Test Suite and Sample Inputs

PSI4 is distributed with an extensive test suite, which can be found in psi4/tests. After building the source code, these can automatically be run by running make tests in the compilation directory. Sample input files can be found in the the psi4/samples subdirectory of the top-level Psi directory. The samples and a brief description are provided below.

Input File	Description
dfmp2-4	conventional and density-fitting mp2 test of mp2 itself and setting scs-mp2
scf2	RI-SCF cc-pVTZ energy of water, with Z-matrix input and cc-pVTZ-RI auxilliary basis.
fnocc2	Test G2 method for H2O
cc22	ROHF-EOM-CCSD/DZ on the lowest two states of each irrep in CH2.
fnocc4	Test FNO-DF-CCSD(T) energy
mcscf2	TCSCF cc-pVDZ energy of asymmetrically displaced ozone, with Z-matrix input.
omp3-4	SCS-OMP3 cc-pVDZ geometry optimization for the H2O molecule.
min_input	This checks that all energy methods can run with a minimal input and set symmetry.
mp2-1	All-electron MP2 6-31G** geometry optimization of water
cc25	Single point gradient of 1-2B2 state of H2O+ with EOM-CCSD
opt6	Various constrained energy minimizations of HOOH with cc-pvdz RHF
omp2_5-grad1	OMP2.5 cc-pVDZ gradient for the H2O molecule.
fd-gradient	SCF STO-3G finite-difference tests
scf6	Tests RHF/ROHF/UHF SCF gradients
psimrcc-ccsd_t-3	Mk-MRCCSD(T) single point. CH2 state described using the Ms = 0 component of the singlet. Uses RHF singlet orbitals.
dfmp2-3	DF-MP2 cc-pVDZ frozen core gradient of benzene, computed at the DF-SCF cc-pVDZ geometry
mcscf1	ROHF 6-31G** energy of the state of CH2, with Z-matrix input. The occupations are specified explicitly.
ci-multi	BH single points, checking that program can run multiple instances of DETCI in a single input, without an intervening clean() call
sapt5	SAPT0 aug-cc-pVTZ computation of the charge transfer energy of the water dimer.
adc2	ADC/aug-cc-pVDZ on two water molecules that are distant from 1000 angstroms from each other
cc40	RHF-CC2-LR/cc-pVDZ optical rotation of H2O2. gauge = length, omega = (589 355 nm)
dcft2	DC-06 calculation for the He dimer. This performs a two-step update of the orbitals and cumulant, using DIIS extrapolation. Four-virtual integrals are handled in the MO Basis.
cc32	CC3/cc-pVDZ H2O geom from Olsen et al., JCP 104, 8007 (1996)
tu1-h2o-energy	Sample HF/cc-pVDZ H2O computation
dcft4	DCFT calculation for the HF+ using DC-06 functional. This performs both two-step and simultaneous update of the orbitals and cumulant using DIIS extrapolation. Four-virtual integrals are first handled in the MO Basis for the first two energy computations. In the next two the ao_basis=disk algorithm is used, where the transformation of integrals for four-virtual case is avoided. The computation is then repeated using the DC-12 functional with the same algorithms.
pywrap-db3	Test that Python Molecule class processes geometry like PsiMod Molecule class.
fci-h2o	6-31G H2O Test FCI Energy Point
ocepa1	OCEPA cc-pVDZ energy for the H2O molecule.
psimrcc-pt2	Mk-MRPT2 single point. F2 state described using the Ms = 0 component of the singlet. Uses TCSCF singlet orbitals.
cc46	EOM-CC2/cc-pVDZ on H2O2 with two excited states in each irrep
mp2_5-grad1	MP2.5 cc-pVDZ gradient for the H2O molecule.
mints4	A demonstration of mixed Cartesian/ZMatrix geometry specification, using variables, for the benzene-hydronium complex. Atoms can be placed using ZMatrix coordinates, whether they belong to the same fragment or not. Note that the Cartesian specification must come before the ZMatrix entries because the former define absolute positions, while the latter are relative.
