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21: 2.1 Definitions and Elementary Properties
§2.1(i) Asymptotic and Order Symbols
As x c in 𝐗
2.1.2 f ( x ) = o ( ϕ ( x ) ) f ( x ) / ϕ ( x ) 0 .
§2.1(ii) Integration and Differentiation
Integration of asymptotic and order relations is permissible, subject to obvious convergence conditions. …
22: 10.64 Integral Representations
23: Bibliography Q
  • C. Quesne (2011) Higher-Order SUSY, Exactly Solvable Potentials, and Exceptional Orthogonal Polynomials. Modern Physics Letters A 26, pp. 1843–1852.
  • 24: 14.11 Derivatives with Respect to Degree or Order
    §14.11 Derivatives with Respect to Degree or Order
    14.11.3 𝖠 ν μ ( x ) = sin ( ν π ) ( 1 + x 1 x ) μ / 2 k = 0 ( 1 2 1 2 x ) k Γ ( k ν ) Γ ( k + ν + 1 ) k ! Γ ( k μ + 1 ) ( ψ ( k + ν + 1 ) ψ ( k ν ) ) .
    25: 24.14 Sums
    §24.14(i) Quadratic Recurrence Relations
    §24.14(ii) Higher-Order Recurrence Relations
    These identities can be regarded as higher-order recurrences. …
    26: 11.4 Basic Properties
    §11.4(i) Half-Integer Orders
    11.4.3 𝐇 n 1 2 ( z ) = ( 1 ) n J n + 1 2 ( z ) ,
    11.4.4 𝐋 n 1 2 ( z ) = I n + 1 2 ( z ) .
    §11.4(vi) Derivatives with Respect to Order
    For derivatives with respect to the order ν , see Apelblat (1989) and Brychkov and Geddes (2005). …
    27: 10.19 Asymptotic Expansions for Large Order
    §10.19 Asymptotic Expansions for Large Order
    §10.19(i) Asymptotic Forms
    §10.19(ii) Debye’s Expansions
    §10.19(iii) Transition Region
    See also §10.20(i).
    28: Need Help?
    We have also tried to use the best technologies available in order to make this information useful and accessible. …
    29: 11.7 Integrals and Sums
    11.7.1 z ν 𝐇 ν 1 ( z ) d z = z ν 𝐇 ν ( z ) ,
    11.7.3 z ν 𝐋 ν 1 ( z ) d z = z ν 𝐋 ν ( z ) ,
    11.7.5 f ν ( z ) = 0 z t ν 𝐇 ν ( t ) d t ,
    §11.7(iv) Integrals with Respect to Order
    For integrals of 𝐇 ν ( x ) and 𝐋 ν ( x ) with respect to the order ν , see Apelblat (1989). …
    30: 14.14 Continued Fractions
    14.14.1 1 2 ( x 2 1 ) 1 / 2 P ν μ ( x ) P ν μ 1 ( x ) = x 0 y 0 + x 1 y 1 + x 2 y 2 + ,
    14.14.3 ( ν μ ) Q ν μ ( x ) Q ν 1 μ ( x ) = x 0 y 0 x 1 y 1 x 2 y 2 , ν μ ,