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0542425519
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This prediction is also supported by Low and Goddard's work; see ref 7 a
-
This prediction is also supported by Low and Goddard's work; see ref 7 a.
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47
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Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Gill, P. M. W.; Johnson, B. G.; Robb, M. A.; Cheeseman, J. R.; Keith, T.; Petersson, G. A.; Montgomery, J. A.; Raghavachari, K.; Al-Laham, M. A.; Zakrzewski, V. G.; Ortiz, J. V.; Foresman, J. B.; Cioslowski, J.; Stefanov, B. B.; Nanayakkara, A.; Challacombe, M.; Peng, C. Y.; Ayala, P. Y.; Chen, W.; Wong, M. W.; Andres, J. L.; Replogle, E. S.; Gomperts, R.; Martin, R. L.; Fox, D. J.; Binkley, J. S.; Defrees, D. J.; Baker, J.; Stewart, J. P.; Head-Gordon, M.; Gonzalez, C.; Pople, J. A. Gaussian 94, Revision B.2; Gaussian, Inc.: Pittsburgh, PA, 1995.
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Frisch, M.J.1
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Johnson, B.G.5
Robb, M.A.6
Cheeseman, J.R.7
Keith, T.8
Petersson, G.A.9
Montgomery, J.A.10
Raghavachari, K.11
Al-Laham, M.A.12
Zakrzewski, V.G.13
Ortiz, J.V.14
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Cioslowski, J.16
Stefanov, B.B.17
Nanayakkara, A.18
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Peng, C.Y.20
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Wong, M.W.23
Andres, J.L.24
Replogle, E.S.25
Gomperts, R.26
Martin, R.L.27
Fox, D.J.28
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Defrees, D.J.30
Baker, J.31
Stewart, J.P.32
Head-Gordon, M.33
Gonzalez, C.34
Pople, J.A.35
more..
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48
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0001869943
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Schaefer, H. F., Ed.; Plenum: New York
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Dunning, T.H.1
Hay, P.J.2
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49
-
-
85088619087
-
-
note
-
2 (+0.643). Thus, our computational evidence clearly shows that the electron-donating ability decreases in the same order as we predicted in the article.
-
-
-
-
50
-
-
0542401602
-
-
note
-
2.
-
-
-
-
51
-
-
0542378007
-
-
note
-
As shown in Table 1, in the case of the Pd series, it was found that the MP2 calculations yield the transition state being more stable than the product, implying that those product optimizations were artificial. Reducing optimization convergence criteria by an order of magnitude still did not change the situation. It appears that the potential energy surfaces for the Pd product complexes are fairly flat. A set of polarization functions on Pd and the ligands and the inclusion of correlation should be essential. This study is, however, beyond the scope of the present work. Nevertheless, our study shows that the single-point MP4 calculations based on the MP2 geometries can provide reliably qualitative conclusions.
-
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52
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33947093400
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Abis, L.1
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Halpern, J.3
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55
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0001177229
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Ozawa, F.; Ito, T.; Nakamura, Y.; Yamamoto, A. Bull. Chem. Soc. Jpn. 1981, 54, 1868.
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Ozawa, F.1
Ito, T.2
Nakamura, Y.3
Yamamoto, A.4
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58
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-
0001702480
-
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(g) Michelin, R. A.; Faglia, S.; Uguagliati, P. Inorg. Chem. 1983, 22, 1831.
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Michelin, R.A.1
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59
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21644442950
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(a) Kitaura, K.; Obara, S.; Morokuma, K. J. Am. Chem. Soc. 1981, 103, 2891.
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Kitaura, K.1
Obara, S.2
Morokuma, K.3
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60
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24544473521
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(b) Balazs, A. C.; Johnson, K. H.; Whitesides, G. M. Inorg. Chem. 1982, 21, 2162.
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Balazs, A.C.1
Johnson, K.H.2
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62
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0001575416
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Obara, S.; Kitaura, K.; Morokuma, K. J. Am. Chem. Soc. 1984, 106, 7482.
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Obara, S.1
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63
-
-
0542378005
-
-
At the MP2/LANL2DZ level, the linear relationship is y = 0.766x -21.0
-
At the MP2/LANL2DZ level, the linear relationship is y = 0.766x -21.0.
-
-
-
-
64
-
-
0542378006
-
-
At the MP2/LANL2DZ level, the linear relationship is y' = 1.03x -44.8
-
At the MP2/LANL2DZ level, the linear relationship is y' = 1.03x -44.8.
-
-
-
-
65
-
-
0003392735
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National Bureau of Standards: Washington, DC. These state splittings were averaged over j states to cancel out spin-orbit coupling
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Moore, C. E. Atomic Energy Levels; National Bureau of Standards: Washington, DC, 1971; Vol. III. (These state splittings were averaged over j states to cancel out spin-orbit coupling.)
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(1971)
Atomic Energy Levels
, vol.3
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Moore, C.E.1
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66
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0542425529
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note
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2) involved in Figure 2, in the CpCoL case there could be three predominant configurations contributing to the total wave function ψ, i.e., a closed-shell singlet, two open-shell triplets (so overall singlet), and un open-shell singlet. This study, however, is beyond the scope of the present work and will not be discussed here.
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