| Name | Last modified | Size | Description | |
|---|---|---|---|---|
| Parent Directory | - | |||
| B4Mo10P2.cif | 2026-11-01 20:56 | 1.4K | ||
| B4Mo10P2.save/ | 2026-11-01 21:20 | - | ||
| B4Mo10P2.xml | 2026-11-01 21:20 | 6.3M | ||
| README.html | 2026-11-01 21:45 | 43K | ||
| config.toml | 2026-11-01 20:56 | 610 | ||
| data/ | 2026-11-01 21:44 | - | ||
| espresso.err | 2026-11-01 21:20 | 6.4K | ||
| espresso.pwi | 2026-11-01 21:02 | 92K | ||
| espresso.pwo | 2026-11-01 21:20 | 2.7M | ||
| force-constants.npy | 2026-11-01 21:42 | 18K | ||
| force-sets/ | 2026-11-01 21:42 | - | ||
| material-modelling-log.txt | 2026-11-01 21:45 | 15K | ||
| phonopy_params.yaml | 2026-11-01 21:42 | 72K | ||
| properties.h5 | 2026-11-01 21:44 | 367M | ||
| properties.toml | 2026-11-01 21:45 | 1.4G | ||
| settings.toml | 2026-11-01 20:56 | 3.3K | ||
This page presents an overview of the calculation performed for B4Mo10P2.
NOTE: This page is refreshed every 3 min as results are produced. Reload manually (Ctrl-R) to force update.The following computations are requested:
The calculator being used is: ESPRESSO which detailed configuration follows:
{'template': , 'profile': , 'directory': PosixPath('/var/lib/material-modelling/data/B4Mo10P2.cif-QuantumEspresso-farhi-20261101-205606'), 'parameters': {'input_data': {'control': {'outdir': '/var/lib/material-modelling/data/B4Mo10P2.cif-QuantumEspresso-farhi-20261101-205606', 'prefix': 'B4Mo10P2', 'verbosity': 'high', 'tstress': True, 'tprnfor': True, 'disk_io': 'low'}, 'system': {'ecutwfc': 45.00000000000001, 'occupations': 'smearing', 'nosym': False, 'noinv': True, 'input_dft': 'PBE', 'smearing': 'mv', 'degauss': 0.009554823852044876}, 'electrons': {'conv_thr': 7.349864501572982e-07, 'electron_maxstep': 100, 'diagonalization': 'david', 'mixing_beta': 0.7}}, 'kpts': (np.int64(4), np.int64(4), np.int64(4)), 'pseudopotentials': {'B': 'b_pbe_v1.4.uspp.F.UPF', 'B1': 'b_pbe_v1.4.uspp.F.UPF', 'B2': 'b_pbe_v1.4.uspp.F.UPF', 'B3': 'b_pbe_v1.4.uspp.F.UPF', 'B4': 'b_pbe_v1.4.uspp.F.UPF', 'B5': 'b_pbe_v1.4.uspp.F.UPF', 'B6': 'b_pbe_v1.4.uspp.F.UPF', 'B7': 'b_pbe_v1.4.uspp.F.UPF', 'B8': 'b_pbe_v1.4.uspp.F.UPF', 'B9': 'b_pbe_v1.4.uspp.F.UPF', 'Mo': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'Mo1': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'Mo2': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'Mo3': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'Mo4': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'Mo5': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'Mo6': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'Mo7': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'Mo8': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'Mo9': 'Mo_ONCV_PBE-1.0.oncvpsp.upf', 'P': 'P.pbe-n-rrkjus_psl.1.0.0.UPF', 'P1': 'P.pbe-n-rrkjus_psl.1.0.0.UPF', 'P2': 'P.pbe-n-rrkjus_psl.1.0.0.UPF', 'P3': 'P.pbe-n-rrkjus_psl.1.0.0.UPF', 'P4': 'P.pbe-n-rrkjus_psl.1.0.0.UPF', 'P5': 'P.pbe-n-rrkjus_psl.1.0.0.UPF', 'P6': 'P.pbe-n-rrkjus_psl.1.0.0.UPF', 'P7': 'P.pbe-n-rrkjus_psl.1.0.0.UPF', 'P8': 'P.pbe-n-rrkjus_psl.1.0.0.UPF', 'P9': 'P.pbe-n-rrkjus_psl.1.0.0.UPF'}}, 'atoms': Atoms(symbols='B4Mo10P2', pbc=True, cell=[[6.00172, 0.0, 0.0], [0.0, 6.00172, 0.0], [-3.0008267402230273, -3.0008267402230273, 5.585497057802902]], spacegroup_kinds=..., calculator=Espresso(...)), 'results': {}, 'use_cache': True} The setting used are:
{'version': '26.10.31', 'atoms': '/var/lib/material-modelling/data/B4Mo10P2.cif-QuantumEspresso-farhi-20261101-205606/B4Mo10P2.cif', 'calculator': 'ESPRESSO', 'compute': 'ELECTRONS_ELECTRONS_3D_PHONONS_PHONONS_3D_DIFFRACTION_FLUORESCENCE_XAS', 'convergence': 1e-05, 'diffraction_B': 0, 'diffraction_bins': 10000, 'diffraction_qmax': 25, 'directory': '/var/lib/material-modelling/data/B4Mo10P2.cif-QuantumEspresso-farhi-20261101-205606', 'displacement': 0.01, 'ecut': 612.2561850000001, 'eigensolver': 'dav', 'epoints': 101, 'hubbard': 'auto', 'kgamma': None, 'kpoints3d': 11, 'kpoints': array([4, 4, 4]), 'label': 'B4Mo10P2', 'log': None, 'maxiter': None, 'mpi': 69, 'mpirun': '/usr/bin/mpirun -np 69', 'nbands': None, 'occupations': 0.13, 'parallel_displacements': 1, 'potentials': '/usr/share/espresso/pseudo', 'qgamma': None, 'qpoints3d': [-1, 1, 21], 'spin': 'auto', 'start_date': 'Sun Nov 1 20:56:07 2026', 'supercell': array([1, 1, 1]), 'temperature': 300, 'to_all': 'True', 'to_hdf5': True, 'to_html': True, 'to_json': True, 'tolerance': 1e-05, 'to_mat': True, 'to_mccode': True, 'to_npy': True, 'to_nrrd': True, 'to_png': True, 'to_svg': True, 'to_toml': True, 'wpoints': 51, 'xas_bins': 10000, 'xas_emax': None, 'xas_emin': None, 'xc': 'PBE', 'xray_energy': 38, 'xray_polar': array([1, 0, 0]), 'smearing': 'semiconductor', 'user_id': 'farhi', 'user_ip': ' [195.221.10.47]', 'chemical_symbols': ['B', 'B', 'B', 'B', 'Mo', 'Mo', 'Mo', 'Mo', 'Mo', 'Mo', 'Mo', 'Mo', 'Mo', 'Mo', 'P', 'P'], 'chemical_formula': 'B4Mo10P2', 'cell_parameters': array([ 6.00172, 6.00172, 7.01482, 115.327 , 115.327 , 90. ]), 'kpts_density': np.int64(1024), 'Atoms': Atoms(symbols='B4Mo10P2', pbc=True, cell=[[6.00172, 0.0, 0.0], [0.0, 6.00172, 0.0], [-3.0008267402230273, -3.0008267402230273, 5.585497057802902]], spacegroup_kinds=..., calculator=Espresso(...))}Generated:

