# ================================================================ # Orca input file made in Gabedit # ================================================================ ! ZINDO/S ! PrintBasis %pointcharges "bafwub.txt" %cis nroots 28 # the number of excited states to be calculated. maxdim 56 # the maximum dimension of the expansion space in the Davidson procedure. # dcorr n # n=1-4. The meaning of the four algorithms # algorithm 1 Is perhaps the best for small systems. May use a # lot of disk space # algorithm 2 Stores less integrals # algorithm 3 Is good if the system is large and only a few # states are to be made. Safes disk and main memory. # algorithm 4 Uses only transformed RI integrals. May be the # fastest for large systems and a larger number of states # Triplets true : do triplets states # EWin -3,100 (orbital energy window in Eh) # Etol 1e-3 the required convergence of the energies of the excited states (in Eh) # Rtol 1e-5 required convergence on the norm of the residual vectors. # essential for metal edges. For ligand edges, the contributions are much smaller. end #cis %output print[p_mos] 1 end #output * xyz -3 1 O 2.256600 -0.355600 -0.119500 O -1.758400 1.570300 -0.072000 O 0.839300 -2.009600 -1.207500 O -1.831300 -1.213800 1.361400 O -2.023100 -0.414000 -1.445300 O 0.465400 -1.732000 1.751500 O 0.068200 1.222300 2.039100 O 1.011800 1.992600 -0.186200 O 0.457200 0.623500 -2.254600 C 1.258500 -3.342400 3.375100 C 0.120600 -2.580500 2.644400 C -1.224500 -2.802100 2.978100 C -2.173400 -2.053400 2.262400 C -3.689600 -2.198000 2.561100 C 1.676300 -3.899300 -2.457500 C 1.889400 -2.641000 -1.572900 C 3.183200 -2.205100 -1.243600 C 3.280400 -1.025100 -0.493400 C 4.666000 -0.436600 -0.111400 C -3.339500 3.395300 -0.025200 C -2.881500 1.995200 -0.515100 C -3.661100 1.272100 -1.425700 C -3.146300 0.036200 -1.854800 C -3.910700 -0.823100 -2.898500 C -0.114100 0.887700 3.450000 C 0.282800 2.679300 2.002400 C 1.268500 2.961100 0.881700 C 1.789800 2.432500 -1.349700 C 1.081400 1.903800 -2.586300 C 0.163700 -0.051300 -3.528900 F 0.831800 -4.366200 4.180200 F 1.997400 -2.532800 4.201500 F 2.168500 -3.915700 2.527400 F -4.469800 -2.252200 1.437300 F -4.021100 -3.318500 3.277200 F -4.190200 -1.151600 3.295000 F 1.199700 -3.583500 -3.706600 F 0.774600 -4.791000 -1.942500 F 2.809200 -4.633600 -2.690700 F 4.862500 -0.317400 1.238900 F 5.743200 -1.147700 -0.567700 F 4.853600 0.833500 -0.604600 F -2.971100 3.675100 1.266500 F -2.804100 4.422300 -0.763900 F -4.691900 3.602600 -0.059500 F -5.155900 -0.352800 -3.223400 F -3.244700 -0.905500 -4.097400 F -4.109500 -2.119600 -2.508600 H -1.520100 -3.536100 3.735500 H 4.072200 -2.769600 -1.546700 H -4.632800 1.640500 -1.772700 H -0.400100 -0.190000 3.517400 H 0.854400 1.061100 3.977200 H -0.932700 1.524300 3.863800 H 0.703500 3.043100 2.972200 H -0.726200 3.128100 1.800000 H 2.329900 2.813200 1.207800 H 1.104600 3.997900 0.492000 H 1.838100 3.548700 -1.392100 H 2.812300 1.985500 -1.224900 H 0.259100 2.587500 -2.918900 H 1.837400 1.756900 -3.399800 H 0.681800 -1.041500 -3.480900 H 0.523700 0.538500 -4.401300 H -0.947400 -0.172300 -3.574600 *