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formally self adjoint linear operator

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11: 3.10 Continued Fractions
Every convergent, asymptotic, or formal series … We say that it corresponds to the formal power series … We say that it is associated with the formal power series f ( z ) in (3.10.7) if the expansion of its n th convergent C n in ascending powers of z , agrees with (3.10.7) up to and including the term in z 2 n 1 , n = 1 , 2 , 3 , . … ( is the backward difference operator.) …
12: 16.11 Asymptotic Expansions
§16.11(i) Formal Series
For subsequent use we define two formal infinite series, E p , q ( z ) and H p , q ( z ) , as follows:
16.11.1 E p , q ( z ) = ( 2 π ) ( p q ) / 2 κ ν ( 1 / 2 ) e κ z 1 / κ k = 0 c k ( κ z 1 / κ ) ν k , p < q + 1 ,
16.11.2 H p , q ( z ) = m = 1 p k = 0 ( 1 ) k k ! Γ ( a m + k ) ( = 1 m p Γ ( a a m k ) / = 1 q Γ ( b a m k ) ) z a m k .
The formal series (16.11.2) for H q + 1 , q ( z ) converges if | z | > 1 , and …
13: 1.17 Integral and Series Representations of the Dirac Delta
Formal interchange of the order of integration in the Fourier integral formula ((1.14.1) and (1.14.4)): …Then comparison of (1.17.2) and (1.17.9) yields the formal integral representation … In the language of physics and applied mathematics, these equations indicate the normalizations chosen for these non- L 2 improper eigenfunctions of the differential operators (with derivatives respect to spatial co-ordinates) which generate them; the normalizations (1.17.12_1) and (1.17.12_2) are explicitly derived in Friedman (1990, Ch. 4), the others follow similarly. … Formal interchange of the order of summation and integration in the Fourier summation formula ((1.8.3) and (1.8.4)): … By analogy with §1.17(ii) we have the formal series representation …
14: How to Cite
When citing DLMF from a formal publication, we suggest a format similar to the following: …
15: Bibliography K
  • A. A. Kapaev (2004) Quasi-linear Stokes phenomenon for the Painlevé first equation. J. Phys. A 37 (46), pp. 11149–11167.
  • E. H. Kaufman and T. D. Lenker (1986) Linear convergence and the bisection algorithm. Amer. Math. Monthly 93 (1), pp. 48–51.
  • T. H. Koornwinder (2006) Lowering and Raising Operators for Some Special Orthogonal Polynomials. In Jack, Hall-Littlewood and Macdonald Polynomials, Contemp. Math., Vol. 417, pp. 227–238.
  • J. J. Kovacic (1986) An algorithm for solving second order linear homogeneous differential equations. J. Symbolic Comput. 2 (1), pp. 3–43.
  • S. G. Krivoshlykov (1994) Quantum-Theoretical Formalism for Inhomogeneous Graded-Index Waveguides. Akademie Verlag, Berlin-New York.
  • 16: DLMF Project News
    error generating summary
    17: 10.70 Zeros
    Let μ = 4 ν 2 and f ( t ) denote the formal series …
    18: Bibliography B
  • A. W. Babister (1967) Transcendental Functions Satisfying Nonhomogeneous Linear Differential Equations. The Macmillan Co., New York.
  • P. M. Batchelder (1967) An Introduction to Linear Difference Equations. Dover Publications Inc., New York.
  • L. J. Billera, C. Greene, R. Simion, and R. P. Stanley (Eds.) (1996) Formal Power Series and Algebraic Combinatorics. DIMACS Series in Discrete Mathematics and Theoretical Computer Science, Vol. 24, American Mathematical Society, Providence, RI.
  • R. Blackmore and B. Shizgal (1985) Discrete ordinate solution of Fokker-Planck equations with non-linear coefficients. Phys. Rev. A 31 (3), pp. 1855–1868.
  • C. Brezinski (1999) Error estimates for the solution of linear systems. SIAM J. Sci. Comput. 21 (2), pp. 764–781.
  • 19: 2.3 Integrals of a Real Variable
    In both cases the n th error term is bounded in absolute value by x n 𝒱 a , b ( q ( n 1 ) ( t ) ) , where the variational operator 𝒱 a , b is defined by
    2.3.6 𝒱 a , b ( f ( t ) ) = a b | f ( t ) | d t ;
    Then the series obtained by substituting (2.3.7) into (2.3.1) and integrating formally term by term yields an asymptotic expansion: … The desired uniform expansion is then obtained formally as in Watson’s lemma and Laplace’s method. …
    20: 18.2 General Orthogonal Polynomials
    §18.2(ii) x -Difference Operators
    It is to be noted that, although formally correct, the results of (18.2.30) are of little utility for numerical work, as Hankel determinants are notoriously ill-conditioned. … where f ( t ) and u ( t ) are formal power series in t , with f ( 0 ) = 1 , u ( 0 ) = 0 and u ( 0 ) = 1 . …If v ( s ) is the formal power series such that v ( u ( t ) ) = t then a property equivalent to (18.2.45) with c n = 1 is that … …