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Currently, the handling of point group symmetry in LASSCF and LASSI only supports symmetry elements that leave each fragment in place. So for instance, trans-butadiene split into two (2,2) π-orbital fragments on either end can be calculated with Cs point group but not the full C2h point group, because the C2 rotation permutes each fragment with the other. Symmetry elements that permute one fragment with another are mandatory for PBC-related applications such as band structures because such features represent the only rigorous way to consistently enforce a particular phase convention of the wave function.
The main obstacles here seem to be:
Applying a symmetry operator to an entire multielectron wave function defined in an active subspace such that it changes places with a different active subspace. Symmetry operators applied to individual orbitals are, of course, already implemented in PySCF
Deriving and implementing the energy derivatives with respect to symmetry-adapted unitary group generators.
Deriving the equations describing a symmetry-adapted LASSI model space and applying this framework to the LASSI logical scaffolding.
The text was updated successfully, but these errors were encountered:
Currently, the handling of point group symmetry in LASSCF and LASSI only supports symmetry elements that leave each fragment in place. So for instance, trans-butadiene split into two (2,2) π-orbital fragments on either end can be calculated with Cs point group but not the full C2h point group, because the C2 rotation permutes each fragment with the other. Symmetry elements that permute one fragment with another are mandatory for PBC-related applications such as band structures because such features represent the only rigorous way to consistently enforce a particular phase convention of the wave function.
The main obstacles here seem to be:
The text was updated successfully, but these errors were encountered: