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FCI example
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parent
2090aca15e
commit
a8ed512c93
17
ci/lib/ci.ml
17
ci/lib/ci.ml
@ -11,6 +11,7 @@ module Ci_matrix_element = Ci_matrix_element
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module Ds = Determinant_space
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module Sd = Spindeterminant
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module Si = Simulation
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type num_states
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@ -23,8 +24,11 @@ type t =
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m_S2 : (Determinant.t, Determinant.t) Matrix.t lazy_t ;
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eigensystem : ((Determinant.t, num_states) Matrix.t * num_states Vector.t) lazy_t;
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n_states : int;
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simulation : Simulation.t;
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}
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let simulation t = t.simulation
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let det_space t = t.det_space
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let n_states t = t.n_states
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@ -620,8 +624,10 @@ let create_matrix_spin_computed ?(nmax=2) f det_space =
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)
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let nuclear_repulsion t =
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Si.nuclear_repulsion (simulation t)
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let make ?(n_states=1) ?(algo=`Direct) det_space =
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let make ?(n_states=1) ?(algo=`Direct) ~det_space simulation =
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let mo_basis = Ds.mo_basis det_space in
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@ -635,7 +641,7 @@ let make ?(n_states=1) ?(algo=`Direct) det_space =
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Ds.determinant_stream det_space
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|> Stream.next
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in
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h_ij_non_zero mo_basis 0 0 d0 d0
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(h_ij_non_zero mo_basis 0 0 d0 d0)
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in
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let m_H =
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@ -680,11 +686,14 @@ let make ?(n_states=1) ?(algo=`Direct) det_space =
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let eigenvectors, eigenvalues =
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Davidson.make ~threshold:1.e-6 ~n_states diagonal matrix_prod
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in
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let eigenvalues = Vector.map (fun x -> x +. e_shift) eigenvalues in
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let nuclear_repulsion =
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Si.nuclear_repulsion simulation
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in
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let eigenvalues = Vector.map (fun x -> x +. e_shift +. nuclear_repulsion) eigenvalues in
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(Conventions.rephase eigenvectors), eigenvalues
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)
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in
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{ det_space ; e_shift ; m_H ; m_S2 ; eigensystem ; n_states }
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{ det_space ; e_shift ; m_H ; m_S2 ; eigensystem ; n_states ; simulation }
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@ -1,5 +1,6 @@
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(executables
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(names
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ex_fci
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ex_integrals
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ex_hartree_fock
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ex_localization
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102
examples/ex_fci.ml
Normal file
102
examples/ex_fci.ml
Normal file
@ -0,0 +1,102 @@
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(* [[file:ex_fci.org::*Header][Header:1]] *)
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open Qcaml
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open Common
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open Linear_algebra
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let () =
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(* Header:1 ends here *)
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(* [[file:ex_fci.org::*Definition][Definition:1]] *)
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let open Command_line in
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begin
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set_header_doc (Sys.argv.(0));
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set_description_doc "Computes the one- and two-electron hartree_fock on the Gaussian atomic basis set.";
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set_specs
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[ { short='b' ; long="basis" ; opt=Mandatory;
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arg=With_arg "<string>";
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doc="Name of the file containing the basis set"; } ;
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{ short='x' ; long="xyz" ; opt=Mandatory;
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arg=With_arg "<string>";
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doc="Name of the file containing the nuclear coordinates in xyz format"; } ;
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{ short='m' ; long="multiplicity" ; opt=Optional;
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arg=With_arg "<int>";
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doc="Spin multiplicity (2S+1). Default is singlet"; } ;
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{ short='c' ; long="charge" ; opt=Optional;
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arg=With_arg "<int>";
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doc="Total charge of the molecule. Specify negative charges with 'm' instead of the minus sign, for example m1 instead of -1. Default is 0"; } ;
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]
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end;
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(* Definition:1 ends here *)
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(* [[file:ex_fci.org::*Interpretation][Interpretation:1]] *)
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let basis_file = Util.of_some @@ Command_line.get "basis" in
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let nuclei_file = Util.of_some @@ Command_line.get "xyz" in
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let charge =
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match Command_line.get "charge" with
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| Some x -> ( if x.[0] = 'm' then
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~- (int_of_string (String.sub x 1 (String.length x - 1)))
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else
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int_of_string x )
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| None -> 0
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in
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let multiplicity =
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match Command_line.get "multiplicity" with
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| Some x -> int_of_string x
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| None -> 1
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in
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(* Interpretation:1 ends here *)
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(* [[file:ex_fci.org::*Computation][Computation:1]] *)
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let nuclei =
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Particles.Nuclei.of_xyz_file nuclei_file
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in
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(* Computation:1 ends here *)
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(* [[file:ex_fci.org::*Computation][Computation:2]] *)