fd-freq-gradient-large	SCF DZ finite difference frequencies by energies for C4NH4
dft1-alt	DFT Functional Test
pywrap-checkrun-rohf	This checks that all energy methods can run with a minimal input and set symmetry.
cc48	reproduces dipole moments in J.F. Stanton’s “biorthogonal” JCP paper
psimrcc-fd-freq2	Mk-MRCCSD frequencies. O$_3` state described using the Ms = 0 component of the singlet. Uses TCSCF orbitals.
cc28	CCSD/cc-pVDZ optical rotation calculation (length gauge only) on Z-mat H2O2
cc6	Frozen-core CCSD(T)/cc-pVDZ on C4H4N anion with disk ao algorithm
ghosts	Density fitted MP2 cc-PVDZ/cc-pVDZ-RI computation of formic acid dimer binding energy using explicit specification of ghost atoms. This is equivalent to the dfmp2_1 sample but uses both (equivalent) specifications of ghost atoms in a manual counterpoise correction.
cc8	UHF-CCSD(T) cc-pVDZ frozen-core energy for the state of the CN radical, with Z-matrix input.
cepa2	cc-pvdz H2O Test ACPF Energy/Properties
rasci-ne	Ne atom RASCI/cc-pVQZ Example of split-virtual CISD[TQ] from Sherrill and Schaefer, J. Phys. Chem. XXX This uses a “primary” virtual space 3s3p (RAS 2), a “secondary” virtual space 3d4s4p4d4f (RAS 3), and a “tertiary” virtual space consisting of the remaining virtuals. First, an initial CISD computation is run to get the natural orbitals; this allows a meaningful partitioning of the virtual orbitals into groups of different importance. Next, the RASCI is run. The split-virtual CISD[TQ] takes all singles and doubles, and all triples and quadruples with no more than 2 electrons in the secondary virtual subspace (RAS 3). If any electrons are present in the tertiary virtual subspace (RAS 4), then that excitation is only allowed if it is a single or double.
cc5a	RHF CCSD(T) STO-3G frozen-core energy of C4NH4 Anion
ocepa2	OCEPA cc-pVDZ energy with B3LYP initial guess for the NO radical
mcscf3	RHF 6-31G** energy of water, using the MCSCF module and Z-matrix input.
frac	Carbon/UHF Fractionally-Occupied SCF Test Case
pywrap-basis	SAPT calculation on bimolecular complex where monomers are unspecified so driver auto-fragments it. Basis set and auxiliary basis sets are assigned by atom type.
psimrcc-sp1	Mk-MRCCSD single point. O2 state described using the Ms = 0 component of the triplet. Uses ROHF triplet orbitals.
fd-freq-gradient	STO-3G frequencies for H2O by finite-differences of gradients
dfmp2-1	Density fitted MP2 cc-PVDZ/cc-pVDZ-RI computation of formic acid dimer binding energy using automatic counterpoise correction. Monomers are specified using Cartesian coordinates.
cc13	UHF-CCSD/cc-pVDZ CH2 geometry optimization via analytic gradients
cc34	RHF-CCSD/cc-pVDZ energy of H2O partitioned into pair energy contributions.
cepa3	cc-pvdz H2O Test coupled-pair CISD against DETCI CISD
cisd-opt-fd	H2O CISD/6-31G** Optimize Geometry by Energies
omp2-grad2	OMP2 cc-pVDZ gradient for the NO radical
mrcc1	CCSDT cc-pVDZ energy for the H2O molecule using MRCC
cc49	EOM-CC3(UHF) on CH radical with user-specified basis and properties for particular root
cc41	RHF-CC2-LR/cc-pVDZ optical rotation of H2O2. gauge = both, omega = (589 355 nm)
sapt1	SAPT0 cc-pVDZ computation of the ethene-ethyne interaction energy, using the cc-pVDZ-JKFIT RI basis for SCF and cc-pVDZ-RI for SAPT. Monomer geometries are specified using Cartesian coordinates.
