{
  "visual_id": "E24-correlated-clusters",
  "title": "Correlated finite nuclei through oxygen-16",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260930T164749835215Z-E35-finite-clusters"
  ],
  "claim_ids": [
    "C02",
    "C06"
  ],
  "input_files": [
    {
      "path": "runs/20260930T164749835215Z-E35-finite-clusters/finite-range-correlations.csv",
      "sha256": "a77031d20a2251cba39adb514b8cd61e181f7cfe376728b23668aa4644f523db"
    }
  ],
  "configurations": {
    "E35-finite-clusters": {
      "parents": [
        "20260930T010050322377Z-E35-lattice-HF",
        "20260930T015504482144Z-E35-lattice-matching",
        "20260930T030807570905Z-E35-finite-CCSD"
      ],
      "L": [
        3,
        4
      ],
      "A": [
        4,
        8,
        12,
        16
      ],
      "a_inverse_MeV": 0.01,
      "gA": 1.287,
      "mass_MeV": 938.92,
      "m_pi_MeV": 134.98,
      "f_pi_MeV": 92.2,
      "iteration_fixed_point_tolerance": 1e-10,
      "maximum_iterations": 1200,
      "solver": "real-coefficient DIIS for complex amplitudes",
      "damping": 0.25,
      "history": 8,
      "DIIS_SVD_cutoff": 1e-10,
      "amplitude_tolerance": 2e-06,
      "exact_A2_tolerance_MeV": 2e-05,
      "contractions": "CSR finite-sum acceleration, checked against upstream complex diagrams",
      "kinetic_representation": "include explicit zero entries so source Fock construction retains all interaction contractions",
      "initial_singles": "best ordinary HF Thouless amplitudes; pivoted-QR site reference",
      "initial_doubles": "verified saved amplitudes where available; otherwise zero",
      "recovery_parent": "20260930T042010353624Z-E35-finite-clusters"
    }
  },
  "assumptions": {
    "E35-finite-clusters": [
      "Use the same pinned finite-range A/B two-body Hamiltonians as the independently matched mean-field calculation, without refitting.",
      "The complex source CCSD equations retain OPE spin mixing. Test the exact two-nucleon limit against an independent Fourier Hamiltonian.",
      "There is no three-body operator in this A/B Hamiltonian: the on-site benchmark NO2B error is absent, while CCSD state truncation remains.",
      "Larger-nucleus references use pivoted QR of the occupied HF orbitals to choose well-conditioned localized sites; no interaction or measured datum is adjusted. The alpha control must reproduce the previous result under this translated reference.",
      "Replace only the sparse particle-only contraction loops by CSR matrix products; compare random complex contractions against the original routines before every solve.",
      "The source Fock builder skips an interaction contraction when the corresponding kinetic entry is absent. Supply every kinetic entry, including exact zeros, and verify the result against the full independent Wick field. Preserve and report the literal sparse-input discrepancy.",
      "The frozen pair/alpha parent supplies exact two-body connected-equation controls. This run repeats the alpha energy as a reserved reference-change check, then predicts larger nuclei from HF singles and zero doubles.",
      "The unchanged source amplitude equations are solved with real-coefficient, SVD-stabilized DIIS on complex coordinates. Original nonconverged source iterations remain archived.",
      "Compare finite alpha energies to the existing best Hartree-Fock values. A CCSD energy is not a variational bound or an infinite-volume prediction.",
      "Two volumes do not provide a thermodynamic phase boundary, finite-field response, interface energy or lifetime.",
      "If recovering an external interruption, reuse only saved amplitudes with frozen interruption hashes; rebuild and recheck every operator, contraction, energy and residual. Never copy a lost validation verdict. Pairwise residual inner products avoid duplicated large DIIS histories without changing their metric."
    ]
  },
  "plotted_values": {
    "path": "E24-correlated-clusters-data.json",
    "sha256": "ad595b77ea6affb488595b7c798a778389a7cdd83877943e4da52ac1c2313fdf"
  },
  "caption": "Sixteen CCSD solutions use the previously audited finite-range A/B two-body Hamiltonians, in two periodic boxes and at A=4,8,12,16. No three-body NO2B approximation enters this Hamiltonian. Pivoted QR selects localized references with nonzero overlap with the existing best HF state; it changes no interaction. The alpha energy is reserved to check the reference change. Every final energy has independent complex-contraction, Wick-field and fixed-point checks. An interrupted predecessor is retained; saved amplitudes only initialize recomputed and rechecked roots. The right panel compares computed finite-box energies with computed alphas in that same box. CCSD is nonvariational, two volumes are not an infinite-volume extrapolation, and a negative energy difference does not establish a thermodynamic phase, lifetime or physical field trajectory.",
  "alt_text": "Correlations shift the energies of the tested finite nuclei. Interaction and box size also change their relation to the same-box alpha threshold; these are finite-system diagnostics.",
  "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": "5c27b1dbacbf88a8c935f2542193b844ed3b3fae52cddf48a8c5755ed11f8c3b",
    "png": "d46221e1382e03f06723e644448f8d3d7ee8cddfb523659d6359c2106db8bbb4"
  }
}