{
  "visual_id": "E81-axisymmetric-backreaction",
  "title": "Resolved nonlinear angular feedback in a finite field evolution",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261003T023731930584Z-W27-axisymmetric-production"
  ],
  "claim_ids": [
    "C06"
  ],
  "input_files": [
    {
      "path": "runs/20261003T023731930584Z-W27-axisymmetric-production/base.npz",
      "sha256": "dacb1b5202fcec616a6efdf9550794d755c24ef5c6dc317b86a34f8bb8d3e2d5"
    },
    {
      "path": "runs/20261003T023731930584Z-W27-axisymmetric-production/results.json",
      "sha256": "cde369048e6fdfd0b304413dbca30d9e8d2e661e015d7cf6aa4935980c0fb80e"
    },
    {
      "path": "runs/20261003T023731930584Z-W27-axisymmetric-production/array-schema.json",
      "sha256": "52ad8f8863215dbee5c70f28b98f80bd9157da4da5515ad8ff8829dd17556390"
    }
  ],
  "configurations": {
    "W27-axisymmetric-production": {
      "stage": "preregistered_production",
      "epsilon": 0.1,
      "potential": "phi^2/2-phi^4/4+phi^6/6",
      "amplitudes": [
        0.0001,
        0.001
      ],
      "seed_radius": 10.0,
      "core_radius": 60.0,
      "absorber_start_fraction": 0.8,
      "energy_relative_gate": 0.005,
      "waveform_relative_gate": 0.03,
      "threads": 1,
      "whole_run_timeout_seconds": 600,
      "maximum_RSS_bytes": 3221225472,
      "scope": "Finite-time even axisymmetric nonlinear conditional classical dynamics; no general 3D stability, formation or lifetime",
      "duration_mass_times": 200.0,
      "save_every_mass_times": 1.0,
      "benchmark_run": "20261003T023151938798Z-W27-axisymmetric-benchmark",
      "cases": [
        {
          "label": "base",
          "dr": 0.2,
          "dt": 0.02,
          "outer": 120.0,
          "lmax": 6
        },
        {
          "label": "l4",
          "dr": 0.2,
          "dt": 0.02,
          "outer": 120.0,
          "lmax": 4
        },
        {
          "label": "l8",
          "dr": 0.2,
          "dt": 0.02,
          "outer": 120.0,
          "lmax": 8
        },
        {
          "label": "space",
          "dr": 0.1,
          "dt": 0.02,
          "outer": 120.0,
          "lmax": 6
        },
        {
          "label": "time",
          "dr": 0.2,
          "dt": 0.01,
          "outer": 120.0,
          "lmax": 6
        },
        {
          "label": "box",
          "dr": 0.2,
          "dt": 0.02,
          "outer": 180.0,
          "lmax": 6
        }
      ],
      "waveform_contract": "Core-node common-mode concatenated all-snapshot L2 relative to reference same induced mode; .03 for dr,dt,R,lmax,small-amplitude tangent, and A^2 l0/l4 amplitude scaling. No floor/jitter.",
      "initialization": "phi=.1*f(.1*r)+A*(e/2)*(r/10)^2 exp(-r^2/200)*Y20; seed continuum maximum1 at r=sqrt(2)*10 independent of grid; exact BVP spline envelope, not epsilon series; all momenta zero; endpoint field forced zero; u_l=r*phi_l; even parity only.",
      "core_interface": "nodes r<60 plus half spring at 60-dr/2; canonical u flux, not radiative power",
      "preserved_pilot_run": "20261003T023541561134Z-W27-axisymmetric-production",
      "pilot_difference": "Pilot used sampled seed maximum, causing1.5666e-5 grid-dependent amplitude difference. Final uses analytic2/e maximum; all gates/window unchanged."
    }
  },
  "assumptions": {
    "W27-axisymmetric-production": [
      "Specified finite-time initial condition only; no formation, general 3D stability or lifetime.",
      "Exact polynomial difference representation of nonlinear Galerkin equations; fixed mass/reference units."
