turbomole.nomadmetainfo.json

{
  "type": "nomad_meta_info_1_0",
  "description": "meta info used by the TURBOMOLE parser, all names are expected to start with x_turbomole_",
  "dependencies": [ {
      "relativePath": "common.nomadmetainfo.json"
    }, {
      "relativePath": "meta_types.nomadmetainfo.json"
    }],
  "metaInfos": [ {
      "description": "CC2 total energies",
      "dtypeStr": "f",
      "name": "x_turbomole_CC2_total_energy_final",
      "repeats": true,
      "shape": [],
      "superNames": [
        "energy_component",
        "section_single_configuration_calculation"
      ],
      "units": "J"
    }, {
      "description": "CCSD total energies",
      "dtypeStr": "f",
      "name": "x_turbomole_CCSD_total_energy_final",
      "repeats": true,
      "shape": [],
      "superNames": [
        "energy_component",
        "section_single_configuration_calculation"
      ],
      "units": "J"
    }, {
      "description": "CCSD(T) total energies",
      "dtypeStr": "f",
      "name": "x_turbomole_CCSDparT_total_energy_final",
      "repeats": true,
      "shape": [],
      "superNames": [
        "energy_component",
        "section_single_configuration_calculation"
      ],
      "units": "J"
    }, {
      "description": "The label of the atoms in the system",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_atom_label",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "The number of atoms in the system",
      "dtypeStr": "f",
      "name": "x_turbomole_controlIn_atom_number",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "Status mean here ON or OFF",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_basis_status",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "Status mean here ON or OFF",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_cartesian_status",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "f",
      "name": "x_turbomole_controlIn_damping_parameter_min",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "f",
      "name": "x_turbomole_controlIn_damping_parameter_start",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "f",
      "name": "x_turbomole_controlIn_damping_parameter_step",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "Status mean here ON or OFF",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_dipole_status",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "Status mean here ON or OFF",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_global_status",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "Status mean here ON or OFF",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_hessian_status",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "Status mean here ON or OFF",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_interconversion_status",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "f",
      "name": "x_turbomole_controlIn_number_of_integral_stored",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "The kind of operating system",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_operating_system",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_pople_kind",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "i",
      "name": "x_turbomole_controlIn_scf_conv",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "i",
      "name": "x_turbomole_controlIn_scf_iter_limit",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_scfintunit_file",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "i",
      "name": "x_turbomole_controlIn_scfintunit_size",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "i",
      "name": "x_turbomole_controlIn_scfintunit_unit",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "The given symmetry of the system",
      "dtypeStr": "C",
      "name": "x_turbomole_controlIn_symmetry",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "-",
      "dtypeStr": "i",
      "name": "x_turbomole_controlIn_time_for_integral_calc",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "type of the used correlation functional",
      "dtypeStr": "C",
      "name": "x_turbomole_functional_type_correlation",
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "type of the used exchange functional",
      "dtypeStr": "C",
      "name": "x_turbomole_functional_type_exchange",
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "The integration cells",
      "dtypeStr": "i",
