,
    133,
    137
  ],
  "clutch": 14
}
```

**Results**

```json
{
  "parent_only": [
    161,
    166,
    133,
    123,
    119,
    123
  ],
  "both_ends": [
    175,
    180,
    147,
    137,
    133,
    137
  ],
  "Isaac_only_Abraham_fixed": 189,
  "derived_terminal_to_fixed_Exodus": 66
}
```

**Finding.** One-end translation contracts each lifespan; whole-rail translation preserves it. Outputs166 and119 remain part of the family. Moving Isaac alone makes189, showing why endpoint roles are indispensable.

**Reassessment.** Determine the exact local composition law for half and full clutch.

## C555 — Specify the finite clutch action

**Question.** What symmetry is licensed by the three admitted displacement states?

**Sources.** File61 §7.3A; File62 §1

**Inputs**

```json
{
  "displacements": [
    0,
    7,
    14
  ],
  "example": 1933
}
```

**Results**

```json
{
  "rail": [
    1933,
    1926,
    1919
  ],
  "half_step_edges": [
    [
      0,
      7
    ],
    [
      7,
      14
    ]
  ],
  "composite_edge": [
    0,
    14
  ],
  "third_half_step": 1912,
  "third_step_admitted": false
}
```

**Finding.** H7 composed twice equals T14 on the declared original-to-full domain. The admitted rails form a finite directed chain, not a closed translation group. Historical event anchors remain fixed.

**Reassessment.** Generate Joseph collateral intervals from the same root boundaries.

## C556 — Generate all collateral Joseph intervals

**Question.** Do two fixed-offset constructions account for every source Joseph rail?

**Sources.** File61 §§11.2–11.3A; File62 §5.2

**Inputs**

```json
{
  "Levi": 1933,
  "Kohath": 1796,
  "Joseph_life": 110
}
```

**Results**

```json
{
  "intervals": [
    [
      1933,
      1823
    ],
    [
      1906,
      1796
    ],
    [
      1926,
      1816
    ],
    [
      1899,
      1789
    ],
    [
      1919,
      1809
    ],
    [
      1892,
      1782
    ],
    [
      "3873/2",
      "3653/2"
    ],
    [
      "3819/2",
      "3599/2"
    ],
    [
      "3859/2",
      "3639/2"
    ],
    [
      "3805/2",
      "3585/2"
    ],
    [
      "3845/2",
      "3625/2"
    ],
    [
      "3791/2",
      "3571/2"
    ]
  ],
  "matches": 12
}
```

**Finding.** Two collateral constructors, (L,L−110) and (K+110,K), generate all12 exact-phase Joseph intervals. Joseph remains a collateral interval, not an added trunk generation.

**Reassessment.** Derive the invariant geometry shared by these interval pairs.

## C557 — Derive Joseph overlap geometry

**Question.** Why do all six paired states share27|83|27?

**Sources.** File61 §11; File62 §§5–6

**Inputs**

```json
{
  "trunk": 137,
  "collateral": 110
}
```

**Results**

```json
{
  "partition": [
    27,
    83,
    27
  ],
  "overlap": 83,
  "translation_commutes_with_collateral_construction": [
    true,
    true,
    true,
    true,
    true,
    true
  ]
}
```

**Finding.** The27|83|27 geometry follows from lengths137 and110. Translation commutes with fixed-offset collateral construction, so twelve intervals reduce to one shape in six placements.

**Reassessment.** Compare the moving collateral lives with fixed regular Joseph.

## C558 — Generate the fixed-Joseph comparison family

**Question.** Can one flank-transfer formula reproduce all nine comparison states?

**Sources.** File62 §§6.1–6.4

**Inputs**

```json
{
  "regular_Joseph": [
    1915,
    1805
  ],
  "phases": [
    0,
    3,
    "7/2"
  ],
  "clutch": [
    0,
    7,
    14
  ]
}
```

**Results**

