“…Some of these studies focused on the determination of accurate geometries, frequencies and relative stabilities of three local minima: trans-, cis-, and iso-N 2 H 2 [3,7,[14][15][16][17][18][19]11,10]. Moreover, there has been considerable theoretical work [2,1,9,4,8,6,5,12,13] on the determination of the barriers involved in the diimide isomerization or formation processes, often for testing the accuracy of theoretical methods that are used to study chemical reactions [13,12,4,6]. All published work agrees on the structures of the above minima (trans-, cis-, and iso-) for N 2 H 2 , although the agreement for transition states (TSs) stands only for the TS associated to the trans-iso conversion.…”
Section: Introductionmentioning
confidence: 99%
“…There have been several theoretical [1][2][3][4][5][6][7][8][9][10][11][12][13] and experimental [14][15][16][17][18][19] studies of the title system (a more complete list of earlier theoretical and experimental work is given in Refs. [3,2]).…”
Extensive ab initio calculations have been performed to determine the energy, geometry and vibrational frequencies of all stationary points of the N 2 H 2 ground-state potential energy surface. The geometries of trans-, cis-and iso-minima as well as transition states are reported at the MCSCF/aug-cc-pVQZ level, while the relative energetics is established by single point MRCI/aug-cc-pVQZ calculations including the Davidson size-consistency correction. The data is useful for modeling a single-sheeted global potential energy surface for the title system.
“…Some of these studies focused on the determination of accurate geometries, frequencies and relative stabilities of three local minima: trans-, cis-, and iso-N 2 H 2 [3,7,[14][15][16][17][18][19]11,10]. Moreover, there has been considerable theoretical work [2,1,9,4,8,6,5,12,13] on the determination of the barriers involved in the diimide isomerization or formation processes, often for testing the accuracy of theoretical methods that are used to study chemical reactions [13,12,4,6]. All published work agrees on the structures of the above minima (trans-, cis-, and iso-) for N 2 H 2 , although the agreement for transition states (TSs) stands only for the TS associated to the trans-iso conversion.…”
Section: Introductionmentioning
confidence: 99%
“…There have been several theoretical [1][2][3][4][5][6][7][8][9][10][11][12][13] and experimental [14][15][16][17][18][19] studies of the title system (a more complete list of earlier theoretical and experimental work is given in Refs. [3,2]).…”
Extensive ab initio calculations have been performed to determine the energy, geometry and vibrational frequencies of all stationary points of the N 2 H 2 ground-state potential energy surface. The geometries of trans-, cis-and iso-minima as well as transition states are reported at the MCSCF/aug-cc-pVQZ level, while the relative energetics is established by single point MRCI/aug-cc-pVQZ calculations including the Davidson size-consistency correction. The data is useful for modeling a single-sheeted global potential energy surface for the title system.
“…[27,28]) calculations on the relative stability of the trans-diazene, cis-diazene, and isodiazene isomers have consistently shown a stability ordering trans > cis > iso, as well as high (in excess of 40 kcal/mol) isomerization barriers between the isomers. (Very recently, the rigid cis-trans rotation of the molecule was proposed and studied [29] as a test case for a new multireference coupled cluster method [29], the transition state being a 'real-life' alternative for H 4 as an essentially perfect two-configuration reference problem. )…”
A benchmark ab initio study on the thermochemistry of the trans-HNNH, cis-HNNH, and H 2 NN isomers of diazene has been carried out using the CCSD(T) coupled cluster method, basis sets as large as [7s6p5d4f 3g2h/5s4p3d2f 1g], and extrapolations towards the 1-particle basis set limit. The effects on innershell correlation and of anharmonicity in the zero-point energy were taken into account: accurate geometries and anharmonic force fields were thus obtained as by-products. Our best computed ∆H
“…The direct use of the final energy expressions in CC calculations, as is done in our MMCC theory [7,[118][119][120][121][122][123] and its multi-reference extension discussed here and in Ref. 117, which may result in the introduction of unlinked terms, is also exploited in the Brillouin-Wigner MRCC method [32][33][34][35][36][37]. As in the approximate MMCC case, the Brillouin-Wigner MRCC approach is not size extensive.…”
Section: ⊥(P)mentioning
confidence: 99%
“…In this paper, we focus on the genuine multi-reference CC (MRCC) theories, which are based on the concept of effective Hamiltonian acting in a multi-dimensional reference or model space [4,6,[8][9][10][11][12] and which use the exponential CC ansatz to parametrize the solutions of the generalized Bloch equation [8]. The state-specific (SS) MRCC methods [4,6], including the active-space CC approaches of Adamowicz, Piecuch, Bartlett, and their collaborators [13][14][15][16][17][18][19][20][21][22][23][24][25][26] and their more recent excited-state extensions [27][28][29], the SSMRCC approach of Mahapatra et al [30,31], and the highly promising Brillouin-Wigner MRCC approach [32][33][34][35][36][37], will not be discussed in this work, although the similarity of the wave function ansatz used in the genuine state-universal MRCC theory [4,6,, considered in this paper, and the form of the wave function exploited by the SSMRCC and Brillouin-Wigner MRCC approaches of Refs. 30, 31 and 32-37, respectively, should be noted.…”
Some recent advances in the area of multi-reference coupled-cluster theory of the state-universal type are overviewed. An emphasis is placed on the following new developments: (i) the idea of combining the state-universal multi-reference coupled-cluster singles and doubles method (SUMRCCSD) with the multi-reference many-body perturbation theory (MRMBPT), in which cluster amplitudes of the SUM-RCCSD formalism that carry only core and virtual orbital indices are replaced by their first-order MRMBPT estimates; and (ii) the idea of combining the recently proposed method of moments of coupled-cluster equations with the SUMRCC formalism. It is demonstrated that the new SUMRCCSD(1) method, obtained by approximating the SUMRCCSD cluster amplitudes carrying only core and virtual orbital indices by their first-order MRMBPT values, provides the results that are comparable to those obtained with the complete SUMRCCSD approach.
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