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let ao_basis =
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Ao.Basis.of_nuclei_and_basis_filename ~nuclei basis_file
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in
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(* Computation:2 ends here *)
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(* [[file:ex_fci.org::*Computation][Computation:3]] *)
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let simulation =
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Simulation.make ~multiplicity ~charge ~nuclei ao_basis
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in
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(* Computation:3 ends here *)
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(* [[file:ex_fci.org::*Computation][Computation:4]] *)
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let hf =
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Mo.Hartree_fock.make ~guess:`Huckel simulation
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in
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(* Computation:4 ends here *)
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(* [[file:ex_fci.org::*Computation][Computation:5]] *)
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let mo_basis =
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Mo.Basis.of_hartree_fock hf
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in
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let frozen_core =
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Mo.Frozen_core.(make Large nuclei)
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in
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let det_space =
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Ci.Determinant_space.fci_of_mo_basis ~frozen_core mo_basis
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in
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(* Computation:5 ends here *)
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(* [[file:ex_fci.org::*Computation][Computation:6]] *)
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let ci =
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Ci.make ~det_space simulation
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in
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(* Computation:6 ends here *)
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(* [[file:ex_fci.org::*Output][Output:1]] *)
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Format.printf "@[HF energy : %f@]\n" (Mo.Hartree_fock.energy hf) ;
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Format.printf "@[FCI energy : %a@]\n" Vector.pp (Ci.eigenvalues ci)
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(* Output:1 ends here *)
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142
examples/ex_fci.org
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142
examples/ex_fci.org
Normal file
@ -0,0 +1,142 @@
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#+TITLE: Full-CI
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#+PROPERTY: header-args :tangle ex_fci.ml :comments link :exports code
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In this example, we write a program that makes a valence Full CI calculation with
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Hartree-Fock orbitals. The molecule is read in =xyz= format and a Gaussian
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atomic basis set in GAMESS format.
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* Header
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#+BEGIN_SRC ocaml
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open Qcaml
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open Common
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open Linear_algebra
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let () =
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#+END_SRC
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* Command-line arguments
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We use the =Command_line= module to define the following possible
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arguments:
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- =-b --basis= : The name of the file containing the basis set
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- =-x --xyz= : The name of the file containing the atomic coordinates
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- =-c --charge= : The charge of the molecule
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- =-m --multiplicity= : The spin multiplicity
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** Definition
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#+BEGIN_SRC ocaml
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let open Command_line in
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begin
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set_header_doc (Sys.argv.(0));
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set_description_doc "Computes the one- and two-electron hartree_fock on the Gaussian atomic basis set.";
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set_specs
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[ { short='b' ; long="basis" ; opt=Mandatory;
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arg=With_arg "<string>";
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doc="Name of the file containing the basis set"; } ;
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{ short='x' ; long="xyz" ; opt=Mandatory;
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arg=With_arg "<string>";
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doc="Name of the file containing the nuclear coordinates in xyz format"; } ;
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{ short='m' ; long="multiplicity" ; opt=Optional;
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arg=With_arg "<int>";
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doc="Spin multiplicity (2S+1). Default is singlet"; } ;
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{ short='c' ; long="charge" ; opt=Optional;
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arg=With_arg "<int>";
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doc="Total charge of the molecule. Specify negative charges with 'm' instead of the minus sign, for example m1 instead of -1. Default is 0"; } ;
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]
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end;
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#+END_SRC
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** Interpretation
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#+BEGIN_SRC ocaml
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let basis_file = Util.of_some @@ Command_line.get "basis" in
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let nuclei_file = Util.of_some @@ Command_line.get "xyz" in
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let charge =
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match Command_line.get "charge" with
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| Some x -> ( if x.[0] = 'm' then
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~- (int_of_string (String.sub x 1 (String.length x - 1)))
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else
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int_of_string x )
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| None -> 0
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in
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let multiplicity =
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match Command_line.get "multiplicity" with
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| Some x -> int_of_string x
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| None -> 1
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in
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#+END_SRC
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* Computation
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We first read the =xyz= file to create a molecule:
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#+BEGIN_SRC ocaml
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let nuclei =
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Particles.Nuclei.of_xyz_file nuclei_file
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in
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#+END_SRC
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Then we create a Gaussian AO basis using the atomic coordinates:
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#+BEGIN_SRC ocaml
