{
  "visual_id": "E19-finite-range-HF",
  "title": "Mean-field tests of the source A/B interactions",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260930T010050322377Z-E35-lattice-HF",
    "20260930T011129639631Z-E35-HF-stability"
  ],
  "claim_ids": [
    "C02",
    "C06"
  ],
  "input_files": [
    {
      "path": "runs/20260930T010050322377Z-E35-lattice-HF/finite-range-HF.csv",
      "sha256": "1f0d26d0f1f0aeb68f586fce663837acd6a0738876f0fd28218b04a0977ab190"
    },
    {
      "path": "runs/20260930T010050322377Z-E35-lattice-HF/all-HF-starts.csv",
      "sha256": "6e9a76f5c62850b440097ebc9113bcef345f0d1079a57699daaa392ac5bbffb0"
    },
    {
      "path": "runs/20260930T011129639631Z-E35-HF-stability/orbital-stability.csv",
      "sha256": "758afb2efb780c233ac13fc53d60386c74d4761e72b0411d21fb3dc55affd4a1"
    }
  ],
  "configurations": {
    "E35-lattice-HF": {
      "L": [
        3,
        4
      ],
      "A": [
        4,
        8,
        12,
        16
      ],
      "a_inverse_MeV": 0.01,
      "internal_occupancy": "four species per spatial orbital",
      "gA": 1.287,
      "mass_MeV": 938.92,
      "m_pi_MeV": 134.98,
      "f_pi_MeV": 92.2,
      "seeds": [
        0,
        314
      ],
      "mix": 0.5,
      "density_tolerance": 1e-09,
      "maximum_iterations": 6400
    },
    "E35-HF-stability": {
      "parent": "20260930T010050322377Z-E35-lattice-HF",
      "curvature_zero_tolerance_MeV": 1e-05,
      "finite_difference_step": 0.001
    }
  },
  "assumptions": {
    "E35-lattice-HF": [
      "Use the pinned public NuLattice finite-range A/B operators, including OPE, without refitting.",
      "Apply its explicit NLEFT constants to both families. The B example omits these keyword arguments and would otherwise inherit different constants.",
      "This is the continuous Hamiltonian, not the original finite-time transfer matrix. The pinned source gA=1.287 differs from the original rounded 1.29.",
      "Restrict to spin/isospin-saturated real Slater determinants with four internal species per spatial orbital. No claim of an unrestricted or correlated ground state.",
      "The reduced contraction is checked against the public full one-body contraction and an independent energy derivative.",
      "Two spatial starts and two periodic volumes test this mean-field calculation. No infinite-volume or thermodynamic phase claim follows.",
      "All nonconverged attempts are retained; a stationary branch need not be the global minimum."
    ],
    "E35-HF-stability": [
      "Evaluate every real occupied/unoccupied orbital rotation in the parent four-species-saturated Slater space.",
      "The Hessian includes both orbital energy differences and the residual interaction from the same stored source Hamiltonian.",
      "Check curvature by independently rotating the orbitals with a matrix exponential and differentiating the total energy.",
      "A negative eigenvalue proves a saddle in this space. A positive Hessian is only a local minimum in this restricted space, not a full many-body metastable state.",
      "Spin/isospin-breaking fluctuations, correlations, zero-point motion, interface formation and decay rates are not inferred."
    ]
  },
  "plotted_values": {
    "path": "E19-finite-range-HF-data.json",
    "sha256": "e355312f97b072ade6c8856bcec67bb1f6ad2c1e37f5b92b5e18442e2538d623"
  },
  "caption": "The pinned public finite-range A/B operators, including pion exchange, are evaluated in spin/isospin-saturated Slater determinants at two periodic volumes. A reduced contraction agrees with the full source operator and its energy derivative. Both spatial starts pass density and commutator checks; their sometimes large energy difference is retained, and neither is guaranteed to be the global minimum. An independent orbital-Hessian audit finds all 32 states locally stable within the real saturated Slater space. The next figure expands that test to independent complex spinors. Source NLEFT constants are applied to both families. This is a continuous-Hamiltonian mean-field calculation, not the original finite-time correlated lattice calculation. Finite-volume breakup diagnostics and different local minima do not determine a thermodynamic phase boundary, barrier or lifetime.",
  "alt_text": "Interaction B produces stronger collective binding in the tested mean-field states. Large differences between spatial starts and finite volumes limit the inference.",
  "generator": "src/metastable/public_report.py",
  "generator_sha256": "9e263878b7237d781a41d94693004412279b5cfa808ccd6e335b7b07269910d4",
  "generator_dependencies_sha256": {
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    "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": "98e4085b1cb5f1aa5df34f97bd589a8afbe8413464922ea39872dc8904eb708f",
    "png": "38094ab36ba50524398225630faf2f9070793796a8bf19bf529041af9d21b250"
  }
}