1986
DOI: 10.1088/0022-3700/19/23/019
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Near-threshold vibrational excitation and elastic electron scattering from N2

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Cited by 40 publications
(23 citation statements)
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“…We begin with three energies below the resonance (0.55, 1.0, and 1.5 eV), then turn to six above it (4.0, 5.0, 6.0, 7.0, 8.0, and 10.0 eV)energies chosen in part to facilitate comparison to the several other measured and' calculated elastic e-N2 DCSs in the literature. Our results at below-resonance energies appear in Tables IV and V. Figure 7(a) compares the present elastic DCSs at our lowest energy, 0.55 eV, with those from previous measurements by Sohn et al [54] and by Shi, Stephen, and Burrow [58]. Agreement between the present experimental and theoretical results is generally good.…”
Section: Nonresonant Elastic Scatteringsupporting
confidence: 85%
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“…We begin with three energies below the resonance (0.55, 1.0, and 1.5 eV), then turn to six above it (4.0, 5.0, 6.0, 7.0, 8.0, and 10.0 eV)energies chosen in part to facilitate comparison to the several other measured and' calculated elastic e-N2 DCSs in the literature. Our results at below-resonance energies appear in Tables IV and V. Figure 7(a) compares the present elastic DCSs at our lowest energy, 0.55 eV, with those from previous measurements by Sohn et al [54] and by Shi, Stephen, and Burrow [58]. Agreement between the present experimental and theoretical results is generally good.…”
Section: Nonresonant Elastic Scatteringsupporting
confidence: 85%
“….2~I i I I i~I i I In addition to the present experimental (solid circles) and theoretical (solid lines) results, we show the data of Sohn et al. [54] (open triangles) and in (a) and (c) of Shi, Stephen, and Burrow [58] (open squares). Also shown in (c) are measured DCSs of Shyn and Carignan [45] (open circles) and the hybrid-theory results of Chandra and Temkin [34] (long-dashed line) and Schwinger multichannel DCSs of Huo et al.…”
Section: Nonresonant Elastic Scatteringsupporting
confidence: 53%
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“…[42] The elastic scattering cross sections are based on the work by LaBahn and Callaway [1970], Williams [1975], Blaha and Davis [1975], Williams and Allen [1989], Bray et al [1991] and Mayol and Salvat [1997] for atomic species (H, He, N and O), Sohn et al [1986], García and Blanco [2001] and Itikawa [2006] for N 2 , Itikawa [2002] and Morrison et al [1977] for CO 2 , Kanik et al [1992] for CO, as well as Jain and Baluja [1992] and Brunger et al [1991] for H 2 . For the electronic excitation of atomic species, we adopt the cross sections of Stone et al [2002] for H and He, Laher and Gilmore [1990] for O, Goembel [1991, 1992] and Yang and Doering [1996] for N. For electron impact ionization, the cross sections of Bartlett and Stelbovics [2004] are used for H, He and N, and those of Laher and Gilmore [1990] are used for O.…”
Section: Discussionmentioning
confidence: 99%
“…The cross section is dominated by the well-known 2 Π g resonance centered around 2.3 eV. [14], and the theoretical results of Feng et al [15,16] (DSG model) are shown for comparison. three incident energies marked by bars in figure 2.…”
Section: Nitrogenmentioning
confidence: 95%