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let ao_basis =
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Ao.Basis.of_nuclei_and_basis_filename ~nuclei basis_file
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in
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#+END_SRC
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We create a simulation from the nuclei and the basis set:
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#+BEGIN_SRC ocaml
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let simulation =
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Simulation.make ~multiplicity ~charge ~nuclei ao_basis
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in
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#+END_SRC
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and we make the Hartree-Fock computation:
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#+BEGIN_SRC ocaml
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let hf =
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Mo.Hartree_fock.make ~guess:`Huckel simulation
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in
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#+END_SRC
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We define the FCI determinant space:
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#+BEGIN_SRC ocaml
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let mo_basis =
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Mo.Basis.of_hartree_fock hf
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in
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let frozen_core =
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Mo.Frozen_core.(make Large nuclei)
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in
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let det_space =
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Ci.Determinant_space.fci_of_mo_basis ~frozen_core mo_basis
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in
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#+END_SRC
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And we run the FCI calculation:
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#+BEGIN_SRC ocaml
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let ci =
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Ci.make ~det_space simulation
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in
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#+END_SRC
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* Output
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We print the FCI energy:
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#+BEGIN_SRC ocaml
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Format.printf "@[HF energy : %f@]\n" (Mo.Hartree_fock.energy hf) ;
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Format.printf "@[FCI energy : %a@]\n" Vector.pp (Ci.eigenvalues ci)
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#+END_SRC
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@ -1,6 +1,7 @@
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#+TITLE: Hartree-Fock
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#+PROPERTY
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#+PROPERTY: header-args :tangle ex_hartree_fock.ml :comments link :exports code
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In this example, we write a program that makes a Hartree-Fock
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calculation. The molecule is read in =xyz= format and a Gaussian
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@ -8,7 +9,7 @@ atomic basis set in GAMESS format.
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* Header
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#+BEGIN_SRC ocaml :comments link :exports code :tangle ex_hartree_fock.ml
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#+BEGIN_SRC ocaml
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module Command_line = Qcaml.Common.Command_line
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module Util = Qcaml.Common.Util
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@ -26,7 +27,7 @@ let () =
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** Definition
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#+BEGIN_SRC ocaml :comments link :exports code :tangle ex_hartree_fock.ml
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#+BEGIN_SRC ocaml
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let open Command_line in
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begin
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set_header_doc (Sys.argv.(0));
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@ -54,7 +55,7 @@ end;
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** Interpretation
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#+BEGIN_SRC ocaml :comments link :exports code :tangle ex_hartree_fock.ml
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#+BEGIN_SRC ocaml
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let basis_file = Util.of_some @@ Command_line.get "basis" in
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let nuclei_file = Util.of_some @@ Command_line.get "xyz" in
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@ -78,33 +79,33 @@ in
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We first read the =xyz= file to create a molecule:
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#+BEGIN_SRC ocaml :comments link :exports code :tangle ex_hartree_fock.ml
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#+BEGIN_SRC ocaml
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let nuclei =
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Qcaml.Particles.Nuclei.of_xyz_file nuclei_file
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in
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#+END_SRC
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Then we create a Gaussian AO basis using the atomic coordinates:
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#+BEGIN_SRC ocaml :comments link :exports code :tangle ex_hartree_fock.ml
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#+BEGIN_SRC ocaml
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let ao_basis =
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Qcaml.Ao.Basis.of_nuclei_and_basis_filename ~nuclei basis_file
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in
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#+END_SRC
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We create a simulation from the nuclei and the basis set:
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#+BEGIN_SRC ocaml :comments link :exports code :tangle ex_hartree_fock.ml
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#+BEGIN_SRC ocaml
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let simulation = Qcaml.Simulation.make ~multiplicity ~charge ~nuclei ao_basis in
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#+END_SRC
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and we can make the Hartree-Fock computation:
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#+BEGIN_SRC ocaml :comments link :exports code :tangle ex_hartree_fock.ml
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#+BEGIN_SRC ocaml
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let hf = Qcaml.Mo.Hartree_fock.make ~guess:`Huckel simulation in
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#+END_SRC
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* Output
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We print the convergence of the calculation:
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#+BEGIN_SRC ocaml :comments link :exports code :tangle ex_hartree_fock.ml
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#+BEGIN_SRC ocaml
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Format.printf "@[%a@]" (Mo.Hartree_fock.pp) hf
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#+END_SRC
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@ -9,3 +9,7 @@ module Operators = Operators
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module Particles = Particles
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module Perturbation = Perturbation
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module Simulation = Simulation
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let (%.) = Linear_algebra.Vector.(%.) ;;
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let (%:) = Linear_algebra.Matrix.(%:) ;;
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2950
test/sto-6g
Normal file
2950
test/sto-6g
Normal file
File diff suppressed because it is too large
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