cc39	RHF-CC2-LR/cc-pVDZ dynamic polarizabilities of HOF molecule.
cisd-h2o+-2	6-31G** H2O+ Test CISD Energy Point
mints2	A test of the basis specification. A benzene atom is defined using a ZMatrix containing dummy atoms and various basis sets are assigned to different atoms. The symmetry of the molecule is automatically lowered to account for the different basis sets.
dft-b2plyp	Double-hybrid density functional B2PYLP. Reproduces portion of Table I in S. Grimme’s J. Chem. Phys 124 034108 (2006) paper defining the functional.
props3	DF-SCF cc-pVDZ multipole moments of benzene, up to 7th order and electrostatic potentials evaluated at the nuclear coordinates
opt2-fd	SCF DZ allene geometry optimzation, with Cartesian input
dcft6	DCFT calculation for the triplet O2 using DC-06, DC-12 and CEPA0 functionals. Only two-step algorithm is tested.
sapt2	SAPT0 aug-cc-pVDZ computation of the benzene-methane interaction energy, using the aug-pVDZ-JKFIT DF basis for SCF, the aug-cc-pVDZ-RI DF basis for SAPT0 induction and dispersion, and the aug-pVDZ-JKFIT DF basis for SAPT0 electrostatics and induction. This example uses frozen core as well as asyncronous I/O while forming the DF integrals and CPHF coefficients.
cc19	CCSD/cc-pVDZ dipole polarizability at two frequencies
scf-guess-read	Sample UHF/cc-pVDZ H2O computation on a doublet cation, using RHF/cc-pVDZ orbitals for the closed-shell neutral as a guess
cc4	RHF-CCSD(T) cc-pVQZ frozen-core energy of the BH molecule, with Cartesian input. After the computation, the checkpoint file is renamed, using the PSIO handler.
cc10	ROHF-CCSD cc-pVDZ energy for the state of the CN radical
castup3	SCF with various combinations of pk/density-fitting, castup/no-castup, and spherical/cartesian settings. Demonstrates that puream setting is getting set by orbital basis for all df/castup parts of calc. Demonstrates that answer doesn’t depend on presence/absence of castup. Demonstrates (by comparison to castup2) that output file doesn’t depend on options (scf_type) being set global or local. This input uses local.
cc8c	ROHF-CCSD cc-pVDZ frozen-core energy for the state of the CN radical, with Cartesian input.
scf1	RHF cc-pVQZ energy for the BH molecule, with Cartesian input.
cisd-h2o+-0	6-31G** H2O+ Test CISD Energy Point
cc43	RHF-CC2-LR/STO-3G optical rotation of (S)-methyloxirane. gauge = both, omega = (589 355 nm)
cc27	Single point gradient of 1-1B2 state of H2O with EOM-CCSD
cisd-sp-2	6-31G** H2O Test CISD Energy Point
opt1	SCF STO-3G geometry optimzation, with Z-matrix input
dft2	DFT Functional Test
cc15	RHF-B-CCD(T)/6-31G** H2O single-point energy (fzc, MO-basis )
dft1	DFT Functional Test
cc18	RHF-CCSD-LR/cc-pVDZ static polarizability of HOF
mom	Maximum Overlap Method (MOM) Test. MOM is designed to stabilize SCF convergence and to target excited Slater determinants directly.
fci-h2o-fzcv	6-31G H2O Test FCI Energy Point
pywrap-cbs1	Various basis set extrapolation tests
fd-freq-energy	SCF STO-3G finite-difference frequencies from energies
dcft5	DC-06 calculation for the O2 molecule (triplet ground state). This performs geometry optimization using two-step and simultaneous solution of the response equations for the analytic gradient.
