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Eötvös Quantum Utilities
v4.9.146
Providing the Horsepowers in the Quantum Realm
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Structure Opt contains the basic computational parameters used in EQuUs. More...
Public Attributes | |
| BdG | |
| Set 1 to use the Bogoliubov de Gennes model, 0 (default) for normal systems. More... | |
| custom_Hamiltonians | |
| Set 'siesta' to import Hamiltonians from Siesta, 'custom' to use custom defined Hamiltonians. More... | |
| debug | |
| Set 1 to export debug informations into the debug.txt file, or 0 otherwise. More... | |
| Decimate_only_Dyson | |
| Obsolete parameter. More... | |
| Decimation | |
| Option for using decimation algorith. (see more details at the documenatation of class Decimation) More... | |
| Decimation_block | |
| The maximal number of the sites to be decimated at once. More... | |
| eta | |
Scalar value representing the strength of the bult-in vector potential: with standing for the atom-atom distance. More... | |
| gauge | |
| String containining a bult-in vector potential. Possible values are: 'LandauX', 'LandauY'. More... | |
| Just_Create_Hamiltonians | |
| Obsolete parameter. More... | |
| Lattice_Type | |
| String describing the preprogrammed lattice type. See the documentation of lattice types for details. More... | |
| Linear_Regression_in_B | |
| Set 1 to use linear interpolation for the vector potential between the atomic sites to calculate the Peierls phases. Useful when dealing with a homogeneous magnetic field. More... | |
| magnetic_field | |
| Set true if a magnetic field is involved in the calculations, false (default) otherwise. More... | |
| magnetic_field_trans_invariant | |
| Set true (default) if a magnetic field is translational invariant along the scattering center, or false otherwise. More... | |
| NofLeads | |
| Number of leads attached to the scattering region. More... | |
| Silent | |
| Set 1 in order to supress output messages. More... | |
| Simple_Green_Function | |
| Set 1 if a simple analytical surface greens function computational method is about to be used, 0 otherwise (Only for square lattice without magnetic field). More... | |
| Spin | |
| Set 1 to use 1/2 spin degree of freedom in the Hamiltonians, or 0 otherwise. More... | |
| usingDualModes | |
| Set 1 to use dual modes in the calculations, or 0 to use the left and right sided eigenvectors instead. More... | |
| workers | |
| Number of workers in the parallel pool. More... | |
Structure Opt contains the basic computational parameters used in EQuUs.
Definition at line 60 of file structures.m.
| Opt::BdG |
Set 1 to use the Bogoliubov de Gennes model, 0 (default) for normal systems.
Definition at line 64 of file structures.m.
| Opt::custom_Hamiltonians |
Set 'siesta' to import Hamiltonians from Siesta, 'custom' to use custom defined Hamiltonians.
Definition at line 96 of file structures.m.
| Opt::debug |
Set 1 to export debug informations into the debug.txt file, or 0 otherwise.
Definition at line 92 of file structures.m.
| Opt::Decimate_only_Dyson |
Obsolete parameter.
Definition at line 84 of file structures.m.
| Opt::Decimation |
Option for using decimation algorith. (see more details at the documenatation of class Decimation)
Definition at line 88 of file structures.m.
| Opt::Decimation_block |
The maximal number of the sites to be decimated at once.
Definition at line 86 of file structures.m.
| Opt::eta |
Scalar value representing the strength of the bult-in vector potential:
with
standing for the atom-atom distance.
Definition at line 74 of file structures.m.
| Opt::gauge |
String containining a bult-in vector potential. Possible values are: 'LandauX', 'LandauY'.
Definition at line 72 of file structures.m.
| Opt::Just_Create_Hamiltonians |
Obsolete parameter.
Definition at line 66 of file structures.m.
| Opt::Lattice_Type |
String describing the preprogrammed lattice type. See the documentation of lattice types for details.
Definition at line 80 of file structures.m.
| Opt::Linear_Regression_in_B |
Set 1 to use linear interpolation for the vector potential between the atomic sites to calculate the Peierls phases. Useful when dealing with a homogeneous magnetic field.
Definition at line 76 of file structures.m.
| Opt::magnetic_field |
Set true if a magnetic field is involved in the calculations, false (default) otherwise.
Definition at line 68 of file structures.m.
| Opt::magnetic_field_trans_invariant |
Set true (default) if a magnetic field is translational invariant along the scattering center, or false otherwise.
Definition at line 70 of file structures.m.
| Opt::NofLeads |
Number of leads attached to the scattering region.
Definition at line 82 of file structures.m.
| Opt::Silent |
Set 1 in order to supress output messages.
Definition at line 62 of file structures.m.
| Opt::Simple_Green_Function |
Set 1 if a simple analytical surface greens function computational method is about to be used, 0 otherwise (Only for square lattice without magnetic field).
Definition at line 78 of file structures.m.
| Opt::Spin |
Set 1 to use 1/2 spin degree of freedom in the Hamiltonians, or 0 otherwise.
Definition at line 98 of file structures.m.
| Opt::usingDualModes |
Set 1 to use dual modes in the calculations, or 0 to use the left and right sided eigenvectors instead.
Definition at line 90 of file structures.m.
| Opt::workers |
Number of workers in the parallel pool.
Definition at line 94 of file structures.m.
1.8.16