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MPQC
3.0.0-alpha
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PT2R12: a universal spin-free second-order R12 correction. More...
#include <chemistry/qc/mbptr12/pt2r12.h>

Public Member Functions | |
| PT2R12 (const Ref< KeyVal > &keyval) | |
| A KeyVal constructor is used to generate a PT2R12 object from the input. | |
| PT2R12 (StateIn &s) | |
| void | save_data_state (StateOut &s) |
| Save the base classes (with save_data_state) and the members in the same order that the StateIn CTOR initializes them. | |
| void | compute () |
| Recompute at least the results that have compute true and are not already computed. | |
| void | print (std::ostream &os=ExEnv::out0()) const |
| Print information about the object. | |
| RefSymmSCMatrix | density () |
| Returns the SO density. | |
| int | spin_polarized () |
| Return 1 if the alpha density is not equal to the beta density. | |
| int | value_implemented () const |
| void | set_desired_value_accuracy (double acc) |
| Set the accuracy to which the value is to be computed. | |
| const Ref< R12WavefunctionWorld > & | r12world () const |
| PT2R12 is an R12 Wavefunction. | |
| Ref< R12IntEval > & | get_r12eval () |
| RefSCMatrix | transform_MO () |
| void | obsolete () |
| Marks all results as being out of date. | |
| int | nelectron () |
| Returns the number of electrons. | |
Static Public Member Functions | |
| static double | zero_occupancy () |
PT2R12: a universal spin-free second-order R12 correction.
| sc::PT2R12::PT2R12 | ( | const Ref< KeyVal > & | keyval | ) |
A KeyVal constructor is used to generate a PT2R12 object from the input.
This constructor uses keywords of R12WavefunctionWorld, plus following list of keywords.
| Keyword | Type | Default | Description |
reference | Wavefunction | none | the Wavefunction object |
rdm2 | SpinFreeRDM<Two> | none | the SpinFreeRDM<Two> object that provides the 2-RDM. It must be constructed from the object provided by the |
omit_uocc | boolean | false | if set to true, orbitals not occupied in reference will be omitted from consideration. This is useful if only geminal functions are used to treat electron correlation. |
cabs_singles | boolean | true | if set to true, compute 2nd-order CABS singes correction. |
cabs_singles_h0 | string | dyall_1 | the other options include dyall_2/complete/CI. dyall_1 uses Fock operator as H(1); dyall_2 includes both 1- and 2-particle operator in H(1), thus more complete; 'complete' refers to the partition that all operators inducing (real and pesudo) one-partilce occ->CABS transition are taken as H(1) while the other operators are classified as H(0); CI refers to a CI diagonalization procedure to account basis incompleteness (for one state). |
cabs_singles_coupling | boolean | true | if set to true, include coupling between CABS and OBS virtuals; this is the preferred choice and it corresponds to the CABS singles correction without assuming EBC in single reference limit. |
| void sc::PT2R12::compute | ( | ) | [virtual] |
Recompute at least the results that have compute true and are not already computed.
This should only be called by Result's members.
Implements sc::Compute.
| void sc::PT2R12::obsolete | ( | ) | [virtual] |
Marks all results as being out of date.
Any subsequent access to results will cause Compute::compute() to be called.
Reimplemented from sc::Wavefunction.
| void sc::PT2R12::save_data_state | ( | StateOut & | ) | [virtual] |
Save the base classes (with save_data_state) and the members in the same order that the StateIn CTOR initializes them.
This must be implemented by the derived class if the class has data.
Reimplemented from sc::Wavefunction.
| int sc::PT2R12::value_implemented | ( | ) | const [inline, virtual] |
Reimplemented from sc::Function.