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21: 10.72 Mathematical Applications
The canonical form of differential equation for these problems is given by … In regions in which (10.72.1) has a simple turning point z 0 , that is, f ( z ) and g ( z ) are analytic (or with weaker conditions if z = x is a real variable) and z 0 is a simple zero of f ( z ) , asymptotic expansions of the solutions w for large u can be constructed in terms of Airy functions or equivalently Bessel functions or modified Bessel functions of order 1 3 9.6(i)). …
22: 18.2 General Orthogonal Polynomials
First Form
Second Form
Monic and Orthonormal Forms
The recurrence relations (18.2.10) can be equivalently written as …
Confluent Form
23: 28.29 Definitions and Basic Properties
Equivalently, …It has the formThe case c = 0 is equivalent to …
24: 3.7 Ordinary Differential Equations
The remaining two equations are supplied by boundary conditions of the formIf q ( x ) is C on the closure of ( a , b ) , then the discretized form (3.7.13) of the differential equation can be used. … The method consists of a set of rules each of which is equivalent to a truncated Taylor-series expansion, but the rules avoid the need for analytic differentiations of the differential equation. …
25: 19.18 Derivatives and Differential Equations
or equivalently, … The next four differential equations apply to the complete case of R F and R G in the form R a ( 1 2 , 1 2 ; z 1 , z 2 ) (see (19.16.20) and (19.16.23)). …
26: 25.5 Integral Representations
25.5.20 ζ ( s ) = Γ ( 1 s ) 2 π i ( 0 + ) z s 1 e z 1 d z , s 1 , 2 , ,
Equivalently, …
27: 33.11 Asymptotic Expansions for Large ρ
§33.11 Asymptotic Expansions for Large ρ
An equivalent formulation is given by …
28: 33.5 Limiting Forms for Small ρ , Small | η | , or Large
§33.5 Limiting Forms for Small ρ , Small | η | , or Large
§33.5(i) Small ρ
Equivalently, …
§33.5(iii) Small | η |
§33.5(iv) Large
29: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
These are based on the Liouville normal form of (1.13.29). … compare (1.18.30) and (1.18.45), and the eigenfunction expansions are of the formConsider formally self-adjoint operators of the form
30: 27.11 Asymptotic Formulas: Partial Sums
It is more fruitful to study partial sums and seek asymptotic formulas of the form
27.11.11 p x p h ( mod k ) ln p p = 1 ϕ ( k ) ln x + O ( 1 ) ,
Letting x in (27.11.9) or in (27.11.11) we see that there are infinitely many primes p h ( mod k ) if h , k are coprime; this is Dirichlet’s theorem on primes in arithmetic progressions. … Each of (27.11.13)–(27.11.15) is equivalent to the prime number theorem (27.2.3). The prime number theorem for arithmetic progressions—an extension of (27.2.3) and first proved in de la Vallée Poussin (1896a, b)—states that if ( h , k ) = 1 , then the number of primes p x with p h ( mod k ) is asymptotic to x / ( ϕ ( k ) ln x ) as x .