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#include "io/Globals.hpp" |
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#include "nonbonded/SlaterIntegrals.hpp" |
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#include "utils/PhysicalConstants.hpp" |
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#include "math/erfc.hpp" |
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namespace OpenMD { |
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Electrostatic::Electrostatic(): name_("Electrostatic"), initialized_(false), |
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// throw warning |
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sprintf( painCave.errMsg, |
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"Electrostatic::initialize: dampingAlpha was not specified in the input file.\n" |
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"\tA default value of %f (1/ang) will be used for the cutoff of\n\t%f (ang).\n", |
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"Electrostatic::initialize: dampingAlpha was not specified in the\n" |
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"\tinput file. A default value of %f (1/ang) will be used for the\n" |
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"\tcutoff of %f (ang).\n", |
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dampingAlpha_, cutoffRadius_); |
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painCave.severity = OPENMD_INFO; |
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painCave.isFatal = 0; |
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vector<RealType> rvals; |
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vector<RealType> J1vals; |
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vector<RealType> J2vals; |
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for (int i = 0; i < np_; i++) { |
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// don't start at i = 0, as rval = 0 is undefined for the slater overlap integrals. |
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for (int i = 1; i < np_+1; i++) { |
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rval = RealType(i) * dr; |
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rvals.push_back(rval); |
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J1vals.push_back( sSTOCoulInt( a, b, m, n, rval * PhysicalConstants::angstromsToBohr ) ); |
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J1vals.push_back(sSTOCoulInt( a, b, m, n, rval * PhysicalConstants::angstromToBohr ) * PhysicalConstants::hartreeToKcal ); |
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// may not be necessary if Slater coulomb integral is symmetric |
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J2vals.push_back( sSTOCoulInt( b, a, n, m, rval * PhysicalConstants::angstromsToBohr ) ); |
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J2vals.push_back(sSTOCoulInt( b, a, n, m, rval * PhysicalConstants::angstromToBohr ) * PhysicalConstants::hartreeToKcal ); |
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} |
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CubicSpline* J1 = new CubicSpline(); |
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if (j_is_Charge) { |
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q_j = data2.fixedCharge; |
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if (i_is_Fluctuating) |
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if (j_is_Fluctuating) |
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q_j += *(idat.flucQ2); |
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if (idat.excluded) { |
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if (j_is_Charge) { |
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if (screeningMethod_ == DAMPED) { |
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// assemble the damping variables |
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//res = erfcSpline_->getValueAndDerivativeAt( *(idat.rij) ); |
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//erfcVal = res.first; |
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//derfcVal = res.second; |
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res = erfcSpline_->getValueAndDerivativeAt( *(idat.rij) ); |
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erfcVal = res.first; |
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derfcVal = res.second; |
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erfcVal = erfc(dampingAlpha_ * *(idat.rij)); |
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derfcVal = - alphaPi_ * exp(-alpha2_ * *(idat.r2)); |
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//erfcVal = erfc(dampingAlpha_ * *(idat.rij)); |
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//derfcVal = - alphaPi_ * exp(-alpha2_ * *(idat.r2)); |
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c1 = erfcVal * riji; |
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c2 = (-derfcVal + c1) * riji; |
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c2 = c1 * riji; |
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} |
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preVal = *(idat.electroMult) * pre11_ * q_i * q_j; |
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preVal = *(idat.electroMult) * pre11_; |
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if (summationMethod_ == esm_SHIFTED_POTENTIAL) { |
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vterm = preVal * (c1 - c1c_); |
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} |
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vpair += vterm; |
629 |
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epot += *(idat.sw) * vterm; |
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dVdr += dudr * rhat; |
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vpair += vterm * q_i * q_j; |
629 |
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epot += *(idat.sw) * vterm * q_i * q_j; |
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dVdr += dudr * rhat * q_i * q_j; |
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if (i_is_Fluctuating) { |
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if (idat.excluded) { |
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// vFluc1 is the difference between the direct coulomb integral |
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// and the normal 1/r-like interaction between point charges. |
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coulInt = J1->getValueAt( *(idat.rij) ); |
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vFluc1 = pre11_ * coulInt * q_i * q_j - (*(idat.sw) * vterm); |
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vFluc1 = coulInt - (*(idat.sw) * vterm); |
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} else { |
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vFluc1 = 0.0; |
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} |
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*(idat.dVdFQ1) += ( *(idat.sw) * vterm + vFluc1 ) / q_i; |
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*(idat.dVdFQ1) += ( *(idat.sw) * vterm + vFluc1 ) * q_j; |
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} |
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if (j_is_Fluctuating) { |
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// vFluc2 is the difference between the direct coulomb integral |
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// and the normal 1/r-like interaction between point charges. |
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coulInt = J2->getValueAt( *(idat.rij) ); |
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vFluc2 = pre11_ * coulInt * q_i * q_j - (*(idat.sw) * vterm); |
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vFluc2 = coulInt - (*(idat.sw) * vterm); |
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} else { |
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vFluc2 = 0.0; |
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} |
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*(idat.dVdFQ2) += ( *(idat.sw) * vterm + vFluc2 ) / q_j; |
653 |
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*(idat.dVdFQ2) += ( *(idat.sw) * vterm + vFluc2 ) * q_i; |
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} |
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// indirect reaction field terms. |
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*(idat.vpair) += indirect_vpair; |
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(*(idat.excludedPot))[ELECTROSTATIC_FAMILY] += (*(idat.sw) * vterm + |
1055 |
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vFluc1 ) * q_i * q_j; |
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(*(idat.pot))[ELECTROSTATIC_FAMILY] += indirect_Pot; |
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*(idat.f1) += indirect_dVdr; |
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} |
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void Electrostatic::calcSelfCorrection(SelfData &sdat) { |
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RealType mu1, preVal, chg1, self; |
1065 |
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1069 |
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RealType mu1, preVal, self; |
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if (!initialized_) initialize(); |
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ElectrostaticAtomData data = ElectrostaticMap[sdat.atype]; |
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// logicals |
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bool i_is_Charge = data.is_Charge; |
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bool i_is_Dipole = data.is_Dipole; |
1077 |
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bool i_is_Fluctuating = data.is_Fluctuating; |
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RealType chg1 = data.fixedCharge; |
1079 |
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|
1080 |
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if (i_is_Fluctuating) { |
1081 |
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chg1 += *(sdat.flucQ); |
1082 |
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// dVdFQ is really a force, so this is negative the derivative |
1083 |
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*(sdat.dVdFQ) -= *(sdat.flucQ) * data.hardness + data.electronegativity; |
1084 |
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(*(sdat.excludedPot))[ELECTROSTATIC_FAMILY] += (*sdat.flucQ) * |
1085 |
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(*(sdat.flucQ) * data.hardness * 0.5 + data.electronegativity); |
1086 |
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} |
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if (summationMethod_ == esm_REACTION_FIELD) { |
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if (i_is_Dipole) { |
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} |
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} else if (summationMethod_ == esm_SHIFTED_FORCE || summationMethod_ == esm_SHIFTED_POTENTIAL) { |
1102 |
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if (i_is_Charge) { |
1089 |
– |
chg1 = data.fixedCharge; |
1103 |
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if (screeningMethod_ == DAMPED) { |
1104 |
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self = - 0.5 * (c1c_ + alphaPi_) * chg1 * (chg1 + *(sdat.skippedCharge)) * pre11_; |
1105 |
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} else { |