1965
DOI: 10.1115/1.3625776
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Handbook of Mathematical Functions With Formulas, Graphs and Mathematical Tables (National Bureau of Standards Applied Mathematics Series No. 55)

Abstract: t he spectroscopy of transition-group complexes, Kihara the interact.ions of convex molecules, Koide and Oguchi t he magnetic properties of compounds, Liehr forbidden t.ransitions, :l\IcLennan the formal statist.ical theOl'~' of t.l'Unsport proces es, Scrocco the interpretation of quaClrupole coupling data, and finally Widom the collision t heory of reactiolt rates.This reviewer foulld t he contributions by IGhara and Widom the most st.imulating and interesting. The former is a clear :1ccount of how measured q… Show more

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Cited by 2,961 publications
(3,281 citation statements)
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“…Substituting the expression for f ′ e in Eq. (24) and taking the factor exp(−µ e /T ) out of the integration, we find that the remaining integral depends only on one parameter t r = k B T /(m e c 2 ) = 0.1686 T 9 , where T 9 = T /10 9 K, and can be expressed through a McDonald function (e.g., Abramowitz and Stegun 1964). In the limiting cases t r ≪ 1 (nonrelativistic positrons) and t r ≫ 1 (ultrarelativistic positrons) the integral is done analytically.…”
Section: Annihilation Of Electron-positron Pairs (A) Emissivitymentioning
confidence: 99%
“…Substituting the expression for f ′ e in Eq. (24) and taking the factor exp(−µ e /T ) out of the integration, we find that the remaining integral depends only on one parameter t r = k B T /(m e c 2 ) = 0.1686 T 9 , where T 9 = T /10 9 K, and can be expressed through a McDonald function (e.g., Abramowitz and Stegun 1964). In the limiting cases t r ≪ 1 (nonrelativistic positrons) and t r ≫ 1 (ultrarelativistic positrons) the integral is done analytically.…”
Section: Annihilation Of Electron-positron Pairs (A) Emissivitymentioning
confidence: 99%
“…where ζ denotes the scale factor, L (α) n (x) are the generalized Laguerre polynomials which are the eigenfunctions of the FourierBessel transform [54]. The notation (a) n denotes the Pochhammer symbol and 1F1 denotes the confluent hyper-geometric function.…”
Section: Spherical Polar Fourier Expansionmentioning
confidence: 99%
“…For orders n larger than the Bessel function argument, it is necessary to compute the ratios of the Bessel functions and of their derivative using recursion relationships obtained from the recursion equations [Abramowitz and Stegun, 1964]. The use of quadruple precision can be an alternative solution but is faced to enormous memory requirement and long computation time without preventing numerical instabilities.…”
Section: 1002/2014rs005532mentioning
confidence: 99%
“…Owing to the behavior of the Bessel functions with respect to their order and argument, they are calculated differently for low and high orders. For the low orders n the Bessel function are calculated using the recursion equations [Abramowitz and Stegun, 1964]. When the order n is close to the Bessel function argument for large values, the numerical calculation of the Bessel functions is an issue and widely discussed [Berry, 1964;Houdzoumis, 1994] and is still the most challenging part in this study.…”
Section: 1002/2014rs005532mentioning
confidence: 99%