Abstract:=An approach for a space-separated calculation of the wave function in the valence and core regions of a molecule is proposed. As the first step, the calculation of the orbitals (or two-component spinors in the relativistic case) in the valence region by the effective core potential (ECP) method is performed. Then, it is followed by a restoration of orbitals (four-component spinors) expanded on spherical harmonics in the core regions of heavy atoms. Theoretical questions of the variational calculation of the m… Show more
“…Recently, the E eff value for the 3 ∆ 1 state was estimated in the scalar-relativistic approximation by Meyer et al [16] and the method used for calculation of E eff is close in essence to that developed by us earlier [17] and applied to first two-step calculations of the PbF molecule [14,17]. In the present work, a more reliable value of E eff is calculated using the advanced two-step techniques developed by us later [18,19,20,21] is not the ground state, its radiative lifetime is also required. In the present work these data are obtained, though precise studying of the compounds with transition elements is a difficult problem for modern molecular theory.…”
mentioning
confidence: 59%
“…Before calculating core properties the shapes of the fourcomponent molecular spinors are restored in the inner core region after the two-component GRECP calculation of the molecule. For this purpose the nonvariational onecenter restoration (NOCR) method [17,18,20,21,27,33] is applied.…”
We report first ab initio relativistic correlation calculations of potential curves for ten low-lying electronic states, effective electric field on the electron and hyperfine constants for the 3 ∆1 state of cation of a heavy transition metal fluoride, HfF + , that is suggested to be used as the working state in experiments to search for the electric dipole moment of the electron. It is shown that HfF + has deeply bound 1 Σ + ground state, its dissociation energy is De = 6.4 eV. The 3 ∆1 state is obtained to be the relatively long-lived first excited state lying about 0.2 eV higher. The calculated effective electric field E eff = W d |Ω| acting on an electron in this state is 5.84 × 10 24 Hz/(e·cm).
“…Recently, the E eff value for the 3 ∆ 1 state was estimated in the scalar-relativistic approximation by Meyer et al [16] and the method used for calculation of E eff is close in essence to that developed by us earlier [17] and applied to first two-step calculations of the PbF molecule [14,17]. In the present work, a more reliable value of E eff is calculated using the advanced two-step techniques developed by us later [18,19,20,21] is not the ground state, its radiative lifetime is also required. In the present work these data are obtained, though precise studying of the compounds with transition elements is a difficult problem for modern molecular theory.…”
mentioning
confidence: 59%
“…Before calculating core properties the shapes of the fourcomponent molecular spinors are restored in the inner core region after the two-component GRECP calculation of the molecule. For this purpose the nonvariational onecenter restoration (NOCR) method [17,18,20,21,27,33] is applied.…”
We report first ab initio relativistic correlation calculations of potential curves for ten low-lying electronic states, effective electric field on the electron and hyperfine constants for the 3 ∆1 state of cation of a heavy transition metal fluoride, HfF + , that is suggested to be used as the working state in experiments to search for the electric dipole moment of the electron. It is shown that HfF + has deeply bound 1 Σ + ground state, its dissociation energy is De = 6.4 eV. The 3 ∆1 state is obtained to be the relatively long-lived first excited state lying about 0.2 eV higher. The calculated effective electric field E eff = W d |Ω| acting on an electron in this state is 5.84 × 10 24 Hz/(e·cm).
“…However, experimental support of the second Cd-C bond fission via reaction (2) was not evident with our detectors because the electronic Raman spectrum of the Cd atom is not detectable, i.e. since atomic Cd has a closed outer shell, and its lifetime for the transition between the ground state and the first excited state is too short to be detected in our system.…”
Section: Resultsmentioning
confidence: 83%
“…[13] Although the homolytic fission reactions (1) and (2) are likely the dominant reactions in the gas phase, the suggested pathways for the decomposition of other group II alkyls often include additional reactions contributing to the deposition process. [14] Computational chemistry is a good companion to assist in designing and interpreting experiments and to explore various reaction pathways.…”
Computational chemistry has been widely used to understand homogeneous reactions and to support spectroscopy analysis. Thus, it is a useful tool to understand gas-phase dynamics of metal organic chemical vapor deposition (MOCVD). In this study, we report that the basis set selection possibly results in unequivocal peak assignment in Raman spectroscopy, especially when an effective core potential (ECP) is employed. The basis set selection for the decompositionof dimethylcadmium (DMCd), for example, was examined using five different ECPs (i.e. CRENBS, CRENBL, SDD, LanL2DZ and SBKJC for Cd atom combined with STO-3G, 3-21G, 6-31G(d), 6-311G(d) and 6-311++G(2d,
2p) for C and H atoms). The analyses demonstrated that the SDD/STO-3G/3-21G combination for Cd/C/H atoms best reproduce the experimentally reported Cd-C vibrational stretching modes of Cd(CH 3 ) 2 (DMCd) and •CdCH 3 (MMCd). Although the SDD/STO-3G/3-21G combination consists of simple and basic basis sets,we found that a good potential balance between metal (Cd) and auxiliary (C) atoms is essential to estimate frequencies suitable for spectroscopy analysis computationally. The same combination of basis set was then used to examine other possible reaction steps, and Raman experiments successfully detected one of the suggested intermediates of (CdCH 3 ) 2 .
“…The polarization of the innercore electrons is usually negligible. These circumstances allow us to use a two-step technique, advanced by our group [23][24][25][26][27] and recently applied for calculation of E eff in molecular systems [28,29]. At the first step we exclude inactive inner-core orbitals from correlation calculation with the help of a very accurate generalized relativistic effective core potential method (GRECP) [30][31][32] to reduce computational efforts.…”
Towards the search of electron electric dipole moment: correlation calculations of the P,T-violation effect in the Eu ++ cation. Recently the Eu0.5Ba0.5TiO3 solid was suggested as a promising candidate for experimental search of the electron electric dipole moment. To interpret the results of this experiment one should calculate the effective electric field acting on an unpaired (spin-polarized) electrons of europium cation in the crystal because the value of this field cannot be measured experimentally. The Eu ++ cation is considered in the paper in the uniform external electric field Eext as our first and simplest model simulating the state of europium in the crystal. We have performed high-level electronic structure correlation calculation using coupled clusters theory (and scalar-relativistic approximation for valence and outer core electrons at the molecular pseudopotential calculation stage that is followed by the four-component spinor restoration of the core electronic structure) to evaluate the enhancement coefficient K = E eff /Eext (where Eext is the applied external electric field and E eff is the induced effective electric field acting on an unpaired electron in Eu ++ ). A detailed computation analysis is presented. The calculated value of K is -4.6.
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