.\" Man page generated from reStructuredText. . .TH "CIS" "1" "Jun 15, 2019" "2.0" "Quantum Package" .SH NAME cis \- | Quantum Package > . .nr rst2man-indent-level 0 . .de1 rstReportMargin \\$1 \\n[an-margin] level \\n[rst2man-indent-level] level margin: \\n[rst2man-indent\\n[rst2man-indent-level]] - \\n[rst2man-indent0] \\n[rst2man-indent1] \\n[rst2man-indent2] .. .de1 INDENT .\" .rstReportMargin pre: . RS \\$1 . nr rst2man-indent\\n[rst2man-indent-level] \\n[an-margin] . nr rst2man-indent-level +1 .\" .rstReportMargin post: .. .de UNINDENT . RE .\" indent \\n[an-margin] .\" old: \\n[rst2man-indent\\n[rst2man-indent-level]] .nr rst2man-indent-level -1 .\" new: \\n[rst2man-indent\\n[rst2man-indent-level]] .in \\n[rst2man-indent\\n[rst2man-indent-level]]u .. .INDENT 0.0 .INDENT 3.5 Configuration Interaction with Single excitations. .sp This program takes a reference Slater determinant of ROHF\-like occupancy, and performs all single excitations on top of it. Disregarding spatial symmetry, it computes the \fIn_states\fP lowest eigenstates of that CI matrix. (see \fBdeterminants n_states\fP) .sp This program can be useful in many cases: .INDENT 0.0 .IP 1. 3 Ground state calculation .sp To be sure to have the lowest SCF solution, perform an scf (see the module_hartree_fock module), then a \fI\%cis\fP, save the natural orbitals (see save_natorb) and re\-run an scf optimization from this MO guess. .IP 2. 3 Excited states calculations .sp The lowest excited states are much likely to be dominated by single\-excitations. Therefore, running a \fI\%cis\fP will save the \fIn_states\fP lowest states within the CIS space in the \fI\%EZFIO\fP directory, which can afterwards be used as guess wave functions for a further multi\-state FCI calculation if \fBdeterminants read_wf\fP is set to \fBtrue\fP before running the fci executable. .UNINDENT .sp If \fBdeterminants s2_eig\fP is set to \fBtrue\fP, the CIS will only retain states having the expected \ewidehat{S^2} value (see \fBdeterminants expected_s2\fP). Otherwise, the CIS will take the lowest \fBdeterminants n_states\fP, whatever multiplicity they are. .sp \fBNOTE:\fP .INDENT 0.0 .INDENT 3.5 To discard some orbitals, use the qp_set_mo_class command to specify: .INDENT 0.0 .IP \(bu 2 \fIcore\fP orbitals which will be always doubly occupied .IP \(bu 2 \fIact\fP orbitals where an electron can be either excited from or to .IP \(bu 2 \fIdel\fP orbitals which will be never occupied .UNINDENT .UNINDENT .UNINDENT .sp Needs: .INDENT 0.0 .INDENT 2.0 .IP \(bu 2 \fBread_wf\fP .UNINDENT .INDENT 2.0 .UNINDENT .INDENT 2.0 .UNINDENT .UNINDENT .sp Calls: .INDENT 0.0 .INDENT 2.0 .IP \(bu 2 \fBrun()\fP .UNINDENT .INDENT 2.0 .UNINDENT .INDENT 2.0 .UNINDENT .UNINDENT .sp Touches: .INDENT 0.0 .INDENT 2.0 .IP \(bu 2 \fBfock_matrix_ao_alpha\fP .IP \(bu 2 \fBfock_matrix_ao_alpha\fP .UNINDENT .INDENT 2.0 .IP \(bu 2 \fBmo_coef\fP .IP \(bu 2 \fBlevel_shift\fP .UNINDENT .INDENT 2.0 .IP \(bu 2 \fBmo_coef\fP .IP \(bu 2 \fBread_wf\fP .UNINDENT .UNINDENT .UNINDENT .UNINDENT .SH AUTHOR A. Scemama, E. Giner .SH COPYRIGHT 2019, A. Scemama, E. Giner .\" Generated by docutils manpage writer. .