Abstract

For optimized molecules of free-base porphin and magnesium-porphin (at Hartree-Fock level and 6-31G* basis set) excitation spectra were determined using several ab initio methods: CIS, RPA, CASSCF, and TDDFT. Obtained values were compared with semiempirical ZINDO method, other calculations found recently in literature and experimental data. It was demonstrated that for qualitatively correct spectra description the AO basis must include both the polarization and diffuse functions. The later play an important role in formation of Rydberg MOs. Estimated energies of the spectra transitions using the CIS method remain relatively far from the measured values. RPA method can be already considered as a quantitatively accurate method when sufficiently large basis set is used. For CASSCF approach, it was shown that even the lowest energy transitions are insufficiently described in CAS formalism and much larger active space or inclusion of more inactive orbitals in correlation treatment would be necessary for obtaining sufficient accuracy. It can be stated that without sufficiently large correlation contributions, the determined spectra are not able to reach quantitative agreement with experimental data. From the methods treated in this study, only TDDFT can be considered as a useful tool for spectra prediction, at least for calculations of lower excited states. It is relatively fast and feasible for calculation of middle-size molecules. ZINDO approximation is also relatively successful for such large systems. Acceptable predictions of experimentally observed energy transitions in the range of Q and B bands were obtained. Until higher (UV) part of spectra is examined where the excitations to Rydberg orbital will happen, it can be considered as a good candidate for electron spectra calculations.

Highlights

  • Free-based porphin (FBP) and metalo-porphin molecules serve as test systems for practically all methods developed for electron spectra calculations.[1,2,3,4,5,6,7,8,9,10,11,12,13,14]

  • Two years later Similarity transformed equation of motion (STEOM-CC) study on excited states of FBP appeared by Nooijen.[20]

  • These calculations show similar deviation from the experiment (RMS=0.46). These authors point for the first time on the discrepancy between the intensities from calculated and expetimental results. Their results support the original spectra assignment, where the B and N lines from the Soret band belong to two consequent pairs of B2u and B3u lines, in contrary with assignment suggested in SAC-CI studies

Read more

Summary

Transition spectra computations

CIS, RPA, and ZINDO electron spectra were calculated with the Gaussian 98 program package, multiconfiguration tasks were run with the Molpro program. The smallest basis sets without any polarization and diffusion functions exhibit remarkable blue shifts of all the calculated lines. The first two lines (1B3u and 1B2u) are more substantially influenced by polarization functions than by diffuse ones This is easy to understand, since these lines originate from HOMO and HOMO-1 transitions to LUMO and LUMO+1. Their character is correctly described even in smaller bases but polarization functions allow substantially higher flexibility necessary for better description, e.g. passing from 6-31G to 6-31G(d,p) improves 1B3u by 0.07a.u. while 2B3u by only 0.03 and for the basis set extent by diffuse function the corresponding changes are 0.01 and 0.09 a.u., respectively. Even for the most extended basis set the RMS remains above 2.6

RPA Mini
Experime nt
Comparison with recent computations
Conclusions
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.