/**********************************************************************
qeq.cpp - A OBChargeModel to handle QEq charges

Copyright (C) 2010 by Jiahao Chen <jiahao@mit.edu>

This file is part of the Open Babel project.
For more information, see <http://openbabel.org/>

This program is free software; you can redistribute it and/or modify
it under the terms of the GNU General Public License as published by
the Free Software Foundation version 2 of the License.

This program 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 General Public License for more details.
***********************************************************************/

#if (defined(HAVE_EIGEN2))

#include "qeq.h"
#include <openbabel/locale.h>

using namespace std;

#ifdef _MSC_VER
// MSVC doesn't have error function erf, use local implementation
#include <openbabel/math/erf.h>
using temperf::erf;
#endif

namespace OpenBabel
{

  /*! \class QEqCharges qeq.h "qeq.h" 
   
    \brief Assigns partial charges according to the charge equilibration (QEq) model of Rappé and Goddard, 1991.
    
    The QEq model solves for charges by minimizing an energy function of the form
    
    \f[

    E\left(\mathbf{q}\right)=\mathbf{q}\cdot\boldsymbol{\chi}+\frac{1}{2}\mathbf{q}\boldsymbol{\eta}\mathbf{q}

    \f]

    where \f$\mathbf q\f$ is the vector of atomic charges, \f$\boldsymbol \chi\f$ are atomic electronegativities
    and \f$\boldsymbol \eta \f$ is the matrix of Coulomb interactions with chemical hardnesses along the diagonal,
    such that the overall charge is \f$Q\f$, i.e.

    \f[

    \mathbf{q} \cdot \mathbf{1} = \sum_{i=1}^N q_i = Q

    \f]

	in the current implementation, we assume \f$Q = 0\f$ always.

    The off-diagonal Coulomb interactions are screened using the following integral
    
    \f[

    \eta_{ij}=\int\frac{\phi_{i}^{2}\left(\mathbf{r}\right)\phi_{j}^{2}\left(\mathbf{r}^{\prime}\right)}
          {\left|\mathbf{r}-\mathbf{r}^{\prime}\right|}d^{3}\mathbf{r}d^{3}\mathbf{r}^{\prime}

    \f]

    where the orbitals \f$ \phi_{i}(\mathbf{r}) \f$ are s-type Gaussian orbitals (GTOs) of the form

    \f[

    \phi_i\left(\mathbf{r}\right)=\left(\frac{2}{\pi\sigma_{i}^{2}}\right)^{3/4}
          \exp\left(-\frac{\left|\mathbf{r}-\mathbf{R}_{i}\right|^{2}}{\sigma_{i}^{2}}\right)
    
    \f]

    where \f$ \sigma_i \f$ is the Gaussian screening radius and \f$ \mathbf R_i \f$ is the Cartesian coordinate of atom \f$ i \f$. 

    The parameters in this model are the atomic electronegativities \$f \chi_i = \chi_i^0 \$f in volts (V),
    hardnesses \$f \eta_{ii} = \eta_i^0 \f$ in V/e, and screening radii \$f \sigma_i \$f in Angstroms.

    The default parameter set uses the published values for the elements H, Li, C, N, O, F, Na, Si, P, S, Cl, K, Br, Rb, I and Cs.
    Other parameters are taken from the unpublished values that are distributed with UFF. 

    Reference:
      A. K. Rappé and W. A. Goddard, III, J. Phys. Chem. 95 (1991): 3358-3363.
      doi:10.1021/j100161a070
   
      The method of solving the model is given by
      J. Chen and T. J. Martínez, J. Chem. Phys. 131 (2009): 044114.
      doi:10.1063/1.3183167

    \note This code differs from the published description in two ways:

    \par 1. This code does _not_ compute the charge-dependent chemical hardness and screening exponent for hydrogen
    which is specified in the original publication. Instead, they are set to the \f$q = 0\f$ parameters regardless
    of the actual charge on hydrogen.

    \par 2. The screening of the Coulomb interaction is not calculated in terms of Slater-type orbitals,
    but rather recast in terms of Gaussian-type orbitals that are chosen to best reproduce the Coulomb integrals.
    The maximum error in this approximation is on the order of 0.01 Hartree/e^2, which is on par with the level
    of accuracy upon which the original parameters were chosen.

