The definition of polarization energy lowering in the original ALMO-EDA used the full AO space of each fragment as the variational degrees of freedom. This is based on the assumption that the AO basis functions are fragment-ascribable based on their atomic centers. However, this assumption becomes inappropriate when very large basis sets are used, especially those with diffuse functions (e.g. def2-QZVPPD). In such scenarios, basis functions on a given fragment tend to describe other fragments so that the “absolute localization" constraint becomes weaker and finally gets effectively removed. This is why the original ALMO-EDA scheme does not have a well-defined basis set limit for its polarization energy.
To overcome this problem, Horn and Head-Gordon proposed a new definition for the POL term in the ALMO-EDA method based on fragment electrical response functions (FERFs).397 FERFs on a given fragment are prepared by solving CPSCF equations after its SCF solution is found:
where is SCF orbital Hessian and is a component () of a multipole matrix with a certain order. The resulting fragment response matrices () are a set of matrices. Then, a singular value decomposition (SVD) is performed on :
and the left vectors (not including the null vectors) will be used to construct a truncated virtual space, which is used to define the variational degrees of freedom for the SCFMI problem:
where denotes the original virtual orbitals of the given fragment.
The basic spirit of using FERFs is to obtain a subset of virtuals that is most pertinent to the electrical polarization of a given fragment, while the redundant variational degrees of freedom (which might be CT-like) are excluded. This scheme is shown to give a well-defined basis set limit for the polarization energy that relies on the SCFMI calculation. The multipole orders (dipole (D), quadrupole (Q), and octopole (O)) included on the RHS of eq. 12.2 decide the span of FERFs on each fragment. Numerical experiments suggest that the inclusion of dipole- and quadrupole-type responses is able to long-range induced electrostatics correctly and also gives a well-defined basis set limit, which is thus recommended as the working basis of the SCFMI problem. The full span of the polarization subspace of fragment is thus:
Therefore, each occupied orbital will be paired with eight virtual orbitals (if the employed AO basis is large enough).
The polarization subspaces constructed as in eq. 12.4 are non-orthogonal between fragments. Therefore, it is named as the “nDQ" model for polarization. There is another version of this method which enforces interfragment orthogonality between the polarization subspaces and it is correspondingly termed as “oDQ" (or with other multipole orders). The preparation of orthogonal FERFs is more complicated (see ref. 397 for the details) and usually gives less favorable polarization energies. For most general cases, we recommend the use of the “nDQ" model. Calculations using FERFs are performed using the generalized SCFMI procedure introduced in Section 12.7.1.
$molecule 0 1 -- 0 1 O -1.551007 -0.114520 0.000000 H -1.934259 0.762503 0.000000 H -0.599677 0.040712 0.000000 -- 0 1 O 1.350625 0.111469 0.000000 H 1.680398 -0.373741 -0.758561 H 1.680398 -0.373741 0.758561 $end $rem JOBTYPE sp METHOD wb97x-v GEN_SCFMAN true BASIS 6-31+G(d) GEN_SCFMAN true SCF_ALGORITHM diis SCF_CONVERGENCE 8 THRESH 14 SYMMETRY false SYM_IGNORE true SCF_FINAL_PRINT 1 FRGM_METHOD stoll SCFMI_MODE 1 !nonortho gen scfmi CHILD_MP true CHILD_MP_ORDERS 232 !DQ FD_MAT_VEC_PROD false $end