Charge transfer in collisions between diatomic molecular ions and atomic hydrogen using merged beams
A merged-beams technique is used to measure charge transfer (CT) cross sections for the (O2+,D) and (CO+,D) systems from 2 keV/u to 20 eV/u, which covers a wide range of energy: high energies where the collision is ro-vibrationally frozen to low energies where ro-vibrational modes become important....
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Published in: | Physical review. A, Atomic, molecular, and optical physics Vol. 84; no. 6 |
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27-12-2011
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Abstract | A merged-beams technique is used to measure charge transfer (CT) cross sections for the (O2+,D) and (CO+,D) systems from 2 keV/u to 20 eV/u, which covers a wide range of energy: high energies where the collision is ro-vibrationally frozen to low energies where ro-vibrational modes become important. At high energies where the differences in the Q-values of the CT process can be neglected, the cross sections all converge to (7.5 0.5) x 10-16 cm2 at 2 keV/u and are consistent with a H2+ + H calculation which assumes the ro-vibrational modes are frozen. Toward lower velocities, (O2+,D) and (CO+,D) have consistently similar cross sections, as one might expect from the comparison of their characteristic vibrational time, but diverge below 60eV/u. In contrast, previously reported merged-beams measurements for (D2+,H), a system with fewer electrons on the molecular core, no electronic excited states and with relatively less charge transfer channels, shows a decreasing cross section toward lower energies. These different trends are compared to merged-beams measurements of charge transfer for several 4+ atomic ions that have a different number of electrons on the core. |
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AbstractList | A merged-beams technique is used to measure charge transfer (CT) cross sections for the (O2+,D) and (CO+,D) systems from 2 keV/u to 20 eV/u, which covers a wide range of energy: high energies where the collision is ro-vibrationally frozen to low energies where ro-vibrational modes become important. At high energies where the differences in the Q-values of the CT process can be neglected, the cross sections all converge to (7.5 0.5) x 10-16 cm2 at 2 keV/u and are consistent with a H2+ + H calculation which assumes the ro-vibrational modes are frozen. Toward lower velocities, (O2+,D) and (CO+,D) have consistently similar cross sections, as one might expect from the comparison of their characteristic vibrational time, but diverge below 60eV/u. In contrast, previously reported merged-beams measurements for (D2+,H), a system with fewer electrons on the molecular core, no electronic excited states and with relatively less charge transfer channels, shows a decreasing cross section toward lower energies. These different trends are compared to merged-beams measurements of charge transfer for several 4+ atomic ions that have a different number of electrons on the core. |
ArticleNumber | 062716 |
Author | Seely, D. G. Havener, C. C. Andrianarijaona, V. M. Draganić, I. N. |
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BackLink | https://www.osti.gov/biblio/1032477$$D View this record in Osti.gov |
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CitedBy_id | crossref_primary_10_1016_j_nimb_2015_01_040 crossref_primary_10_1016_j_pnmrs_2020_08_002 crossref_primary_10_1016_j_nimb_2015_01_002 |
Cites_doi | 10.1016/0375-9601(68)91141-9 10.1103/PhysRevA.66.042717 10.1016/j.nima.2011.02.090 10.1103/PhysRevA.71.034702 10.1103/PhysRevA.83.054701 10.1103/PhysRevA.56.426 10.1016/0031-8914(70)90237-5 10.1088/0022-3700/15/23/025 10.1103/PhysRevA.67.022708 10.1051/0004-6361:20064981 10.1016/j.nimb.2005.03.206 10.1103/PhysRevA.54.R13 10.1063/1.1696966 10.1063/1.1730857 10.1103/PhysRev.172.1 10.1088/0953-4075/31/18/016 10.1103/PhysRevA.39.1725 10.1103/PhysRevA.51.3685 10.1103/PhysRevA.14.579 10.1103/PhysRevA.64.062712 10.1016/0009-2614(87)80810-2 10.1103/PhysRevA.57.4462 10.3390/i8111158 10.1103/PhysRevA.76.012702 10.1088/1742-6596/4/1/025 10.1103/PhysRevA.5.1726 10.1119/1.9797 10.1063/1.1682048 10.1063/1.479264 10.1103/PhysRevLett.54.2663 10.1016/j.nimb.2007.04.103 10.1088/1742-6596/194/1/012043 10.1016/j.nima.2007.10.041 10.1103/PhysRevLett.52.2084 |
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References | C. C. Havener (PhysRevA.84.062716Cc11R1) 1997 PhysRevA.84.062716Cc27R1 PhysRevA.84.062716Cc28R1 PhysRevA.84.062716Cc29R1 PhysRevA.84.062716Cc23R1 C. C. Havener (PhysRevA.84.062716Cc12R1) 2003 PhysRevA.84.062716Cc24R1 PhysRevA.84.062716Cc25R1 PhysRevA.84.062716Cc26R1 PhysRevA.84.062716Cc20R1 C. C. Havener (PhysRevA.84.062716Cc9R1) 2011 PhysRevA.84.062716Cc21R1 PhysRevA.84.062716Cc22R1 J. D. Thomas (PhysRevA.84.062716Cc17R1) 2009 PhysRevA.84.062716Cc8R1 PhysRevA.84.062716Cc16R1 PhysRevA.84.062716Cc39R1 PhysRevA.84.062716Cc7R1 PhysRevA.84.062716Cc38R1 PhysRevA.84.062716Cc6R1 PhysRevA.84.062716Cc18R1 PhysRevA.84.062716Cc34R1 PhysRevA.84.062716Cc13R1 PhysRevA.84.062716Cc35R1 PhysRevA.84.062716Cc14R1 PhysRevA.84.062716Cc37R1 PhysRevA.84.062716Cc15R1 PhysRevA.84.062716Cc36R1 PhysRevA.84.062716Cc30R1 PhysRevA.84.062716Cc31R1 PhysRevA.84.062716Cc10R1 PhysRevA.84.062716Cc32R1 PhysRevA.84.062716Cc33R1 PhysRevA.84.062716Cc40R1 PhysRevA.84.062716Cc4R1 PhysRevA.84.062716Cc3R1 PhysRevA.84.062716Cc2R1 PhysRevA.84.062716Cc1R1 |
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Title | Charge transfer in collisions between diatomic molecular ions and atomic hydrogen using merged beams |
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