scholarly journals Extended Coupled Cluster Approach for Molecular Properties: Study of H2O and HF Complexes

2001 ◽  
Vol 2 (2) ◽  
pp. 89-102 ◽  
Author(s):  
Nayana Vaval ◽  
Aparna Kumar ◽  
Sourav Pal
1989 ◽  
Vol 157 (4) ◽  
pp. 359-366 ◽  
Author(s):  
John D. Watts ◽  
Gary W. Trucks ◽  
Rodney J. Bartlett

1994 ◽  
Vol 89 (1) ◽  
pp. 33-57 ◽  
Author(s):  
J. Planelles ◽  
J. Paldus ◽  
X. Li

2012 ◽  
Vol 110 (19-20) ◽  
pp. 2349-2357 ◽  
Author(s):  
Hanying Xu ◽  
Svein Saebo ◽  
Charles U. Pittman

2011 ◽  
Vol 134 (11) ◽  
pp. 114102 ◽  
Author(s):  
Francesco A. Evangelista ◽  
Jürgen Gauss

Atoms ◽  
2019 ◽  
Vol 7 (3) ◽  
pp. 62 ◽  
Author(s):  
A. Kudrin ◽  
A. Zaitsevskii ◽  
T. Isaev ◽  
D. Maison ◽  
L. Skripnikov

Molecular properties of the thallium monocyanide (Tl·CN) system in its ground electronic state are studied using high-precision ab initio relativistic two-component pseudopotential replacing 60 inner-core electrons of Tl. A relativistic coupled-cluster method with single, double and perturbative triple amplitudes is employed to account for electronic correlations. Extrapolation of results to the complete basis set limit is used for all studied properties. The global potential energy minimum of Tl·CN corresponds to the linear cyanide (TlCN) isomer, while the non-rigid isocyanide-like (TlNC) structure lies by approximately 11 kJ/mol higher in energy. The procedure of restoration of the wavefunction in the “core” region of Tl atom was applied to calculate the interaction of the Tl nuclear Schiff moment with electrons. The parameter X of the interaction of the Tl nuclear Schiff moment with electrons in the linear TlCN molecule equals 7150 a.u. The prospects of using the TlCN molecule for the experimental detection of the nuclear Schiff moment are discussed.


2005 ◽  
Vol 70 (8) ◽  
pp. 1109-1132 ◽  
Author(s):  
Robert Moszynski ◽  
Piotr S. Żuchowski ◽  
Bogumił Jeziorski

A novel, time-independent formulation of the coupled-cluster theory of the polarization propagator is presented. This formulation, unlike the equation-of-motion coupled-cluster approach, is fully size-extensive and, unlike the conventional time-dependent coupled-cluster method, is manifestly Hermitian, which guarantees that the polarization propagator is always real for purely imaginary frequencies and that the resulting polarizabilities exhibit time-reversal symmetry (are even functions of frequency) for purely real or purely imaginary perturbations. This new formulation is used to derive compact expressions for the three leading terms in the Møller-Plesset expansion for the polarization propagator. The true and apparent correlation contributions to the second-order term are analyzed and separated at the operator level. Explicit equations for the polarization propagator at the non-perturbative, singles and doubles level (CCSD) are presented.


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