The development of basis sets suitable to use in relativistic calculations reflects the relatively lateness of the field’s development. Because the more consistent efforts in method development started at about the mid 1980’s, it wasn’t until well into the late 1990’s that the pioneering works of the early and mid 1990’s were substantially complemented and improved upon.

This situations has dramatically improved in recent years, notably with the work of K. G. Dyall, and Dirac users are strongly advised to use Dyall’s basis sets whenever they are available. These sets follow roughly the “correlation-consistent” philosophy introduced by Dunning and coworkers [Dunning1989], so they already contain polarization functions, but the SCF sets are designed for an adequate SCF representation rather than to match correlating sets for the valence shells.

As of July 2013, the Dyall sets are available from Li to Uuo for double-zeta and triple-zeta quality, and B - Ca, Ga - Uuo for quadruple-zeta quality (and a detailed description can be found at the dirac website, under the “Basis Set Repository” link`[1] <http://dirac.chem.sdu.dk/basisarchives/dyall/index.html>`_. For convenience, Dirac collects all of Dyall’s available basis sets (those published and areadly in distributable form, as the ones listed in the repository below, as well as those in preparation) in basis set files. One must keep in mind that currently these files support only the use of fully uncontracted basis sets.

The following files are present in Dirac’s distribution:

dyall.v2z contains the double-zeta basis dyall.v3z contains the triple-zeta basis dyall.v4z contains the quadruple-zeta basis dyall.av2z contains the double-zeta basis (as in dyall.v2z) plus diffuse functions (p-block only) dyall.av3z contains the triple-zeta basis (as in dyall.v3z) plus diffuse functions (p-block only) dyall.av4z contains the quadruple-zeta basis (as in dyall.v4z) plus diffuse functions (p-block only)

With the recent addition of Dyall basis sets for the light elements, it is no longer necessary to use the standard non-relativistic basis sets, such as the correlation-consistent sets of Dunning and coworkers. However, because the Dyall basis sets are quite a bit larger, you might want to continue using these basis sets. It is advisable that, in order to have a balanced description when light and heavy elements are present, that one uses either contracted or uncontracted sets thoughout.

Apart from Dyall’s sets, one can choose several different basis sets based upon geometric progressions of exponents. One such set is that of K. Faegri, also available in the basis set library, but with the drawback that the user needs to extended it by adding polarization functions.

The DIRAC distribution shares a large library of standard
non-relativistic and scalar-relativistic basis sets with the
Dalton program.
These basis sets can be found
in the directory **basis_dalton** of the DIRAC distribution.

These basis sets are not all suitable for relativistic calculations,
especially not for the heavier elements.
Basis sets developed for full relativistic calculations (including
spin-orbit coupling) can be found in the directory **basis**.

As Ken Dyall extends the archive actively, the latest of these basis
sets may not be available in the **basis** directory of your DIRAC
distribution.

See the Dyall basis set repository for the latest updates by Ken Dyall and the appropriate basis set references.

We recommend that you use Dyall basis sets (see, for instance http://dirac.chem.sdu.dk/basisarchives/dyall/index.html) whenever they are available for the elements of interest. In order to make that usage as convenient as possible, the following files, containing all sets currently available at the URL above (published or to be published), are made available:

quality | valence | core-valence | all-electron |
---|---|---|---|

double-zeta | dyall.v2z | dyall.cv2z | dyall.ae2z |

triple-zeta | dyall.v3z | dyall.cv3z | dyall.ae3z |

quadruple-zeta | dyall.v4z | dyall.cv4z | dyall.ae4z |

While the division in “valence” and “core-valence” can be at times not so clear-cut as for lighter elements, the option was made to stick to the usual jargon of non-relativistic theory, particularly in relation to the “correlation-consistent” family of basis sets.

The valence basis sets are defined to include functions for correlation of the outer ns shell and the (n-1)s and p shells for the s elements, the outer ns and np shells for the p elements, the ns, np, nd, and (n+1)s for the d elements, and the ns, np, nd, nf, (n+1)s, (n+1)p, (n+1)d, and (n+2)s for the f elements. The choice for the f block of these is necessary to cover correlation of the open f shell, which becomes a semicore shell towards the end of the row.

The core-valence basis sets include the (n-2) shell for the s elements, the (n-1) shell for the p elements, the (n-1) shell for the d elements, and nothing extra for the f elements.

The all-electron basis sets include correlating functions for all shells, down to the 1s for all elements. These are intended for use when correlating all electrons.

Users are encouraged to look in these files and in the original archives published at Theor. Chem. Acc. (as, for instance, for the 5p TZ basis, http://dirac.chem.sdu.dk/basisarchives/dyall/5p_tz_archive) to get a feel for what is included in each case.

In the case of p-block elements, additional files containing the corresponding diffuse functions, in addition to the valence and core-valence basis sets mentioned above, are also provided.

quality | valence | core-valence |
---|---|---|

double-zeta | dyall.av2z | dyall.acv2z |

triple-zeta | dyall.av3z | dyall.acv3z |

quadruple-zeta | dyall.av4z | dyall.acv4z |

In case of errors or omissions on any of the files in this directory, users are kindly asked to contact the authors of DIRAC.