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11: 24.4 Basic Properties
§24.4(iv) Finite Expansions
24.4.31 B n ( 1 4 ) = ( 1 ) n B n ( 3 4 ) = 1 2 1 n 2 n B n n 4 n E n 1 , n = 1 , 2 , .
Let P ( x ) denote any polynomial in x , and after expanding set ( B ( x ) ) n = B n ( x ) and ( E ( x ) ) n = E n ( x ) . …
§24.4(ix) Relations to Other Functions
For the relation of Bernoulli numbers to the Riemann zeta function see §25.6, and to the Eulerian numbers see (26.14.11).
12: Foreword
22 2 D. R. Lide (ed.), A Century of Excellence in Measurement, Standards, and Technology, CRC Press, 2001. The success of the original handbook, widely referred to as “Abramowitz and Stegun” (“A&S”), derived not only from the fact that it provided critically useful scientific data in a highly accessible format, but also because it served to standardize definitions and notations for special functions. … Particular attention is called to the generous support of the National Science Foundation, which made possible the participation of experts from academia and research institutes worldwide. …
13: 24.10 Arithmetic Properties
§24.10 Arithmetic Properties
The denominator of B 2 n is the product of all these primes p . …
§24.10(ii) Kummer Congruences
Let B 2 n = N 2 n / D 2 n , with N 2 n and D 2 n relatively prime and D 2 n > 0 . …
§24.10(iv) Factors
14: Viewing DLMF Interactive 3D Graphics
WebGL is supported in the current versions of most common web browsers. … 1, some advanced features of X3DOM are currently not fully supported (see x3dom.org). …If you have trouble viewing the WebGL visualizations in your web browser, see x3dom.org or caniuse.com/webgl for information on WebGL browser support. … Please see caniuse.com/webgl or x3dom.org for information on WebGL browser support.
15: 35 Functions of Matrix Argument
16: Gloria Wiersma
 1937 in Washington, DC) joined the NIST staff in 1973, where she occupied various positions providing support for the Physics Laboratory until 1993. …
17: 24.5 Recurrence Relations
§24.5 Recurrence Relations
§24.5(ii) Other Identities
24.5.6 k = 2 n ( n k 2 ) B k k = 1 ( n + 1 ) ( n + 2 ) B n + 1 , n = 2 , 3 , ,
24.5.8 k = 0 n 2 2 k B 2 k ( 2 k ) ! ( 2 n + 1 2 k ) ! = 1 ( 2 n ) ! , n = 1 , 2 , .
§24.5(iii) Inversion Formulas
18: Bibliography Y
  • K. Yang and M. de Llano (1989) Simple Variational Proof That Any Two-Dimensional Potential Well Supports at Least One Bound State. American Journal of Physics 57 (1), pp. 85–86.
  • A. Yu. Yeremin, I. E. Kaporin, and M. K. Kerimov (1985) The calculation of the Riemann zeta function in the complex domain. USSR Comput. Math. and Math. Phys. 25 (2), pp. 111–119.
  • F. L. Yost, J. A. Wheeler, and G. Breit (1936) Coulomb wave functions in repulsive fields. Phys. Rev. 49 (2), pp. 174–189.
  • 19: 24.6 Explicit Formulas
    §24.6 Explicit Formulas
    The identities in this section hold for n = 1 , 2 , . …
    24.6.1 B 2 n = k = 2 2 n + 1 ( 1 ) k 1 k ( 2 n + 1 k ) j = 1 k 1 j 2 n ,
    24.6.3 B 2 n = k = 1 n ( k 1 ) ! k ! ( 2 k + 1 ) ! j = 1 k ( 1 ) j 1 ( 2 k k + j ) j 2 n .
    24.6.11 B n = n 2 n ( 2 n 1 ) k = 1 n j = 0 k 1 ( 1 ) j + 1 ( n k ) j n 1 ,
    20: 24.9 Inequalities
    §24.9 Inequalities
    Except where otherwise noted, the inequalities in this section hold for n = 1 , 2 , . …
    24.9.2 ( 2 2 1 2 n ) | B 2 n | | B 2 n ( x ) B 2 n | , 1 x 0 .
    (24.9.3)–(24.9.5) hold for 1 2 > x > 0 . … (24.9.6)–(24.9.7) hold for n = 2 , 3 , . …