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  • Default: 0

  • +

    SCF (Expert) — Screening criteria for basis function values on snLinK grids

    + +
    +

    SCF (Expert) — Screening criteria for shell-pair densities in snLinK

    + +
    +

    SCF (Expert) — Force snLinK to use cartesian coordinates

    + +
    +

    SCF (Expert) — Proportion (in %) of available GPU memory to allocate to snLinK.

    + +
    +

    SCF (Expert) — Maximum number of grid points per grid block for GauXC

    + +
    +

    SCF (Expert) — Integrator execution kernel for snLinK GauXC also has SHELLBATCHED, but it is incompatible with Psi4 due to not being yet implemented with sn-LinK.

    + +
    +

    SCF — Screening criteria for integrals and intermediates in snLinK

    + +
    +

    SCF (Expert) — Load Balancer kernel for snLinK

    + +
    +

    SCF (Expert) — Integrator local work driver kernel for snLinK GauXC also has SCHEME1-CUTLASS, but it is disabled in Psi4 for now due to compile-time issues and requiring very modern CUDA CCs (>=80)

    + +
    +

    SCF (Expert) — Molecular Weights kernel for snLinK

    + +
    +

    SCF (Expert) — Pruning scheme for snLinK grids

    + +
    +

    SCF — Number of radial points in snLinK grid.

    + +
    +

    SCF — Radial Scheme for snLinK grid. MURA is default here as it matches the GauXC default option

    + +
    +

    SCF (Expert) — Integrator reduction kernel for snLinK GauXC also has NCCL, but it is incompatible with Psi4 due to requiring MPI.

    + +
    +

    SCF — Number of spherical points in snLinK grid.

    + +
    +

    SCF (Expert) — Overwrite sn-LinK grid options with debug grid matching GauXC’s Ultrafine grid spec

    + +
    +

    SCF — Use GPU for GauXC?

    + +
    SOCC (GLOBALS)

    GLOBALS — An array containing the number of singly-occupied orbitals per irrep (in Cotton order). The value of DOCC should also be set.

  • ConvergenceError +
  • +
  • coord() (psi4.core.GaussianShell method)
  • copy() (psi4.core.CIVector method) @@ -4658,6 +4660,8 @@

    G

  • get_schwarz_cutoff() (psi4.core.DFHelper method)
  • get_scratch_filename() (psi4.core.Wavefunction method) +
  • +
  • get_snLinK_max_am() (psi4.core.CompositeJK method)
  • get_space_size() (psi4.core.DFHelper method)
  • @@ -8458,8 +8462,6 @@

    S

  • set_color() (psi4.driver.p4util.InPsight method)
  • - - +
    +
    SNLINK

    An algorithm based on the “seminumerical Linear Exchange” (sn-LinK) +approach described in [Laqua:2020:1456], SNLINK is only available if PSI4 +is compiled with the GauXC library, described in [Williams-Young:2023:234104]. +Algorithmically, SNLINK is very similar to COSX, differing primarily in screening of +the analytic 3-center integrals. In terms of implementation, SNLINK is more efficient, +owing to more highly-optimized integral contraction kernels; and supports execution +on Graphics Processing Units (GPUs). See Seminumerical Linear Exchange for more information.

    +

    In some cases the above algorithms have multiple implementations that return the same result, but are optimal under different molecules sizes and hardware @@ -819,10 +826,10 @@

    Navigation

    \[(PQ|RS) <= \sqrt{(PQ|PQ)(RS|RS)}\]
    -
    CSAM

    An extension of the Schwarz estimate that also screens over the long range 1/r operator, described in [Thompson:2017:144101].

    +
    CSAM

    An extension of the Schwarz estimate that also screens over the long range 1/r operator, described in [Thompson:2017:144101].

    DENSITY

    An extension of the Schwarz estimate that also screens over elements of the density matrix. -For the RHF case, described in [Haser:1989:104]

    +For the RHF case, described in [Haser:1989:104]

    @@ -830,7 +837,7 @@

    Navigation

    \[DCON(PQ, RS) = max(4D_{PQ}, 4D_{RS}, D_{PR}, D_{PS}, D_{QR}, D_{QS})\]

    When using density-matrix based integral screening, it is useful to build the J and K matrices -incrementally, also described in [Haser:1989:104], using the difference in the density matrix between iterations, rather than the +incrementally, also described in [Haser:1989:104], using the difference in the density matrix between iterations, rather than the full density matrix. To turn on this option, set INCFOCK to true.

