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11: 22.22 Software
However, in some cases no research software has been found. …
12: 18.32 OP’s with Respect to Freud Weights
Of special interest are the cases Q ( x ) = x 2 m , m = 1 , 2 , , and the case Q ( x ) = 1 4 x 4 t x 2 ( t ), see §32.15. …For a uniform asymptotic expansion in terms of Airy functions (§9.2) for the OP’s in the case Q ( x ) = x 4 see Bo and Wong (1999). … The case Q ( x ) = | x | β ( β > 0 ) was already introduced by Freud (1976). The special case Q ( x ) = 1 4 x 4 t x 2 is of particular interest, see Clarkson and Jordaan (2018). …
13: Guide to Searching the DLMF
All terms are taken to be case-insensitive, except those taken to represent math expressions (see Case Sensitivity). …
Case Sensitivity
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. In the following situations, DLMF search is case-sensitive: …
14: Sidebar 5.SB1: Gamma & Digamma Phase Plots
The fluid flow analogy in this case involves a line of vortices of alternating sign of circulation, resulting in a near cancellation of flow far from the real axis.
15: 6.9 Continued Fraction
6.9.1 E 1 ( z ) = e z z + 1 1 + 1 z + 2 1 + 2 z + 3 1 + 3 z + , | ph z | < π .
16: 9.17 Methods of Computation
However, in the case of Ai ( z ) and Bi ( z ) this accuracy can be increased considerably by use of the exponentially-improved forms of expansion supplied in §9.7(v). … In the case of Ai ( z ) , for example, this means that in the sectors 1 3 π < | ph z | < π we may integrate along outward rays from the origin with initial values obtained from §9.2(ii). … In the case of the Scorer functions, integration of the differential equation (9.12.1) is more difficult than (9.2.1), because in some regions stable directions of integration do not exist. …In these cases boundary-value methods need to be used instead; see §3.7(iii). …
17: 12.20 Approximations
As special cases of these results a Chebyshev-series expansion for U ( a , x ) valid when λ x < follows from (12.7.14), and Chebyshev-series expansions for U ( a , x ) and V ( a , x ) valid when 0 x λ follow from (12.4.1), (12.4.2), (12.7.12), and (12.7.13). …
18: 23.4 Graphics
§23.4(i) Real Variables
Line graphs of the Weierstrass functions ( x ) , ζ ( x ) , and σ ( x ) , illustrating the lemniscatic and equianharmonic cases. …
See accompanying text
Figure 23.4.1: ( x ; g 2 , 0 ) for 0 x 9 , g 2 = 0. …(Lemniscatic case.) Magnify
See accompanying text
Figure 23.4.2: ( x ; 0 , g 3 ) for 0 x 9 , g 3 = 0. …(Equianharmonic case.) Magnify
See accompanying text
Figure 23.4.3: ζ ( x ; g 2 , 0 ) for 0 x 8 , g 2 = 0. …(Lemniscatic case.) Magnify
19: 23.5 Special Lattices
This happens in the cases treated in the following four subsections. …
§23.5(iii) Lemniscatic Lattice
Note also that in this case τ = i . …
§23.5(iv) Rhombic Lattice
§23.5(v) Equianharmonic Lattice
20: 25.17 Physical Applications
The zeta function arises in the calculation of the partition function of ideal quantum gases (both Bose–Einstein and Fermi–Dirac cases), and it determines the critical gas temperature and density for the Bose–Einstein condensation phase transition in a dilute gas (Lifshitz and Pitaevskiĭ (1980)). …