```json
{
  "partitions": [
    [
      18,
      9,
      83
    ],
    [
      11,
      16,
      83
    ],
    [
      4,
      23,
      83
    ],
    [
      "43/2",
      "11/2",
      83
    ],
    [
      "29/2",
      "25/2",
      83
    ],
    [
      "15/2",
      "39/2",
      83
    ],
    [
      21,
      6,
      83
    ],
    [
      14,
      13,
      83
    ],
    [
      7,
      20,
      83
    ]
  ],
  "formula": [
    "18+p−d",
    "9−p+d",
    "83"
  ]
}
```

**Finding.** The clutch transfers duration between two flanks while preserving their27 total and the83 overlap. All nine states follow without moving regular Joseph1915–1805.

**Reassessment.** Test whether the reported cyclic symmetry acts on dates or on duration components.

## C559 — Locate the Joseph cyclic symmetry

**Question.** Does a three-cycle act consistently on the complete component family?

**Sources.** File62 §§6.1–6.4; C558

**Inputs**

```json
{
  "rotation": "(a,b,c)→(b,c,a)"
}
```

**Results**

```json
{
  "states": 9,
  "component_displays": 27,
  "example": [
    [
      4,
      23,
      83
    ],
    [
      23,
      83,
      4
    ],
    [
      83,
      4,
      23
    ]
  ],
  "action_domain": "ordered duration triples"
}
```

**Finding.** A genuine C3 action rotates duration components and returns after three applications. It does not establish a permutation of historical people or complete chronology states.

**Reassessment.** Test how whole-year and exact phase choices change crossed containers.

## C560 — Unify crossed Joseph containers by phase

**Question.** Are140 and140.5 conflicting containers or different declared states?

**Sources.** File61 §§12.1–12.3

**Inputs**

```json
{
  "Levi_span": 137,
  "phases": [
    3,
    "7/2"
  ]
}
```

**Results**

```json
{
  "phase_family": {
    "3": {
      "parts": [
        30,
        80,
        30
      ],
      "outer": 140,
      "other_diagonal": 134
    },
    "7/2": {
      "parts": [
        "61/2",
        "159/2",
        "61/2"
      ],
      "outer": "281/2",
      "other_diagonal": "267/2"
    }
  },
  "exact_diagonal_center": 137,
  "exact_diagonal_separation": 7
}
```

**Finding.** Whole-year30|80|30 and exact30.5|79.5|30.5 are evaluations of one phase formula. Exact diagonals140.5 and133.5 are centered on137 and separated by7.

**Reassessment.** Reconstruct the430/460 Joseph-to-Joshua routes with their declared phase states.

## C561 — Resolve the two Joshua translations

**Question.** Which Joseph states yield the source430 and460 routes?

**Sources.** File61 §§14.1–14.3

**Inputs**

```json
{
  "target": [
    1476,
    1366
  ],
  "source_intervals": [
    [
      1906,
      1796
    ],
    [
      1936,
      1826
    ],
    [
      1933,
      1823
    ],
    [
      "3873/2",
      "3653/2"
    ]
  ]
}
```

**Results**

```json
{
  "translations": [
    [
      430,
      430
    ],
    [
      460,
      460
    ],
    [
      457,
      457
    ],
    [
      "921/2",
      "921/2"
    ]
  ],
  "states": [
    "backward Nisan",
    "forward Aaron whole-year",
    "forward Nisan diagnostic",
    "forward Aaron exact diagnostic"
  ]
}
```

**Finding.** The430/460 pair is exact in its declared mixed states. Other forward phases require457 or460.5, so460 is not a phase-independent property of Joseph.

**Reassessment.** Follow the fixed regular Joshua interval into the cumulative Joshua interval.

## C562 — Compose Joshua interval translations

**Question.** Does the regular-to-cumulative Joshua link close the Joseph routes without changing fixed event anchors?

**Sources.** File61 §14.3A; File62 §9

**Inputs**

```json
{
  "regular": [
    1476,
    1366
  ],
  "cumulative": [
    1406,
    1296
  ],
  "terminal_starts": [
    1526,
    1512
  ]
}
```

**Results**

