Charge Transfer Collisions in Ionospheres, Exospheres,
Magnetospheres, and Interstellar Clouds
Fine-Structure Effects in O+ - O Collisions
Resonant charge exchange collisions of atomic oxygen positive ions with
neutral oxygen atoms is a principal mechanism of energy coupling
between the terrestrial magnetosphere, ionosphere, and thermosphere.
At high geomagnetic latitudes, direct electrical coupling of the
magnetosphere with the ionosphere induces F-region ion convection that
is strongly impressed on the neutral gas in the thermosphere through
the ion-drag force. At the atomic level, ion drag corresponds to the
process
O+(fast) + O(slow) -> O(fast) + O+(slow)
The long-range nature of such resonant charge exchange collisions means
that the kinetic energy of each nucleus tends to be conserved. Thus,
exchange of an electron has the same effect as a very efficient
transfer of momentum and leads to an apparent slowing down of the ion.
Laboratory experimental measurement of resonant oxygen atom charge
exchange cross sections at atmospherically relevant energies has proved
to be extremely difficult. Lehigh University and SRI International
collaborated on a new theoretical approach that
included, for the first time, the fine-structure splitting of atomic
oxygen as well as spin-orbit and rotational coupling between the states
of the oxygen molecular ion, O2+, during the
collision [1,2].
Accidental Resonance in H+ - O and O+ - H
Collisions
The ionization potentials of O(3P1) and H atoms
are equal to within the current experimental uncertainty. This means
that the charge transfer reactions
O + H+ <--> O+ + H
have very large cross sections in both directions, and thus play
central roles in interactions with the solar wind and atomic escape in
the exospheres of Venus, Earth, and Mars, as well as in interstellar
clouds. We are performing ab initio electronic structure
calculations [3] and quantum mechanical coupled channels calculations,
including spin-orbit coupling, of differential and momentum transfer
cross sections for charge exchange and fine structure excitation in
this system. The work builds on previous theoretical [4-7] and
photodissociation spectroscopy studies [5,8] of the OH+
molecule and parallels our previous calculations on collisions of
O+ with O [1,2] (described above). For several transitions,
collision mechanisms based on curve crossings have been identified. The
results indicate that long range coupling terms in the OH+
potentials (internuclear distances 10-15 a0) contribute to
the cross sections.
References
- A. P. Hickman, M. Medikeri-Naphade, C. D. Chapin,
and D. L. Huestis, "Fine Structure Effects in the O+-O
Collision Frequency," Geophys. Res. Lett. 24, 119-122 (1997)
- A. P. Hickman, M. Medikeri-Naphade, C. D. Chapin,
and D. L. Huestis, "Calculation of Fine Structure Effects in the
O+-O Collisions," Phys. Rev. A 56, 4633-4643 (1997).
- J. A. Spirko, J. T. Mallis, and A. P. Hickman,
"Calculation of Adiabatic and Diabatic 3Sigma-
States of OH+," J. Phys. B 33, 2395-2407 (2000).
- G. Chambaud, J. M. Launay, B. Levy, P. Millie,
E. Roueff, and F. T. Minh, "Charge Exchange and Fine-Structure Excitation
in O-H+ Collisions," J. Phys. B 13, 4205-4216 (1980).
- H. Helm, P. C. Cosby, and D. L. Huestis, "Photofragment
Spectroscopy of the Shape Resonances in OH+," Phys. Rev.
A 30, 851-857 (1984).
- R. P. Saxon and B. Liu, "Theoretical Study of OH+:
Potential Curves, Transition Moments, and Photodissociation Cross
Sections," J. Chem. Phys. 85, 2099-2104 (1986).
- P. C. Stancil, D. R. Schultz, M. Kimura, J.-P.
Gu, G. Hirsch, and R. J. Buenker, "Charge Transfer in Collisions
of O+ with H and H+ with O," Astron. Astrophys.
Supp. Ser. 140, 225-236 (1999).
- J. Levin, U. Hechtfischer, L. Knoll, M. Lange,
G. Saathoff, R. Wester, A. Wolf, D. Schwalm, and D. Zajfman, "Photodissociation
Spectroscopy of OH+ Molecular Ions at the TSR Storage
Ring," Hyperfine Interactions 127, 267-270 (2000).
Acknowlegements
This research was supported by the NSF Aeronomy program.
Principal Investigators
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