12.9 The XPol+SAPT (XSAPT) Method
12.9.1 Theory
XPol+SAPT, or “XSAPT”, was introduced by Jacobson and Herbert [689, 456] as a low-order-scaling, systematically-improvable method applicable to large systems. The idea is simply to replace the need for empirical parameters in the XPol method with on-the-fly evaluation of exchange-repulsion and dispersion interactions via pairwise-additive SAPT. (This basic idea has spawned several related approaches; see Ref. Lao:2015 for an overview of XSAPT-based methods.) Stated differently, XSAPT uses XPol to evaluate many-body (non-pairwise-additive) polarization effects, but then assumes that dispersion and exchange-repulsion interactions are pairwise additive, and evaluates them via pairwise SAPT0 or SAPT(KS) calculations.
In particular, the zeroth-order Hamiltonian for XSAPT is taken by the the sum of fragment Fock operators defined by the XPol procedure, and the perturbation is the usual SAPT intermolecular perturbation [Eq. eq:pairwise_perturbation] less the intermolecular interactions contained in the XPol fragment Fock operators. A standard SAPT0 correction is then computed for each pair of monomers, using Eq. eq:SAPT_interaction in conjunction with the modified perturbation, to obtain dimer interaction energy 
. The total XSAPT energy is then
![\begin{equation} \label{eq:XSAPT_ total_ E} E^{}_{\rm XSAPT} = \sum _ A \left( \sum _ a \Bigl [ 2\, \epsilon _ a^ A - \mathbf{c}_ a^\dagger ( \mathbf{J}^ A - \tfrac {1}{2}\mathbf{K}^ A)\mathbf{c}_ a\Bigr ] + E_{nuc}^ A + \sum _{B>A} E_{int}^{AB} \right) \; . \end{equation}](images/img-1862.png) |
(12.22) |
In this expression, we have removed the over-counting of two-electron interactions present in Hartree-Fock theory, effectively taking the intrafragment perturbation to first order. The generalization to a Kohn-Sham description of the monomers is straightforward, and is available in Q-Chem.
The inclusion of many-body polarization within the zeroth-order Hamiltonian makes the subsequent SAPT corrections less meaningful in terms of energy decomposition analysis. For instance, the first-order electrostatic correction in XSAPT is not the total electrostatic energy, since the former corrects for errors in the approximate electrostatic treatment at zeroth order (i.e., the electrostatic embedding). The dispersion correction may be less contaminated, since all of the XSAPT modifications to the traditional SAPT perturbation are one-electron operators and therefore the pairwise dispersion correction differs from its traditional SAPT analogue only insofar as the MOs are perturbed by the electrostatic embedding. This should be kept in mind when interpreting the output of an XSAPT calculation, although Lao and Herbert [694, 695] later proposed a many-body energy decomposition scheme for XSAPT that extends traditional SAPT energy decomposition to systems containing more than two monomers. (The aforementioned contamination problems are avoid through pairwise 
corrections, comparing XSAPT results to traditional SAPT based on gas-phase monomers.) An XSAPT calculation is requested by setting the $rem variables XPOL and SAPT equal to TRUE and also setting XPOL_MPOL_ORDER = CHARGES.
Researchers who use Q-Chem’s XPol+SAPT code are asked to cite Refs. Jacobson:2011 and Herbert:2012. The latter contains a thorough discussion of the theory; a briefer summary can be found in Ref. Jacobson:2013.
Example 12.276 Example showing an XPol+SAPT0 calculation using CHELPG charges and CPHF.
$rem BASIS CC-PVDZ METHOD HF XPOL TRUE XPOL_MPOL_ORDER CHARGES XPOL_CHARGE_TYPE QCHELPG SAPT TRUE SAPT_CPHF TRUE SYM_IGNORE TRUE $end $molecule 0 1 -- formic acid 0 1 C -1.888896 -0.179692 0.000000 O -1.493280 1.073689 0.000000 O -1.170435 -1.166590 0.000000 H -2.979488 -0.258829 0.000000 H -0.498833 1.107195 0.000000 -- formic acid 0 1 C 1.888896 0.179692 0.000000 O 1.493280 -1.073689 0.000000 O 1.170435 1.166590 0.000000 H 2.979488 0.258829 0.000000 H 0.498833 -1.107195 0.000000 $end
12.9.2 XSAPT(KS)+D
As mentioned above, the dispersion components of the (X)SAPT(KS) interaction energy are not of benchmark quality, even when tuned LRC functionals are employed [713]. The dispersion and exchange-dispersion terms are also the most expensive part of a SAPT0 or SAPT(KS) calculation, scaling as the fourth and fifth powers, respectively, of monomer size, whereas other terms are cubic scaling at worst. Both the efficiency and the accuracy of XSAPT(KS) calculations are thus improved if 
is replaced by an empirical atom–atom dispersion potential. The resulting method is called XSAPT(KS)+D [693, 694, 695]; consult Ref. Lao:2015 for an overview.
An XSAPT(KS)+D calculation is requested by setting the $rem variable SAPT_DISP_CORR equal to TRUE. There are three versions of the dispersion potential, a “first generation" (+D1) version [693], second-generation (+D2) version [694], and third-generation (+D3) version [695]; the user can select amongst these using SAPT_DISP_VERSION. Although all three versions exhibit similar performance for total binding energies [695], the +D2 and +D3 potentials were fit directly to ab initio dispersion potentials and do a much better job of reproducing individual energy components, as compared to +D1 [694, 695]. Furthermore, the training set was expanded in the third generation to eliminate the largest errors in +D2 calculations, which tend to be 
-stacked systems, and +D3 is the recommended dispersion correction.
