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Lanczos vectors

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21: 31.17 Physical Applications
We use vector notation [ 𝐬 , 𝐭 , 𝐮 ] (respective scalar ( s , t , u ) ) for any one of the three spin operators (respective spin values). …
22: 1.16 Distributions
1.16.30 𝐃 = ( 1 i x 1 , 1 i x 2 , , 1 i x n ) .
1.16.32 P ( 𝐃 ) = 𝜶 c 𝜶 𝐃 α = 𝜶 c 𝜶 ( 1 i x 1 ) α 1 ( 1 i x n ) α n .
1.16.33 ( P ( 𝐃 ) ϕ ) ( 𝐱 ) = P ( 𝐱 ) ϕ ( 𝐱 ) ,
1.16.36 ( P ( 𝐃 ) u ) , ϕ = P ( u ) , ϕ = ( u ) , P ϕ ,
1.16.37 ( P u ) , ϕ = P ( 𝐃 ) ( u ) , ϕ ,
23: Bibliography D
  • H. F. Davis and A. D. Snider (1987) Introduction to Vector Analysis. 5th edition, Allyn and Bacon Inc., Boston, MA.
  • R. McD. Dodds and G. Wiechers (1972) Vector coupling coefficients as products of prime factors. Comput. Phys. Comm. 4 (2), pp. 268–274.
  • 24: 3.5 Quadrature
    The monic and orthonormal recursion relations of this section are both closely related to the Lanczos recursion relation in §3.2(vi). …
    25: Bibliography H
  • J. H. Hubbard and B. B. Hubbard (2002) Vector Calculus, Linear Algebra, and Differential Forms: A Unified Approach. 2nd edition, Prentice Hall Inc., Upper Saddle River, NJ.
  • 26: 35.5 Bessel Functions of Matrix Argument
    27: Bibliography K
  • T. H. Koornwinder and F. Bouzeffour (2011) Nonsymmetric Askey-Wilson polynomials as vector-valued polynomials. Appl. Anal. 90 (3-4), pp. 731–746.
  • 28: Bibliography L
  • A. E. Lynas-Gray (1993) VOIGTL – A fast subroutine for Voigt function evaluation on vector processors. Comput. Phys. Comm. 75 (1-2), pp. 135–142.
  • 29: 1.11 Zeros of Polynomials
    where the column vector h k ( m ) consists of the first k members of the sequence a m , a m 1 , a m 2 , with a j = 0 if j < 0 or j > n . …
    30: 35.6 Confluent Hypergeometric Functions of Matrix Argument