Difference between revisions of "CamCASP/Programming/5"
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[[ CamCASP/Programming/5/example1| Here]] are the input files for a simple CamCASP calculation that demonstrates this. |
[[ CamCASP/Programming/5/example1| Here]] are the input files for a simple CamCASP calculation that demonstrates this. |
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+ | The example calculates the nuclear integral of the occupied orbital with itself. The exact integral is <math>2.60588</math>, and what we get is: |
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+ | * Cartesian: 2.60588 |
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+ | * Spherical: 2.53362 |
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+ | I.e., a 2.8% error in the spherical case. This error is reflected in the normalization constraints. These are satisfied exactly with the Cartesian auxiliary basis, but the spherical basis results in a normalization constraint of 1.1227 for the occupied x occupied orbital product. This should be exactly one. |
Revision as of 16:04, 12 May 2009
CamCASP => Programming => Auxiliary basis sets
Spherical versus Cartesian GTOs
- What are the advantages of the two basis types: Spherical and Cartesian?
- Which one results in more accurate energies and why?
Spherical GTOs:
- Smaller in size
- More well-defined set of linear equations during DF
- Lower accuracy.
- Seemingly erratic behaviour in aug-cc-pVnZ series.
- Rotations made easy as we have the Wigner rotation matrices.
Cartesian GTOs:
- Larger in size
- DF equations seem OK.
- Higher accuracy of energies
- More consistent behaviour of aug-cc-pVnZ series.
- Don't have rotation matrices coded, but these have been derived.
Simple example: 1
Here's an example that demonstrates the inadequacy of the spherical GTOs. Consider a 1p1s (yes, in this order) main basis and a single occupied orbital. This would be the px orbital. The space the auxiliary basis needs to span is 1p1s x 1p1s = 1s1p1d. So let us construct this auxiliary basis and perform the DF.
Here's the question: Can the density be exactly fitted using this auxiliary basis?
The answer depends on which basis type is used for the auxiliary basis.
- Cartesian: The auxiliary basis consists of the following combinations:
<math>
s \ \ x \ \ y \ \ z \ \ x^2 \ \ xy \ \ xz \ \ y^2 \ \ yz \ \ z^2
</math>
So the density, <math>x^2</math>, can be exactly described.
- Spherical: Now the auxiliary basis consists of the functions:
<math>
s \ \ x \ \ y \ \ z \ \ \sqrt{3}xy \ \ \sqrt{3}yz \ \ z^2-1/2(x^2+y^2) \ \ \sqrt{3}xz \ \ \sqrt{3}/2(x^2+y^2)
</math>
Amazingly, the density <math>x^2</math> cannot be exactly written as a linear combination of these functions.
Here are the input files for a simple CamCASP calculation that demonstrates this. The example calculates the nuclear integral of the occupied orbital with itself. The exact integral is <math>2.60588</math>, and what we get is:
- Cartesian: 2.60588
- Spherical: 2.53362
I.e., a 2.8% error in the spherical case. This error is reflected in the normalization constraints. These are satisfied exactly with the Cartesian auxiliary basis, but the spherical basis results in a normalization constraint of 1.1227 for the occupied x occupied orbital product. This should be exactly one.