{
  "model": "Heisenberg",
  "lattice": "pyrochlore-2x2x2",
  "n_sites": 32,
  "boundary": "P",
  "params": {},
  "instance_id": "Heisenberg/pyrochlore-2x2x2_32_P",
  "rows": [
    {
      "energy": -66.1514,
      "sigma": 0,
      "energy_variance": 0,
      "dof": 32,
      "einf": 0,
      "v_score": 0,
      "method": "Exact diagonalization",
      "bound_type": "exact",
      "bound_type_reason": "exact diagonalization|ex",
      "reference": "[paper](https://journals.aps.org/prx/abstract/10.1103/PhysRevX.11.041021)",
      "source": "varbench@2024-10-22",
      "provenance": "imported"
    },
    {
      "energy": -65.949,
      "sigma": 0.003,
      "energy_variance": 6.08,
      "dof": 32,
      "einf": 0,
      "v_score": 0.044733937675725685,
      "method": "RBM with symmetry projections",
      "bound_type": "variational",
      "bound_type_reason": "vmc|\\brbm\\b|\\brnn\\b|jast",
      "reference": "[paper](https://journals.aps.org/prx/abstract/10.1103/PhysRevX.11.041021)",
      "source": "varbench@2024-10-22",
      "provenance": "imported"
    },
    {
      "energy": -66.082,
      "sigma": 0.003,
      "energy_variance": 4.36,
      "dof": 32,
      "einf": 0,
      "v_score": 0.03194994466655219,
      "method": "mVMC with SU(2) and symmetry projections",
      "bound_type": "variational",
      "bound_type_reason": "vmc|\\brbm\\b|\\brnn\\b|jast",
      "reference": "[paper](https://journals.aps.org/prx/abstract/10.1103/PhysRevX.11.041021)",
      "source": "varbench@2024-10-22",
      "provenance": "imported"
    }
  ],
  "url": "https://qmbl.org/i/Heisenberg/pyrochlore-2x2x2_32_P/",
  "per_site_divisor": 128,
  "per_site_label": "E/N (S.S)",
  "record": {
    "energy": -66.082,
    "sigma": 0.003,
    "method": "mVMC with SU(2) and symmetry projections",
    "reference": "[paper](https://journals.aps.org/prx/abstract/10.1103/PhysRevX.11.041021)",
    "energy_per_site": -0.516265625
  },
  "no_record_reason": null
}