1974
DOI: 10.1088/0022-3727/7/18/314
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Diffusion and ionization studies for electron swarms in carbon monoxide and carbon dioxide

Abstract: The ratio of the radial diffusion coefficient to mobility Dr/μ has been measured for electron swarms moving through uniform electric fields in carbon monoxide and carbon dioxide for the range 3 less-than-or-eq, slant E/p less-than-or-eq, slant 500 and 10 less-than-or-eq, slant E/p less-than-or-eq, slant 550 V cm−1 Torr−1 at 0 °C respectively using the analytical methods described by Kontoleon et al (1972). The values of Dr/μ in the range E/p>50 are the first results in both the gases. The ionization coefficien… Show more

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Cited by 31 publications
(7 citation statements)
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“…Values of DTII1 were measured by Warren and Parker (1962) in the low E/N range at 77 K. The room-temperature results of Skinker and White (1923) and Roznerski and Mechlinska-Drewko (1979) extend over the entire range of E/N covered by us in the present study, while the lower end of the E/N range investigated by Lakshminarasimha et al (1974) overlaps the upper range of our measurements. Nelson and Davis (1969) measured the diffusion coefficient for thermal electrons, while Wagner et al (1967) measured values of the longitudinal diffusion coefficient DL.…”
Section: Previous Measurements (A) Carbon Monoxidesupporting
confidence: 78%
See 1 more Smart Citation
“…Values of DTII1 were measured by Warren and Parker (1962) in the low E/N range at 77 K. The room-temperature results of Skinker and White (1923) and Roznerski and Mechlinska-Drewko (1979) extend over the entire range of E/N covered by us in the present study, while the lower end of the E/N range investigated by Lakshminarasimha et al (1974) overlaps the upper range of our measurements. Nelson and Davis (1969) measured the diffusion coefficient for thermal electrons, while Wagner et al (1967) measured values of the longitudinal diffusion coefficient DL.…”
Section: Previous Measurements (A) Carbon Monoxidesupporting
confidence: 78%
“…Lack of reliable transport data limited their determination of the cross sections to energies less than 1 eV. With the availability of new drift velocity (Vdr) data (Milloy 1977), Land (1978) was able to extend the analysis to include the resonance, basing his work on Milloy's data and also data for the transverse diffusion coefficient to mobility ratio Drill of Skipker and White (1923) and Lakshminarasimha et al (1974). A significant result of this work was his conclusion that, in order to obtain reasonable agreeme~ between calculated and measured transport coeffiCients, it was necessary to apply a scaling factor of 1·9 to the set of vibrational excitational cross sections determined by Ehrhardt et al (1968) from their beam experiment.…”
Section: Introductionmentioning
confidence: 99%
“…In this work, it is essential to validate the data with the experiment results [11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28]. In fact, it should be noted that for now there are only available data for air at elevated temperatures.…”
Section: Selection Of the Cross Section Setsmentioning
confidence: 99%
“…After the electron pulsed source is shut off, a small current remains generated by both the secondary electron processes and the space-charge current of the positive ions. The current ratio is analysed by using a trial-and-error computer technique in (19) together with the CXT values of Lakshminarasimha et al (1974) 6 for E/N up to 5650 Td. The results for (Dr/p)exp by Lakshminarasimha et a1 (1974) are shown for comparison.…”
Section: Resultsmentioning
confidence: 99%