pywrap-all	Intercalls among python wrappers- database, cbs, optimize, energy, etc. Though each call below functions individually, running them all in sequence or mixing up the sequence is aspirational at present. Also aspirational is using the intended types of gradients.
opt2	SCF DZ allene geometry optimzation, with Cartesian input
mp3-grad1	MP3 cc-pVDZ gradient for the H2O molecule.
scf11-freq-from-energies	Test frequencies by finite differences of energies for planar C4NH4 TS
opt5	6-31G** UHF CH2 3B1 optimization. Uses a Z-Matrix with dummy atoms, just for demo and testing purposes.
cc23	ROHF-EOM-CCSD/DZ analytic gradient lowest state of H2O+ (A1 excitation)
cc54	CCSD dipole with user-specified basis set
ocepa-freq1	OCEPA cc-pVDZ freqs for C2H2
cc26	Single-point gradient, analytic and via finite-differences of 2-1A1 state of H2O with EOM-CCSD
fci-tdm	He2+ FCI/cc-pVDZ Transition Dipole Moment
rasci-c2-active	6-31G* C2 Test RASCI Energy Point, testing two different ways of specifying the active space, either with the ACTIVE keyword, or with RAS1, RAS2, RESTRICTED_DOCC, and RESTRICTED_UOCC
ocepa-grad1	OCEPA cc-pVDZ gradient for the H2O molecule.
dft3	DFT integral algorithms test, performing w-B97 RKS and UKS computations on water and its cation, using all of the different integral algorithms. This tests both the ERI and ERF integrals.
tu2-ch2-energy	Sample UHF/6-31G** CH2 computation
cc16	UHF-B-CCD(T)/cc-pVDZ CH2 single-point energy (fzc, MO-basis )
sapt4	SAPT2+(3) aug-cc-pVDZ computation of the formamide dimer interaction energy, using the aug-cc-pVDZ-JKFIT DF basis for SCF and aug-cc-pVDZ-RI for SAPT. This example uses frozen core as well as MP2 natural orbital approximations.
cc47	EOM-CCSD/cc-pVDZ on H2O2 with two excited states in each irrep
dft-freq	Frequencies for H2O B3LYP/6-31G* at optimized geometry
mp2-grad1	MP2 cc-pVDZ gradient for the H2O molecule.
scf3	are specified explicitly.
ocepa-grad2	OCEPA cc-pVDZ gradient for the NO radical
dftd3-energy	Exercises the various DFT-D corrections, both through python directly and through c++
pywrap-db1	Database calculation, so no molecule section in input file. Portions of the full databases, restricted by subset keyword, are computed by sapt0 and dfmp2 methods.
cc52	CCSD Response for H2O2
pywrap-db2	Database calculation, run in sow/reap mode.
cc50	EOM-CC3(ROHF) on CH radical with user-specified basis and properties for particular root
omp2-2	OMP2 cc-pVDZ energy with ROHF initial guess orbitals for the NO radical
cc12	Single point energies of multiple excited states with EOM-CCSD
cisd-sp	6-31G** H2O Test CISD Energy Point
mints6	Patch of a glycine with a methyl group, to make alanine, then DF-SCF energy calculation with the cc-pVDZ basis set
mrcc4	CCSDT cc-pVDZ optimization and frequencies for the H2O molecule using MRCC
omp2-5	SOS-OMP2 cc-pVDZ geometry optimization for the H2O molecule.
props1	RHF STO-3G dipole moment computation, performed by applying a finite electric field and numerical differentiation.
cc42	RHF-CC2-LR/STO-3G optical rotation of (S)-methyloxirane. gauge = length, omega = (589 355 nm)
omp2_5-1	OMP2 cc-pVDZ energy for the H2O molecule.