    \par The procedure is described in:
      J. Chen and T. J. Martínez, Prog. Theor. Chem. Phys. 19 (2009): 397-416.
      doi:10.1007/978-90-481-2596-8_19

    \author Jiahao Chen
    
    \since version 2.3.
  */    
    
  /////////////////////////////////////////////////////////////////
  QEqCharges theQEqCharges("qeq"); //Global instance

  /////////////////////////////////////////////////////////////////

  void QEqCharges::ParseParamFile()
  {
    vector<string> vs;
    char buffer[BUFF_SIZE];

    // open data/qeq.txt
    ifstream ifs;
    if (OpenDatafile(ifs, "qeq.txt").length() == 0) {
      obErrorLog.ThrowError(__FUNCTION__, "Cannot open qeq.txt", obError);
      return;
    }

    // Set the locale for number parsing to avoid locale issues: PR#1785463
    obLocale.SetLocale();
    Vector3d P;
    float radius;
    while (ifs.getline(buffer, BUFF_SIZE)) {
      if (buffer[0] == '#')
        continue;

      tokenize(vs, buffer);
      if (vs.size() < 4)
        continue;

      // Reads in a line of parameters
      // The format is:              code converts to
      //   Element
      //   Electronegativity (V) ->  Electronegativity (a.u.)
      //   Hardness (V/e)        ->  Hardness (a.u.)
      //   radius (Angstrom)     ->  Gaussian exponent (bohr^-2)
     
      radius = atof(vs[3].c_str())*Angstrom;
      P << atof(vs[1].c_str())*eV, atof(vs[2].c_str())*eV, 1.0/(radius*radius);
      _parameters.push_back(P);
    }
  }

  //!Returns a triple of numbers: electronegativity (in eV), hardness (in eV), and Gaussian exponent (in bohr^-2)
  Vector3d QEqCharges::GetParameters(unsigned int Z, int Q)
  {

    Vector3d P;
    //For now, completely ignore the formal charge
    if (_parameters.size() == 0)
      ParseParamFile();

    if (Z > 0 && Z < _parameters.size()-1)
      return _parameters[Z - 1];

    P<<0., 1.e10, 1.e10; //Magic value
    return P;
  }

  //! \return whether partial charges were successfully assigned to this molecule
  bool QEqCharges::ComputeCharges(OBMol &mol)
  {

    ///////////////////////////////////////////////////////////////////////////////
    //Some OpenBabel bookkeeping that I copied from the Gasteiger scheme
    mol.SetPartialChargesPerceived();

    OBPairData *dp = new OBPairData;
    dp->SetAttribute("PartialCharges");
    dp->SetValue("QEq");
    dp->SetOrigin(perceived);
    mol.SetData(dp);


    ///////////////////////////////////////////////////////////////////////////////
    //Read in atomic information from OpenBabel molecule and parameterize

    //Read in total number of atoms
    int i, N = mol.NumAtoms();

    Hardness = MatrixXd::Zero(N+1, N+1);
    Voltage = VectorXd::Zero(N+1);
    Electronegativity = VectorXd::Zero(N);
    VectorXd BasisSet = VectorXd::Zero(N);

    Vector3d Parameters;

    FOR_ATOMS_OF_MOL(atom, mol)
      {
       	Parameters = GetParameters(atom->GetAtomicNum(), atom->GetFormalCharge());
        i = atom->GetIdx() - 1;

        if (Parameters[0] == 0.)
          {
            stringstream msg;
            msg << "Some QEq Parameters not found!" << endl
                << "Parameters not found for atom no. " << i+1 << endl
                << "Atom will be ignored in the charge computation.";
            obErrorLog.ThrowError(__FUNCTION__, msg.str(), obError);
          }

        Electronegativity[i] = Parameters[0];
        Hardness(i,i) = Parameters[1];
        BasisSet[i] = Parameters[2];
      }

    //Read in total charge of molecule
    double Z = (double)(mol.GetTotalCharge());

    ///////////////////////////////////////////////////////////////////////////////
    // Now populate integrals

    // Calculate integral pre-screening threshold
    double SmallestGaussianExponent = BasisSet.minCoeff();
    double CoulMaxDistance = 2 * sqrt(-log(CoulombThreshold) / SmallestGaussianExponent);

    int j;
    double R, Coulomb;
    FOR_ATOMS_OF_MOL(atom1, mol)
      {
        i = atom1->GetIdx() - 1;
        FOR_ATOMS_OF_MOL(atom2, mol)
          {
            j = atom2->GetIdx() - 1;
            if (i>j)
              {
                //For some reason, this did _not_ produce the expected pairwise distances
                //(2,1) evaluated to the same distance as (2,0) in H2O: bug?
                // - jiahao@mit.edu 2010-04-20 r3691
                ////R = atom1->GetDistance(atom2)*Angstrom;
                //
                R = atom1->GetDistance(j+1)*Angstrom;
                if (R<CoulMaxDistance)
                  Coulomb = CoulombInt(BasisSet[i], BasisSet[j], R);
                else
                  Coulomb = 1./R;
                Hardness(i,j) = Coulomb;
                Hardness(j,i) = Coulomb;
              }
          }
      }

