std::vector<double> LinearApproximation::solveDeterminates(const std::vector<std::vector<std::vector<double> > > &t_matrices) const
{
std::vector<double> retval;
for (const auto & matrix : t_matrices)
{
retval.push_back(determinate(matrix));
}
return retval;
}
//---------------------------------------
Matrix3 Matrix3::inverse() const
{
Real det = determinate();
if( realCompare( det, 0.0 ) )
{
return cIdentity;
}
Matrix3 ret;
doInvert( *this, ret, det );
return ret;
}
Matrix3 Matrix3::inverse()
{
double det = determinate();
Matrix3 m = Matrix3();
if (det == 0) return m;
Matrix3 t = transpose();
m.a11 = (t.a22*t.a33 - t.a23*t.a32);
m.a12 = -(t.a21*t.a33 - t.a23*t.a31);
m.a13 = (t.a21*t.a32 - t.a22*t.a31);
m.a21 = -(t.a12*t.a33 - t.a13*t.a32);
m.a22 = (t.a11*t.a33 - t.a13*t.a31);
m.a23 = -(t.a11*t.a32 - t.a12*t.a31);
m.a31 = (t.a12*t.a23 - t.a13*t.a22);
m.a32 = -(t.a11*t.a23 - t.a13*t.a21);
m.a33 = (t.a11*t.a22 - t.a12*t.a21);
m /= det;
return m;
}
bool_t getBarklemactivecross(AtomicLine *line)
{
bool_t determined = TRUE, useBarklem = FALSE;
int index, Ll, Lu, nq, i, j, ic;
double Sl, Su, Jl, Ju;
double Z, neff1, neff2, findex1, findex2, reducedmass, meanvelocity,
crossmean, E_Rydberg, deltaEi, deltaEj;
Atom *atom;
Barklemstruct bs;
atom = line->atom;
j = line->j;
i = line->i;
/* ---
JdlCR: Interpolate the tables only if sigma is smaller than 20
otherwise assume that we are already giving Barklem cross-sections
--- */
if(line->cvdWaals[0] < 20.0){
/* --- ABO tabulations are only valid for neutral atoms -- -------- */
if (atom->stage[i] > 0) return FALSE;
/* --- Get the quantum numbers for orbital angular momentum -- ---- */
determined &= determinate(atom->label[i], atom->g[i],
&nq, &Sl, &Ll, &Jl);
determined &= determinate(atom->label[j], atom->g[j],
&nq, &Su, &Lu, &Ju);
/* --- See if one of the Barklem cases applies -- -------------- */
if (determined) {
if ((Ll == S_ORBIT && Lu == P_ORBIT) ||
(Ll == P_ORBIT && Lu == S_ORBIT)) {
useBarklem = readBarklemTable(SP, &bs);
} else if ((Ll == P_ORBIT && Lu == D_ORBIT) ||
(Ll == D_ORBIT && Lu == P_ORBIT)) {
useBarklem = readBarklemTable(PD, &bs);
} else if ((Ll == D_ORBIT && Lu == F_ORBIT) ||
(Ll == F_ORBIT && Lu == D_ORBIT)) {
useBarklem = readBarklemTable(DF, &bs);
}
}
if (!determined || !useBarklem) return FALSE;
/* --- Determine the index of the appropriate continuum level -- -- */
Z = atom->stage[j] + 1;
for (ic = j + 1; atom->stage[ic] < atom->stage[j]+1; ic++);
deltaEi = atom->E[ic] - atom->E[i];
deltaEj = atom->E[ic] - atom->E[j];
E_Rydberg = E_RYDBERG / (1.0 + M_ELECTRON / (atom->weight * AMU));
neff1 = Z * sqrt(E_Rydberg / deltaEi);
neff2 = Z * sqrt(E_Rydberg / deltaEj);
if (Ll > Lu) SWAPDOUBLE(neff1, neff2);
/* --- Interpolate according to effective principal quantum number */
if (neff1 < bs.neff1[0] || neff1 > bs.neff1[bs.N1-1])
return FALSE;
Locate(bs.N1, bs.neff1, neff1, &index);
findex1 =
(double) index + (neff1 - bs.neff1[index]) / BARKLEM_DELTA_NEFF;
if (neff2 < bs.neff2[0] || neff2 > bs.neff2[bs.N2-1])
return FALSE;
Locate(bs.N2, bs.neff2, neff2, &index);
findex2 =
(double) index + (neff2 - bs.neff2[index]) / BARKLEM_DELTA_NEFF;
/* --- Find interpolation in table -- -------------- */
line->cvdWaals[0] = cubeconvol(bs.N2, bs.N1,
bs.cross[0], findex2, findex1);
line->cvdWaals[1] = cubeconvol(bs.N2, bs.N1,
bs.alpha[0], findex2, findex1);
}
reducedmass = AMU / (1.0/atmos.atoms[0].weight + 1.0/atom->weight);
meanvelocity = sqrt(8.0 * KBOLTZMANN / (PI * reducedmass));
crossmean = SQ(RBOHR) * pow(meanvelocity / 1.0E4, -line->cvdWaals[1]);
line->cvdWaals[0] *= 2.0 * pow(4.0/PI, line->cvdWaals[1]/2.0) *
exp(gammln((4.0 - line->cvdWaals[1])/2.0)) * meanvelocity * crossmean;
/* --- Use UNSOLD for the contribution of Helium atoms -- ---------- */
line->cvdWaals[2] = 1.0;
line->cvdWaals[3] = 0.0;
return TRUE;
}
jarl::Matrix jarl::Matrix::inverse() const
{
jarl::Matrix inverted(lr, -ll, -ur, ul);
inverted /= determinate();
return inverted;
}
