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31: 18.39 Applications in the Physical Sciences
The fundamental quantum Schrödinger operator, also called the Hamiltonian, , is a second order differential operator of the form … Analogous to (18.39.7) the 3D Schrödinger operator is …where L 2 is the (squared) angular momentum operator (14.30.12). … Here tridiagonal representations of simple Schrödinger operators play a similar role. The radial operator (18.39.28) …
32: Preface
 Stegun, editors); and to disseminate essentially the same information from a public website operated by NIST. … The Web pages contain many active links, for example, to the definitions of symbols within the DLMF, and to external sources of reviews, full texts of articles, and items of mathematical software. …
33: Bibliography L
  • S. Lai and Y. Chiu (1990) Exact computation of the 3 - j and 6 - j symbols. Comput. Phys. Comm. 61 (3), pp. 350–360.
  • S. Lai and Y. Chiu (1992) Exact computation of the 9 - j symbols. Comput. Phys. Comm. 70 (3), pp. 544–556.
  • L. Lapointe and L. Vinet (1996) Exact operator solution of the Calogero-Sutherland model. Comm. Math. Phys. 178 (2), pp. 425–452.
  • B. M. Levitan and I. S. Sargsjan (1975) Introduction to spectral theory: selfadjoint ordinary differential operators. Translations of Mathematical Monographs, Vol. 39, American Mathematical Society, Providence, R.I..
  • J. H. Luscombe and M. Luban (1998) Simplified recursive algorithm for Wigner 3 j and 6 j symbols. Phys. Rev. E 57 (6), pp. 7274–7277.
  • 34: 3.11 Approximation Techniques
    Here the single prime on the summation symbol means that the first term is to be halved. … δ k , being Kronecker’s symbol and the bar denoting complex conjugate. … In consequence of this structure the number of operations can be reduced to n m = n log 2 n operations. …
    35: 18.3 Definitions
  • 1.

    As eigenfunctions of second order differential operators (Bochner’s theorem, Bochner (1929)). See the differential equations A ( x ) p n ′′ ( x ) + B ( x ) p n ( x ) + λ n p n ( x ) = 0 , in Table 18.8.1.

  • 36: 18.27 q -Hahn Class
    The q -Hahn class OP’s comprise systems of OP’s { p n ( x ) } , n = 0 , 1 , , N , or n = 0 , 1 , 2 , , that are eigenfunctions of a second order q -difference operator. …In the q -Hahn class OP’s the role of the operator d / d x in the Jacobi, Laguerre, and Hermite cases is played by the q -derivative 𝒟 q , as defined in (17.2.41). …
    18.27.9 v x = ( a 1 x , c 1 x ; q ) ( x , b c 1 x ; q ) , 0 < a < q 1 , 0 < b < q 1 , c < 0 ,
    18.27.12 v x = ( q x / c , q x / d ; q ) ( q α + 1 x / c , q β + 1 x / d ; q ) , α , β > 1 , c , d > 0 .
    18.27.14_1 h n = ( a q ) n 1 a b q 2 n + 1 ( q , b q ; q ) n ( a q ; q ) n ( a b q n + 1 ; q ) ( a q ; q ) .
    37: 1.5 Calculus of Two or More Variables
    1.5.3 f x = D x f = f x = lim h 0 f ( x + h , y ) f ( x , y ) h ,
    1.5.4 f y = D y f = f y = lim h 0 f ( x , y + h ) f ( x , y ) h .
    For mathematicians the symbols θ and ϕ now are usually interchanged. …
    38: Bibliography S
  • I. J. Schwatt (1962) An Introduction to the Operations with Series. 2nd edition, Chelsea Publishing Co., New York.
  • J. Segura and A. Gil (1999) Evaluation of associated Legendre functions off the cut and parabolic cylinder functions. Electron. Trans. Numer. Anal. 9, pp. 137–146.
  • J. Shapiro (1970) Arbitrary 3 n j symbols for SU ( 2 ) . Comput. Phys. Comm. 1 (3), pp. 207–215.
  • B. Simon (1976) The Bound State of Weakly Coupled Schrödinger Operators in One and Two Dimensions. Annals of Physics 97 (2), pp. 279–288.
  • B. Simon (1995) Operators with Singular Continuous Spectrum: I. General Operators. Annals of Mathematics 141 (1), pp. 131–145.