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functions f(ϵ,ℓ;r),h(ϵ,ℓ;r)

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21: 32.14 Combinatorics
32.14.1 lim N Prob ( N ( 𝝅 ) 2 N N 1 / 6 s ) = F ( s ) ,
where the distribution function F ( s ) is defined here by
32.14.2 F ( s ) = exp ( s ( x s ) w 2 ( x ) d x ) ,
The distribution function F ( s ) given by (32.14.2) arises in random matrix theory where it gives the limiting distribution for the normalized largest eigenvalue in the Gaussian Unitary Ensemble of n × n Hermitian matrices; see Tracy and Widom (1994). …
22: 33.11 Asymptotic Expansions for Large ρ
33.11.4 H ± ( η , ρ ) = e ± i θ ( f ( η , ρ ) ± i g ( η , ρ ) ) ,
33.11.7 g ( η , ρ ) f ^ ( η , ρ ) f ( η , ρ ) g ^ ( η , ρ ) = 1 .
23: 27.4 Euler Products and Dirichlet Series
Every multiplicative f satisfies the identity … The completely multiplicative function f ( n ) = n s gives the Euler product representation of the Riemann zeta function ζ ( s ) 25.2(i)): … The Riemann zeta function is the prototype of series of the form
27.4.4 F ( s ) = n = 1 f ( n ) n s ,
The function F ( s ) is a generating function, or more precisely, a Dirichlet generating function, for the coefficients. …
24: Bibliography Q
  • F. Qi and J. Mei (1999) Some inequalities of the incomplete gamma and related functions. Z. Anal. Anwendungen 18 (3), pp. 793–799.
  • 25: 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. …
    28.19.2 f ( z ) = n = f n me ν + 2 n ( z , q ) ,
    28.19.3 f n = 1 π 0 π f ( z ) me ν + 2 n ( z , q ) d z .
    26: 33.1 Special Notation
    The main functions treated in this chapter are first the Coulomb radial functions F ( η , ρ ) , G ( η , ρ ) , H ± ( η , ρ ) (Sommerfeld (1928)), which are used in the case of repulsive Coulomb interactions, and secondly the functions f ( ϵ , ; r ) , h ( ϵ , ; r ) , s ( ϵ , ; r ) , c ( ϵ , ; r ) (Seaton (1982, 2002a)), which are used in the case of attractive Coulomb interactions. …
  • Greene et al. (1979):

    f ( 0 ) ( ϵ , ; r ) = f ( ϵ , ; r ) , f ( ϵ , ; r ) = s ( ϵ , ; r ) , g ( ϵ , ; r ) = c ( ϵ , ; r ) .

  • 27: 8.14 Integrals
    8.14.5 0 x a 1 e s x γ ( b , x ) d x = Γ ( a + b ) b ( 1 + s ) a + b F ( 1 , a + b ; 1 + b ; 1 / ( 1 + s ) ) , s > 0 , ( a + b ) > 0 ,
    8.14.6 0 x a 1 e s x Γ ( b , x ) d x = Γ ( a + b ) a ( 1 + s ) a + b F ( 1 , a + b ; 1 + a ; s / ( 1 + s ) ) , s > 1 , ( a + b ) > 0 , a > 0 .
    For the hypergeometric function F ( a , b ; c ; z ) see §15.2(i). …
    28: 16.2 Definition and Analytic Properties
    §16.2(i) Generalized Hypergeometric Series
    Equivalently, the function is denoted by F q p ( 𝐚 𝐛 ; z ) or F q p ( 𝐚 ; 𝐛 ; z ) , and sometimes, for brevity, by F q p ( z ) . …
    16.2.5 𝐅 q p ( 𝐚 ; 𝐛 ; z ) = F q p ( a 1 , , a p b 1 , , b q ; z ) / ( Γ ( b 1 ) Γ ( b q ) ) = k = 0 ( a 1 ) k ( a p ) k Γ ( b 1 + k ) Γ ( b q + k ) z k k ! ;
    When p q + 1 and z is fixed and not a branch point, any branch of 𝐅 q p ( 𝐚 ; 𝐛 ; z ) is an entire function of each of the parameters a 1 , , a p , b 1 , , b q .
    29: 33.5 Limiting Forms for Small ρ , Small | η | , or Large
    §33.5(i) Small ρ
    §33.5(ii) η = 0
    For the functions 𝗃 , 𝗒 , J , Y see §§10.47(ii), 10.2(ii). …
    §33.5(iii) Small | η |
    §33.5(iv) Large
    30: 33.14 Definitions and Basic Properties
    §33.14(ii) Regular Solution f ( ϵ , ; r )
    The function f ( ϵ , ; r ) is recessive (§2.7(iii)) at r = 0 , and is defined by …The choice of sign in the last line of (33.14.6) is immaterial: the same function f ( ϵ , ; r ) is obtained. … f ( ϵ , ; r ) is real and an analytic function of r in the interval < r < , and it is also an analytic function of ϵ when < ϵ < . …
    §33.14(iii) Irregular Solution h ( ϵ , ; r )