365 |
|
for (int i = 1; i < np_+1; i++) { |
366 |
|
rval = RealType(i) * dr; |
367 |
|
rvals.push_back(rval); |
368 |
< |
J1vals.push_back(electrostaticAtomData.hardness * sSTOCoulInt( a, b, m, n, rval * PhysicalConstants::angstromsToBohr ) ); |
368 |
> |
J1vals.push_back(sSTOCoulInt( a, b, m, n, rval * PhysicalConstants::angstromToBohr ) * PhysicalConstants::hartreeToKcal ); |
369 |
|
// may not be necessary if Slater coulomb integral is symmetric |
370 |
< |
J2vals.push_back(eaData2.hardness * sSTOCoulInt( b, a, n, m, rval * PhysicalConstants::angstromsToBohr ) ); |
370 |
> |
J2vals.push_back(sSTOCoulInt( b, a, n, m, rval * PhysicalConstants::angstromToBohr ) * PhysicalConstants::hartreeToKcal ); |
371 |
|
} |
372 |
|
|
373 |
|
CubicSpline* J1 = new CubicSpline(); |