      "name": "x_turbomole_controlInOut_grid_integration_cells",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_functionals"
      ]
    }, {
      "description": "type of the used grid integration",
      "dtypeStr": "C",
      "name": "x_turbomole_controlInOut_grid_integration",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_functionals"
      ]
    }, {
      "description": "Type of the partition function used",
      "dtypeStr": "C",
      "name": "x_turbomole_controlInOut_grid_partition_func",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_functionals"
      ]
    }, {
      "description": "Sharpness of the partition function",
      "dtypeStr": "i",
      "name": "x_turbomole_controlInOut_grid_partition_sharpness",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_functionals"
      ]
    }, {
      "description": "Grid points number",
      "dtypeStr": "i",
      "name": "x_turbomole_controlInOut_grid_points_number",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_functionals"
      ]
    }, {
      "description": "The size of the radial grid",
      "dtypeStr": "i",
      "name": "x_turbomole_controlInOut_grid_radial_grid_size",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_functionals"
      ]
    }, {
      "description": "The radial integration type",
      "dtypeStr": "C",
      "name": "x_turbomole_controlInOut_grid_radial_integration",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_functionals"
      ]
    }, {
      "description": "The size of the used grid",
      "dtypeStr": "i",
      "name": "x_turbomole_controlInOut_grid_size",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_functionals"
      ]
    }, {
      "description": "D1 diagnostic of CCSD",
      "dtypeStr": "f",
      "name": "x_turbomole_D1_diagnostic",
      "repeats": true,
      "shape": [],
      "superNames": [
        "energy_component",
        "section_single_configuration_calculation"
      ]
    }, {
      "description": "change of the eigenvalues in the current SCF iteration",
      "dtypeStr": "f",
      "name": "x_turbomole_delta_eigenvalues",
      "shape": [],
      "superNames": [
        "energy_component",
        "section_scf_iteration"
      ],
      "units": "J"
    }, {
      "description": "Correlation energy at a given eigenstate from perturbative GW",
      "dtypeStr": "f",
      "name": "x_turbomole_eigenvalue_correlation_perturbativeGW",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_eigenvalues_GW"
      ],
      "units": "J"
    }, {
      "description": "Exact exchange energy at given eigenstate from perturbative GW",
      "dtypeStr": "f",
      "name": "x_turbomole_eigenvalue_ExactExchange_perturbativeGW",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_eigenvalues_GW"
      ],
      "units": "J"
    }, {
      "description": "Self-energy at a given eigenstate from perturbative GW",
      "dtypeStr": "f",
      "name": "x_turbomole_eigenvalue_ExchangeCorrelation_perturbativeGW",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_eigenvalues_GW"
      ],
      "units": "J"
    }, {
      "description": "KS exchange correlation energy at a given eigenstate needed to calculate the quasi-particle energy in perturbative GW",
      "dtypeStr": "f",
      "name": "x_turbomole_eigenvalue_ks_ExchangeCorrelation",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_eigenvalues_GW"
      ],
      "units": "J"
    }, {
      "description": "KS ground state energy at a given eigenstate needed in perturbative GW",
      "dtypeStr": "f",
      "name": "x_turbomole_eigenvalue_ks_GroundState",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_eigenvalues_GW"
      ],
      "units": "J"
    }, {
      "description": "Quasiparticle energy at a given eigenstate from perturbative GW",
      "dtypeStr": "f",
      "name": "x_turbomole_eigenvalue_quasiParticle_energy",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_eigenvalues_GW"
      ],
      "units": "J"
    }, {
      "description": "Charges of the point charges in the unit cell used by the PCEEM embedding model",
      "dtypeStr": "f",
      "name": "x_turbomole_pceem_charges",
      "shape": [
        "number_of_atoms"
      ],
      "superNames": [
        "section_system"
      ]
    }, {
    "description": "Total energy contribution from one-electron integrals",
      "dtypeStr": "f",
