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Ion-Atom Collisions Electron capture reactions in N2 , O2 H

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Laboratorio asociado al CIEMAT de F sica At mica y Molecular en Plasmas de Fusi n ... GTO bases (Widmark et al. Theor.Chim. Acta. 77, 291 (1990) ... – PowerPoint PPT presentation

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Title: Ion-Atom Collisions Electron capture reactions in N2 , O2 H


1
Ion-Atom CollisionsElectron capture reactions in
N2, O2 H
patricia.barragan_at_uam.es barragan_at_phys.ksu.edu
  • Patricia Barragán
  • Laboratorio asociado al CIEMAT de Física Atómica
    y Molecular en Plasmas de Fusión
  • Departamento de Química, Universidad Autónoma de
    Madrid

September 28, 2005
2
Motivation
  • Fusion plasmas.
  • Plasma-wall interaction
    Impurities.
  • Plasma diagnostics (CXS).
  • Astrophysics.
  • Comets X-ray emission .

3
  • N2 H and O2 H collisions.
  • Presence of metastable ions in beams.
  • Calculation of rate coefficients.
  • Computational characteristics
  • Many electron systems. Use of Quantum Chemistry
    techniques.
  • Calculation in a wide energy range Quantal and
    semiclassical treatments.

4
N2 H collisions
Reaction (1)
Reaction (2)
5
O2 H collisions
  • Reaction (3)

Reaction (4)
Reaction (5)
6
Quantal treatment
  • Schrödinger equation
  • Boundary conditions (one electron systems)

7
Molecular expansion
?k are eigenfunctions of Helec
? is the Common Reaction Coordinate, which
ensures that a truncated expansion satisfies the
scattering boundary conditions
8
Cross Sections
are solutions of the system of differential
equations
The total Cross Section for transition i?j is
given by
9
Semiclassical treatment
  • The nuclei follow straight-line trajectories
  • The electronic motion is described by the eikonal
    equation
  • Molecular close-coupling treatment
  • where D(r,t) is a common translation factor.

10
Cross Sections

where the probability Pij for transition to the
final state is calculated from the coefficient
aj(t)
11
Computational scheme
  • Calculation of electronic energiesMRCI (MELDF)
  • - GTO bases (Widmark et al. Theor.Chim. Acta. 77,
    291 (1990))
  • - 80 reference configurations, iterative process
    to select the set of reference configurations at
    each R.
  • - Frozen core approximation.
  • - Perturbative selection.
  • Calculation of dynamical couplings.
  • - Numerical differentation (Castillo et al. J
    Chem. Phys. 03,2113(1995))
  • - Sign consistency calculation of the delayed
    overlap matrix (Errea et al. J Chem. Phys.
    121,1663 (2004))

12
N2 H Potential energy curves singlets
c.e.
13
N2 H Potential energy curves triplets
c.e.
c.e.
14
N2 H Potential energy curves triplets
15
N2 H Potential energy curves triplets
16
N2 H Potential energy curves quintets
17
N2 H Total cross sections
18
N2 H Total cross sections
19
N2 H Total cross sections
20
N2 H Total cross sections
21
N2 H Branching ratios
22
O2 H Potential energy curves doublets
23
O2 H Potential energy curves cuadruplets
24
O2 H Total cross sections
25
O2 H Total cross sections
26
O2 H Branching ratios
27
Rate coefficients
28
Rate coefficients
29
Concluding remarks
  • N2 H, O2 H collisions.
  • Quantal calculation for low energy and
    semiclassical for high energy.
  • Presence of metastable ions in beams Possible
    presence of N2(2s2p2 4P) in merged beams
    experiments. Not noted in other experiments.
  • Very large cross sections at low energies - shape
    resonances?
  • Calculation of partial EC cross sections
    (diagnostics).

30
Thanks to
  • L. Méndez, I. Rabadán, L. F. Errea and A. Riera
  • who have participated directly in this work.
  • And the other group members
  • L. Fernández, F. Guzmán, C. Illescas, A. Macías
  • and J. Suarez
  • Group web-site http//tcam.qui.uam.es
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