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/*
 * @BEGIN LICENSE
 *
 * @plugin@ by Psi4 Developer, a plugin to:
 *
 * Psi4: an open-source quantum chemistry software package
 *
 * Copyright (c) 2007-2017 The Psi4 Developers.
 *
 * The copyrights for code used from other parties are included in
 * the corresponding files.
 *
 * This file is part of Psi4.
 *
 * Psi4 is free software; you can redistribute it and/or modify
 * it under the terms of the GNU Lesser General Public License as published by
 * the Free Software Foundation, version 3.
 *
 * Psi4 is distributed in the hope that it will be useful,
 * but WITHOUT ANY WARRANTY; without even the implied warranty of
 * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
 * GNU Lesser General Public License for more details.
 *
 * You should have received a copy of the GNU Lesser General Public License along
 * with Psi4; if not, write to the Free Software Foundation, Inc.,
 * 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
 *
 * @END LICENSE
 */

#include "psi4/psi4-dec.h"
#include "psi4/libparallel/parallel.h"
#include "psi4/liboptions/liboptions.h"
#include "psi4/libmints/wavefunction.h"
#include "psi4/libmints/molecule.h"
#include "psi4/libmints/basisset.h"
#include "psi4/libmints/matrix.h"
#include "psi4/libmints/mintshelper.h"

namespace psi{ namespace @plugin@ {

extern "C"
int read_options(std::string name, Options &options)
{
    if (name == "@PLUGIN@"|| options.read_globals()) {
        /*- The amount of information printed
            to the output file -*/
        options.add_int("PRINT", 1);
        /*- Whether to compute two-electron integrals -*/
        options.add_bool("DO_TEI", true);
    }

    return true;
}

extern "C"
SharedWavefunction @plugin@(SharedWavefunction ref_wfn, Options& options)
{
    // Grab options from the options object
    int print = options.get_int("PRINT");
    int doTei = options.get_bool("DO_TEI");

    // Have the Wavefunction from python-side

    // Molecule is a member of the wavefunction option
    // Lets print out some molecule information here
    ref_wfn->molecule()->print();
    double nucrep = ref_wfn->molecule()->nuclear_repulsion_energy();
    psi::outfile->Printf("\n    Nuclear repulsion energy: %16.8f\n\n", nucrep);

    // MintsHelper are convenient objects that take a basisset, options, and print level
    // After this object is formed we can request a variety of matrix types
    MintsHelper mints(MintsHelper(ref_wfn->basisset(), options, 0));

    // mints is a reference, so we use the "." operator to access this object
    SharedMatrix sMat = mints.ao_overlap();
    SharedMatrix tMat = mints.ao_kinetic();
    SharedMatrix vMat = mints.ao_potential();

    // The SharedMatrix class is a std::shared_ptr to a Matrix
    // Since we have a point to the object we can access it through the "->" operator
    sMat->print();
    tMat->print();
    vMat->print();

    // Now that we have these matrices we can manipulate them in various ways
    // Form h = T + V by first cloning T and then adding V
    SharedMatrix hMat = tMat->clone();
    hMat->add(vMat);

    // Before we print lets give hMat a name so that we know what it is
    hMat->set_name("Core Hamiltonian Matrix");
    hMat->print();

    // We can build the two-electron integrals in a similar manner
    if(doTei){
        // As a note building the ERI's in this way is typically for debugging purposes and not normally recommended

        // First lets make sure this Matrix is not too large, lets stop at 100 basis function
        size_t nbf = ref_wfn->basisset()->nbf();
        if (nbf > 100){
            throw PSIEXCEPTION("There are too many basis function to construct the two-electron integrals!");
        }

        SharedMatrix eri = mints.ao_eri();

    }

    return ref_wfn;
}

}} // End Namespaces