fci-dipole	6-31G H2O Test FCI Energy Point
fnocc3	Test FNO-QCISD(T) computation
tu4-h2o-freq	Frequencies for H2O HF/cc-pVDZ at optimized geometry
dcft3	DC-06 calculation for the He dimer. This performs a simultaneous update of the orbitals and cumulant, using DIIS extrapolation. Four-virtual integrals are handled in the AO Basis, using integrals stored on disk.
cc4a	RHF-CCSD(T) cc-pVQZ frozen-core energy of the BH molecule, with Cartesian input. This version tests the FROZEN_DOCC option explicitly
cisd-h2o+-1	6-31G** H2O+ Test CISD Energy Point
dft-psivar	HF and DFT variants single-points on zmat methane, mostly to test that PSI variables are set and computed correctly.
pywrap-alias	Test parsed and exotic calls to energy() like zapt4, mp2.5, and cisd are working
cc8b	ROHF-CCSD cc-pVDZ frozen-core energy for the state of the CN radical, with Cartesian input.
mints3	Test individual integral objects for correctness.
omp3-2	OMP3 cc-pVDZ energy with ROHF initial guess for the NO radical
cc2	6-31G** H2O CCSD optimization by energies, with Z-Matrix input
pywrap-checkrun-convcrit	Advanced python example sets different sets of scf/post-scf conv crit and check to be sure computation has actually converged to the expected accuracy.
cepa0-grad2	CEPA cc-pVDZ gradient for the NO radical
cc45	RHF-EOM-CC2/cc-pVDZ lowest two states of each symmetry of H2O.
fci-tdm-2	BH-H2+ FCI/cc-pVDZ Transition Dipole Moment
psimrcc-ccsd_t-2	Mk-MRCCSD(T) single point. CH2 state described using the Ms = 0 component of the singlet. Uses RHF singlet orbitals.
sad1	Test of the superposition of atomic densities (SAD) guess, using a highly distorted water geometry with a cc-pVDZ basis set. This is just a test of the code and the user need only specify guess=sad to the SCF module’s (or global) options in order to use a SAD guess. The test is first performed in C2v symmetry, and then in C1.
psimrcc-fd-freq1	Mk-MRCCSD single point. O2 state described using the Ms = 0 component of the triplet. Uses ROHF triplet orbitals.
rasci-h2o	RASCI/6-31G** H2O Energy Point
cc17	Single point energies of multiple excited states with EOM-CCSD
tu3-h2o-opt	Optimize H2O HF/cc-pVDZ
mrcc2	CCSDT(Q) cc-pVDZ energy for the H2O molecule using MRCC. This example builds up from CCSD. First CCSD, then CCSDT, finally CCSDT(Q).
cc21	ROHF-EOM-CCSD/DZ analytic gradient lowest excited state of H2O+ (B1 excitation)
opt4	SCF cc-pVTZ geometry optimzation, with Z-matrix input
cc13a	UHF-CCSD(T)/cc-pVDZ CH2 geometry optimization via analytic gradients
mpn-bh	MP(n)/aug-cc-pVDZ BH Energy Point, with n=2-19. Compare against M. L. Leininger et al., J. Chem. Phys. 112, 9213 (2000)
pywrap-checkrun-uhf	This checks that all energy methods can run with a minimal input and set symmetry.
omp2_5-grad2	OMP2.5 cc-pVDZ gradient for the NO radical
cc38	RHF-CC2-LR/cc-pVDZ static polarizabilities of HOF molecule.
mrcc3	CCSD(T) cc-pVDZ geometry optimization for the H2O molecule using MRCC.
opt3	SCF cc-pVDZ geometry optimzation, with Z-matrix input
omp2_5-2	OMP2 cc-pVDZ energy for the H2O molecule.
