Gas Discharge Closing Switches 1990
DOI: 10.1007/978-1-4899-2130-7_5
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Field Distortion Three Electrode Gaps

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Cited by 18 publications
(22 citation statements)
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“…Although earlier investigations indicated that scaling via the ratio of the square root of reduced masses gave reasonable estimates for collisional rate coefficients, the current study, shows that this agreement was fortuitous (see also Schaefer 1990 for similar findings for HD). The constant factor of ∼1.4 frequently used to predict the rate coefficients of para-H 2 from that of He generally lead to inaccurate results due to the fact that the underlying assumptions are not valid.…”
Section: Resultssupporting
confidence: 56%
“…Although earlier investigations indicated that scaling via the ratio of the square root of reduced masses gave reasonable estimates for collisional rate coefficients, the current study, shows that this agreement was fortuitous (see also Schaefer 1990 for similar findings for HD). The constant factor of ∼1.4 frequently used to predict the rate coefficients of para-H 2 from that of He generally lead to inaccurate results due to the fact that the underlying assumptions are not valid.…”
Section: Resultssupporting
confidence: 56%
“…While we are unaware of any existing experimental data for He-HD inelastic collisions, the current results can be assessed by comparing to the previous calculations. Rotational transitions for v = 0 have been computed by Schaefer (1990) and Roueff & Zeippen (1999) which were found to be in good agreement. Our rotational transitions are also found to agree with the previous work.…”
Section: Resultsmentioning
confidence: 81%
“…Here, we have focused on collisions due to He, but H and H 2 are also important impactors. In fact, most modeling studies of primordial gas collapse have adopted the H-HD cooling function of Galli & Palla (1998), which was actually obtained by mass-scaling the He-HD {v = 0, j = 0} → {v = 0, j = 1} rotational excitation rate coefficients of Schaefer (1990). More elaborate cooling functions have been constructed by Flower et al (2000) and Lipovka et al (2005) with the former considering H, He, and H 2 colliders, but the latter limited to H (see the summary in Glover & Abel 2008).…”
Section: Astrophysical Implicationsmentioning
confidence: 99%
“…Since the energy spacing of the rotational levels of HD is quite large, E 1 /k = 128 K, E 2 /k = 383 K, E 3 /k = 764 K, etc., GP computed the HD cooling function with a simple four-level system (J = 0-3) adopting the collisional coefficients of Schaefer (1990). Flower et al (2000) updated the calculations of GP adopting the collisional rate coefficients of Flower & Roueff (1999) and Roueff & Zeippen (1999).…”
Section: Heating and Coolingmentioning
confidence: 99%
“…The coefficients for inelastic scattering of He-HD were computed by Green (1974) and Schaefer (1990) at temperatures T ≤ 600 K, for 0 ≤ J ≤ 3 and ∆J = +1, +2. Collisional coefficients for rotational excitation of the system H-HD were usually derived by scaling the He-HD values with the square root of the ratio of the reduced masses of the two systems, γ H−HD = (µ He−HD /µ H−HD ) 1/2 γ He−HD , where (µ He−HD /µ H−HD ) 1/2 = 1.51 (see e.g.…”
Section: Heating and Coolingmentioning
confidence: 99%