10
1
mirror of https://gitlab.com/scemama/QCaml.git synced 2024-07-04 18:35:50 +02:00

Added RS operators

This commit is contained in:
Anthony Scemama 2020-09-28 00:24:36 +02:00
parent 8cb1d58a27
commit 99a78616fd
11 changed files with 198 additions and 28 deletions

View File

@ -1,4 +0,0 @@
include Qcaml_common
include Qcaml_particles
include Qcaml_linear_algebra
include Qcaml_gaussian_basis

View File

@ -0,0 +1,65 @@
(** Long-range electron-electron repulsion integrals.
See Eq(52) in 10.1039/b605188j
*)
open Qcaml_common
open Qcaml_gaussian_basis
open Qcaml_operators
module Csp = Contracted_shell_pair
module Cspc = Contracted_shell_pair_couple
module T = struct
let name = "Long-range electron repulsion integrals"
open Zero_m_parameters
let zero_m z =
let mu_erf =
match z.operator with
| Some (Operator.Range_sep mu) -> mu
| _ -> assert false
in
let m = mu_erf *. mu_erf in
let expo_pq_inv = z.expo_p_inv +. z.expo_q_inv in
let fG_inv = expo_pq_inv +. 1. /. m in
let fG = 1. /. fG_inv in
assert (expo_pq_inv <> 0.);
let t =
if z.norm_pq_sq > Constants.integrals_cutoff then
z.norm_pq_sq *. fG
else 0.
in
let maxm = z.maxm in
let result = Util.boys_function ~maxm t in
let rec aux accu k = function
| 0 -> result.(k) <- result.(k) *. accu
| l ->
begin
result.(k) <- result.(k) *. accu;
let new_accu = -. accu *. fG in
(aux [@tailcall]) new_accu (k+1) (l-1)
end
in
let f = Constants.two_over_sq_pi *. (sqrt fG) in
aux f 0 maxm;
result
let class_of_contracted_shell_pair_couple ?operator shell_pair_couple =
let shell_p = Cspc.shell_pair_p shell_pair_couple
and shell_q = Cspc.shell_pair_q shell_pair_couple
in
if Array.length (Csp.shell_pairs shell_p) +
(Array.length (Csp.shell_pairs shell_q)) < 4 then
Two_electron_rr.contracted_class_shell_pair_couple
?operator ~zero_m shell_pair_couple
else
Two_electron_rr_vectorized.contracted_class_shell_pairs
?operator ~zero_m shell_p shell_q
end
module M = Two_electron_integrals.Make(T)
include M

View File

@ -0,0 +1,93 @@
(** Screened Electron-electron repulsion integrals (Yukawa potential). Required for F12/r12. *)
open Qcaml_common
open Qcaml_gaussian_basis
open Qcaml_operators
module Csp = Contracted_shell_pair
module Cspc = Contracted_shell_pair_couple
module T = struct
let name = "Screened electron repulsion integrals"
open Zero_m_parameters
let zero_m z =
let expo_pq_inv = z.expo_p_inv +. z.expo_q_inv in
assert (expo_pq_inv <> 0.);
let expo_G_inv, coef_G =
let g =
match z.operator with
| Some (Operator.F12 f) -> f.F12_operator.gaussian
| _ -> assert false
in
g.Gaussian_operator.expo_g_inv,
g.Gaussian_operator.coef_g
in
let expo_pq = 1. /. expo_pq_inv in
let maxm = z.maxm in
let result = Array.init (maxm+1) (fun _ -> 0.) in
Util.array_range 0 (Array.length coef_G)
|> Array.iter (fun i ->
let fG_inv = expo_pq_inv +. expo_G_inv.(i) in
let fG = 1. /. fG_inv in
let t =
if z.norm_pq_sq > Constants.integrals_cutoff then
z.norm_pq_sq *. (expo_pq -. fG)
else 0.
in
let fm = Util.boys_function ~maxm t in
let tmp_array =
let result = Array.init (maxm+1) (fun _ -> 1.) in
Util.array_range 1 maxm
|> Array.iter (fun k -> result.(k) <- result.(k-1) *. expo_pq *. expo_G_inv.(i));
result
in
let tmp_result = Array.init (maxm+1) (fun _ -> 0.) in
let rec aux accu m = function
| 0 -> tmp_result.(m) <- fm.(m) *. accu
| j ->
begin
let f =
Util.array_range 0 m
|> Array.fold_left (fun v k ->
v +. (Util.binom_float m k) *. tmp_array.(k) *. fm.(k)) 0.
in
tmp_result.(m) <- accu *. f;
let new_accu = -. accu *. expo_pq in
(aux [@tailcall]) new_accu (m+1) (j-1)
end
in
let f =
Constants.two_over_sq_pi *. (sqrt expo_pq) *. fG *.
expo_G_inv.(i) *. exp (-.fG *. z.norm_pq_sq)
in
aux f 0 maxm;
Array.iteri (fun k v ->
result.(k) <- result.(k) +. coef_G.(i) *. v
) tmp_result) ;
result
let class_of_contracted_shell_pair_couple ?operator shell_pair_couple =
let shell_p = Cspc.shell_pair_p shell_pair_couple
and shell_q = Cspc.shell_pair_q shell_pair_couple
in
if Array.length (Csp.shell_pairs shell_p) +
(Array.length (Csp.shell_pairs shell_q)) < 4 then
Two_electron_rr.contracted_class_shell_pair_couple
?operator ~zero_m shell_pair_couple
else
Two_electron_rr_vectorized.contracted_class_shell_pairs
?operator ~zero_m shell_p shell_q
end
module M = Two_electron_integrals.Make(T)
include M

