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zengő–Szász inequality

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11: 7.8 Inequalities
§7.8 Inequalities
7.8.7 sinh x 2 x < e x 2 F ( x ) = 0 x e t 2 d t < e x 2 1 x , x > 0 .
7.8.8 erf x < 1 e 4 x 2 / π , x > 0 .
12: 24.9 Inequalities
§24.9 Inequalities
Except where otherwise noted, the inequalities in this section hold for n = 1 , 2 , . …
13: 4.5 Inequalities
§4.5 Inequalities
§4.5(i) Logarithms
For more inequalities involving the logarithm function see Mitrinović (1964, pp. 75–77), Mitrinović (1970, pp. 272–276), and Bullen (1998, pp. 159–160).
§4.5(ii) Exponentials
(When x = 0 the inequalities become equalities.) …
14: 4.18 Inequalities
§4.18 Inequalities
Jordan’s Inequality
For more inequalities see Mitrinović (1964, pp. 101–111), Mitrinović (1970, pp. 235–265), and Bullen (1998, pp. 250–254).
15: 5.6 Inequalities
§5.6 Inequalities
Gautschi’s Inequality
Kershaw’s Inequality
16: 19.24 Inequalities
§19.24 Inequalities
§19.24(i) Complete Integrals
Other inequalities can be obtained by applying Carlson (1966, Theorems 2 and 3) to (19.16.20)–(19.16.23). …
§19.24(ii) Incomplete Integrals
17: Donald St. P. Richards
Richards has published numerous papers on special functions of matrix argument, harmonic analysis, multivariate statistical analysis, probability inequalities, and applied probability. …
18: 18.39 Applications in the Physical Sciences
Note that violation of the Favard inequality, l + 1 + ( 2 Z / s ) > 0 , possible when Z < 0 , results in a zero or negative weight function. … For applications and an extension of the Szegő–Szász inequality (18.14.20) for Legendre polynomials ( α = β = 0 ) to obtain global bounds on the variation of the phase of an elastic scattering amplitude, see Cornille and Martin (1972, 1974). …
19: 10.14 Inequalities; Monotonicity
§10.14 Inequalities; Monotonicity
Kapteyn’s Inequality
For inequalities for the function Γ ( ν + 1 ) ( 2 / x ) ν J ν ( x ) with ν > 1 2 see Neuman (2004). …
20: 13.22 Zeros