Third-order connection between the collision source η(v, μ) and the isotropic componentf 0 of the usual distribution functionf(v, μ) for electrons in a weakly ionized gas
Author:
Publisher
Springer Science and Business Media LLC
Subject
General Medicine
Link
http://link.springer.com/content/pdf/10.1007/BF02739164.pdf
Reference12 articles.
1. G. Cavalleri, E. Gatti andF. Gonzalez-Gascon:Nuovo Cimento B,55, 291 (1980).
2. S. Paveri-Fontana:Lett. Nuovo Cimento,4, 1259 (1970).
3. G. Cavalleri andG. Sesta:Phys. Rev.,170, 286 (1968).
4. For the application of theP 3 approximation seeG. Cavalleri:Nuovo Cimento B,55, 360 (1980).
5. G. L. Braglia:Lett. Nuovo Cimento,3, 295 (1970), eq. (2′), where the collision source is denoted by η(v, μ)=g(v, μ)/T withT=〈t〉 andg(v, μ), is, like in ref. (3),G. Cavalleri andG. Sesta:Phys. Rev.,170, 286 (1968). improperly called «the initial distribution function». Actually ag(v, μ) so defined is still the collision source (to within a dimensional constant): see eq. (A.11) and relevant comment of appendix A of ref. (1).G. Cavalleri, E. Gatti andF. Gonzalez-Gascon:Nuovo Cimento B,55, 291 (1980).
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1. Highly accurate, explicit expression of lateral-and longitudinal-diffusion coefficients for free electrons in a scattering medium;Il Nuovo Cimento B Series 11;1981-03
2. Solution with Third-order Accuracy for the Electron Distribution Function in Weakly Ionized Gases (or in Intrinsic Semiconductors): Application to the Drift Velocity;Australian Journal of Physics;1981
3. A highly accurate and simple expression of electron drift velocity in gases and semiconductors;Il Nuovo Cimento B Series 11;1980-02
4. Evaluation of the auxiliary termb introduced for making the expansions of transport quantities convergent;Il Nuovo Cimento B Series 11;1980-02
5. Highly accurate explicit expressions of electron drift velocity and distribution function for experimentalists;Il Nuovo Cimento B Series 11;1980-02
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