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21: 34.5 Basic Properties: 6 j Symbol
34.5.6 { j 1 j 2 j 3 1 j 3 1 j 2 + 1 } = ( 1 ) J ( ( J 2 j 2 1 ) ( J 2 j 2 ) ( J 2 j 3 + 1 ) ( J 2 j 3 + 2 ) ( 2 j 2 + 1 ) ( 2 j 2 + 2 ) ( 2 j 2 + 3 ) ( 2 j 3 1 ) 2 j 3 ( 2 j 3 + 1 ) ) 1 2 ,
34.5.9 { j 1 j 2 j 3 l 1 l 2 l 3 } = { j 1 1 2 ( j 2 + l 2 + j 3 l 3 ) 1 2 ( j 2 l 2 + j 3 + l 3 ) l 1 1 2 ( j 2 + l 2 j 3 + l 3 ) 1 2 ( j 2 + l 2 + j 3 + l 3 ) } ,
34.5.14 j 3 ( 2 j 3 + 1 ) ( 2 l 3 + 1 ) { j 1 j 2 j 3 l 1 l 2 l 3 } { j 1 j 2 j 3 l 1 l 2 l 3 } = δ l 3 , l 3 .
34.5.16 ( 1 ) j 1 + j 2 + j 3 + j 1 + j 2 + l 1 + l 2 { j 1 j 2 j 3 l 1 l 2 l 3 } { j 1 j 2 j 3 l 1 l 2 l 3 } = j ( 1 ) l 3 + l 3 + j ( 2 j + 1 ) { j 1 j 1 j j 2 j 2 j 3 } { l 3 l 3 j j 1 j 1 l 2 } { l 3 l 3 j j 2 j 2 l 1 } .
34.5.23 ( j 1 j 2 j 3 m 1 m 2 m 3 ) { j 1 j 2 j 3 l 1 l 2 l 3 } = m 1 m 2 m 3 ( 1 ) l 1 + l 2 + l 3 + m 1 + m 2 + m 3 ( j 1 l 2 l 3 m 1 m 2 m 3 ) ( l 1 j 2 l 3 m 1 m 2 m 3 ) ( l 1 l 2 j 3 m 1 m 2 m 3 ) .
22: 34.4 Definition: 6 j Symbol
§34.4 Definition: 6 j Symbol
The 6 j symbol is defined by the following double sum of products of 3 j symbols: …where the summation is taken over all admissible values of the m ’s and m ’s for each of the four 3 j symbols; compare (34.2.2) and (34.2.3). Except in degenerate cases the combination of the triangle inequalities for the four 3 j symbols in (34.4.1) is equivalent to the existence of a tetrahedron (possibly degenerate) with edges of lengths j 1 , j 2 , j 3 , l 1 , l 2 , l 3 ; see Figure 34.4.1. … where F 3 4 is defined as in §16.2. …
23: 34.1 Special Notation
The main functions treated in this chapter are the Wigner 3 j , 6 j , 9 j symbols, respectively,
( j 1 j 2 j 3 m 1 m 2 m 3 ) ,
{ j 1 j 2 j 3 l 1 l 2 l 3 } ,
An often used alternative to the 3 j symbol is the Clebsch–Gordan coefficient …For other notations for 3 j , 6 j , 9 j symbols, see Edmonds (1974, pp. 52, 97, 104–105) and Varshalovich et al. (1988, §§8.11, 9.10, 10.10).
24: 34.10 Zeros
§34.10 Zeros
In a 3 j symbol, if the three angular momenta j 1 , j 2 , j 3 do not satisfy the triangle conditions (34.2.1), or if the projective quantum numbers do not satisfy (34.2.3), then the 3 j symbol is zero. Similarly the 6 j symbol (34.4.1) vanishes when the triangle conditions are not satisfied by any of the four 3 j symbols in the summation. …However, the 3 j and 6 j symbols may vanish for certain combinations of the angular momenta and projective quantum numbers even when the triangle conditions are fulfilled. …
25: 34.8 Approximations for Large Parameters
§34.8 Approximations for Large Parameters
For large values of the parameters in the 3 j , 6 j , and 9 j symbols, different asymptotic forms are obtained depending on which parameters are large. …
34.8.1 { j 1 j 2 j 3 j 2 j 1 l 3 } = ( 1 ) j 1 + j 2 + j 3 + l 3 ( 4 π ( 2 j 1 + 1 ) ( 2 j 2 + 1 ) ( 2 l 3 + 1 ) sin θ ) 1 2 ( cos ( ( l 3 + 1 2 ) θ 1 4 π ) + o ( 1 ) ) , j 1 , j 2 , j 3 l 3 1 ,
Uniform approximations in terms of Airy functions for the 3 j and 6 j symbols are given in Schulten and Gordon (1975b). For approximations for the 3 j , 6 j , and 9 j symbols with error bounds see Flude (1998), Chen et al. (1999), and Watson (1999): these references also cite earlier work.
26: 22.9 Cyclic Identities
22.9.10 d 1 , 3 ( 2 ) d 2 , 3 ( 2 ) + d 2 , 3 ( 2 ) d 3 , 3 ( 2 ) + d 3 , 3 ( 2 ) d 1 , 3 ( 2 ) = d 1 , 3 ( 4 ) d 2 , 3 ( 4 ) + d 2 , 3 ( 4 ) d 3 , 3 ( 4 ) + d 3 , 3 ( 4 ) d 1 , 3 ( 4 ) = κ ( κ + 2 ) .
§22.9(iii) Typical Identities of Rank 3
22.9.13 s 1 , 3 ( 4 ) s 2 , 3 ( 4 ) s 3 , 3 ( 4 ) = 1 1 κ 2 ( s 1 , 3 ( 4 ) + s 2 , 3 ( 4 ) + s 3 , 3 ( 4 ) ) ,
22.9.22 s 1 , 3 ( 2 ) c 1 , 3 ( 2 ) d 2 , 3 ( 2 ) d 3 , 3 ( 2 ) + s 2 , 3 ( 2 ) c 2 , 3 ( 2 ) d 3 , 3 ( 2 ) d 1 , 3 ( 2 ) + s 3 , 3 ( 2 ) c 3 , 3 ( 2 ) d 1 , 3 ( 2 ) d 2 , 3 ( 2 ) = κ 2 + k 2 1 1 κ 2 ( s 1 , 3 ( 2 ) c 1 , 3 ( 2 ) + s 2 , 3 ( 2 ) c 2 , 3 ( 2 ) + s 3 , 3 ( 2 ) c 3 , 3 ( 2 ) ) ,
22.9.23 s 1 , 3 ( 4 ) d 1 , 3 ( 4 ) c 2 , 3 ( 4 ) c 3 , 3 ( 4 ) + s 2 , 3 ( 4 ) d 2 , 3 ( 4 ) c 3 , 3 ( 4 ) c 1 , 3 ( 4 ) + s 3 , 3 ( 4 ) d 3 , 3 ( 4 ) c 1 , 3 ( 4 ) c 2 , 3 ( 4 ) = κ 2 1 κ 2 ( s 1 , 3 ( 4 ) d 1 , 3 ( 4 ) + s 2 , 3 ( 4 ) d 2 , 3 ( 4 ) + s 2 , 3 ( 4 ) d 2 , 3 ( 4 ) ) .
27: 3 Numerical Methods
Chapter 3 Numerical Methods
28: 4.43 Cubic Equations
A = ( 4 3 p ) 1 / 2 ,
B = ( 4 3 p ) 1 / 2 .
  • (a)

