QNANO
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#include <Finite_Manybody_Hilbert_Space.h>
Public Member Functions | |
int | get_dim_e () const |
dimensions of the electron and hole parts separately. Calculated in recalc_nr_blocks() | |
int | get_dim_h () const |
virtual size_t | size () const |
virtual void | resize (int rk_e, int rk_h, int n_e, int n_h) |
virtual void | setup (Parameter_Map ¶m_map) |
virtual void | recalc_dims () |
virtual int | get_Index_from_Fermion_Index (const Fermion_Index &fi, bool hole) const |
virtual int | get_index (const Fermion_Double_Index &fi) const |
virtual Fermion_Index | get_Fermion_Index_from_Index (int index, bool hole) const |
virtual Fermion_Double_Index | get_Fermion_Double_Index (int index) const |
virtual void | dump_indices (const std::string &filename) const |
virtual Finite_Manybody_Hilbert_Space * | clone () const |
Clone & Constructors. | |
virtual void | copy (const Finite_Manybody_Hilbert_Space &other) |
Finite_Manybody_Hilbert_Space & | operator= (const Finite_Manybody_Hilbert_Space &other) |
Finite_Manybody_Hilbert_Space (const Finite_Manybody_Hilbert_Space &other) | |
Finite_Manybody_Hilbert_Space (Parameter_Map ¶m_map) | |
Finite_Manybody_Hilbert_Space (int rk_e, int rk_h, int n_e, int n_h) | |
virtual bool | is_Full_Hilbert_Space () const |
indicates if Instance is the full Hilbert space with all states defined by rank_e/h and nr_e/h | |
Public Member Functions inherited from Manybody_Hilbert_Space | |
int | get_rank_e () const |
nr of electron/hole states | |
int | get_rank_h () const |
int | get_nr_e () const |
int | get_nr_h () const |
Manybody_Hilbert_Space (Parameter_Map ¶m_map) | |
Protected Attributes | |
int | dim_e |
int | dim_h |
Additional Inherited Members | |
Static Public Member Functions inherited from Manybody_Hilbert_Space | |
static std::string | print_index (size_t line_counter, void *spi_ctx) |
Public Attributes inherited from Manybody_Hilbert_Space | |
int | rank_e |
int | rank_h |
int | nr_e |
nr of electrons/holes | |
int | nr_h |
Class that translates between Fermion indices (Slater determinants) and their respective indices in the finite Hamiltonian to be diagonalized.
Here, we take a dense Hilbert Space as base class but might later inherit, e.g. for selected state CI