1998
DOI: 10.1063/1.476745
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Positron chemistry by quantum Monte Carlo. II. Ground-state of positron-polar molecule complexes

Abstract: The stability of the ground-state of positron-polar molecule complexes ͓M,e ϩ ͔ has been explored for MϭLiH,HF,H 2 O,BeO,LiF using variational and diffusion Monte Carlo techniques. Our simulations show that the ground-state of the complexes ͓LiH,e ϩ ͔ 2,1 ⌺ ϩ , ͓BeO,e ϩ ͔ 2,1 ⌺ ϩ , and ͓LiF,e ϩ ͔ 2,1 ⌺ ϩ is stable against the dissociation either in the two fragments M and e ϩ or in the other two fragments M ϩ and Psϭ͓e ϩ ,e Ϫ ͔, while the ground-state of ͓H 2 O,e ϩ ͔ 2,1 A 1 , and of ͓HF,e ϩ ͔ 2,1 ⌺ ϩ has an e… Show more

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Cited by 63 publications
(66 citation statements)
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“…We notice that a similar behavior of δ(r −+ ) may be expected also for e + LiF due to the polarization of the positronic density of the PsF fragment by the Li + core. The situation could be quite different for the e + BeO case where the positron density is expected to be centered on Be at large nuclear distances (the two fragments e + Be and O have lower total energy than Be + and PsO [39]), and to move on the O side of the molecule when the distance decreases. This effect is due to the electron transfer from Be to O that creates the large molecular dipole moment.…”
Section: Discussionmentioning
confidence: 99%
“…We notice that a similar behavior of δ(r −+ ) may be expected also for e + LiF due to the polarization of the positronic density of the PsF fragment by the Li + core. The situation could be quite different for the e + BeO case where the positron density is expected to be centered on Be at large nuclear distances (the two fragments e + Be and O have lower total energy than Be + and PsO [39]), and to move on the O side of the molecule when the distance decreases. This effect is due to the electron transfer from Be to O that creates the large molecular dipole moment.…”
Section: Discussionmentioning
confidence: 99%
“…The many-body wave functions of small positronic systems composed by a positron interacting with a light atom or a small molecule can be calculated to a good accuracy using the quantum Monte Carlo (QMC) [11][12][13][14][15][16] and configurationinteraction (CI) [17] methods. In this work, we have obtained accurate positron energies and densities for positronic atoms including a positron (e + H, e + He, e + Li, and e + Be) and Ps (HPs and LiPs) by an exact diagonalization stochastic variational method (SVM) using an explicitly correlated Gaussian (ECG) function basis set.…”
Section: Introductionmentioning
confidence: 99%
“…In such situation, establishing the energetic stability of AB requires explicit calculation of D 0 with Eq. (10).…”
Section: Methodsmentioning
confidence: 99%
“…Further calculations on various positronic atoms quickly followed (see [3] for a review and [4][5][6][7][8] for more recent results). Besides of variational calculations with ECG functions, diffusion quantum Monte Carlo simulations appeared to be able to provide accurate energies for positronic systems [9][10][11][12][13]. Unfortunately, the computational cost of both methods increases quickly with the number of active electrons, limiting in practice their applicability to rather small atoms and molecules.…”
Section: Introductionmentioning
confidence: 99%