{
  "candidate": {
    "amplitude": -0.45,
    "position": 4.25,
    "IR_epsilon": 1e-09,
    "IR_cutoff": 0.01,
    "mu_at_zero": 1.0,
    "radial_stiffness_at_zero": 1.0,
    "numerical_force_splice_interval": [
      5e-05,
      0.0002
    ],
    "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
    "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
    "IR_spectral_coefficient": 1.00000010000001e-09,
    "shape_parameters_refitted": false,
    "metric_sector_derived_from_this_module": false,
    "galaxy_scale_m_s2": 1.5716639863145666e-10,
    "rar_rms_dex": 0.14717628635765218,
    "previous_rar_rms_same_grid_dex": 0.14717628635940785,
    "maximum_RAR_prediction_change_dex": 3.327009778786305e-10,
    "minimum_RAR_predicted_x": 0.07651872527871907,
    "rar_rows": 2693,
    "scale_refitted": false,
    "scope": "Frozen previous galaxy scale; full-sample spherical RAR proxy",
    "IR_parameter_acceleration_m_s2": 1.5716639863145667e-19,
    "IR_cutoff_acceleration_m_s2": 1.5716639863145666e-12
  },
  "cases": [
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.272536634684777,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.700228421e-11,
        "picard_iterations": 42,
        "cg_iterations": 59138,
        "quadrupole_coefficients": [
          -0.0032542289657699567,
          -0.0032364761737237535,
          0.0013244981113980992
        ],
        "Q2_s_minus2": [
          1.669731076710206e-27,
          1.660622194425119e-27,
          -6.795943619542223e-28
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 77.808
      },
      "field": "outputs/dark_micro/solar_da8d74d740e3b901.csv",
      "field_sha256": "642b1624a87aebf8a3f60f0bee41ca4e88a229fcb0d92ec0642488af6cc46f6e",
      "table": "outputs/dark_micro/solar_da8d74d740e3b901_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.0400000000000002e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.0400000000000002e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.2979873673784725,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.6092433518e-11,
        "picard_iterations": 42,
        "cg_iterations": 58046,
        "quadrupole_coefficients": [
          -0.002467698297175421,
          -0.0024495434846948114,
          0.0022809911501285125
        ],
        "Q2_s_minus2": [
          1.2661655274043588e-27,
          1.2568503701398952e-27,
          -1.1703668823344152e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 76.393
      },
      "field": "outputs/dark_micro/solar_bdf2d9f963b126b2.csv",
      "field_sha256": "b4d3a586fc7dfe82bbb8b846ba0c7eb8458bf33433bbc22c81180808802a867a",
      "table": "outputs/dark_micro/solar_bdf2d9f963b126b2_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.08e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.08e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.323438100072168,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 3.411631939e-11,
        "picard_iterations": 41,
        "cg_iterations": 58534,
        "quadrupole_coefficients": [
          -0.0017455124855910175,
          -0.001726919286951554,
          0.00317767151265827
        ],
        "Q2_s_minus2": [
          8.956150512560549e-28,
          8.86074959913277e-28,
          -1.6304497723032427e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 83.759
      },
      "field": "outputs/dark_micro/solar_08f12ad10a172195.csv",
      "field_sha256": "5ce02e28d07255d6051e01472157186327fe26e646c1583efd1ee9cbcbebbc91",
      "table": "outputs/dark_micro/solar_08f12ad10a172195_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.1200000000000002e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.1200000000000002e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.3488888327658637,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 3.025754332e-11,
        "picard_iterations": 41,
        "cg_iterations": 58660,
        "quadrupole_coefficients": [
          -0.00109479565494347,
          -0.0010757265341056507,
          0.004007524178956525
        ],
        "Q2_s_minus2": [
          5.617350060289639e-28,
          5.519507210252455e-28,
          -2.056243654843151e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 86.231
      },
      "field": "outputs/dark_micro/solar_c19cf175eb8a2777.csv",
      "field_sha256": "47b4eb8a70b4c4b534d5315762c647d2b765f59bd183baf10b2921d39799afc5",
      "table": "outputs/dark_micro/solar_c19cf175eb8a2777_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.1600000000000003e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.1600000000000003e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.3743395654595594,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.7454883509e-11,
        "picard_iterations": 41,
        "cg_iterations": 58737,
        "quadrupole_coefficients": [
          -0.0005230120901776348,
          -0.0005034266834057315,
