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11: 16.24 Physical Applications
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. …
12: 35.5 Bessel Functions of Matrix Argument
35.5.5 𝟎 < 𝐗 < 𝐓 A ν 1 ( 𝐒 1 𝐗 ) | 𝐗 | ν 1 A ν 2 ( 𝐒 2 ( 𝐓 𝐗 ) ) | 𝐓 𝐗 | ν 2 d 𝐗 = | 𝐓 | ν 1 + ν 2 + 1 2 ( m + 1 ) A ν 1 + ν 2 + 1 2 ( m + 1 ) ( ( 𝐒 1 + 𝐒 2 ) 𝐓 ) , ν j , ( ν j ) > 1 , j = 1 , 2 ; 𝐒 1 , 𝐒 2 𝓢 ; 𝐓 𝛀 .
13: 1.2 Elementary Algebra
Multiplication of Matrices
§1.2(vi) Square Matrices
Special Forms of Square Matrices
Norms of Square Matrices
Non-Defective Square Matrices
14: 29.18 Mathematical Applications
§29.18(iv) Other Applications
Patera and Winternitz (1973) finds bases for the rotation group.
15: 4.29 Graphics
The conformal mapping w = sinh z is obtainable from Figure 4.15.7 by rotating both the w -plane and the z -plane through an angle 1 2 π , compare (4.28.8). …
16: 35.3 Multivariate Gamma and Beta Functions
35.3.2 Γ m ( s 1 , , s m ) = 𝛀 etr ( 𝐗 ) | 𝐗 | s m 1 2 ( m + 1 ) j = 1 m 1 | ( 𝐗 ) j | s j s j + 1 d 𝐗 , s j , ( s j ) > 1 2 ( j 1 ) , j = 1 , , m .
35.3.3 B m ( a , b ) = 𝟎 < 𝐗 < 𝐈 | 𝐗 | a 1 2 ( m + 1 ) | 𝐈 𝐗 | b 1 2 ( m + 1 ) d 𝐗 , ( a ) , ( b ) > 1 2 ( m 1 ) .
17: Bille C. Carlson
In theoretical physics he is known for the “Carlson-Keller Orthogonalization”, published in 1957, Orthogonalization Procedures and the Localization of Wannier Functions, and the “Carlson-Keller Theorem”, published in 1961, Eigenvalues of Density Matrices. …
18: 21.1 Special Notation
g , h positive integers.
g × h set of all g × h matrices with integer elements.
Uppercase boldface letters are g × g real or complex matrices. …
19: 35.2 Laplace Transform
35.2.1 g ( 𝐙 ) = 𝛀 etr ( 𝐙 𝐗 ) f ( 𝐗 ) d 𝐗 ,
35.2.3 f 1 f 2 ( 𝐓 ) = 𝟎 < 𝐗 < 𝐓 f 1 ( 𝐓 𝐗 ) f 2 ( 𝐗 ) d 𝐗 .
20: 21.6 Products
21.6.1 𝒦 = g × h 𝐓 / ( g × h 𝐓 g × h ) ,
that is, 𝒦 is the set of all g × h matrices that are obtained by premultiplying 𝐓 by any g × h matrix with integer elements; two such matrices in 𝒦 are considered equivalent if their difference is a matrix with integer elements. …
21.6.3 j = 1 h θ ( k = 1 h T j k 𝐳 k | 𝛀 ) = 1 𝒟 g 𝐀 𝒦 𝐁 𝒦 e 2 π i tr [ 1 2 𝐀 T 𝛀 𝐀 + 𝐀 T [ 𝐙 + 𝐁 ] ] j = 1 h θ ( 𝐳 j + 𝛀 𝐚 j + 𝐛 j | 𝛀 ) ,
21.6.4 j = 1 h θ [ k = 1 h T j k 𝐜 k k = 1 h T j k 𝐝 k ] ( k = 1 h T j k 𝐳 k | 𝛀 ) = 1 𝒟 g 𝐀 𝒦 𝐁 𝒦 e 2 π i j = 1 h 𝐛 j 𝐜 j j = 1 h θ [ 𝐚 j + 𝐜 j 𝐛 j + 𝐝 j ] ( 𝐳 j | 𝛀 ) ,