      "name": "x_turbomole_energy_1electron_scf_iteration",
      "shape": [],
      "superNames": [
        "energy_component",
        "section_scf_iteration"
      ],
      "units": "J"
    }, {
      "description": "Damping of the two-electron contributions to Fock matrix in the present SCF iteration",
      "dtypeStr": "f",
      "name": "x_turbomole_damping_scf_iteration",
      "shape": [],
      "superNames": [
        "section_scf_iteration"
      ]
    }, {
      "description": "Total energy contribution from two-electron integrals",
      "dtypeStr": "f",
      "name": "x_turbomole_energy_2electron_scf_iteration",
      "shape": [],
      "superNames": [
        "energy_component",
        "section_scf_iteration"
      ],
      "units": "J"
    }, {
      "description": "TODO:",
      "dtypeStr": "f",
      "name": "x_turbomole_ExchangeCorrelation_perturbativeGW_derivation",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_eigenvalues_GW"
      ]
    }, {
      "description": "Determines whether a geoemtry optimization is converged.",
      "dtypeStr": "C",
      "name": "x_turbomole_geometry_optimization_converged",
      "repeats": false,
      "shape": [],
      "superNames": [
        "section_run"
      ]
    }, {
      "description": "Maximum multipole moment used in the PCEEM embedding",
      "dtypeStr": "i",
      "name": "x_turbomole_pceem_max_multipole",
      "shape": [],
      "superNames": [
        "section_system"
      ]
    }, {
      "description": "Norm of the DIIS error in an SCF-iteration",
      "dtypeStr": "f",
      "name": "x_turbomole_norm_diis_scf_iteration",
      "shape": [],
      "superNames": [
        "section_scf_iteration"
      ]
    }, {
      "description": "Maximal resid. norm for Fia-block in an SCF-iteration",
      "dtypeStr": "f",
      "name": "x_turbomole_norm_fia_scf_iteration",
      "shape": [],
      "superNames": [
        "section_scf_iteration"
      ]
    }, {
      "description": "Maximal resid. fock norm in an SCF-iteration",
      "dtypeStr": "f",
      "name": "x_turbomole_norm_fock_scf_iteration",
      "shape": [],
      "superNames": [
        "section_scf_iteration"
      ]
    }, {
      "description": "Minimum separation between cells in PCEEM embedding for periodic fast multipole treatment",
      "dtypeStr": "f",
      "name": "x_turbomole_pceem_min_separation_cells",
      "shape": [],
      "superNames": [
        "section_system"
      ]
    }, {
      "description": "MP2 total energies",
      "dtypeStr": "f",
      "name": "x_turbomole_MP2_total_energy_final",
      "repeats": true,
      "shape": [],
      "superNames": [
        "energy_component",
        "section_single_configuration_calculation"
      ],
      "units": "J"
    }, {
      "description": "Multipole precision parameter for PCEEM embedding",
      "dtypeStr": "f",
      "name": "x_turbomole_pceem_multipole_precision",
      "shape": [],
      "superNames": [
        "section_system"
      ]
    }, {
      "description": "compute node",
      "dtypeStr": "C",
      "name": "x_turbomole_nodename",
      "shape": [],
      "superNames": [
        "section_run"
      ]
    }, {
      "description": "orbital with the largest residual norm for the Fia block in this iteration",
      "dtypeStr": "C",
      "name": "x_turbomole_norm_fia_orbital_scf_iteration",
      "shape": [],
      "superNames": [
        "section_scf_iteration"
      ]
    }, {
      "description": "orbital with the largest residual Fock norm in this iteration",
      "dtypeStr": "C",
      "name": "x_turbomole_norm_fock_orbital_scf_iteration",
      "shape": [],
      "superNames": [
        "section_scf_iteration"
      ]
    }, {
      "description": "Final potential energy",
      "dtypeStr": "f",
      "name": "x_turbomole_potential_energy_final",
      "repeats": false,
      "shape": [],
      "superNames": [
        "energy_component",
        "section_single_configuration_calculation"
      ],
      "units": "J"
    }, {
      "description": "section for the eigenvalues of a GW calculation (at present only pertubative G0W0)",
      "kindStr": "type_section",
      "name": "x_turbomole_section_eigenvalues_GW",
      "repeats": true,
      "superNames": [
        "section_eigenvalues"
      ]
    }, {
      "description": "section for one list of XC functionals",
      "kindStr": "type_section",
