#+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 = { 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; } module Am = Angular_momentum module Co = Coordinate module Cs = Contracted_shell #+end_src ** Access #+begin_src ocaml :tangle (eval mli) 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 #+end_src | ~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~. | #+begin_example #+end_example #+begin_src ocaml :tangle (eval ml) :exports none 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 #+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 | 0 -> true | i -> if Cs.center contr.(i) = center then (unique_center [@tailcall]) (i-1) else false in if not (unique_center (Array.length contr - 1)) then invalid_arg "ContractedAtomicShell.make Coordinate.t differ"; let ang_mom = Cs.ang_mom contr.(0) in let rec unique_angmom = function | 0 -> true | i -> if Cs.ang_mom contr.(i) = ang_mom then (unique_angmom [@tailcall]) (i-1) else false in if not (unique_angmom (Array.length contr - 1)) then invalid_arg "Contracted_shell.make: Angular_momentum.t differ"; 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 "@["; Array.iter2 (fun e c -> fprintf ppf "@[%16.8e %16.8e@]@;" e c) e_arr c_arr; fprintf ppf "@;@]") s.expo s.coef; fprintf ppf "@]" #+end_src