Analytic expressions fitted to cross section data on collisions of H + , H + 2 , H + 3 , H, H 2 , and H -with H 2 are given. The data used are those recommended by Phelps [J. Chem. Phys. Ref. Data 19, 653 (1990)] and additional experimental data, when available, up to a projectile energy of about 10
Three-dimensional finite element method for electronic properties of small polyatomic molecules: H+2, H2, H2+3 and H+3
✍ Scribed by Hengtai Yu; André D. Bandrauk; Vijay Sonnad
- Publisher
- Elsevier Science
- Year
- 1994
- Tongue
- English
- Weight
- 591 KB
- Volume
- 222
- Category
- Article
- ISSN
- 0009-2614
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✦ Synopsis
A fully numerical solution of the SCF equations is presented for the small polyatomic molecules: Hz, HZ, Hi+ and Hz by a finite element method in Cartesian coordinates in three dimensions. A new method to remove the singularities of nuclear potentials is given. A block Lanczos method is used to avoid large matrix storage problems for large finite element basis sets.
📜 SIMILAR VOLUMES
The electronic stopping power of amorphous carbon targets for H 2 and H 3 molecular beams has been analysed within the framework of the dielectric formalism. Coulomb explosion between the partners of the molecule has been taken into account to evaluate the average stopping power ratio during the dwe
## Abstract A finite element method approach for solving the three‐dimensional Schrödinger equation expressed in hyperspherical coordinates is applied to the calculation of rovibrational states of H~2~O and D~2~O. Comparisons to experimental values and other theoretical calculations are offered.
A coupled three-dimensional model calculation of the low-frequency large-amplitude intermolecular torsional states in (H20) 3 and (D20) 3 is presented, based on the analytical modEPEN intermolecular potential surface and a three-dimensional discrete variable representation approach. The lowest torsi
2.5 , monoclinic C2/m, a ؍ 18.425(4) A ˚, c ؍ 8.954(2) A ˚,  ؍ 93.69(2) 0 , V ؍ 1221.1(4) A ˚3, Z ؍ 4, D calc ؍ 2.423 g cm ؊3 ; 2 ؒ H 2 O, H 4 F 2 K 2 O 13 P 2 V 3 , triclinic P1, a ؍ 7.298(1) A ˚, b ؍ 8.929(2) A ˚, c ؍ 10.090(2) A ˚, ␣ ؍ 104.50(2) 0 ,  ؍ 100.39(2) 0 , ␦ ؍