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11: Guide to Searching the DLMF
Table 1: Query Examples
Query Matching records contain
"Fourier transform" and series both the phrase “Fourier transform” and the word “series”.
Fourier (transform or series) at least one of “Fourier transform” or “Fourier series”.
1/(2pi) and "Fourier transform" both 1 / ( 2 π ) and the phrase “Fourier transform”.
sin^2 +cos^2 the expression sin 2 + cos 2 .
DeMoivre and cos (n theta) both the word “DeMoivre” and the expression cos ( n θ ) .
12: 10.32 Integral Representations
10.32.14 K ν ( z ) = 1 2 π 2 i ( π 2 z ) 1 2 e z cos ( ν π ) i i Γ ( t ) Γ ( 1 2 t ν ) Γ ( 1 2 t + ν ) ( 2 z ) t d t , ν 1 2 , | ph z | < 3 2 π .
13: 15.9 Relations to Other Functions
The Jacobi transform is defined as
15.9.12 f ~ ( λ ) = 0 f ( t ) ϕ λ ( α , β ) ( t ) ( 2 sinh t ) 2 α + 1 ( 2 cosh t ) 2 β + 1 d t ,
with inverse … … Any hypergeometric function for which a quadratic transformation exists can be expressed in terms of associated Legendre functions or Ferrers functions. …
14: 24.7 Integral Representations
24.7.7 B 2 n ( x ) = ( 1 ) n + 1 2 n 0 cos ( 2 π x ) e 2 π t cosh ( 2 π t ) cos ( 2 π x ) t 2 n 1 d t , n = 1 , 2 , ,
24.7.8 B 2 n + 1 ( x ) = ( 1 ) n + 1 ( 2 n + 1 ) 0 sin ( 2 π x ) cosh ( 2 π t ) cos ( 2 π x ) t 2 n d t .
24.7.9 E 2 n ( x ) = ( 1 ) n 4 0 sin ( π x ) cosh ( π t ) cosh ( 2 π t ) cos ( 2 π x ) t 2 n d t ,
24.7.10 E 2 n + 1 ( x ) = ( 1 ) n + 1 4 0 cos ( π x ) sinh ( π t ) cosh ( 2 π t ) cos ( 2 π x ) t 2 n + 1 d t .
24.7.11 B n ( x ) = 1 2 π i c i c + i ( x + t ) n ( π sin ( π t ) ) 2 d t , 0 < c < 1 .
15: 7.7 Integral Representations
7.7.15 0 e a t cos ( t 2 ) d t = π 2 f ( a 2 π ) , a > 0 ,
16: 12.5 Integral Representations
12.5.9 V ( a , z ) = 2 π e 1 4 z 2 z a 1 2 2 π i Γ ( 1 2 a ) i i Γ ( t ) Γ ( 1 2 a 2 t ) 2 t z 2 t cos ( π t ) d t , a 1 2 , 3 2 , 5 2 , , | ph z | < 1 4 π ,
17: 14.20 Conical (or Mehler) Functions
14.20.3 𝖰 ^ 1 2 + i τ μ ( x ) = π e τ π sin ( μ π ) sinh ( τ π ) 2 ( cosh 2 ( τ π ) sin 2 ( μ π ) ) 𝖯 1 2 + i τ μ ( x ) + π ( e τ π cos 2 ( μ π ) + sinh ( τ π ) ) 2 ( cosh 2 ( τ π ) sin 2 ( μ π ) ) 𝖯 1 2 + i τ μ ( x ) .
14.20.9 𝖯 1 2 + i τ ( cos θ ) = 2 π 0 θ cosh ( τ ϕ ) 2 ( cos ϕ cos θ ) d ϕ .
From (14.20.9) or (14.20.10) it is evident that 𝖯 1 2 + i τ ( cos θ ) is positive for real θ .
§14.20(vi) Generalized Mehler–Fock Transformation
18: Bibliography F
  • J. Faraut (1982) Un théorème de Paley-Wiener pour la transformation de Fourier sur un espace riemannien symétrique de rang un. J. Funct. Anal. 49 (2), pp. 230–268.
  • H. E. Fettis (1965) Calculation of elliptic integrals of the third kind by means of Gauss’ transformation. Math. Comp. 19 (89), pp. 97–104.
  • F. Feuillebois (1991) Numerical calculation of singular integrals related to Hankel transform. Comput. Math. Appl. 21 (2-3), pp. 87–94.
  • A. S. Fokas and M. J. Ablowitz (1982) On a unified approach to transformations and elementary solutions of Painlevé equations. J. Math. Phys. 23 (11), pp. 2033–2042.
  • C. L. Frenzen (1987b) On the asymptotic expansion of Mellin transforms. SIAM J. Math. Anal. 18 (1), pp. 273–282.
  • 19: 19.8 Quadratic Transformations
    §19.8 Quadratic Transformations
    §19.8(ii) Landen Transformations
    Descending Landen Transformation
    Ascending Landen Transformation
    §19.8(iii) Gauss Transformation
    20: 13.10 Integrals
    §13.10(ii) Laplace Transforms
    §13.10(iii) Mellin Transforms
    §13.10(iv) Fourier Transforms
    §13.10(v) Hankel Transforms