Title: Theoretical study of ion-pair formation in electron recombination with H3
1Theoretical 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)
3High-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)
4More 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)
5High-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)
6Measured 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)
7H3 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
8H3 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?
9Theoretical study of the ion-pair formation
- Calculate the resonant states using the Complex
Kohn Variational method ?
Note all calculations are carried out in 2D!
10Theoretical 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.
11Theoretical 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. ?
12Theoretical 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)
13Theoretical 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)
141D 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.
151D study
Add the couplings to the Rydbergs at small z.
Add also the couplings to the Rydbergs at large z
161D 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!
172D 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.
18Add 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.
19Use 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.
20Summary
- 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