Comments (1)
Agreement is to parts in
Roughly the same level of agreement between Brueckner orbitals and Spectrum orbitals using Goldstone technique for
However, agreement drops to parts in
Could be related to B-spline code, but more likely is due to calculation of
HF | HF/Bruckner | Spectrum | |
---|---|---|---|
-0.1273682 | -0.1273681 | 1E-06 | |
-0.0551874 | -0.0551874 | 9E-07 | |
-0.0309525 | -0.0309525 | 6E-07 | |
-0.0198146 | -0.0198146 | -1E-06 | |
Goldstone(2) | |||
-0.1475863 | -0.1475867 | -3E-06 | |
-0.0593160 | -0.0593161 | -2E-06 | |
-0.0325347 | -0.0325347 | -6E-07 | |
-0.0205929 | -0.0205930 | -2E-06 | |
Feynman(2) | |||
-0.1478421 | -0.1478491 | -5E-05 | |
-0.0593860 | -0.0593874 | -2E-05 | |
-0.0325636 | -0.0325641 | -2E-05 | |
-0.0206073 | -0.0206076 | -1E-05 | |
Feynman( |
|||
-0.1432236 | -0.1431959 | 2E-04 | |
-0.0584265 | -0.0584218 | 8E-05 | |
-0.0321932 | -0.0321915 | 5E-05 | |
-0.0204248 | -0.0204240 | 4E-05 |
Full code input/output:
SpectrumStability.txt
from ampsci.
Related Issues (20)
- Add l-dependence to Radiative Potential HOT 1
- Hartree-Fock update: in-homogeneous method
- Matrix elements, frequency dependent, omega = each
- Add self-energy vertex and magnetic loop Uehling (VP vertex) HOT 1
- DiracOperator
- Correlations
- Feynman
- Hartree Fock + Wavefunction
- DiracODE
- Coulomb and Angular Tables
- B-spline stability HOT 1
- Breit, s2
- StrucRad to use full RPA methods HOT 1
- Breit with RPA [probably no issue] HOT 4
- TDHF for frequency-dependent operators HOT 2
- Breit into Green's function
- Add ".amp" or similar to all binary outputs to help cleanup HOT 1
- Generalised input options for RPA (+SR) HOT 2
- Add third-order matrix element method
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