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11: 26.13 Permutations: Cycle Notation
§26.13 Permutations: Cycle Notation
An explicit representation of σ can be given by the 2 × n matrix: … In cycle notation, the elements in each cycle are put inside parentheses, ordered so that σ ( j ) immediately follows j or, if j is the last listed element of the cycle, then σ ( j ) is the first element of the cycle. … is ( 1 , 3 , 2 , 5 , 7 ) ( 4 ) ( 6 , 8 ) in cycle notation. …They are often dropped from the cycle notation. …
12: 3.7 Ordinary Differential Equations
where 𝐀 ( τ , z ) is the matrix
3.7.6 𝐀 ( τ , z ) = [ A 11 ( τ , z ) A 12 ( τ , z ) A 21 ( τ , z ) A 22 ( τ , z ) ] ,
Let 𝐀 P be the ( 2 P ) × ( 2 P + 2 ) band matrix
3.7.13 𝐀 P 𝐰 = 𝐛 .
This converts the problem into a tridiagonal matrix problem in which the elements of the matrix are polynomials in λ ; compare §3.2(vi). …
13: 35.4 Partitions and Zonal Polynomials
For any partition κ , the zonal polynomial Z κ : 𝓢 is defined by the properties … Alternative notations for the zonal polynomials are C κ ( 𝐓 ) (Muirhead (1982, pp. 227–239)), 𝒴 κ ( 𝐓 ) (Takemura (1984, p. 22)), and Φ κ ( 𝐓 ) (Faraut and Korányi (1994, pp. 228–236)). …
14: Bibliography H
  • C. S. Herz (1955) Bessel functions of matrix argument. Ann. of Math. (2) 61 (3), pp. 474–523.
  • 15: 18.2 General Orthogonal Polynomials
    The matrix on the left-hand side is an (infinite tridiagonal) Jacobi matrix. This matrix is symmetric iff c n = a n 1 ( n 1 ). … With notation (18.2.4_5), (18.2.5), (18.2.7) … When the Jacobi matrix in (18.2.11_9) is truncated to an n × n matrix
    16: 1.1 Special Notation
    §1.1 Special Notation
    (For other notation see Notation for the Special Functions.)
    x , y real variables.
    𝐀 1 inverse of the square matrix 𝐀
    𝐈 identity matrix
    In the physics, applied maths, and engineering literature a common alternative to a ¯ is a , a being a complex number or a matrix; the Hermitian conjugate of 𝐀 is usually being denoted 𝐀 .
    17: 21.2 Definitions
    21.2.1 θ ( 𝐳 | 𝛀 ) = 𝐧 g e 2 π i ( 1 2 𝐧 𝛀 𝐧 + 𝐧 𝐳 ) .
    21.2.2 θ ^ ( 𝐳 | 𝛀 ) = e π [ 𝐳 ] [ 𝛀 ] 1 [ 𝐳 ] θ ( 𝐳 | 𝛀 ) .
    21.2.6 θ [ 𝜶 𝜷 ] ( 𝐳 | 𝛀 ) = e 2 π i ( 1 2 𝜶 𝛀 𝜶 + 𝜶 [ 𝐳 + 𝜷 ] ) θ ( 𝐳 + 𝛀 𝜶 + 𝜷 | 𝛀 ) ,
    21.2.7 θ [ 𝟎 𝟎 ] ( 𝐳 | 𝛀 ) = θ ( 𝐳 | 𝛀 ) .
    For g = 1 , and with the notation of §20.2(i), …
    18: Bibliography C
  • F. Cajori (1929) A History of Mathematical Notations, Volume II. Open Court Publishing Company, Chicago.
  • R. Campbell (1955) Théorie Générale de L’Équation de Mathieu et de quelques autres Équations différentielles de la mécanique. Masson et Cie, Paris (French).
  • L. Carlitz (1960) Note on Nörlund’s polynomial B n ( z ) . Proc. Amer. Math. Soc. 11 (3), pp. 452–455.
  • A. Csótó and G. M. Hale (1997) S -matrix and R -matrix determination of the low-energy He 5 and Li 5 resonance parameters. Phys. Rev. C 55 (1), pp. 536–539.
  • A. R. Curtis (1964a) Coulomb Wave Functions. Roy. Soc. Math. Tables, Vol. 11, Cambridge University Press, Cambridge.
  • 19: Mathematical Introduction
    Notation for the Special Functions
    This section may also include important alternative notations that have appeared in the literature. … The exceptions are ones for which the existing notations have drawbacks. … The Notations section includes all the notations for the special functions adopted in this Handbook. …
    Common Notations and Definitions
    20: 18.39 Applications in the Physical Sciences
    This is also the normalization and notation of Chapter 33 for Z = 1 , and the notation of Weinberg (2013, Chapter 2). … , the J-matrix elements) as in Gautschi (1968), Golub and Welsch (1969), Gordon (1968). …
    §18.39(iv) Coulomb–Pollaczek Polynomials and J-Matrix Methods
    Discretized and Continuum Expansions of Scattering Eigenfunctions in terms of Pollaczek Polynomials: J-matrix Theory
    As this follows from the three term recursion of (18.39.46) it is referred to as the J-Matrix approach, see (3.5.31), to single and multi-channel scattering numerics. …