          0.004763197458603242
        ],
        "Q2_s_minus2": [
          2.6835528466207224e-28,
          2.5830609553584855e-28,
          -2.4439764087881728e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 75.571
      },
      "field": "outputs/dark_micro/solar_f7b8e13e97393992.csv",
      "field_sha256": "234af3e940608bc6c588557e0ed8c5b685fc188ddfc5e2f5a28bf126dc862bec",
      "table": "outputs/dark_micro/solar_f7b8e13e97393992_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.2000000000000002e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.2000000000000002e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.3997902981532548,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.5557606677e-11,
        "picard_iterations": 41,
        "cg_iterations": 58524,
        "quadrupole_coefficients": [
          -3.677642854028316e-05,
          -1.6632080824997204e-05,
          0.005438176092918277
        ],
        "Q2_s_minus2": [
          1.8869829464994025e-29,
          8.533850111952114e-30,
          -2.79030508254963e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 75.413
      },
      "field": "outputs/dark_micro/solar_ba4a10333142003c.csv",
      "field_sha256": "00b8c79113459036d8ea15b6c00ea2d3eb418bc69ef4295854358e592cd086bd",
      "table": "outputs/dark_micro/solar_ba4a10333142003c_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.2400000000000003e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.2400000000000003e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.4252410308469503,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.0759876286e-11,
        "picard_iterations": 42,
        "cg_iterations": 58440,
        "quadrupole_coefficients": [
          0.00035756036524171354,
          0.0003783093731843604,
          0.0060262012299532345
        ],
        "Q2_s_minus2": [
          -1.8346270650402213e-28,
          -1.9410893445453362e-28,
          -3.092018285745134e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 77.667
      },
      "field": "outputs/dark_micro/solar_93ba2de0e5a0aaa1.csv",
      "field_sha256": "3d2e0fc473baaf7f4d51267cdf384d8f1979b19b6d1e659332a9b02041d24af6",
      "table": "outputs/dark_micro/solar_93ba2de0e5a0aaa1_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.2800000000000004e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.2800000000000004e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.450691763540646,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.1272884092e-11,
        "picard_iterations": 42,
        "cg_iterations": 58798,
        "quadrupole_coefficients": [
          0.0006529545558115072,
          0.0006743538477909363,
          0.006520336136904384
        ],
        "Q2_s_minus2": [
          -3.3502821251547216e-28,
          -3.460080984465146e-28,
          -3.3455568102012424e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 78.078
      },
      "field": "outputs/dark_micro/solar_9e4f6d0134be32e2.csv",
      "field_sha256": "009f968b19f5d60790c4ef140e07b484012c08fa04b3807a60415a84718b0a23",
      "table": "outputs/dark_micro/solar_9e4f6d0134be32e2_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.3200000000000003e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.3200000000000003e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.4761424962343415,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.1661183801e-11,
        "picard_iterations": 42,
        "cg_iterations": 59235,
        "quadrupole_coefficients": [
          0.0008423101691907715,
          0.0008644028186551198,
          0.006913585767504432
        ],
        "Q2_s_minus2": [
          -4.321857744247872e-28,
          -4.435214191398662e-28,
          -3.547331527353743e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 79.497
      },
      "field": "outputs/dark_micro/solar_128709ea79e73d61.csv",
      "field_sha256": "e90506fce47d06513fdebf292ff8813b59cfb132acf728b6c86ad82ee5365bd1",
      "table": "outputs/dark_micro/solar_128709ea79e73d61_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.3600000000000006e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.3600000000000006e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.5015932289280371,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.2431032064e-11,
        "picard_iterations": 42,
        "cg_iterations": 59576,
        "quadrupole_coefficients": [
          0.0009193671504001432,
          0.0009422150387767386,
          0.007199804449278795
        ],
        "Q2_s_minus2": [
          -4.717233845794924e-28,
          -4.834465391764465e-28,
          -3.694189118728113e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 79.689
      },
      "field": "outputs/dark_micro/solar_7f3b490278cdf803.csv",
      "field_sha256": "c302c3b24261a3e8982c22b3a79cec4b105ea1758f2b2860fc6383480b989e81",
