7.2 Uncorrelated Wave Function Methods

7.2.4 Spin-Flip Extended CIS (SF-XCIS)

Spin-flip extended CIS (SF-XCIS)142 is a spin-complete extension of the spin-flip single excitation configuration interaction (SF-CIS) method.502 The method includes all configurations in which no more than one virtual level of the high spin triplet reference becomes occupied and no more than one doubly occupied level becomes vacant.

SF-XCIS is defined only from a restricted open shell Hartree-Fock triplet ground state reference. The final SF-XCIS wave functions correspond to spin-pure MS=0 (singlet or triplet) states. The fully balanced treatment of the half-occupied reference orbitals makes it very suitable for applications with two strongly correlated electrons, such as single bond dissociation, systems with important diradical character or the study of excited states with significant double excitation character.

The computational cost of SF-XCIS scales in the same way with molecule size as CIS itself, with a pre-factor 13 times larger.

Example 7.3  A SF-XCIS calculation of ground and excited states of trimethylenemethane (TMM) diradical, for which double substitutions make considerable contributions to low-lying excited states.

$molecule
   0 3
   C
   C 1 CC1
   C 1 CC2   2 A2
   C 1 CC2   2 A2    3 180.0
   H 2 C2H   1 C2CH  3 0.0
   H 2 C2H   1 C2CH  4 0.0
   H 3 C3Hu  1 C3CHu 2 0.0
   H 3 C3Hd  1 C3CHd 4 0.0
   H 4 C3Hu  1 C3CHu 2 0.0
   H 4 C3Hd  1 C3CHd 3 0.0

   CC1    = 1.35
   CC2    = 1.47
   C2H    = 1.083
   C3Hu   = 1.08
   C3Hd   = 1.08
   C2CH   = 121.2
   C3CHu  = 120.3
   C3CHd  = 121.3
   A2     = 121.0
$end

$rem
  UNRESTRICTED    = false   SF-XCIS runs from ROHF triplet reference
  EXCHANGE        = HF
  BASIS           = 6-31G*
  SCF_CONVERGENCE = 10
  SCF_ALGORITHM   = DM
  MAX_SCF_CYCLES  = 100
  SPIN_FLIP_XCIS  = true    Do SF-XCIS
  CIS_N_ROOTS     = 3
  CIS_SINGLETS    = true    Do singlets
  CIS_TRIPLETS    = true    Do triplets
$end