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21: 28.12 Definitions and Basic Properties
They have the following pseudoperiodic and orthogonality properties: …
22: 9.13 Generalized Airy Functions
Properties and graphs of U m ( t ) , V m ( t ) , V ¯ m ( t ) are included in Olver (1977a) together with properties and graphs of real solutions of the equation …
23: 4.37 Inverse Hyperbolic Functions
4.37.6 Arccoth z = Arctanh ( 1 / z ) .
§4.37(v) Fundamental Property
With k , the general solutions of the equations …
24: 4.23 Inverse Trigonometric Functions
4.23.6 Arccot z = Arctan ( 1 / z ) .
§4.23(v) Fundamental Property
With k , the general solutions of the equations …
25: Bibliography F
  • A. S. Fokas and Y. C. Yortsos (1981) The transformation properties of the sixth Painlevé equation and one-parameter families of solutions. Lett. Nuovo Cimento (2) 30 (17), pp. 539–544.
  • 26: 9.12 Scorer Functions
    The general solution is given by …Standard particular solutions are …
    §9.12(iv) Numerically Satisfactory Solutions
    In , numerically satisfactory sets of solutions are given by … For the above properties and further results, including the distribution of complex zeros, asymptotic approximations for the numerically large real or complex zeros, and numerical tables see Gil et al. (2003c). …
    27: 9.16 Physical Applications
    Again, the quest for asymptotic approximations that are uniformly valid solutions to this equation in the neighborhoods of critical points leads (after choosing solvable equations with similar asymptotic properties) to Airy functions. …
    28: 13.2 Definitions and Basic Properties
    Another standard solution of (13.2.1) is U ( a , b , z ) , which is determined uniquely by the property
    29: 10.47 Definitions and Basic Properties
    §10.47 Definitions and Basic Properties
    §10.47(ii) Standard Solutions
    §10.47(iii) Numerically Satisfactory Pairs of Solutions
    For (10.47.1) numerically satisfactory pairs of solutions are given by Table 10.2.1 with the symbols J , Y , H , and ν replaced by 𝗃 , 𝗒 , 𝗁 , and n , respectively. …
    30: 31.8 Solutions via Quadratures
    §31.8 Solutions via Quadratures
    are two independent solutions of (31.2.1). … The curve Γ reflects the finite-gap property of Equation (31.2.1) when the exponent parameters satisfy (31.8.1) for m j . …For more details see Smirnov (2002). The solutions in this section are finite-term Liouvillean solutions which can be constructed via Kovacic’s algorithm; see §31.14(ii).