cc3	cc3: RHF-CCSD/6-31G** H2O geometry optimization and vibrational frequency analysis by finite-differences of gradients
scf-bz2	Benzene Dimer Out-of-Core HF/cc-pVDZ
cc51	EOM-CC3/cc-pVTZ on H2O
fci-h2o-2	6-31G H2O Test FCI Energy Point
mp2-grad2	MP2 cc-pVDZ gradient for the NO radical
cc31	CCSD/sto-3g optical rotation calculation (both gauges) at two frequencies on methyloxirane
psimrcc-ccsd_t-1	Mk-MRCCSD(T) single point. CH2 state described using the Ms = 0 component of the singlet. Uses RHF singlet orbitals.
cc11	Frozen-core CCSD(ROHF)/cc-pVDZ on CN radical with disk-based AO algorithm
pywrap-checkrun-rhf	This checks that all energy methods can run with a minimal input and set symmetry.
fd-freq-energy-large	SCF DZ finite difference frequencies by energies for C4NH4
cc33	CC3(UHF)/cc-pVDZ H2O geom from Olsen et al., JCP 104, 8007 (1996)
dft-grad	DF-BP86-D2 cc-pVDZ frozen core gradient of S22 HCN
tu6-cp-ne2	Example potential energy surface scan and CP-correction for Ne2
cc30	CCSD/sto-3g optical rotation calculation (length gauge only) at two frequencies on methyloxirane
omp3-3	OMP3 cc-pVDZ energy with B3LYP initial guess for the NO radical
sapt3	SAPT2+3(CCD) aug-cc-pVDZ computation of the water dimer interaction energy, using the aug-cc-pVDZ-JKFIT DF basis for SCF and aug-cc-pVDZ-RI for SAPT.
scf5	Test of all different algorithms and reference types for SCF, on singlet and triplet O2, using the cc-pVTZ basis set.
pywrap-opt-sowreap	Finite difference optimization, run in sow/reap mode.
cc8a	ROHF-CCSD(T) cc-pVDZ frozen-core energy for the state of the CN radical, with Cartesian input.
opt1-fd	SCF STO-3G geometry optimzation, with Z-matrix input, by finite-differences
dft-dldf	Dispersionless density functional (dlDF+D) internal match to Psi4 Extensive testing has been done to match supplemental info of Szalewicz et. al., Phys. Rev. Lett., 103, 263201 (2009) and Szalewicz et. al., J. Phys. Chem. Lett., 1, 550-555 (2010)
castup1	Test of SAD/Cast-up (mainly not dying due to file weirdness)
omp3-5	SOS-OMP3 cc-pVDZ geometry optimization for the H2O molecule.
adc1	ADC/6-31G** on H2O
cc9	UHF-CCSD(T) cc-pVDZ frozen-core energy for the state of the CN radical, with Z-matrix input.
pubchem1	Benzene vertical singlet-triplet energy difference computation, using the PubChem database to obtain the initial geometry, at the UHF an ROHF levels of theory.
cc44	Test case for some of the PSI4 out-of-core codes. The code is given only 2.0 MB of memory, which is insufficient to hold either the A1 or B2 blocks of an ovvv quantity in-core, but is sufficient to hold at least two copies of an oovv quantity in-core.
cc35	CC3(ROHF)/cc-pVDZ H2O geom from Olsen et al., JCP 104, 8007 (1996)
omp2-4	SCS-OMP2 cc-pVDZ geometry optimization for the H2O molecule.
mp2_5-grad2	MP2.5 cc-pVDZ gradient for the NO radical
cc9a	ROHF-CCSD(T) cc-pVDZ energy for the state of the CN radical, with Z-matrix input.
dfmp2-2	Density fitted MP2 energy of H2, using density fitted reference and automatic looping over cc-pVDZ and cc-pVTZ basis sets. Results are tabulated using the built in table functions by using the default options and by specifiying the format.
omp2-grad1	OMP2 cc-pVDZ gradient for the H2O molecule.
cc1	RHF-CCSD 6-31G** all-electron optimization of the H2O molecule
scf4	RHF cc-pVDZ energy for water, automatically scanning the symmetric stretch and bending coordinates using Python’s built-in loop mechanisms. The geometry is apecified using a Z-matrix with variables that are updated during the potential energy surface scan, and then the same procedure is performed using polar coordinates, converted to Cartesian coordinates.
