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31: Guide to Searching the DLMF
Table 1: Query Examples
Query Matching records contain
J_n@(z)= the math fragment J n ( z ) = , emphasizing more that J n is a function.
Wildcards allow matching patterns and marking parts of an expression that don’t matter (as for example, which variable name the author uses for a function): … You can use in math queries all the symbols and commands defined in  (you can omit the \ ), and some additional convenient ones, as well as the special functions’ names: … The syntax of the special functions can be -like or as employed in widely used computer algebra systems. … DLMF search is generally case-insensitive except when it is important to be case-sensitive, as when two different special functions have the same standard names but one name has a lower-case initial and the other is has an upper-case initial, such as si and Si, gamma and Gamma. …
32: 29.20 Methods of Computation
The eigenvalues a ν m ( k 2 ) , b ν m ( k 2 ) , and the Lamé functions 𝐸𝑐 ν m ( z , k 2 ) , 𝐸𝑠 ν m ( z , k 2 ) , can be calculated by direct numerical methods applied to the differential equation (29.2.1); see §3.7. … A third method is to approximate eigenvalues and Fourier coefficients of Lamé functions by eigenvalues and eigenvectors of finite matrices using the methods of §§3.2(vi) and 3.8(iv). …
33: Bibliography E
  • Á. Elbert and A. Laforgia (1994) Interlacing properties of the zeros of Bessel functions. Atti Sem. Mat. Fis. Univ. Modena XLII (2), pp. 525–529.
  • Á. Elbert and A. Laforgia (2008) The zeros of the complementary error function. Numer. Algorithms 49 (1-4), pp. 153–157.
  • A. Erdélyi (1941b) On Lamé functions. Philos. Mag. (7) 31, pp. 123–130.
  • A. Erdélyi (1941c) On algebraic Lamé functions. Philos. Mag. (7) 32, pp. 348–350.
  • A. Erdélyi (1942a) Integral equations for Heun functions. Quart. J. Math., Oxford Ser. 13, pp. 107–112.
  • 34: 28.19 Expansions in Series of me ν + 2 n Functions
    Let q be a normal value (§28.12(i)) with respect to ν , and f ( z ) be a function that is analytic on a doubly-infinite open strip S that contains the real axis. …
    28.19.3 f n = 1 π 0 π f ( z ) me ν + 2 n ( z , q ) d z .
    35: Sidebar 21.SB2: A two-phase solution of the Kadomtsev–Petviashvili equation (21.9.3)
    Such a solution is given in terms of a Riemann theta function with two phases. …
    36: 4.40 Integrals
    4.40.8 0 sinh ( a x ) sinh ( π x ) d x = 1 2 tan ( 1 2 a ) , π < a < π ,
    4.40.9 e a x ( cosh ( 1 2 x ) ) 2 d x = 4 π a sin ( π a ) , 1 < a < 1 ,
    4.40.10 0 tanh ( a x ) tanh ( b x ) x d x = ln ( a b ) , a > 0 , b > 0 .
    37: 11.1 Special Notation
    The functions treated in this chapter are the Struve functions 𝐇 ν ( z ) and 𝐊 ν ( z ) , the modified Struve functions 𝐋 ν ( z ) and 𝐌 ν ( z ) , the Lommel functions s μ , ν ( z ) and S μ , ν ( z ) , the Anger function 𝐉 ν ( z ) , the Weber function 𝐄 ν ( z ) , and the associated Anger–Weber function 𝐀 ν ( z ) .
    38: 8.2 Definitions and Basic Properties
    The general values of the incomplete gamma functions γ ( a , z ) and Γ ( a , z ) are defined by …However, when the integration paths do not cross the negative real axis, and in the case of (8.2.2) exclude the origin, γ ( a , z ) and Γ ( a , z ) take their principal values; compare §4.2(i). … The function γ ( a , z ) is entire in z and a . When z 0 , Γ ( a , z ) is an entire function of a , and γ ( a , z ) is meromorphic with simple poles at a = n , n = 0 , 1 , 2 , , with residue ( 1 ) n / n ! . …
    39: 5.12 Beta Function
    5.12.2 0 π / 2 sin 2 a 1 θ cos 2 b 1 θ d θ = 1 2 B ( a , b ) .
    5.12.3 0 t a 1 d t ( 1 + t ) a + b = B ( a , b ) .
    5.12.6 0 π ( sin t ) a 1 e i b t d t = π 2 a 1 e i π b / 2 a B ( 1 2 ( a + b + 1 ) , 1 2 ( a b + 1 ) ) , a > 0 .
    5.12.10 1 2 π i 0 ( 1 + ) t a 1 ( t 1 ) b 1 d t = sin ( π b ) π B ( a , b ) , a > 0 ,
    5.12.12 P ( 1 + , 0 + , 1 , 0 ) t a 1 ( 1 t ) b 1 d t = 4 e π i ( a + b ) sin ( π a ) sin ( π b ) B ( a , b ) ,
    40: 8.23 Statistical Applications
    The functions P ( a , x ) and Q ( a , x ) are used extensively in statistics as the probability integrals of the gamma distribution; see Johnson et al. (1994, pp. 337–414). …The function B x ( a , b ) and its normalization I x ( a , b ) play a similar role in statistics in connection with the beta distribution; see Johnson et al. (1995, pp. 210–275). In queueing theory the Erlang loss function is used, which can be expressed in terms of the reciprocal of Q ( a , x ) ; see Jagerman (1974) and Cooper (1981, pp. 80, 316–319). …