{
  "scope": "T128: exact triangulation accounting and the original SI two-dislocation model.\n\nSource: Irvine et al., Nature 2010 SI \u00a73, equations 1/17/23/24, with declared\nweak-cylinder assumptions. Source SI equation 16 contains an extra b inconsistent\nwith its source equation and with 17/22; the curvature-only Airy function below\nuses the coefficient fixed by those equations. This is recorded, not silently\ndescribed as an execution of the literal inconsistent expression.\n",
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    },
    {
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      "interior_charge": 0,
      "boundary_charge": 6,
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    {
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      "interior_charge": 0,
      "boundary_charge": 0,
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    "energy_unit": "Y_2D H\u00b2; example input, no experimental parameter fit",
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  ],
  "source_consistency": {
    "eq16_extra_b": "Source PDF p12 literally includes b. The source-free equation1, equation22 and force17 instead require curvature-only Chi=Y/(24RzRphi)*(z\u00b2-H\u00b2/4)\u00b2.",
    "eq25_cutoff": "Evaluate dimensional equation23 directly; do not silently treat the separately printed a-prime as an independently verified dimensional core cutoff."
  },
  "limits": [
    "Topology alone does not determine extra neutral defects or their energetic benefit.",
    "Original SI weak-cylinder pair model; flat logarithmic interaction, core and geometric energy, not a full global defect configuration optimization.",
    "Optimizing the full pair shifts the geometric-only position; neither negative relative energy nor an illustrative separation path proves experimental nucleation rates.",
    "Frozen substrate geometry and modulus; bending, particle tracking, exact curved-surface Green function and driven spinner dynamics not reproduced."
  ]
}