    ]
  },
  "plotted_values": {
    "path": "E81-axisymmetric-backreaction-data.json",
    "sha256": "8cd1afa8e2ef84a34f7e1f68c10480f1e51c3513275f4d354861af4135fac7a5"
  },
  "caption": "The canonical phi6 field starts from the same radial envelope with quadrupole amplitudes A=1e\u22124 and 1e\u22123. Solid and dashed curves nearly coincide after division by A\u00b2; the independently measured l0/l4 scaling discrepancies are 0.00150 and 0.00337. The right panel takes the worst all-snapshot core waveform discrepancy over both amplitudes and l0/l2/l4, normalized to each reference mode rather than the large spherical background. Angular truncations reach lmax8. Fixed-boundary and damping energy ledgers pass separately. This is a finite-time even-axisymmetric control, not a general three-dimensional lifetime or outgoing-radiation prediction.",
  "alt_text": "The two perturbation amplitudes generate nearly matching scaled induced modes; all four refinement comparisons stay below the unchanged threshold.",
  "generator": "src/metastable/public_report.py",
  "generator_sha256": "9e263878b7237d781a41d94693004412279b5cfa808ccd6e335b7b07269910d4",
  "generator_dependencies_sha256": {
    "src/metastable/render.py": "ff4837be5102588b6614aeb2b7880b10c0a0c20a155e2eb7b409014a47a3de01",
    "src/metastable/spin_report.py": "dd5c64c5c658938948672a7dc767aa02c34dde012c3fc4aedfc3642f88796847",
    "src/metastable/continuation_report.py": "f9bbce6d0e201a9f55c826d6e9c47ab901e51a71b4a1f962b52eb08a63ba5fe9",
    "src/metastable/refinement_report.py": "4539c0ec814603105ab3a2b5cc82ce291c0151113b5bd3916cdc235aadb9bfb0",
    "src/metastable/atomic_mass_report.py": "46dd1cdb56a5a02cafe001a1f6a7fb201e149461850df41e012f77a580c3694b",
    "src/metastable/closure_report.py": "b34a03a9e0058eed65722df542dbb92691dd138787e2078b43ee9f18e221f75c",
    "src/metastable/october_report.py": "f93e7f89e43165d8d25e2184b9b32e6e21c3e1ffe66020d35944f263aaecb726",
    "src/metastable/october_followup_report.py": "925d905ff3bddf97a7ace2f68a4a28e7dfea2238c4f81d891dda2a9e70c6d4f6",
    "src/metastable/october_dynamics_report.py": "6b8d84c0ce0d78f52d064c68697f0d9c885cdc736e215b54eba46821dbe59a33",
    "src/metastable/october_calibration_report.py": "f714ef7ccfaa26e847c6135054f53528b3ff1d7096e7d113cffeea333e77e3d2",
    "src/metastable/october_interface_report.py": "2fc8826a33c952d7898154f84830748c26842c9a165d14aa7b7fb9721fac00bd",
    "src/metastable/october_checkpoint8_report.py": "f3b54f23510b9bfeffc5ff04e6df54e967228f43ba25a15e12e34f898cdfe0af",
    "src/metastable/october_checkpoint9_report.py": "4bd987aac59964ccb4768a95e0cb6f7d1fdccbeffe9483860da7b431f2224ae4",
    "src/metastable/october_checkpoint10_report.py": "9da673d773b63298e041914447ffd97065c1cf2b8966c90fc4ebcbee25a0ed63",
    "src/metastable/october_checkpoint11_report.py": "5f01064f02f4c76d0059d348a763b285c92c3677e6cb0ba0bbf7faa1a4b98248",
    "src/metastable/october_checkpoint12_report.py": "46022030652e3a1e274dfd27b36dfab25d90a97fde439b1da44d6f1fdc5140b5",
    "src/metastable/october_checkpoint13_report.py": "997c59be3af1b6b7be95fd4314e0f3b98c562629901a639572284045a65980c2",
    "src/metastable/october_checkpoint14_report.py": "d84de7d8516d8a4d8e21b5f9f279476f3035f719c1c8ab03b7ac1e44bf822240",
    "src/metastable/october_checkpoint15_report.py": "1f6e17b9549dc31fbb58ba578c4d8ed8e219b4ad30810df0a9d7d2d00e63efdc",
    "src/metastable/october_checkpoint16_report.py": "74cb8aac45d1d5ce0e6eb6678e9b6cdf98cd46fd6e264a513b612ab763fcd034",
    "src/metastable/october_checkpoint17_report.py": "9daceb74e91f6f8db0f7d89929226d46c464c284d06d0694f525fecf0c736bf6",
    "src/metastable/october_checkpoint18_report.py": "f33f88e316cae93af87cef75d8df41ce82970c8f8bc466dd7a094a92c5f00f8b",
    "src/metastable/october_checkpoint19_report.py": "ce2250507145354b6478cafaaff98c2b8ae2795c3c309f0d903a920365a77090",
    "src/metastable/october_checkpoint20_report.py": "e2ea0a8a374036254008cf6de8f10352dfb2585c4ccb18c1e850c017e6128294",
    "src/metastable/october_checkpoint21_report.py": "596b873676167227b2c92d358fcdbc0614908a5a9daad1da6227b81fce203eec",
    "src/metastable/publication_files.py": "e68bd0ee4e849a72fa828f0cfcf34cb6b1b9f2a8bbdbb3d51085054915039607"
  },
  "command": "python run.py full public-report",
  "output_sha256": {
    "svg": "d41e77760e5e59104a01c7aa1d71d923e161702d2164a92880313cfc44e04797",
    "png": "88ed8e42e2af348938761cd334228b41956a04f013d7158a84b42b7ba3dea45b"
  }
}