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11: Nico M. Temme
  • In November 2015, Temme was named Senior Associate Editor of the DLMF and Associate Editor for Chapters 3, 6, 7, and 12.
    12: 16.24 Physical Applications
    §16.24(iii) 3 j , 6 j , and 9 j Symbols
    The 3 j symbols, or Clebsch–Gordan coefficients, play an important role in the decomposition of reducible representations of the rotation group into irreducible representations. They can be expressed as F 2 3 functions with unit argument. The coefficients of transformations between different coupling schemes of three angular momenta are related to the Wigner 6 j symbols. These are balanced F 3 4 functions with unit argument. …
    13: 34.5 Basic Properties: 6 j Symbol
    §34.5 Basic Properties: 6 j Symbol
    §34.5(ii) Symmetry
    §34.5(iv) Orthogonality
    §34.5(vi) Sums
    Equation (34.5.23) can be regarded as an alternative definition of the 6 j symbol. …
    14: 34.12 Physical Applications
    §34.12 Physical Applications
    The angular momentum coupling coefficients ( 3 j , 6 j , and 9 j symbols) are essential in the fields of nuclear, atomic, and molecular physics. … 3 j , 6 j , and 9 j symbols are also found in multipole expansions of solutions of the Laplace and Helmholtz equations; see Carlson and Rushbrooke (1950) and Judd (1976).
    15: 26.10 Integer Partitions: Other Restrictions
    p ( 𝒟 3 , n ) denotes the number of partitions of n into parts with difference at least 3, except that multiples of 3 must differ by at least 6. …The set { 2 , 3 , 4 , } is denoted by T . … where the sum is over nonnegative integer values of k for which n 1 2 ( 3 k 2 ± k ) 0 . … Note that p ( 𝒟 3 , n ) p ( 𝒟 3 , n ) , with strict inequality for n 9 . It is known that for k > 3 , p ( 𝒟 k , n ) p ( A 1 , k + 3 , n ) , with strict inequality for n sufficiently large, provided that k = 2 m 1 , m = 3 , 4 , 5 , or k 32 ; see Yee (2004). …
    16: 24.2 Definitions and Generating Functions
    Table 24.2.5: Coefficients b n , k of the Bernoulli polynomials B n ( x ) = k = 0 n b n , k x k .
    k
    n 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
    12 691 2730 0 5 0 33 2 0 22 0 33 2 0 11 6 1
    Table 24.2.6: Coefficients e n , k of the Euler polynomials E n ( x ) = k = 0 n e n , k x k .
    k
    n 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
    6 0 3 0 5 0 3 1
    12 0 2073 0 3410 0 1683 0 396 0 55 0 6 1
    17: 26.9 Integer Partitions: Restricted Number and Part Size
    Figure 26.9.1: Ferrers graph of the partition 7 + 4 + 3 + 3 + 2 + 1 .
    The conjugate to the example in Figure 26.9.1 is 6 + 5 + 4 + 2 + 1 + 1 + 1 . … Equations (26.9.2)–(26.9.3) are examples of closed forms that can be computed explicitly for any positive integer k . …
    p 3 ( n ) = 1 + n 2 + 6 n 12 .
    equivalently, partitions into at most k parts either have exactly k parts, in which case we can subtract one from each part, or they have strictly fewer than k parts. …
    18: 28.6 Expansions for Small q
    Leading terms of the power series for a m ( q ) and b m ( q ) for m 6 are: … Higher coefficients in the foregoing series can be found by equating coefficients in the following continued-fraction equations: … Here j = 1 for a 2 n ( q ) , j = 2 for b 2 n + 2 ( q ) , and j = 3 for a 2 n + 1 ( q ) and b 2 n + 1 ( q ) . … For m = 3 , 4 , 5 , , … For the corresponding expansions of se m ( z , q ) for m = 3 , 4 , 5 , change cos to sin everywhere in (28.6.26). …
    19: 34.7 Basic Properties: 9 j Symbol
    34.7.1 { j 11 j 12 j 13 j 21 j 22 j 13 j 31 j 31 0 } = ( 1 ) j 12 + j 21 + j 13 + j 31 ( ( 2 j 13 + 1 ) ( 2 j 31 + 1 ) ) 1 2 { j 11 j 12 j 13 j 22 j 21 j 31 } .
    34.7.2 j 12 j 34 ( 2 j 12 + 1 ) ( 2 j 34 + 1 ) ( 2 j 13 + 1 ) ( 2 j 24 + 1 ) { j 1 j 2 j 12 j 3 j 4 j 34 j 13 j 24 j } { j 1 j 2 j 12 j 3 j 4 j 34 j 13 j 24 j } = δ j 13 , j 13 δ j 24 , j 24 .
    34.7.3 j 13 j 24 ( 1 ) 2 j 2 + j 24 + j 23 j 34 ( 2 j 13 + 1 ) ( 2 j 24 + 1 ) { j 1 j 2 j 12 j 3 j 4 j 34 j 13 j 24 j } { j 1 j 3 j 13 j 4 j 2 j 24 j 14 j 23 j } = { j 1 j 2 j 12 j 4 j 3 j 34 j 14 j 23 j } .
    34.7.4 ( j 13 j 23 j 33 m 13 m 23 m 33 ) { j 11 j 12 j 13 j 21 j 22 j 23 j 31 j 32 j 33 } = m r 1 , m r 2 , r = 1 , 2 , 3 ( j 11 j 12 j 13 m 11 m 12 m 13 ) ( j 21 j 22 j 23 m 21 m 22 m 23 ) ( j 31 j 32 j 33 m 31 m 32 m 33 ) ( j 11 j 21 j 31 m 11 m 21 m 31 ) ( j 12 j 22 j 32 m 12 m 22 m 32 ) .
    34.7.5 j ( 2 j + 1 ) { j 11 j 12 j j 21 j 22 j 23 j 31 j 32 j 33 } { j 11 j 12 j j 23 j 33 j } = ( 1 ) 2 j { j 21 j 22 j 23 j 12 j j 32 } { j 31 j 32 j 33 j j 11 j 21 } .
    20: 23.20 Mathematical Applications
    Points P = ( x , y ) on the curve can be parametrized by x = ( z ; g 2 , g 3 ) , 2 y = ( z ; g 2 , g 3 ) , where g 2 = 4 a and g 3 = 4 b : in this case we write P = P ( z ) . … The geometric nature of this construction is illustrated in McKean and Moll (1999, §2.14), Koblitz (1993, §§6, 7), and Silverman and Tate (1992, Chapter 1, §§3, 4): each of these references makes a connection with the addition theorem (23.10.1). … T must have one of the forms / ( n ) , 1 n 10 or n = 12 , or ( / ( 2 ) ) × ( / ( 2 n ) ) , 1 n 4 . …The order of a point (if finite and not already determined) can have only the values 3, 5, 6, 7, 9, 10, or 12, and so can be found from 2 P = P , 4 P = P , 4 P = 2 P , 8 P = P , 8 P = P , 8 P = 2 P , or 8 P = 4 P . … See also Silverman and Tate (1992), Serre (1973, Part 2, Chapters 6, 7), Koblitz (1993), and Cornell et al. (1997). …