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                "CosmicExplorer": 0.0,
                "EinsteinTelescope": 2.220446049250313e-16,
                "aLIGOZeroDetHighPower": 2.220446049250313e-16
              },
              "relative_norm_error": 3.3029695326533984e-08
            }
          },
          "status": "PASSED"
        }
      }
    }
  ],
  "composition_version": "taylorf2-eccentric-nonspinning-e2-3pn/v1",
  "cwd": "/home/xangma/repos/diffgw-worktrees/eccentric-phase-reference",
  "device": "cpu",
  "detailed_projection_results": {
    "method": "Rerun tests.parity_harness.run_oracle_comparison(case, strict=True) for each frozen case and both backends with the JAX public-frontend adapter used by tests/test_taylorf2_eccentric_holdout.py",
    "raw_jsonl_sha256": "6d4e2eb94a2c02a6cb13e2f695991b42e40cc768b90b6a63444cf4c455c32a76"
  },
  "gate": {
    "complex_relative_l2": 1e-06,
    "mismatch": 1e-08
  },
  "harness": "tests.parity_harness.run_oracle_comparison(case, strict=True)",
  "host": "len",
  "id": "taylorf2-eccentric-nonspinning-e2-3pn-two-holdouts/2026-09-27",
  "limitations": [
    "two sampled cases, no domain-wide bound",
    "spinning and optional amplitude branches provisional",
    "hard cutoff boundary not sampled"
  ],
  "oracle": "LAL SimInspiralChooseFDWaveform(TaylorF2Ecc)",
  "precision": "float64/complex128",
  "scope": "nonspinning q<=2, 0<e0<=0.1, 3PN O(e0^2), amplitude off, explicit f0_ecc/f_ref, positive band below Schwarzschild ISCO",
  "source_base_commit": "526d08cc265912bdff4f79ef3ecf6233ea4c17dc",
  "test": "tests/test_taylorf2_eccentric_holdout.py",
  "versions": {
    "jax": "0.11.2",
    "jax_backend": "cpu",
    "lal": "7.7.1",
    "lalsimulation": "6.2.1",
    "torch": "2.14.0+cpu"
  }
}