```json
{
  "Joshua_shift": [
    70,
    70
  ],
  "composed_Joseph_shifts": [
    500,
    530
  ],
  "fixed_Joshua_spans": [
    230,
    216
  ]
}
```

**Finding.** The common70 translation gives total500/530 routes. Holding cumulative Joshua1296 contracts230 to216 when the derived start shifts14; historical Moses1526 remains the original event.

**Reassessment.** Test whether the double Adam square is an independent pattern or translated geometry.

## C563 — Compress the double Adam square

**Question.** Do both110-squared constructions follow from a rigid translation?

**Sources.** File61 §§12.4–12.6

**Inputs**

```json
{
  "base": [
    14006,
    1906,
    1796
  ],
  "apparent_whole_year": [
    14036,
    1936,
    1826
  ]
}
```

**Results**

```json
{
  "differences": [
    [
      12100,
      12210,
      110
    ],
    [
      12100,
      12210,
      110
    ]
  ],
  "pair_translation": [
    30,
    30,
    30
  ],
  "exact_phase_mismatch": "24199/2",
  "square": 12100
}
```

**Finding.** The two square/rectangle displays are the same12100/12210 geometry translated30. Substituting an exact-phase Joseph node alone yields12099.5 and breaks the square; no new head is fitted.

**Reassessment.** Determine how the Isaac macro partition relates to the calendar ratios.

## C564 — Relate the Isaac partition to calendar calibration

**Question.** Does the11760/840/12600 family use an existing ratio?

**Sources.** File61 §§17.3–17.7

**Inputs**

```json
{
  "head": 14006,
  "translated_Isaac": 2246,
  "Conquest": 1406
}
```

**Results**

```json
{
  "partition": [
    11760,
    840,
    12600
  ],
  "units_of35": [
    336,
    24,
    360
  ],
  "whole_over_upper": "15/14",
  "E_over_P": "15/14"
}
```

**Finding.** The Isaac macro partition is35 copies of336+24=360. Its15/14 completion ratio is exactly E/P, connecting the cumulative partition to the existing calendar calibration.

**Reassessment.** Check which part survives an exact common phase shift.

## C565 — Localize phase invariance in the Isaac partition

**Question.** Can the complete dated partition be carried unchanged into the exact Aaron phase?

**Sources.** File61 §§17.3–17.7

**Inputs**

```json
{
  "phase": "7/2",
  "fixed_Conquest": 1406
}
```

**Results**

```json
{
  "upper_common_phase": 11760,
  "lower_fixed_terminal": "1687/2",
  "changed_total": "25207/2"
}
```

**Finding.** The upper11760 leg is phase-invariant when both ends move. The fixed-Conquest lower leg becomes843.5, so the840 and12600 dated partition belongs to its declared Nisan state.

**Reassessment.** Separate the Cainan and Apparent inputs in the12250 variant.

## C566 — Generate the12250 cumulative variant

**Question.** How do the separate Cainan and Apparent operations combine in this source state?

**Sources.** File61 §§17.6–17.7

**Inputs**

```json
{
  "base_head": 14006,
  "Isaac": 2246,
  "cumulative_Cainan": 460,
  "Apparent": 30
}
```

**Results**

```json
{
  "heads": [
    14006,
    14466,
    14036,
    14496
  ],
  "upper_legs": [
    11760,
    12220,
    11790,
    12250
  ],
  "combined_factorization": [
    25,
    490
  ]
}
```

**Finding.** Separate source operations+460 and+30 combine additively to a490 increment. The combined upper leg12250 is25×490; numerical summation does not identify the two state changes or regular Cainan130 with cumulative460.

**Reassessment.** Recover the full, half and quarter Key family behind clutch magnitudes.

## C567 — Unify full half and quarter Key scales

**Question.** Do14,7 and3.5 require separate expansion laws?

**Sources.** File62 §8.3; File60 §7

**Inputs**