As with XPol, the XSAPT and XSAPT(KS)+D methods do not function with a solvation model or with external changes. Currently, only single-point energies are available, and only for closed-shell (restricted) calculations with no frozen orbitals.
Researchers who use XSAPT(KS)+D are asked to cite Ref. Lao:2012b for +D1, Ref. Lao:2013 for +D2, or Ref. Lao:2015 for +D3.
Example 12.277 XSAPT(KS)+D2 calculation of benzene–methane interaction.
$rem sym_ignore true exchange gen basis aug-cc-pvtz aux_basis rimp2-aug-cc-pvtz xpol true ! must be set to true for sapt jobs too xpol_mpol_order charges xpol_charge_type qchelpg xpol_omega true risapt true sapt_order 2 sapt_basis projected sapt_disp_corr true sapt_disp_version 2 ! +D2 thresh 14 scf_convergence 7 basis_lin_dep_thresh 12 lrc_dft true $end $xc_functional x wPBE 1.0 c PBE 1.0 $end $lrc_omega 275 450 $end $molecule 0 1 -- benzene 0 1 C 1.3932178 0.0362913 -0.6332803 C 0.7280364 -1.1884015 -0.6333017 C -0.6651797 -1.2247077 -0.6332803 C -1.3932041 -0.0362972 -0.6333017 C -0.7280381 1.1884163 -0.6332803 C 0.6651677 1.2246987 -0.6333017 H 2.4742737 0.0644484 -0.6317240 H 1.2929588 -2.1105409 -0.6317401 H -1.1813229 -2.1750081 -0.6317240 H -2.4742614 -0.0644647 -0.6317401 H -1.2929508 2.1105596 -0.6317240 H 1.1813026 2.1750056 -0.6317401 -- methane 0 1 C 0.0000000 0.0000000 3.0826195 H 0.5868776 0.8381742 3.4463772 H -1.0193189 0.0891638 3.4463772 H 0.0000000 0.0000000 1.9966697 H 0.4324413 -0.9273380 3.4463772 $end
For energy decomposition analysis using, e.g., XSAPT(KS)+D3, three individual calculations must be performed: XSAPT(KS)+D3, SAPT(KS)+D3, and SAPT0, as demonstrated in the example below. The electrostatic, exchange, and dispersion energies can be obtained in the SAPT(KS)+D3 calculation by searching the keywords “E1_elst”, “E1_exch”, and “Empirical E2_disp + E2_exch-disp”, respectively. The induction energy includes three parts. First, there is 
(“E2_ind” and “E2_exch-ind”), obtained from the SAPT(KS)+D3 calculation. The second part is the total energy difference between XSAPT(KS)+D3 and SAPT(KS)+D3, and the total energy can be obtained by searching for “SAPT corrected total energy” in both calculations. This second part provides the many-body polarization and approximate infinite-order response correction. The final part of the energy decomposition accounts for higher-order polarization effects that can be approximated by searching the SAPT0 calculation for the keyword “dSCF” (
correction). The total binding energy is the sum of electrostatic, exchange, induction, and dispersion components obtained above.
Example 12.278 The XSAPT(KS)+D3 energy-decomposition analysis for water dimer, which requires three individual calculations.
$comment (1) XSAPT(KS)+D3 $end $rem sym_ignore true exchange gen basis cc-pvdz aux_basis rimp2-cc-pvdz xpol true ! must be set to true for sapt jobs too xpol_mpol_order charges ! gas or charges xpol_charge_type qchelpg ! qlowdin,qmulliken,qchelpg xpol_omega true xpol_print 3 sapt_print 3 risapt true sapt_order 2 ! can be set to 1, ELST or RSPT sapt_basis projected ! monomer, dimer (if only 2 monomers), or projected sapt_disp_corr true sapt_disp_version 3 mem_total 4000 mem_static 2000 ao2mo_disk 35000 scf_convergence 7 thresh 12 lrc_dft true $end $xc_functional x wPBE 1.0 c PBE 1.0 $end $lrc_omega 500 500 $end $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 @@@ $comment (2) SAPT(KS)+D3 $end $rem sym_ignore true exchange gen basis cc-pvdz aux_basis rimp2-cc-pvdz xpol true ! must be set to true for sapt jobs too xpol_mpol_order gas ! gas or charges xpol_omega true xpol_print 3 sapt_print 3 risapt true sapt_order 2 ! can be set to 1, ELST or RSPT sapt_basis projected ! monomer, dimer (if only 2 monomers), or projected sapt_disp_corr true sapt_disp_version 3 mem_total 4000 mem_static 2000 ao2mo_disk 35000 scf_convergence 7 thresh 12 lrc_dft true $end $xc_functional x wPBE 1.0 c PBE 1.0 $end $lrc_omega 500 500 $end $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 @@@ $comment (3) SAPT0 $end $rem sym_ignore true exchange hf basis cc-pvdz aux_basis rimp2-cc-pvdz xpol true ! must be set to true for sapt jobs too xpol_mpol_order gas ! gas or charges xpol_print 3 sapt_print 3 risapt true sapt_order 2 ! can be set to 1, ELST or RSPT sapt_basis dimer ! monomer, dimer (if only 2 monomers), or projected sapt_cphf true sapt_dscf true mem_total 4000 mem_static 2000 ao2mo_disk 35000 scf_convergence 7 thresh 12 $end $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