{ "cells": [ { "cell_type": "code", "execution_count": null, "metadata": {}, "outputs": [], "source": [ "let png_image = print_endline ;;\n", "\n", "(* --------- *)\n", "\n", "(*Mettre le bon chemin ici *)\n", "#cd \"/home/ydamour/QCaml\";;\n", "\n", "#use \"topfind\";;\n", "#require \"jupyter.notebook\";;\n", "\n", "#require \"gnuplot\";;\n", "let png_image name = \n", " Jupyter_notebook.display_file ~base64:true \"image/png\" (name)\n", ";;\n", "\n", "#require \"lacaml.top\";;\n", "#require \"alcotest\";;\n", "#require \"str\";;\n", "#require \"bigarray\";;\n", "#require \"zarith\";;\n", "#require \"getopt\";;\n", "#directory \"_build\";;\n", "#directory \"_build/Basis\";;\n", "#directory \"_build/CI\";;\n", "#directory \"_build/MOBasis\";;\n", "#directory \"_build/Nuclei\";;\n", "#directory \"_build/Parallel\";;\n", "#directory \"_build/Perturbation\";;\n", "#directory \"_build/SCF\";;\n", "#directory \"_build/Utils\";;\n", "\n", "\n", "#load \"Constants.cmo\";;\n", "#load_rec \"Util.cma\";;\n", "#load_rec \"Matrix.cmo\";;\n", "#load_rec \"Simulation.cmo\";;\n", "#load_rec \"Spindeterminant.cmo\";;\n", "#load_rec \"Determinant.cmo\";;\n", "#load_rec \"HartreeFock.cmo\";;\n", "#load_rec \"MOBasis.cmo\";;\n", "#load_rec \"F12CI.cmo\";;\n", "\n", "#install_printer AngularMomentum.pp_string ;;\n", "#install_printer Basis.pp ;;\n", "#install_printer Charge.pp ;;\n", "#install_printer Coordinate.pp ;;\n", "#install_printer Vector.pp;;\n", "#install_printer Matrix.pp;;\n", "#install_printer Util.pp_float_2darray;;\n", "#install_printer Util.pp_float_array;;\n", "#install_printer Util.pp_matrix;;\n", "#install_printer HartreeFock.pp ;;\n", "#install_printer Fock.pp ;;\n", "#install_printer MOClass.pp ;;\n", "(*\n", "#install_printer DeterminantSpace.pp;;\n", "#install_printer SpindeterminantSpace.pp;;\n", "*)\n", "#install_printer Bitstring.pp;;\n", "let pp_mo ppf t = MOBasis.pp ~start:1 ~finish:0 ppf t ;;\n", "#install_printer pp_mo;;\n", "\n", "\n", "(* --------- *)\n", "\n", "open Lacaml.D" ] }, { "cell_type": "code", "execution_count": null, "metadata": {}, "outputs": [], "source": [ "let xyz_string =\n", "\" 6\n", "Hydrogen chain, d=1.8 Bohr\n", "H -2.381297 0.000000 0.000000\n", "H -1.428778 0.000000 0.000000\n", "H -0.476259 0.000000 0.000000\n", "H 0.476259 0.000000 0.000000\n", "H 1.428778 0.000000 0.000000\n", "H 2.381297 0.000000 0.000000\n", "\"\n", "\n", "let basis_string = \n", "\"\n", "HYDROGEN\n", "S 6\n", "1 0.3552322122E+02 0.9163596281E-02\n", "2 0.6513143725E+01 0.4936149294E-01\n", "3 0.1822142904E+01 0.1685383049E+00\n", "4 0.6259552659E+00 0.3705627997E+00\n", "5 0.2430767471E+00 0.4164915298E+00\n", "6 0.1001124280E+00 0.1303340841E+00\n", "\n", "\"" ] }, { "cell_type": "code", "execution_count": null, "metadata": {}, "outputs": [], "source": [ "let nuclei =\n", " Nuclei.of_xyz_string xyz_string\n", " \n", "let basis = \n", " Basis.of_nuclei_and_basis_string nuclei basis_string\n", " \n", "let simulation = \n", " Simulation.make ~charge:0 ~multiplicity:1 ~nuclei basis\n", " \n", "let ao_basis = \n", " Simulation.ao_basis simulation\n", " \n", "let hf = HartreeFock.make simulation\n", "\n", "let mo_basis = MOBasis.of_hartree_fock hf" ] }, { "cell_type": "code", "execution_count": null, "metadata": {}, "outputs": [], "source": [ "let ci =\n", " DeterminantSpace.fci_of_mo_basis mo_basis ~frozen_core:false\n", " |> CI.make\n", " \n", "let ci_coef, ci_energy = Lazy.force ci.eigensystem " ] }, { "cell_type": "code", "execution_count": null, "metadata": {}, "outputs": [], "source": [] }, { "cell_type": "code", "execution_count": null, "metadata": {}, "outputs": [], "source": [] } ], "metadata": { "kernelspec": { "display_name": "OCaml 4.10.0", "language": "OCaml", "name": "ocaml-jupyter" }, "language_info": { "codemirror_mode": "text/x-ocaml", "file_extension": ".ml", "mimetype": "text/x-ocaml", "name": "OCaml", "nbconverter_exporter": null, "pygments_lexer": "OCaml", "version": "4.10.0" } }, "nbformat": 4, "nbformat_minor": 4 }