1979
DOI: 10.1088/0022-3700/12/9/011
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Merged electron-ion beam experiments. III. Temperature dependence of dissociative recombination for atmospheric ions NO+, O2+and N2+

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Cited by 127 publications
(45 citation statements)
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“…However, at lower temperatures the pulsed afterglow values are somewhat larger than the present value which may be a manifestation of ion clustering in the higher pressure pulsed afterglow experiment (Biondi and ") which is in good agreement with the afterglow results. Data obtained by Mul and McGowan (1979) for CrE(O) using the merged beam technique agree within Theoretical descriptions of dissociative recombination distinguish between a 'direct' process and an 'indirect' process (see the review by Bardsley and Biondi 1970). For the direct process, in which the electron is envisaged to be captured directly into a repulsive state of the neutral molecule, a.…”
Section: E Alge N G Adams and D Smithsupporting
confidence: 72%
“…However, at lower temperatures the pulsed afterglow values are somewhat larger than the present value which may be a manifestation of ion clustering in the higher pressure pulsed afterglow experiment (Biondi and ") which is in good agreement with the afterglow results. Data obtained by Mul and McGowan (1979) for CrE(O) using the merged beam technique agree within Theoretical descriptions of dissociative recombination distinguish between a 'direct' process and an 'indirect' process (see the review by Bardsley and Biondi 1970). For the direct process, in which the electron is envisaged to be captured directly into a repulsive state of the neutral molecule, a.…”
Section: E Alge N G Adams and D Smithsupporting
confidence: 72%
“…3,6,7 In order to interpret and quantify the green and red airglow observations and their ionospheric implications, the dependence of the DR reaction on the O 2 + internal excitation and the electron collision energy must be known. It has already been well established, both theoretically and experimentally, that the temperature dependence of the O 2 + thermal rate coefficient follows the power law ␣͑O 2 + ͒ϳT −0.7 or, in terms of electron-energy dependence of the rate coefficient as used in merged-beam experiments, [8][9][10][11][12] k͑O 2 + ͒ϳE c −0.5 . Here T pertains mainly to the electron temperature, while E c is the collision energy between the electron and the ion.…”
Section: Dissociative Recombination ͑Dr͒ Of Omentioning
confidence: 99%
“…Kella et al 20 measured the DR branching behavior of an unknown vibrational population of the mixed isotopomer 16 O 18 O ϩ . In Kella et al's study, only the total quantum yields summed over all the vibrational levels are reported.…”
Section: A O 2 ¿ and Similar Systemsmentioning
confidence: 99%
“…In general, the temperature dependence of the thermal rate coefficient is reported to follow ␣(O 2 ϩ )ϳT Ϫ0.7 with T pertaining mainly to the electron temperature. In merged-beam experiments it is the rate coefficient, k, in terms of the electron collision energy which is commonly reported and its dependence is found [13][14][15][16] to be k(O 2 ϩ )ϳE c Ϫ0. 5 .…”
Section: Introductionmentioning
confidence: 99%
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