View File

@ -19,7 +19,7 @@ module type Two_ei_structure =
sig
val name : string
val class_of_contracted_shell_pair_couple :
?operator:'a Operator.t -> Cspc.t -> float Zmap.t
?operator:Operator.t -> Cspc.t -> float Zmap.t
end

View File

@ -16,7 +16,7 @@ val name : string
(** Name of the kind of integrals, for printing purposes. *)
val class_of_contracted_shell_pair_couple :
?operator:'a Operator.t -> Contracted_shell_pair_couple.t -> float Zmap.t
?operator:Operator.t -> Contracted_shell_pair_couple.t -> float Zmap.t
(** Returns an integral class from a couple of contracted shells.
The results is stored in a Zmap.
*)
@ -28,7 +28,7 @@ module Make : functor (T : Two_ei_structure) ->
sig
include module type of Four_idx_storage
val of_basis : ?operator:'a Operator.t -> Basis.t -> t
val of_basis : ?operator:Operator.t -> Basis.t -> t
(** Compute all ERI's for a given {!Basis.t}. *)
end

View File

@ -1,7 +1,7 @@
open Qcaml_common
open Qcaml_operators
type 'a t =
type t =
{
expo_p_inv : float ;
expo_q_inv : float ;
@ -10,8 +10,8 @@ type 'a t =
center_pq : Coordinate.t ;
center_pa : Coordinate.t ;
center_qc : Coordinate.t ;
zero_m_func : 'a t -> float array ;
operator : 'a Operator.t option;
zero_m_func : t -> float array ;
operator : Operator.t option;
}
let zero ?operator zero_m_func =

View File

@ -7,9 +7,9 @@ type t =
}
let make_gaussian_corr_factor expo_s coef_g expo_sg =
let expo_sg =
Array.map (fun x -> x *. expo_s *. expo_s) expo_sg
let make_gaussian_corr_factor expo_s coef_g expo_sg =
let expo_sg =
Array.map (fun x -> x *. expo_s *. expo_s) expo_sg
in
let gaussian = Gaussian_operator.make coef_g expo_sg in
{ expo_s ; gaussian }
@ -60,10 +60,10 @@ let simple_gaussian_geminal' expo_s =
|]
and expo_sg =
[|
0.63172472556807146570889699432882480323314666748046875;
26.3759196683467962429858744144439697265625;
0.63172102793029016876147352377302013337612152099609375;
7.08429025944207335641067402320913970470428466796875;
0.63172472556807146570889699432882480323314666748046875;
26.3759196683467962429858744144439697265625;
0.63172102793029016876147352377302013337612152099609375;
7.08429025944207335641067402320913970470428466796875;
42.4442841447001910637482069432735443115234375;
391.44036073596890901171718724071979522705078125 ;
|]

View File

@ -8,14 +8,14 @@ type t =
}
let make coef_g expo_g =
let expo_g_inv =
Array.map (fun x -> 1. /. x ) expo_g
let expo_g_inv =
Array.map (fun x -> 1. /. x ) expo_g
in
{ coef_g ; expo_g ; expo_g_inv }
let one_over_r =
let coef_g = [|
841.88478132 ; 70.590185207 ; 18.3616020768 ; 7.2608642093 ;
3.57483416444 ; 2.01376031082 ; 1.24216542801 ; 0.81754348620 ;

View File

@ -1,6 +1,9 @@
type 'a t =
| F12 of F12_operator.t
| Gaussian of Gaussian_operator.t
type t =
| F12 of F12_operator.t
| Gaussian of Gaussian_operator.t
| Range_sep of Rs_operator.t
let of_f12 f = F12 f
let of_gaussian g = Gaussian g
let of_range_separation mu = Range_sep mu

View File

@ -1,9 +1,14 @@
type 'a t =
| F12 of F12_operator.t
| Gaussian of Gaussian_operator.t
type t =
| F12 of F12_operator.t
| Gaussian of Gaussian_operator.t
| Range_sep of Rs_operator.t
val of_f12 : F12_operator.t -> F12_operator.t t
val of_f12 : F12_operator.t -> t
(** Creates a F12 operator *)
val of_gaussian: Gaussian_operator.t -> Gaussian_operator.t t
val of_gaussian: Gaussian_operator.t -> t
(** Creates a Gaussian operator *)
val of_range_separation: Rs_operator.t -> t
(** Creates a range-separated operator *)

View File

@ -0,0 +1,8 @@
(** Type for range-separation parameter *)
type t = float