    We have added the automatic capability to use the extremely fast DF code for intermediate convergence of the orbitals, for SCF_TYPE @@ -849,7 +856,7 @@

    Navigation

    SCF calculations. The reduction in ERI tensor rank also makes DF an appealing option for conventional SCF calculations, where the ERIs are stored in core or on disk. However, even when using DF, I/O becomes a significant bottleneck for systems of a sufficient size when performing conventional SCF calculations. In principle, though, DF approaches can be utilized in an integral-direct context, gaining the benefits of DF methods without suffering the -I/O bottlenecks that conventional DF methods will eventually run into. One such approach, outlined by Weigend in [Weigend:2002:4285], +I/O bottlenecks that conventional DF methods will eventually run into. One such approach, outlined by Weigend in [Weigend:2002:4285], is available for use in Psi4 for the separate construction of the Coulomb contribution to the Fock matrix. This implementation can be used alongside Psi4’s separate Exchange construction algorithms for composite Fock matrix construction by using the keyword DFDIRJ as the Coulomb construction algorithm when specifying SCF_TYPE to use a composite algorithm combination (DFDIRJ+K_alg in general, @@ -860,7 +867,7 @@

    Navigation

    COSX Exchange

    -

    The semi-numerical COSX algorithm described in [Neese:2009:98] evaluates +

    The semi-numerical COSX algorithm described in [Neese:2009:98] evaluates two-electron ERIs analytically over one electron coordinate and numerically over the other electron coordinate, and belongs to the family of pseudospectral methods originally suggested by Friesner. In COSX, numerical integration is performed on standard @@ -897,13 +904,13 @@

    Navigation

    are more amenable to screening. This option is disabled by default because of potential SCF convergence issues, particularly when using diffuse basis functions. The COSX_OVERLAP_FITTING keyword (defaults to true) reduces numerical -integration errors using the method described in [Izsak:2011:144105] and is +integration errors using the method described in [Izsak:2011:144105] and is always recommended.

    Linear Exchange

    Large SCF calculations can benefit from specialized screening procedures that further reduce the scaling of the ERI contribution to the Fock matrix. -LinK, the linear-scaling exchange method described in [Ochsenfeld:1998:1663], is available in Psi4 in conjunction with composite algorithms that build J (SCF_TYPE set to J_alg+LINK). +LinK, the linear-scaling exchange method described in [Ochsenfeld:1998:1663], is available in Psi4 in conjunction with composite algorithms that build J (SCF_TYPE set to J_alg+LINK). LinK achieves linear-scaling by exploiting shell pair sparsity in the density matrix and overlap sparsity between shell pairs. Specifically, LinK exploits the fact that the Exchange term requires only a linear-scaling number of significant elements through reformulating the shell quartet screening process to scale linearly with system size. @@ -914,6 +921,46 @@

    Navigation

    LINK_INTS_TOLERANCE: The integral screening tolerance used for sparsity-prep in the LinK algorithm. Defaults to the INTS_TOLERANCE option.

    +
    +

    Seminumerical Linear Exchange

    +

    Similar to the COSX algorithm provided by PSI4, the seminumerical Linear Exchange (sn-LinK) algorithm, devised +by Ochsenfeld in [Laqua:2020:1456], improves efficiency of the K construction process by +decomposing computation of the ERI tensor into a series of contractions involving grid-computed basis +function components and analytic 3-center integrals. As a “semi-numerical” Exchange construction method, +sn-LinK is also comparable to the pseudospectral method of Friesner.