```json
{
  "scales": [
    7,
    "7/2",
    "7/4"
  ]
}
```

**Results**

```json
{
  "input_output_gain": [
    [
      161,
      175,
      14
    ],
    [
      "161/2",
      "175/2",
      7
    ],
    [
      "161/4",
      "175/4",
      "7/2"
    ]
  ],
  "general_rule": "23u→25u, gain2u"
}
```

**Finding.** The three gains are scaled evaluations of E, not new Keys. They connect the161/175 Covenant unit to80.5/87.5 and40.25/43.75 duration units without making their event placements interchangeable.

**Reassessment.** Compare the two source routes from483 to490.

## C568 — Compare the dual490 constructions

**Question.** Can subset E and whole-span P agree on the source483 partition?

**Sources.** File62 §§8.6A–C; File63 §1.3

**Inputs**

```json
{
  "parts": [
    "805/2",
    "161/2"
  ],
  "total": 483
}
```

**Results**

```json
{
  "partial_E": 490,
  "whole_P": 490,
  "whole_E": 525,
  "common_day_volume": [
    176400,
    176400
  ]
}
```

**Finding.** Expanding only80.5 by E and all483 by P both give490. Whole-span E gives525; the calendar volumes490×360 and525×336 agree. The duration identity needs no deferred endpoint.

**Reassessment.** Derive the general allocation identity that explains this agreement.

## C569 — Derive the Prophetic allocation identity

**Question.** Why does applying E to one sixth reproduce whole-span P?

**Sources.** File63 §1.3; algebraic generalization of C568

**Inputs**

```json
{
  "E": "25/23",
  "P": "70/69"
}
```

**Results**

```json
{
  "required_fraction": "1/6",
  "effective_factor": "70/69",
  "identity": "(5/6)S+E(S/6)=P S",
  "483_selected_part": "161/2"
}
```

**Finding.** P is the total-span effect of allocating E to one sixth of a duration. The source supplies that partition for483; the identity alone does not authorize the partition at every chronological node.

**Reassessment.** Ask whether J has a parallel allocation fraction and an already sourced partition.

## C570 — Derive the Jubilee allocation identity

**Question.** Does J admit the same allocation explanation on the source12558 path?

**Sources.** File63 §§7.3–7.4,9.7; algebraic generalization

**Inputs**

```json
{
  "E": "25/23",
  "J": "300/299",
  "path": [
    14004,
    1929,
    1446
  ]
}
```

**Results**

```json
{
  "fraction": "1/26",
  "partition": [
    12075,
    483
  ],
  "carrier_counts": [
    25,
    1
  ],
  "partial_E": 12600,
  "whole_J": 12600
}
```

**Finding.** J is the total-span effect of E allocated to one26th. The source path14004→1929→1446 already supplies25×483+483, so expanding its final carrier gives12600 without a fitted breakpoint.

**Reassessment.** Check whether equal totals make these complete chronological maps identical.

## C571 — Distinguish endpoint agreement from path identity

**Question.** Do whole J and terminal-cell E have the same intermediate coordinate?

**Sources.** File63 §§7.3–7.4,9.7; C570

**Inputs**

```json
{
  "head": 14004,
  "junction": 1929,
  "terminal": 1446
}
```

**Results**

```json
{
  "whole_J_path": [
    14004,
    "24552/13",
    1404
  ],
  "terminal_E_path": [
    14004,
    1929,
    1404
  ],
  "junction_difference": "525/13"
}
```

**Finding.** Both paths end at1404, but whole J moves the junction to24552/13 while terminal E retains1929. The new compression is equality after evaluating total span, not identity of the ordered chronological path.

**Reassessment.** Use the shared endpoint1404 to reconstruct the Actual-to-Rounded cumulative interface.

## Evidence

Current completion:C532–C571. The accompanying archive includes the sequential journal, exact scripts, source snapshots and independent reviews. Some carried source snapshots provide future or inherited context; only the sections cited by a step are claimed as its evidence.
