About the Project

normal values

AdvancedHelp

(0.001 seconds)

21—30 of 58 matching pages

21: 35.1 Special Notation
All fractional or complex powers are principal values.
a , b complex variables.
| 𝐗 | determinant of 𝐗 (except when m = 1 where it means either determinant or absolute value, depending on the context).
f ( 𝐗 ) complex-valued function with 𝐗 𝛀 .
d 𝐇 normalized Haar measure on 𝐎 ( m ) .
22: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
These are based on the Liouville normal form of (1.13.29). … Applying equations (1.18.29) and (1.18.30), the complete set of normalized eigenfunctions being … Then orthogonality and normalization relations are …
23: 14.33 Tables
  • Zhang and Jin (1996, Chapter 4) tabulates 𝖯 n ( x ) for n = 2 ( 1 ) 5 , 10 , x = 0 ( .1 ) 1 , 7D; 𝖯 n ( cos θ ) for n = 1 ( 1 ) 4 , 10 , θ = 0 ( 5 ) 90 , 8D; 𝖰 n ( x ) for n = 0 ( 1 ) 2 , 10 , x = 0 ( .1 ) 0.9 , 8S; 𝖰 n ( cos θ ) for n = 0 ( 1 ) 3 , 10 , θ = 0 ( 5 ) 90 , 8D; 𝖯 n m ( x ) for m = 1 ( 1 ) 4 , n m = 0 ( 1 ) 2 , n = 10 , x = 0 , 0.5 , 8S; 𝖰 n m ( x ) for m = 1 ( 1 ) 4 , n = 0 ( 1 ) 2 , 10 , 8S; 𝖯 ν m ( cos θ ) for m = 0 ( 1 ) 3 , ν = 0 ( .25 ) 5 , θ = 0 ( 15 ) 90 , 5D; P n ( x ) for n = 2 ( 1 ) 5 , 10 , x = 1 ( 1 ) 10 , 7S; Q n ( x ) for n = 0 ( 1 ) 2 , 10 , x = 2 ( 1 ) 10 , 8S. Corresponding values of the derivative of each function are also included, as are 6D values of the first 5 ν -zeros of 𝖯 ν m ( cos θ ) and of its derivative for m = 0 ( 1 ) 4 , θ = 10 , 30 , 150 .

  • Belousov (1962) tabulates 𝖯 n m ( cos θ ) (normalized) for m = 0 ( 1 ) 36 , n m = 0 ( 1 ) 56 , θ = 0 ( 2.5 ) 90 , 6D.

  • Žurina and Karmazina (1964, 1965) tabulate the conical functions 𝖯 1 2 + i τ ( x ) for τ = 0 ( .01 ) 50 , x = 0.9 ( .1 ) 0.9 , 7S; P 1 2 + i τ ( x ) for τ = 0 ( .01 ) 50 , x = 1.1 ( .1 ) 2 ( .2 ) 5 ( .5 ) 10 ( 10 ) 60 , 7D. Auxiliary tables are included to facilitate computation for larger values of τ when 1 < x < 1 .

  • Žurina and Karmazina (1963) tabulates the conical functions 𝖯 1 2 + i τ 1 ( x ) for τ = 0 ( .01 ) 25 , x = 0.9 ( .1 ) 0.9 , 7S; P 1 2 + i τ 1 ( x ) for τ = 0 ( .01 ) 25 , x = 1.1 ( .1 ) 2 ( .2 ) 5 ( .5 ) 10 ( 10 ) 60 , 7S. Auxiliary tables are included to assist computation for larger values of τ when 1 < x < 1 .

  • 24: 1.13 Differential Equations
    A standard form for second order ordinary differential equations with x , and with a real parameter λ , and real valued functions p ( x ) , q ( x ) , and ρ ( x ) , with p ( x ) and ρ ( x ) positive, is … A regular Sturm-Liouville system will only have solutions for certain (real) values of λ , these are eigenvalues. …
    Transformation to Liouville normal Form
    Equation (1.13.26) with x [ a , b ] may be transformed to the Liouville normal form
    25: 35.4 Partitions and Zonal Polynomials
    Normalization
    Mean-Value
    26: 28.15 Expansions for Small q
    §28.15(i) Eigenvalues λ ν ( q )
    28.15.2 a ν 2 q 2 a ( ν + 2 ) 2 q 2 a ( ν + 4 ) 2 = q 2 a ( ν 2 ) 2 q 2 a ( ν 4 ) 2 .
    28.15.3 me ν ( z , q ) = e i ν z q 4 ( 1 ν + 1 e i ( ν + 2 ) z 1 ν 1 e i ( ν 2 ) z ) + q 2 32 ( 1 ( ν + 1 ) ( ν + 2 ) e i ( ν + 4 ) z + 1 ( ν 1 ) ( ν 2 ) e i ( ν 4 ) z 2 ( ν 2 + 1 ) ( ν 2 1 ) 2 e i ν z ) + ;
    27: 3.7 Ordinary Differential Equations
    §3.7(ii) Taylor-Series Method: Initial-Value Problems
    §3.7(iii) Taylor-Series Method: Boundary-Value Problems
    It will be observed that the present formulation of the Taylor-series method permits considerable parallelism in the computation, both for initial-value and boundary-value problems. … General methods for boundary-value problems for ordinary differential equations are given in Ascher et al. (1995). … The eigenvalues λ k are simple, that is, there is only one corresponding eigenfunction (apart from a normalization factor), and when ordered increasingly the eigenvalues satisfy …
    28: 28.31 Equations of Whittaker–Hill and Ince
    and constant values of A , B , k , and c , is called the Equation of Whittaker–Hill. … The values of η corresponding to C p m ( z , ξ ) , S p m ( z , ξ ) are denoted by a p m ( ξ ) , b p m ( ξ ) , respectively. …The normalization is given by
    28.31.12 1 π 0 2 π ( C p m ( x , ξ ) ) 2 d x = 1 π 0 2 π ( S p m ( x , ξ ) ) 2 d x = 1 ,
    29: 8.12 Uniform Asymptotic Expansions for Large Parameter
    8.12.3 P ( a , z ) = 1 2 erfc ( η a / 2 ) S ( a , η ) ,
    8.12.4 Q ( a , z ) = 1 2 erfc ( η a / 2 ) + S ( a , η ) ,
    For numerical values of d k , n to 30D for k = 0 ( 1 ) 9 and n = 0 ( 1 ) N k , where N k = 28 4 k / 2 , see DiDonato and Morris (1986). …
    8.12.18 Q ( a , z ) P ( a , z ) } z a 1 2 e z Γ ( a ) ( d ( ± χ ) k = 0 A k ( χ ) z k / 2 k = 1 B k ( χ ) z k / 2 ) ,
    8.12.21 Q ( a , x ) = q
    30: 1.2 Elementary Algebra
    1.2.45 𝐯 p = ( i = 1 n | v i | p ) 1 / p , p 1 .
    1.2.47 𝐯 1 = i = 1 n | v i | ,
    A vector of l 2 norm unity is normalized and every non-zero vector 𝐯 can be normalized via 𝐯 𝐯 / 𝐯 . …
    1.2.51 | 𝐮 , 𝐯 | 𝐮 𝐯 ,
    1.2.57 a i j = 0 , for | i j | > 1 .