    +

    sn-LinK and COSX have a number of significant differences in implementation details in PSI4, however. +First and foremost, the COSX implementation is contained within PSI4 itself, and is thus always available +for execution. On the other hand, the sn-LinK implementation in PSI4 is tied to the GauXC standalone +library discussed in [Williams-Young:2023:234104]; thus, the PSI4-GauXC interface must be built +for sn-LinK to be used. Second, the GauXC sn-LinK interface is more +efficient than the PSI4 COSX code on multiple levels. For CPU execution, GauXC’s sn-LinK uses highly-optimized +kernels for the contraction of the analytic integrals, whereas PSI4’s COSX uses a less-optimized, more +general contraction kernel. Additionally, GauXC’s sn-LinK code supports execution on GPUs, allowing for +GPU-enabled construction of the Exchange matrix, while PSI4’s COSX does not. In general, +sn-LinK will provide better runtime performance for hitting a desired accuracy +threshold compared to PSI4’s COSX. Third, some low-level implementation details differ between the two. +For example, PSI4’s COSX uses a dual-grid scheme similar to that originally proposed by Neese, +converging the SCF on a small grid, then running a number of SCF iterations, +equal to the value set by the COSX_MAXITER_FINAL, on a larger grid. +In contrast, sn-LinK only uses a single-grid scheme, simply converging the SCF on one grid. +As another example, while the COSX grid defaults are selected to emphasize speed over accuracy, +the defaults for sn-LinK are selected to achieve higher accuracy (~0.1 kcal/mol error for interaction/conformer energies).

    +

    To control compilation and linking of the optional GauXC dependency required for the sn-LinK algorithm, +here are the list of compile-time options provided.

    +
      +
    • ENABLE_gauxc: Compile Psi4 with support for GauXC.

    • +
    • gauxc_DIR: Location of the external GauXC install to compile Psi4 with, if using an external GauXC instance.

    • +
    • gauxc_ENABLE_GPU: Enable GPU support for the Psi4-GauXC interface class. When building GauXC internally within Psi4, this keyword controls whether to enable GPU support on the internally-built GauXC instance. When using an external GauXC build, this keyword must align with the GPU capabilities of the external GauXC install.

    • +
    +

    To control the sn-LinK algorithm, here are the list of options provided.

    +
    +

    SNLINK_RADIAL_POINTS: Number of radial points to use for the sn-LinK grid. Defaults to 70.

    +

    SNLINK_SPHERICAL_POINTS: Number of spherical points to use for the sn-LinK grid. Defaults to 302.

    +

    SNLINK_RADIAL_SCHEME: Radial quadrature scheme to use for the sn-LinK grid. Defaults to MURA. Note that, although different from the more common Psi4 radial quadrature scheme of TREUTLER, the default of MURA matches the default radial quadrature scheme used by GauXC.

    +

    SNLINK_INTS_TOLERANCE: The integral screening tolerance used in the sn-LinK algorithm. Defaults to the INTS_TOLERANCE option.

    +

    SNLINK_USE_GPU: Select whether to execute the sn-LinK algorithm on GPU or not. Setting this option to true will fail unless the Psi4-GauXC interface is compiled with GPU support.

    +
    +

    Second-order Convergence

    Second-order convergence takes into account both the gradient and Hessian to @@ -996,8 +1043,8 @@

    Navigation

    products are computed instead of the full Hessian. This algorithm is thus much more efficient than the Direct Inversion, but at present, it is only available for UHF \(\rightarrow\) UHF stability analysis. The capabilities of both algorithms are summarized below:

    - - +
    Stability analysis methods available in PSI4
    + @@ -1139,8 +1186,8 @@

    Navigation

    Convergence and Algorithm Defaults

    -
    Stability analysis methods available in PSI4

    Algorithm

    REFERENCE

    - +
    SCF algorithm and convergence criteria defaults by calculation type [1]
    + @@ -1160,7 +1207,7 @@

    Navigation

    - + @@ -1168,29 +1215,29 @@

    Navigation

    - + - + - +
    SCF algorithm and convergence criteria defaults by calculation type [1]

    Ab Initio Method

    Calculation Type

    8

    8

    frequency [7]

    frequency [7]

    8

    8

    energy

    8

    8

    PK [3]

    PK [3]

    optimization

    10

    10

    frequency [7]

    frequency [7]

    10

    10

    CC property [2]

    CC property [2]

    10

    10

    - - +
    Post-SCF convergence criteria defaults by calculation type [4]
    + - - + + @@ -1203,11 +1250,11 @@

    Navigation

    - + - + @@ -1216,7 +1263,7 @@

    Navigation

    Footnotes

    Post-SCF convergence criteria defaults by calculation type [4]

    Ab Initio Method

    Calculation Type

    E_CONVERGENCE [5]

    R_CONVERGENCE [6]

    E_CONVERGENCE [5]

    R_CONVERGENCE [6]

    8

    frequency [7]

    frequency [7]

    8

    CC property [2]

    CC property [2]

    8