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QCaml/gaussian/atomic_shell.org

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#+begin_src elisp tangle: no :results none :exports none
(setq pwd (file-name-directory buffer-file-name))
(setq name (file-name-nondirectory (substring buffer-file-name 0 -4)))
(setq lib (concat pwd "lib/"))
(setq testdir (concat pwd "test/"))
(setq mli (concat lib name ".mli"))
(setq ml (concat lib name ".ml"))
(setq test-ml (concat testdir name ".ml"))
(org-babel-tangle)
#+end_src
* Atomic shell
:PROPERTIES:
:header-args: :noweb yes :comments both
:END:
Set of contracted Gaussians differing only by the powers of $x$, $y$ and $z$, with a
constant ~Angular_momentum.t~, all centered on the same point.
In other words, it is the set of all contracted shells sharing the same center.
\begin{align*}
\chi_{n_x,n_y,n_z}(r) & = f(n_x,n_y,n_z) \sum_{j=1}^{n} \sum_{i=1}^{m} \mathcal{N}_{ij}\, d_{ij}\, g_{ij\,n_x,n_y,n_z}(r) \\
& = (x-X_A)^{n_x} (y-Y_A)^{n_y} (z-Z_A)^{n_z} f(n_x,n_y,n_z) \sum_{j=1}^{n} \sum_{i=1}^{m} \mathcal{N}_{ij}\, d_{ij}\, \exp \left( -\alpha_{ij} |r-R_A|^2 \right)
\end{align*}
where:
- $g_{ij\,n_x,n_y,n_z}(r)$ is the $i$-th ~PrimitiveShell.t~ of the $j$-th ~Contracted_shell.t~
- $n_x + n_y + n_z = l$, the total angular momentum
- $\alpha_{ij}$ are the exponents (tabulated) of the $j$-th ~Contracted_shell.t~
- $d_{ij}$ are the contraction coefficients of the $j$-th ~Contracted_shell.t~
- $\mathcal{N}_{ij}$ is the normalization coefficient of the $i$-th primitive shell
(~PrimitiveShell.norm_coef~) of the $j$-th ~Contracted_shell.t~
- $f(n_x,n_y,n_z)$ is a scaling factor adjusting the normalization coefficient for the
particular powers of $x,y,z$ (~PrimitiveShell.norm_coef_scale~)
** Type
#+begin_src ocaml :tangle (eval mli)
type t
open Common
#+end_src
#+begin_src ocaml :tangle (eval ml) :exports none
open Common
type t = {
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expo : float array array;
coef : float array array;
norm_coef : float array array;
norm_coef_scale : float array;
contr : Contracted_shell.t array;
index : int;
center : Coordinate.t;
ang_mom : Angular_momentum.t;
}
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module Am = Angular_momentum
module Co = Coordinate
module Cs = Contracted_shell
#+end_src
** Access
#+begin_src ocaml :tangle (eval mli)
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val ang_mom : t -> Angular_momentum.t
val center : t -> Coordinate.t
val coefficients : t -> float array array
val contracted_shells : t -> Contracted_shell.t array
val exponents : t -> float array array
val index : t -> int
val normalizations : t -> float array array
val norm_scales : t -> float array
val size_of_shell : t -> int
val size : t -> int
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#+end_src
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| ~ang_mom~ | Total angular momentum : $l = n_x + n_y + n_z$. |
| ~center~ | Coordinate of the center $\mathbf{A} = (X_A,Y_A,Z_A)$. |
| ~coefficients~ | Array of contraction coefficients $d_{ij}$. The first index is the index of the contracted function, and the second index is the index of the primitive. |
| ~contracted_shells:~ | Array of contracted gaussians |
| ~exponents~ | Array of exponents $\alpha_{ij}$. The first index is the index of the contracted function, and the second index is the index of the primitive. |
| ~index~ | Index in the basis set, represented as an array of contracted shells. |
| ~normalizations~ | Normalization coefficients $\mathcal{N}_{ij}$. The first index is the index of the contracted function, and the second index is the index of the primitive. |
| ~norm_scales~ | Scaling factors $f(n_x,n_y,n_z)$, given in the same order as ~Angular_momentum.zkey_array ang_mom~. |
| ~size~ | Number of contracted functions, $n$ in the definition. |
| ~size_of_shell~ | Number of contracted functions in the shell: length of ~norm_coef_scale~. |
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#+begin_example
#+end_example
#+begin_src ocaml :tangle (eval ml) :exports none
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let ang_mom t = t.ang_mom
let center t = t.center
let coefficients t = t.coef
let contracted_shells t = t.contr
let exponents t = t.expo
let index t = t.index
let normalizations t = t.norm_coef
let norm_scales t = t.norm_coef_scale
let size_of_shell t = Array.length t.norm_coef_scale
let size t = Array.length t.contr
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#+end_src
** Creation
#+begin_src ocaml :tangle (eval mli)
val make : ?index:int -> Contracted_shell.t array -> t
val with_index : t -> int -> t
#+end_src
| ~make~ | Creates a contracted shell from a list of coefficients and primitives. |
| ~with_index~ | Returns a copy of the contracted shell with a modified index. |
#+begin_src ocaml :tangle (eval ml) :exports none
let make ?(index=0) contr =
assert (Array.length contr > 0);
let coef = Array.map Cs.coefficients contr
and expo = Array.map Cs.exponents contr
in
let center = Cs.center contr.(0) in
let rec unique_center = function
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| 0 -> true
| i -> if Cs.center contr.(i) = center then (unique_center [@tailcall]) (i-1) else false
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in
if not (unique_center (Array.length contr - 1)) then
invalid_arg "ContractedAtomicShell.make Coordinate.t differ";
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let ang_mom = Cs.ang_mom contr.(0) in
let rec unique_angmom = function
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| 0 -> true
| i -> if Cs.ang_mom contr.(i) = ang_mom then (unique_angmom [@tailcall]) (i-1) else false
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in
if not (unique_angmom (Array.length contr - 1)) then
invalid_arg "Contracted_shell.make: Angular_momentum.t differ";
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let norm_coef =
Array.map Cs.normalizations contr
in
let norm_coef_scale = Cs.norm_scales contr.(0)
in
{ index ; expo ; coef ; center ; ang_mom ; norm_coef ;
norm_coef_scale ; contr }
let with_index a i =
{ a with index = i }
#+end_src
** Printers
#+begin_src ocaml :tangle (eval mli)
val pp : Format.formatter -> t -> unit
#+end_src
#+begin_src ocaml :tangle (eval ml) :exports none
let pp ppf s =
let open Format in
fprintf ppf "@[%3d-%-3d@]" (s.index+1) (s.index+ (size_of_shell s)*(size s));
fprintf ppf "@[%a@ %a@] @[" Am.pp_string s.ang_mom Co.pp s.center;
Array.iter2 (fun e_arr c_arr -> fprintf ppf "@[<v>";
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Array.iter2 (fun e c -> fprintf ppf "@[%16.8e %16.8e@]@;" e c)
e_arr c_arr;
fprintf ppf "@;@]") s.expo s.coef;
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fprintf ppf "@]"
#+end_src