Generated:
Properties:
{'angular_momentum': array([0., 0., 0.]), 'center_of_mass': array([1.5613797 , 1.5613797 , 2.17596015]), 'charges': None, 'dipole_moment': None, 'Fermi_level': 19.974, 'kinetic_energy': 0.0, 'magnetic_moment': None, 'momenta': array([[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.],
[0., 0., 0.]]), 'moments_of_inertia': array([3697.54823296, 9412.40050418, 9808.30854618]), 'potential_energy': -19396.627699056848, 'stress': array([ 1.36823848e-02, 1.36823848e-02, 1.32536052e-02, -9.18157615e-07,
-9.18157615e-07, -1.19360490e-05]), 'total_energy': -19396.627699056848}Generated:
B4Mo10P2 e-DOS in eV wrt Fermi Level 19.974 [ESPRESSO] (open full plot)

Generated:
B4Mo10P2 electronic band structure 1d in eV [ESPRESSO] (open full plot)
B4Mo10P2 electronic band structure 1d in eV [ESPRESSO] ARPES (Ef=19.966 eV, Polar=[1 0 0]) (open full plot)


Generated:
B4Mo10P2 electronic band structure 3d in eV [ESPRESSO] arpes_I H=0.09 [rlu] (open full plot)
B4Mo10P2 electronic band structure 3d in eV [ESPRESSO] Sqw_powder_arpes (log10) (open full plot)

silx view for H5, and paraview for NRRD.Generated:
B4Mo10P2 phonon density of states (harmonic) in meV [ESPRESSO/PhonoPy] (open full plot)

Generated:
B4Mo10P2 phonon dispersion (harmonic) in meV [ESPRESSO] (open full plot)
B4Mo10P2 phonon dispersion (harmonic) in meV [ESPRESSO] Sqw_powder_neutron (log10) (open full plot)
B4Mo10P2 phonon dispersion (harmonic) in meV [ESPRESSO] Sqw_powder_xray (log10) (open full plot)



Generated:
B4Mo10P2 phonon dispersion (harmonic) in meV [ESPRESSO] Sqw_neutron H=0.00 [rlu] (open full plot)
B4Mo10P2 phonon dispersion (harmonic) in meV [ESPRESSO] Sqw_xray H=0.00 [rlu] (open full plot)
B4Mo10P2 phonon dispersion (harmonic) in meV [ESPRESSO] Sqw_powder_neutron (log10) (open full plot)
B4Mo10P2 phonon dispersion (harmonic) in meV [ESPRESSO] Sqw_powder_xray (log10) (open full plot)


silx view for H5, and paraview for NRRD.Generated:
B4Mo10P2 powder diffraction I(q) (open full plot)

Generated:
X-ray fluorescence estimate at Ei=38.0 [keV] (open full plot)

Generated:
X-ray absorption spectrum estimate (open full plot)

Generated:
The computation results are available as an HDF5 file. View it with silx view properties.h5
Duration: 2894.6035017967224
We recommend to use silx to view HDF5 and NPY files, and paraview for NRRD files.
(c) Synchrotron SOLEIL GRADES/EXP Project code at Gitlab