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31344434733
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note
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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.
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4143105620
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4043154044
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27
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31344478197
-
-
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.
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0030934890
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31344446358
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Levchenko, S. V.; Slipchenko, L. V.; Krylov, A. I. Unpublished work
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0030921177
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36
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31344453147
-
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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.
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31344463893
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note
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2 reference state.
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47
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26844534384
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-
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31344450331
-
-
note
-
1 singlets. Calculated at these geometries, changes in the excitation energies of these states are less than 0.1 kcal/ mol.
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50
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0000456290
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Kong, J.; White, C. A.; Krylov, A. I.; Sherrill, C. D.; Adamson, R. D.; Furlani, T. R.; Lee, M. S.; Lee, A. M.; Gwaltney, S. R.; Adams, T. R.; Ochsenfeld, C.; Gilbert, A. T. B.; Kedziora, G. S.; Rassolov, V. A.; Maurice, D. R.; Nair, N.; Shao, Y.; Besley, N. A.; Maslen, P.; Dombroski, J. P.; Daschel, H.; Zhang, W.; Korambath, P. P.; Baker, J.; Bird, E. F. C.; Van Voorhis, T.; Oumi, M.; S. Hirata, C.-P. Hsu; Ishikawa, N.; Florian, J.; Warshel, A.; Johnson, B. G.; Gill, P. M. W.; Head-Gordon, M.; Pople, J. A. J. Comput. Chem. 2000, 21, 1532.
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Furlani, T.R.6
Lee, M.S.7
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Gwaltney, S.R.9
Adams, T.R.10
Ochsenfeld, C.11
Gilbert, A.T.B.12
Kedziora, G.S.13
Rassolov, V.A.14
Maurice, D.R.15
Nair, N.16
Shao, Y.17
Besley, N.A.18
Maslen, P.19
Dombroski, J.P.20
Daschel, H.21
Zhang, W.22
Korambath, P.P.23
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Van Voorhis, T.26
Oumi, M.27
Hirata, S.28
Hsu, C.-P.29
Ishikawa, N.30
Florian, J.31
Warshel, A.32
Johnson, B.G.33
Gill, P.M.W.34
Head-Gordon, M.35
Pople, J.A.36
more..
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53
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0004040381
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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.
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ACES II.
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Stanton, J.F.1
Gauss, J.2
Watts, J.D.3
Lauderdale, W.J.4
Bartlett, R.J.5
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54
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84893169025
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Schmidt, M. W.; Baldridge, K. K.; Boatz, J. A.; Elbert, S. T.; Gordon, M. S.; Jensen, J. H.; Koseki, S.; Mastunaga, N.; Nguyen, K. A.; Su, S.; Windus, T. L.; Dupuis, M.; Montgomery, J. A. J. Comput. Chem. 1993, 14, 1347.
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Schmidt, M.W.1
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Boatz, J.A.3
Elbert, S.T.4
Gordon, M.S.5
Jensen, J.H.6
Koseki, S.7
Mastunaga, N.8
Nguyen, K.A.9
Su, S.10
Windus, T.L.11
Dupuis, M.12
Montgomery, J.A.13
-
55
-
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31344445832
-
-
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
-
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31344481428
-
-
note
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1 state behaves similarly.
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-
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