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Theoretical study of ion-pair formation in electron recombination with H3

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of Applied Science, UC Davis, Davis, California, USA ... G. G. Balint-Kurti et al., Comp. Phys. Comm. 63 126 (1991) 1D study. Ion-pair state alone. ... – PowerPoint PPT presentation

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Title: Theoretical study of ion-pair formation in electron recombination with H3


1
Theoretical study of ion-pair formation in
electron recombination with H3
  • Royal Society Discussion meeting on Physics,
    Chemistry and Astronomy of H3
  • January 18-2006
  • Åsa Larson1, Johanna Roos1 and Ann E. Orel2
  • 1Dept. of Applied Physics, Royal Institute of
    Technology, Stockholm, Sweden
  • 2Dept. of Applied Science, UC Davis, Davis,
    California, USA

2
(Resonant) Ion-Pair formation in electron
recombination (RIP)
3
High-energy resonant states for H3
1979, K. C. Kulander and M. F. Guest 1 1984,
H. H. Michels and R. H. Hobbs 2 1D studies
H2 H-
  • The high-energy resonant states cannot explain
    the DR at low energies if not the taget ions are
    vibrationally excited.
  • The resonant states will produce a high-energy
    peak in the cross section of DR where both
    neutral and ionic fragments are formed (ion-pair
    formation).

1 K. C. Kulander and M. F. Guest, J. Phys B
At. Mol. Phys, 12, L501 (1979) 2 H. H. Michels
and R. H. Hobbs, Astrophys. J, 286, L27 (1984)
4
More detailed calculations
z (a0)
  • 1994, A. E. Orel et al.
  • 2D study using the Complex Kohn Variational
    method
  • Resonance position Ei and width ?i
  • Triple intersection

1 A. E. Orel, K. C. Kulander and B. H.
Lengsfield III, J. Chem. Phys. 100, 1756
(1994)
5
High-energy peak in the DR cross section
  • 1993, First experimental observation of the
    high-energy peak. (CRYRING) 1
  • Neutral fragmants detected
  • 1993, A. E. Orel et al. 2
  • Wave packet propagation in 2D assuming that
    everything dissociates into the neutral fragments
    (no couplings, potentials become flat).

1 M. Larsson et al. Phys. Rev Lett., 70 430
(1993) 2 A. E. Orel and K. C. Kulander, Phys.
Rev. Lett., 71 4315 (1993)
6
Measured cross section for ion-pair formation
  • The H- fragments were detected (the two channels
    H2 H- and H H H- cannot be seperated).
  • Cross section depends on the vibrational
    excitation
  • The magnitude of the cross section is about 2
    10-18 cm2 in all experiments.

1 B. Peart et al. J. Phys. B, 12 3441
(1979) 2 F. B. Yousif et al. J. Phys. B, 26,
4249 (1993) 3 S. Kalhori et al. Phys. Rev. A,
69 022713-1 (2004)
7
H3 vs H2
  • Potentials
  • Lowest resonant state goes diabatically to the
    ion-pair limit
  • ?E 5.4 eV

Potentials Lowest resonant state goes
diabatically to the ion-pair limit ?E 1.91 eV
8
H3 vs H2
  • Cross section for ion-pair formation
  • 2 of total DR cross section
  • A bump in the cross section

Cross section for ion-pair formation 5 of
total DR cross section Resonant structure
due to the quantum interference between competing
pathways
Why are they so different?
9
Theoretical study of the ion-pair formation
  1. Calculate the resonant states using the Complex
    Kohn Variational method ?

Note all calculations are carried out in 2D!
10
Theoretical study of the ion-pair formation
2. Calculate the ionic and neutral adiabatic
potentials using CI with a basis set including
diffuse orbitals to describe Rydberg states.
11
Theoretical study of the ion-pair formation
3. Transform from the adiabatic to the
corresponding diabatic states using the CI
coefficients. Calculate also the couplings beween
the neutral states. ?
12
Theoretical study of the ion-pair formation
4. Study the dynamics using wave packets.
Include autoionization using complex resonant
potentials.
Propagate the wavepackets on coupled potentials
Initiate wave packets on the resonant states
(electron recombination)
13
Theoretical study of the ion-pair formation
5. Calculate the cross section for ion-pair
formation by analyzing the dissociating flux 1.
zstop
1 D. J. Haxton et al., Phys. Rev A., 69
062714-1 (2004) G. G. Balint-Kurti et al.,
Comp. Phys. Comm. 63 126 (1991)
14
1D study
Ion-pair state alone. Autoionization is included
and lowest vibrational level of the ion is
assumed.
Include the second resonance and the direct and
indirect couplings between them.
15
1D study
Add the couplings to the Rydbergs at small z.
Add also the couplings to the Rydbergs at large z
16
1D study
  • Compare with experimental cross section
  • Questions
  • Why is the shape so different ?
  • Why is the magnitude a factor 5 too large?

Perform 2D wave packet calculation!
17
2D study
Diabatic ion-pair state alone
Potential energy (H)
z
r
Much better shape of the cross section! Add the
couplings to the second resonance The 2nd
dimension will smear out the interference effects
between the two resonant states.
18
Add the effects from the Rydberg states (plan B)
  • In the 1D study the couplings to the Rydberg
    states reduced the cross section about 40 ,
    assume the same is true in the 2D study.

19
Use the Landau-Zener model to estimate the loss
of flux to the Rydberg states. Define the
reaction path as the classical path on the
ion-pair state.
  • Assume the flux coupled to the Rydberg state is
    lost.
  • Assume the flux can jump back to the ion-pair
    state.

20
Summary
  • To describe the ion-pair formation in H3 it is
    crucial to include at least two dimensions in the
    dynamics.
  • The second dimension will smear out the
    interference effects.
  • Flux will be lost due to the couplings to the
    Rydberg states.
  • To do
  • The wave packets propagating on 6 coupled
    potentials (two resonant states and 4 Rydberg
    states) are running now.
  • Study the effects from vibrational excitation of
    the ion.
  • Study the reaction for other isotopologous D3,
    HD2 , H2D
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