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Frisch, M.J.1
Trucks, G.W.2
Schlegel, H.B.3
Scuseria, G.E.4
Robb, M.A.5
Cheeseman, J.R.6
Scalmani, G.7
Barone, V.8
Mennucci, B.9
Petersson, G.A.10
Nakatsuji, H.11
Caricato, M.12
Li, X.13
Hratchian, H.P.14
Izmaylov, A.F.15
Bloino, J.16
Zheng, G.17
Sonnenberg, J.L.18
Hada, M.19
Ehara, M.20
Toyota, K.21
Fukuda, R.22
Hasegawa, J.23
Ishida, M.24
Nakajima, T.25
Honda, Y.26
Kitao, O.27
Nakai, H.28
Vreven, T.29
Montgomery Jr., J.A.30
Peralta, J.E.31
Ogliaro, F.32
Bearpark, M.33
Heyd, J.J.34
Brothers, E.35
Kudin, K.N.36
Staroverov, V.N.37
Kobayashi, R.38
Norm, J.39
Raghavachari, K.40
Rendell, A.41
Burant, J.C.42
Iyengar, S.S.43
Tomasi, J.44
Cossi, M.45
Rega, N.46
Millam, J.M.47
Klene, M.48
Knox, J.E.49
Cross, J.B.50
Bakken, V.51
Adamo, C.52
Jaramillo, J.53
Gomperts, R.54
Stratmann, R.E.55
Yazyev, O.56
Austin, A.J.57
Cammi, R.58
Pomelli, C.59
Ochterski, J.W.60
Martin, R.L.61
Morokuma, K.62
Zakrzewski, V.G.63
Voth, G.A.64
Salvador, P.65
Dannenberg, J.J.66
Dapprich, S.67
Daniels, A.D.68
Farkas, O.69
Foresman, J.B.70
Ortiz, J.V.71
Cioslowski, J.72
Fox, D.J.73
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Some elements of the A matrix are never explicitly calculated because the terms in the matrix-vector contractions can be properly organized in order to maintain O (N6) scaling, where N is the number of basis functions, and storage of at most four indexes quantities.1
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Some elements of the A matrix are never explicitly calculated because the terms in the matrix-vector contractions can be properly organized in order to maintain O (N6) scaling, where N is the number of basis functions, and storage of at most four indexes quantities.1.
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7
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79251641151
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Here we assume that the target roots of the similarity transformed Hamiltonian are real. Although a generic non- Hermitian matrix may have complex eigenvalues, the above assumption is justified in the context of the EOM-CCSD method because the eigenvalues are excitation energies, which are real quantities. If complex excitation energies are found among the target roots, this is an indication that there is a problem with the description of the wave function (for example the reference function may not be stable), and the rate of convergence of the diagonalization algorithm is, therefore, not relevant
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Here we assume that the target roots of the similarity transformed Hamiltonian are real. Although a generic non- Hermitian matrix may have complex eigenvalues, the above assumption is justified in the context of the EOM-CCSD method because the eigenvalues are excitation energies, which are real quantities. If complex excitation energies are found among the target roots, this is an indication that there is a problem with the description of the wave function (for example the reference function may not be stable), and the rate of convergence of the diagonalization algorithm is, therefore, not relevant.
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