    A sin a , A sin ( a + 2 3 π ) , and A sin ( a + 4 3 π ) , with sin ( 3 a ) = 4 q / A 3 , when 4 p 3 + 27 q 2 0 .

  • (b)

    A cosh a , A cosh ( a + 2 3 π i ) , and A cosh ( a + 4 3 π i ) , with cosh ( 3 a ) = 4 q / A 3 , when p < 0 , q < 0 , and 4 p 3 + 27 q 2 > 0 .

  • (c)

    B sinh a , B sinh ( a + 2 3 π i ) , and B sinh ( a + 4 3 π i ) , with sinh ( 3 a ) = 4 q / B 3 , when p > 0 .

  • 29: 7.3 Graphics
    See accompanying text
    Figure 7.3.1: Complementary error functions erfc x and erfc ( 10 x ) , 3 x 3 . Magnify
    See accompanying text
    Figure 7.3.5: | erf ( x + i y ) | , 3 x 3 , 3 y 3 . … Magnify 3D Help
    See accompanying text
    Figure 7.3.6: | erfc ( x + i y ) | , 3 x 3 , 3 y 3 . … Magnify 3D Help
    30: 23.5 Special Lattices
    Then Δ > 0 and the parallelogram with vertices at 0 , 2 ω 1 , 2 ω 1 + 2 ω 3 , 2 ω 3 is a rectangle. … Also, e 2 and g 3 have opposite signs unless ω 3 = i ω 1 , in which event both are zero. As functions of ω 3 , e 1 and e 2 are decreasing and e 3 is increasing. … The parallelogram 0 , 2 ω 1 , 2 ω 1 + 2 ω 3 , 2 ω 3 is a square, and … The parallelogram 0 , 2 ω 1 2 ω 3 , 2 ω 1 , 2 ω 3 , is a rhombus: see Figure 23.5.1. …