메뉴 건너뛰기




Volumn 110, Issue 1, 2006, Pages 291-298

Efficient strategies for accurate calculations of electronic excitation and ionization energies: Theory and application to the dehydro-m-xylylene anion

Author keywords

[No Author keywords available]

Indexed keywords

DEGENERATE ORBITALS; ELECTRONIC STATES; ENERGY DIFFERENCES;

EID: 31344472770     PISSN: 10895639     EISSN: None     Source Type: Journal    
DOI: 10.1021/jp0542827     Document Type: Article
Times cited : (14)

References (56)
  • 10
    • 31344434733 scopus 로고    scopus 로고
    • note
    • Indeed, tiny errors in total energies may result in very large errors in energy differences. For example, one percent of the ethylene total energy is about 21 eV, which exceeds even the ionization potential of the molecule! 0.01% of the total energy of ethylene is 0.21 eV, which is a typical error bar for excitation energies calculated by EOM-CCSD, one of the approaches formulated for energy differences.
  • 27
    • 31344478197 scopus 로고    scopus 로고
    • note
    • - with those of neutral DMX. For example, the vertical energy gap between the quartet and the closed-shell doublet in DMX is 13.6 kcal/mol which is comparable with 10 kcal/mol singlet-triplet energy separation in MX. Likewise, the energy separation between the open-shell doublet and the quartet is 3.8 kcal/mol, similar to the 3 kcal/mol singlet-triplet separation in DHT.
  • 34
    • 31344446358 scopus 로고    scopus 로고
    • Levchenko, S. V.; Slipchenko, L. V.; Krylov, A. I. Unpublished work
    • Levchenko, S. V.; Slipchenko, L. V.; Krylov, A. I. Unpublished work.
  • 36
    • 31344453147 scopus 로고    scopus 로고
    • note
    • Contrarily to the EOM approach, in which the total number of simultaneously calculated states does not affect the resulting excitation energies, in a state-averaged calculation by MCSCF, the energies of states depend on the number of the states included in the averaging procedure. Whereas this uncertainty in excitation energies may not be important when vertical excitation energies are calculated, it can become an issue when the adiabatic excitation energies are of interest. For example, at some points of PES, it may be possible to calculate one root in a time, whereas at other points, degeneracy between the states may require root-averaging.
  • 43
    • 31344463893 scopus 로고    scopus 로고
    • note
    • 2 reference state.
  • 49
    • 31344450331 scopus 로고    scopus 로고
    • note
    • 1 singlets. Calculated at these geometries, changes in the excitation energies of these states are less than 0.1 kcal/ mol.
  • 53
    • 0004040381 scopus 로고
    • ACES II. Stanton, J. F.; Gauss, J.; Watts, J. D.; Lauderdale, W. J.; Bartlett, R. J. 1993. The package also contains modified versions of the MOLECULE Gaussian integral program of J. Almlöf and P. R. Taylor, the ABACUS integral derivative program written by T. U. Helgaker, H. J. Aa. Jensen, P. Jørgensen and P. R. Taylor, and the PROPS property evaluation integral code of P. R. Taylor.
    • (1993) ACES II.
    • Stanton, J.F.1    Gauss, J.2    Watts, J.D.3    Lauderdale, W.J.4    Bartlett, R.J.5
  • 55
    • 31344445832 scopus 로고    scopus 로고
    • note
    • The excitation energies presented in Table 1 differ from those reported in ref 26. The previously reported excitation energies were calculated at the EOM-CCSD//B3LYP level of theory, whereas the excitation energies in Table 1 are obtained at the EOM-CCSD/CCSD(T) and EOM-CC(2,3)//CCSD(T) levels of theory.
  • 56
    • 31344481428 scopus 로고    scopus 로고
    • note
    • 1 state behaves similarly.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.