      "table": "outputs/dark_micro/solar_7f3b490278cdf803_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.4e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.4e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.5270439616217324,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.9607440387e-11,
        "picard_iterations": 41,
        "cg_iterations": 60075,
        "quadrupole_coefficients": [
          0.0008781856266958753,
          0.0009018400252631125,
          0.0073731250578592126
        ],
        "Q2_s_minus2": [
          -4.5059331947387845e-28,
          -4.627302910281404e-28,
          -3.783119187701479e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 75.699
      },
      "field": "outputs/dark_micro/solar_a3604832b3b99558.csv",
      "field_sha256": "66a9242026923ea20e0abd84aa71601f5c65a9c999ea45fc9d32ee7aef041316",
      "table": "outputs/dark_micro/solar_a3604832b3b99558_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.44e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.44e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.5524946943154279,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.3194276524e-11,
        "picard_iterations": 42,
        "cg_iterations": 60535,
        "quadrupole_coefficients": [
          0.0007122527360182403,
          0.000736765978666803,
          0.0074271354578730265
        ],
        "Q2_s_minus2": [
          -3.6545385721503555e-28,
          -3.7803149802389575e-28,
          -3.810831694816749e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 76.332
      },
      "field": "outputs/dark_micro/solar_1a448e60fdb982b1.csv",
      "field_sha256": "325bb963082bb36b933e777fca077cf4a242f064b0ce7cbed98fd8bba5a44bdd",
      "table": "outputs/dark_micro/solar_1a448e60fdb982b1_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.48e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.48e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.5779454270091235,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 2.9879310246e-11,
        "picard_iterations": 42,
        "cg_iterations": 61348,
        "quadrupole_coefficients": [
          0.0004149970749405781,
          0.00044042880210783824,
          0.007355367978686225
        ],
        "Q2_s_minus2": [
          -2.1293323858303507e-28,
          -2.2598214990189256e-28,
          -3.774008105709827e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 106.965
      },
      "field": "outputs/dark_micro/solar_189de3af719e053f.csv",
      "field_sha256": "3fca79772028a34b6e232dcfba99d6d4d6e6583db13757497719e865aff9bdd5",
      "table": "outputs/dark_micro/solar_189de3af719e053f_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.52e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.52e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.603396159702819,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 4.2666758796e-11,
        "picard_iterations": 42,
        "cg_iterations": 61945,
        "quadrupole_coefficients": [
          -1.9360673868696613e-05,
          7.049151416825e-06,
          0.007152130063813765
        ],
        "Q2_s_minus2": [
          9.933879626987246e-30,
          -3.61688968690119e-30,
          -3.66972759379814e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 104.721
      },
      "field": "outputs/dark_micro/solar_4d5e643d9d17e04b.csv",
      "field_sha256": "44169e8404ef34a62646447bac521c13d3c924e2a7398ce8d5781e0f64df6e18",
      "table": "outputs/dark_micro/solar_4d5e643d9d17e04b_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.56e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.56e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.6288468923965145,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 6.4126666408e-11,
        "picard_iterations": 42,
        "cg_iterations": 62399,
        "quadrupole_coefficients": [
          -0.0005960351562016007,
          -0.0005685855094194078,
          0.00681228067901532
        ],
        "Q2_s_minus2": [
          3.058231100484855e-28,
          2.917388127359572e-28,
          -3.495352316223119e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 80.272
      },
      "field": "outputs/dark_micro/solar_3cfeee449777cd95.csv",
      "field_sha256": "da1764e66d1760f736f33e1a059ede68423cdbb82a0451d8f41c3e3dcf2c65a3",
      "table": "outputs/dark_micro/solar_3cfeee449777cd95_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.6000000000000003e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.6000000000000003e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.6542976250902102,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 9.6141399854e-11,
        "picard_iterations": 42,
        "cg_iterations": 62890,
        "quadrupole_coefficients": [
          -0.0013204586957067665,
          -0.001291903458598073,
          0.006330473576205547
        ],
