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