cisd-h2o-clpse	6-31G** H2O Test CISD Energy Point with subspace collapse
omp2-3	OMP2 cc-pVDZ energy for the NO radical
cepa1	cc-pvdz H2O Test CEPA(1) Energy
cc24	Single point gradient of 1-2B1 state of H2O+ with EOM-CCSD
dftd3-grad	DF-BP86-D2 cc-pVDZ frozen core gradient of S22 HCN, calling Grimme’s dftd3 program for -D2 gradients
cc14	ROHF-CCSD/cc-pVDZ CH2 geometry optimization via analytic gradients
mp3-grad2	MP3 cc-pVDZ gradient for the NO radical
cc29	CCSD/cc-pVDZ optical rotation calculation (both gauges) on Cartesian H2O2
dfscf-bz2	Benzene Dimer DF-HF/cc-pVDZ
psithon1	Spectroscopic constants of H2, and the full ci cc-pVTZ level of theory
ocepa3	OCEPA cc-pVDZ energy with ROHF initial guess for the NO radical
matrix1	An example of using BLAS and LAPACK calls directly from the Psi input file, demonstrating matrix multiplication, eigendecomposition, Cholesky decomposition and LU decomposition. These operations are performed on vectors and matrices provided from the Psi library.
cc36	CC2(RHF)/cc-pVDZ energy of H2O.
castup2	SCF with various combinations of pk/density-fitting, castup/no-castup, and spherical/cartesian settings. Demonstrates that puream setting is getting set by orbital basis for all df/castup parts of calc. Demonstrates that answer doesn’t depend on presence/absence of castup. Demonstrates (by comparison to castup3) that output file doesn’t depend on options (scf_type) being set global or local. This input uses global.
omp3-grad1	OMP3 cc-pVDZ gradient for the H2O molecule.
cc37	CC2(UHF)/cc-pVDZ energy of H2O+.
fnocc1	Test QCISD(T) for H2O/cc-pvdz Energy
omp2-1	OMP2 cc-pVDZ energy for the H2O molecule.
cepa0-grad1	CEPA0 cc-pVDZ gradient for the H2O molecule.
psimrcc-ccsd_t-4	Mk-MRCCSD(T) single point. O$_3` state described using the Ms = 0 component of the singlet. Uses TCSCF orbitals.
gibbs	Test Gibbs free energies at 298 K of N2, H2O, and CH4.
omp3-grad2	OMP3 cc-pVDZ gradient for the NO radical
dft-pbe0-2	Internal match to psi4, test to match to literature values in litref.in/litref.out
zaptn-nh2	ZAPT(n)/6-31G NH2 Energy Point, with n=2-25
cc5	RHF CCSD(T) aug-cc-pvtz frozen-core energy of C4NH4 Anion
mints1	Symmetry tests for a range of molecules. This doesn’t actually compute any energies, but serves as an example of the many ways to specify geometries in Psi4.
props2	DF-SCF cc-pVDZ of benzene-hydronium ion, scanning the dissociation coordinate with Python’s built-in loop mechanism. The geometry is specified by a Z-matrix with dummy atoms, fixed parameters, updated parameters, and separate charge/multiplicity specifiers for each monomer. One-electron properties computed for dimer and one monomer.
mints5	Tests to determine full point group symmetry. Currently, these only matter for the rotational symmetry number in thermodynamic computations.
omp3-1	OMP3 cc-pVDZ energy for the H2O molecule
tu5-sapt	Example SAPT computation for ethene*ethine (i.e., ethylene*acetylene), test case 16 from the S22 database
dcft1	DC-06 calculation for the He dimer. This performs a simultaneous update of the orbitals and cumulant, using DIIS extrapolation. Four-virtual integrals are handled in the MO Basis.