        "Q2_s_minus2": [
          6.775217548996745e-28,
          6.6287018388093615e-28,
          -3.2481391357729095e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 80.972
      },
      "field": "outputs/dark_micro/solar_d2ccc11a6c1c3cf6.csv",
      "field_sha256": "f19aefaf8f6dcaeac7d8bdc33fa48e9f08faebe8cdb077596b4ccd722cee2b7b",
      "table": "outputs/dark_micro/solar_d2ccc11a6c1c3cf6_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    },
    {
      "spec": {
        "law": {
          "amplitude": -0.45,
          "position": 4.25,
          "IR_epsilon": 1e-09,
          "IR_cutoff": 0.01,
          "mu_at_zero": 1.0,
          "radial_stiffness_at_zero": 1.0,
          "numerical_force_splice_interval": [
            5e-05,
            0.0002
          ],
          "response": "mu_S=mu_previous_smoothed+B*(1/sqrt(x^2+epsilon^2)-1/sqrt(x^2+ell^2))",
          "IR_origin": "Ground energy of two harmonic modes minus a filled four-component fermionic doublet",
          "IR_spectral_coefficient": 1.00000010000001e-09,
          "shape_parameters_refitted": false,
          "metric_sector_derived_from_this_module": false
        },
        "scale": 1.5716639863145666e-10,
        "nr": 384,
        "nu": 288,
        "external": 2.64e-10,
        "rmin": 0.0003,
        "rmax": 40.0,
        "table_nodes": 60001,
        "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
        "response_source_sha256": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
        "solver_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05"
      },
      "result": {
        "model": "Table",
        "nr": 384,
        "nu": 288,
        "rmin": 0.0003,
        "rmax": 40,
        "external_acceleration_m_s2": 2.64e-10,
        "model_scale_m_s2": 1.5716639863145666e-10,
        "eta": 1.6797483577839056,
        "mu_floor": 0,
        "converged": true,
        "nonlinear_residual": 8.5852035357e-11,
        "picard_iterations": 43,
        "cg_iterations": 63875,
        "quadrupole_coefficients": [
          -0.0021982770369991154,
          -0.0021685521476414974,
          0.0057011463044539055
        ],
        "Q2_s_minus2": [
          1.127926621791162e-27,
          1.112674907165592e-27,
          -2.9252339824729975e-27
        ],
        "fit_windows": [
          [
            0.02,
            0.08
          ],
          [
            0.04,
            0.16
          ],
          [
            0.08,
            0.32
          ]
        ],
        "seconds": 98.512
      },
      "field": "outputs/dark_micro/solar_99bc50910fd910fb.csv",
      "field_sha256": "1c572de46859f6ff08a54a06eca6b84a6186a88e091c2c32e2402f297787ab43",
      "table": "outputs/dark_micro/solar_99bc50910fd910fb_table.csv",
      "table_sha256": "e5df03a2bad9fdcf31fed36fe5debfa030fbe535d00db2a7068093c1da24e4b9"
    }
  ],
  "solver": {
    "base_solver": {
      "original_source_sha256": "2dab4dfbb87656a33e64a69855a811e69ed344ad9c053c47387b81e911057a3b",
      "adapter_source_sha256": "af29309a14946e8d95e2a3b3c83d5356cc74d28ef46a0033f01f293539ec9bdc",
      "generated_source_sha256": "baee1545a77be40530f7fef2ee39687e2dc2324897e74acedf107a5ffa5e0377",
      "binary_sha256": "d151d4dbb3537df50a726ff400dab60fede0ec0be53bafe14afa795fe4568c1d",
      "rustc": "rustc 1.94.1 (e408947bf 2026-03-25)",
      "physical_change": "Optional mu(0) and a continuous linear core below the first table row",
      "original_source_unchanged": true
    },
    "adapter_source_sha256": "150d74074b5923b60b69df1d8cb84c0cfff8395385493498650080f2657544cd",
    "generated_source_sha256": "da6ac42930e038599902c659506281502608a16081c643e013b06ce530ea3e05",
    "binary_sha256": "f6b408a79f61e73f026396968bcdd652813c355cb90cf48a94596b474bfa1ebd",
    "interpolation": "Power-law intervals for table responses; increasing x*mu endpoints imply positive stiffness everywhere in each interval",
    "source_of_original_and_published_CMC_solvers_unchanged": true,
    "tests_log_sha256": "8a25044d504ce1a2f516749ed49b00e0c1e5d070512df874319cade152e46a93"
  },
  "source_sha256": "6b7c08cf5766343fd94805e7d5a3326546dc41abbf69123b9d32070ec0286c07",
  "stage": "fields",
  "input_sha256": {
    "dark_micro_response.py": "190d43ba132c061b94a74723b97817465a149685562eb8a0f5c4a4eff7085b45",
    "build_micro_solver.py": "150d74074b5923b60b69df1d8cb84c0cfff8395385493498650080f2657544cd",
    "dark_cmc_model.py": "63495c697f9521ed3f39be5785cb70964d1c45fc1bf9428210e6026955c5a50a",
    "dark_cmc_solar_checks.py": "e155e585f7188e4a35b3ae84176836e3a1d8c73ff9872d71a26d69cedd5cd799",
    "dark_cmc_report.py": "99df0b99b9ddd5534feb631c6a06da7113a51c7dc94b0aa577c5e2b2193ea1c6",
    "MICRO_MACRO_PROTOCOL.md": "8174967caf964f66e5541face5cad38be7943315385b050f59ed5a7f9e160469",
    "outputs/dark_cmc/publication_summary.json": "540668ab708ccfc209e7045099d04b26cfaae35238ced88a0559e166fa89fcde"
  }
}