      "name": "x_turbomole_section_functionals",
      "repeats": true,
      "superNames": ["section_method"]
    }, {
      "description": "XC functional type",
      "dtypeStr": "C",
      "name": "x_turbomole_XC_functional_type",
      "repeats": true,
      "superNames": ["x_turbomole_section_functionals"]
    }, {
      "description": "Type of UHF molecular orbital",
      "dtypeStr": "C",
      "name": "x_turbomole_uhfmo_type",
      "repeats": true,
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "Final value from the virial theorem",
      "dtypeStr": "f",
      "name": "x_turbomole_virial_theorem",
      "shape": [],
      "superNames": [
        "section_single_configuration_calculation"
      ]
    }, {
      "description": "-",
      "dtypeStr": "f",
      "name": "x_turbomole_virtual_orbital_shift",
      "shape": [],
      "superNames": [
        "energy_component",
        "section_scf_iteration"
      ]
    }, {
      "description": "Final Wave Function Norm",
      "dtypeStr": "f",
      "name": "x_turbomole_wave_func_norm",
      "shape": [],
      "superNames": [
        "section_single_configuration_calculation"
      ]
    }, {
      "description": "version of the DFT-D3 van-der-Waals correction that is used",
      "dtypeStr": "C",
      "name": "x_turbomole_dft_d3_version",
      "shape": [],
      "superNames": [
        "section_method"
      ]
    }, {
      "description": "geometry optimization convergence criterion - Root Mean Square of displacements",
      "dtypeStr": "f",
      "name": "x_turbomole_geometry_optimization_geometry_change_rms",
      "shape": [],
      "superNames": [
        "section_sampling_method"
      ],
      "units": "m"
    }, {
      "description": "geometry optimization convergence criterion - Root Mean Square of forces",
      "dtypeStr": "f",
      "name": "x_turbomole_geometry_optimization_threshold_force_rms",
      "shape": [],
      "superNames": [
        "section_sampling_method"
      ],
      "units": "N"
    }, {
      "description": "geometry optimization trust region - maximum radius",
      "dtypeStr": "f",
      "name": "x_turbomole_geometry_optimization_trustregion_max",
      "shape": [],
      "superNames": [
        "section_sampling_method"
      ],
      "units": "m"
    }, {
      "description": "geometry optimization trust region - minimum radius",
      "dtypeStr": "f",
      "name": "x_turbomole_geometry_optimization_trustregion_min",
      "shape": [],
      "superNames": [
        "section_sampling_method"
      ],
      "units": "m"
    }, {
      "description": "geometry optimization trust region - initial radius",
      "dtypeStr": "f",
      "name": "x_turbomole_geometry_optimization_trustregion_initial",
      "shape": [],
      "superNames": [
        "section_sampling_method"
      ],
      "units": "m"
    }, {
      "description": "Irreducible representation the eigenstates belong to.",
      "dtypeStr": "C",
      "name": "x_turbomole_eigenvalues_irreducible_representation",
      "shape": [
        "number_of_spin_channels",
        "number_of_eigenvalues_kpoints",
        "number_of_eigenvalues"
      ],
      "superNames": [
        "section_eigenvalues"
      ]
    }, {
      "description": "TODO:",
      "dtypeStr": "f",
      "name": "x_turbomole_Z_factor",
      "repeats": true,
      "shape": [],
      "superNames": [
        "x_turbomole_section_eigenvalues_GW"
      ]
    }, {
      "description": "The employed GW approximation.",
      "dtypeStr": "C",
      "name": "x_turbomole_gw_approximation",
      "shape": [],
      "superNames": [
        "section_method",
        "settings_GW"
      ]
    }, {
      "description": "If true, the pure RPA response function is calculated. Otherwise, the TDDFT response function is calculated and used to screen the coulomb interaction.",
      "dtypeStr": "b",
      "name": "x_turbomole_gw_use_rpa_response",
      "shape": [],
      "superNames": [
        "section_method",
        "settings_GW"
      ]
    }, {
      "description": "[TO BE VERIFIED]Infinitesimal complex energy shift. Negative value switches to calculating at that value but extrapolating to 0 in linear approximation.",
      "dtypeStr": "f",
      "name": "x_turbomole_gw_eta_factor",
      "repeats": false,
      "shape": [],
      "superNames": [
        "section_method",
        "settings_GW"
      ],
      "units": "J"
    }]
}