{
  "visual_id": "E53-nonspherical-controls",
  "title": "Finite-time angular field perturbations with work and flux accounting",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261002T033859036026Z-W27-W30-nonspherical"
  ],
  "claim_ids": [
    "C04",
    "C06"
  ],
  "input_files": [
    {
      "path": "runs/20261002T033859036026Z-W27-W30-nonspherical/fine.npz",
      "sha256": "946d26c8fc0ef9b907defa363fd3d07e571a5e8935d9fe7f75dbaff9a10d759e"
    },
    {
      "path": "runs/20261002T033859036026Z-W27-W30-nonspherical/array-schema.json",
      "sha256": "3b096fe03ad101605c77260830f2c4cce564c00664b689cc697dbe2f5fd4fdcc"
    },
    {
      "path": "runs/20261002T033859036026Z-W27-W30-nonspherical/results.json",
      "sha256": "5dff7a19753d65d3f950d3b6634ed9d7716071742bbb4134aed9c68aebbe298d"
    }
  ],
  "configurations": {
    "W27-W30-nonspherical": {
      "epsilon": 0.1,
      "duration_mass_times": 200.0,
      "modes": [
        1,
        2,
        2,
        3
      ],
      "perturbation_amplitudes": [
        0.0001,
        0.0001,
        0.0002,
        0.0001
      ],
      "cases": [
        {
          "label": "base",
          "dr": 0.2,
          "dt": 0.04,
          "outer": 120.0
        },
        {
          "label": "fine",
          "dr": 0.1,
          "dt": 0.02,
          "outer": 120.0
        },
        {
          "label": "time",
          "dr": 0.2,
          "dt": 0.02,
          "outer": 120.0
        },
        {
          "label": "box",
          "dr": 0.2,
          "dt": 0.04,
          "outer": 180.0
        }
      ],
      "absorber_start_fraction": 0.8,
      "core_radius": 60.0,
      "seed_radius": 10.0,
      "energy_relative_gate": 0.005,
      "translation_relative_gate": 0.03,
      "early_comparison_duration": 40.0,
      "grid_relative_gate": 0.03,
      "vacuum_frequency_relative_gate": 0.002,
      "tensor_source_relative_gate": 1e-07,
      "tensor_work_relative_gate": 0.0002,
      "threads": 1,
      "whole_run_timeout_seconds": 600,
      "maximum_RSS_bytes": 3221225472,
      "scope": "Linear nonspherical finite-time classical phi6 controls and analytic TT/energy normalization; no nonlinear lifetime, formation, population or detector forecast",
      "pilot": false
    }
  },
  "assumptions": {
    "W27-W30-nonspherical": [
      "V(phi)=phi\u00b2/2\u2212phi\u2074/4+phi\u2076/6; fixed classical initial data, no formation model.",
      "Linear angular modes u_l=r*delta_phi_l satisfy u_tt=u_rr\u2212[l(l+1)/r\u00b2+V\u2033(phi0)]u.",
      "Mode energy exchanges work 1/2 integral u\u00b2 partial_t V\u2033 dr with prescribed radial background; no perturbation backreaction is included.",
      "TT projector and externally prescribed tensor source are normalization controls, not a predicted gravitational signal.",
      "Diatomic chemistry is not coupled to this rapidly varying classical field."
    ]
  },
  "plotted_values": {
    "path": "E53-nonspherical-controls-data.json",
    "sha256": "06b3e863869dd72fc28b89cc719b1733ddf6261793f926ccaab274975d6b97cd"
  },
  "caption": "Linear l=1,2,3 perturbations evolve on a radial canonical phi-six background for200 inverse-mass units. Unit angular norm and the canonical radial core-energy boundary convention are explicit. The l=1 seed tests translations; l=2/3 are particular finite seeds. Independent adaptive integration and grid/time/box controls verify these curves. Work from the time-dependent background is retained. Boundary absorption does not yet define a radiation lifetime. Finite-time seeded behavior supplies neither full nonlinear/Floquet stability nor physical formation, abundance or a gravitational signal.",
  "alt_text": "The selected mode norms oscillate below their initial values while the fine-grid core energy, outgoing flux and background work agree to about two parts in ten thousand.",
  "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": "8cc4419347046483357ad5aa9c3253eae8feeb17fd65af5736d2fe04504e1ee6",
    "png": "3e471d5a006943f50d0f3d14de029d83a580103585645f4b44a0ac54e20a239a"
  }
}