! As atom...Test of relativistic energy correction, ! by the Douglas-Kroll transformation to 3rd order. ! ! the FINAL DK3 energy is -2259.0955118153 ! web page says -2259.095511826 ! =1.997, =2.504 Bohr ! ! convergence of the DK transformation is typical, ! 0th order -2234.2372862734 (non-relativistic) ! 1st order -2264.6131852344 ! 2nd order -2258.9450216276 ! 3rd order -2259.0955118173 ! inf. order -2259.0876044131 ! in that 1st order way undershoots, 2nd order comes ! back close, and 3rd order is not insubstantial. ! ! Compare with -2259.456841 which is the point ! nucleus Dirac-Coulomb numerical Hartree-Fock from ! L.Visscher, K.G.Dyall ! At.Data Nucl.Data Tables 67, 207-224(1997), ! noting that the present run does not include any ! relativistic treatment of the 2e- potential. ! ! The Infinite Order Two Component (relwfn=iotc) ! shows the limit of the Douglas-Kroll method, ! and is preferred in practice. ! ! The uncontracted 20s15p9d basis set below is from ! T.Tsuchiya, M.Abe, T.Nakajima, K.Hirao ! J.Chem.Phys. 115, 4463-4472(2001) ! using exponents downloaded from the web page of ! this group at the University of Tokyo. A general ! contraction of this basis can easily be obtained, ! by manipulating the $VEC coefs produced by this run, ! see ~/gamess/tools/dk3.f. ! ! The semicolon divides two lines of input that happen ! to be given on a single physical line of the file. ! $contrl scftyp=rohf mult=4 relwfn=dk ispher=1 $end $system timlim=2 mwords=2 $end $relwfn norder=3 $end $guess guess=huckel $end $radial nshell=2 idegsh(1)=1,3 memsh(1)=15, 16,17,18 $end $data illustration of 3rd order Douglas-Kroll for As Dnh 2 Arsenic 33.0 S 1 ; 1 7.2421890D+07 1.0 S 1 ; 1 7.7040750D+06 1.0 S 1 ; 1 1.3365730D+06 1.0 S 1 ; 1 3.0394350D+05 1.0 S 1 ; 1 8.3289250D+04 1.0 S 1 ; 1 2.5994450D+04 1.0 S 1 ; 1 8.9795770D+03 1.0 S 1 ; 1 3.3667950D+03 1.0 S 1 ; 1 1.3464700D+03 1.0 S 1 ; 1 5.6774580D+02 1.0 S 1 ; 1 2.4923080D+02 1.0 S 1 ; 1 1.1199520D+02 1.0 S 1 ; 1 4.6328140D+01 1.0 S 1 ; 1 2.2611220D+01 1.0 S 1 ; 1 1.0910110D+01 1.0 S 1 ; 1 4.5498340D+00 1.0 S 1 ; 1 2.1494630D+00 1.0 S 1 ; 1 1.0337510D+00 1.0 S 1 ; 1 3.0892460D-01 1.0 S 1 ; 1 1.1206710D-01 1.0 P 1 ; 1 4.9515580D+04 1.0 P 1 ; 1 8.4637830D+03 1.0 P 1 ; 1 2.2908560D+03 1.0 P 1 ; 1 7.7965970D+02 1.0 P 1 ; 1 3.0545690D+02 1.0 P 1 ; 1 1.3097990D+02 1.0 P 1 ; 1 5.9698960D+01 1.0 P 1 ; 1 2.8408790D+01 1.0 P 1 ; 1 1.3883000D+01 1.0 P 1 ; 1 6.6102210D+00 1.0 P 1 ; 1 3.0821260D+00 1.0 P 1 ; 1 1.3919830D+00 1.0 P 1 ; 1 4.8254700D-01 1.0 P 1 ; 1 1.9228260D-01 1.0 P 1 ; 1 7.2849660D-02 1.0 D 1 ; 1 7.1896480D+02 1.0 D 1 ; 1 2.0798400D+02 1.0 D 1 ; 1 7.9590850D+01 1.0 D 1 ; 1 3.4514110D+01 1.0 D 1 ; 1 1.5730540D+01 1.0 D 1 ; 1 7.2805600D+00 1.0 D 1 ; 1 3.3000700D+00 1.0 D 1 ; 1 1.4173160D+00 1.0 D 1 ; 1 5.4472730D-01 1.0 $end