    Hardness.block(N,0,1,N).setOnes();
    Hardness.block(0,N,N,1).setOnes();

    Voltage.segment(0,N) = Electronegativity;
    Voltage[N] = Z;

    ///////////////////////////////////////////////////////////////////////////////
    // Call linear algebra solver
    //
    bool status = solver(Hardness, Voltage, Charge);
    if (!status)
      {
        obErrorLog.ThrowError(__FUNCTION__, "Charges could not be computed.", obError);
        return false;
      }

    ChemicalPotential = Charge[N];

    //For debugging purposes only
#if 0
    cout << "Ready to solve QEq problem" << endl << endl;
    cout << "Hardness matrix:" << endl << Hardness << endl << endl;
    cout << "Voltage vector:" << endl << Voltage << endl << endl;
    cout << "Charge vector:" << endl << Charge << endl << endl;
#endif

    //Now we are done calculating, pass all this back to OpenBabel molecule
    m_partialCharges.clear();
    m_partialCharges.reserve(mol.NumAtoms());
    m_formalCharges.clear();
    m_formalCharges.reserve(mol.NumAtoms());
    FOR_ATOMS_OF_MOL(atom, mol)
      {
        atom->SetPartialCharge(Charge[atom->GetIdx()-1]);
        m_partialCharges.push_back(Charge[atom->GetIdx() - 1]);
        m_formalCharges.push_back(atom->GetFormalCharge());
      }
    obErrorLog.ThrowError(__FUNCTION__, "QEq charges successfully assigned.", obInfo);
    return true;
  }


  //! Calculates Coulomb integral
  double QEqCharges::CoulombInt(double a, double b, double R)
  {
    double p = sqrt(a * b / (a + b));
    return erf(p * R) / R;
  }

  //! Wrapper around the Eigen linear solver routines
  // First attempts to solve using Gaussian elimination
  // if that fails, tries again using singular value decomposition (SVD)
  bool QEqCharges::solver(MatrixXd A, VectorXd b, VectorXd &x, const double NormThreshold)
  {
    // using a LU factorization
    bool SolverOK = A.lu().solve(b, &x);
    //bool SolverOK = A.svd().solve(b, &x);

    VectorXd resid = A*x - b;
    double resnorm = resid.norm();
    if (IsNan(resnorm) || resnorm > NormThreshold || !SolverOK)
      {
        stringstream msg;
        msg << "Warning, LU solver failed." << endl;
        if (!SolverOK) msg << "Solver returned error." << endl;
        if (IsNan(resnorm)) msg << "NaNs were returned" << endl;
        if (resnorm > NormThreshold) msg << "Residual has norm " << resnorm
                                         << " which exceeds the recommended threshold of " << NormThreshold
                                         << endl;
        msg << "Proceeding with singular value decomposition.";

        obErrorLog.ThrowError(__FUNCTION__, msg.str(), obWarning);

        SolverOK = A.svd().solve(b, &x);
        resid = A*x - b;
        resnorm = resid.norm();

        if (IsNan(resnorm) || !SolverOK)
          {
            obErrorLog.ThrowError(__FUNCTION__, "SVD solver returned an error. Charges may not be reliable!", obError);
            return false;
          }
      }

    stringstream msg_resid;
    msg_resid << "The residual of the solution has norm " << resnorm;
    obErrorLog.ThrowError(__FUNCTION__, msg_resid.str(), obInfo);

    if (resnorm > NormThreshold) {
      stringstream msg_reswarn;
      msg_reswarn << "Warning, the norm of the residual is " << resnorm
                  << "which exceeds the recommended threshold of " << NormThreshold;
      obErrorLog.ThrowError(__FUNCTION__, msg_reswarn.str(), obWarning);
    }
    return true;
  }

}//namespace

#endif //HAVE_EIGEN2

//! \file qeq.cpp
//! \brief Assign QEq partial charges.
