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11: 1.14 Integral Transforms
Sufficient conditions for the integral to converge are that s is a positive real number, and f ( t ) = O ( t δ ) as t , where δ > 0 . …
12: 14.16 Zeros
The number of zeros of 𝖯 ν μ ( x ) in the interval ( 1 , 1 ) is max ( ν | μ | , 0 ) if any of the following sets of conditions hold: … The number of zeros of 𝖯 ν μ ( x ) in the interval ( 1 , 1 ) is max ( ν | μ | , 0 ) + 1 if either of the following sets of conditions holds: …
13: 31.15 Stieltjes Polynomials
31.15.2 j = 1 N γ j / 2 z k a j + j = 1 j k n 1 z k z j = 0 , k = 1 , 2 , , n .
31.15.3 j = 1 N γ j t k a j + j = 1 n 1 1 t k z j = 0 .
If the following conditions are satisfied: …
31.15.6 a j < a j + 1 , j = 1 , 2 , , N 1 ,
14: 27.8 Dirichlet Characters
§27.8 Dirichlet Characters
In other words, Dirichlet characters (mod k ) satisfy the four conditions: … An example is the principal character (mod k ): … If ( n , k ) = 1 , then the characters satisfy the orthogonality relationA divisor d of k is called an induced modulus for χ if …
15: 1.13 Differential Equations
For a regular Sturm-Liouville system, equations (1.13.26) and (1.13.29) have: (i) identical eigenvalues, λ ; (ii) the corresponding (real) eigenfunctions, u ( x ) and w ( t ) , have the same number of zeros, also called nodes, for t ( 0 , c ) as for x ( a , b ) ; (iii) the eigenfunctions also satisfy the same type of boundary conditions, un-mixed or periodic, for both forms at the corresponding boundary points. …
16: 18.2 General Orthogonal Polynomials
The moments for an orthogonality measure d μ ( x ) are the numbers …It is to be noted that, although formally correct, the results of (18.2.30) are of little utility for numerical work, as Hankel determinants are notoriously ill-conditioned. … The OP’s p n ( 1 ) ( x ) may also be calculated from the original recursion (18.2.11_5), but with independent initial conditions for p 0 , p 1 : … are the Christoffel numbers, see also (3.5.18). … Under further conditions on the weight function there is an equiconvergence theorem, see Szegő (1975, Theorem 13.1.2). …
17: 3.11 Approximation Techniques
A sufficient condition for p n ( x ) to be the minimax polynomial is that | ϵ n ( x ) | attains its maximum at n + 2 distinct points in [ a , b ] and ϵ n ( x ) changes sign at these consecutive maxima. … The matrix is symmetric and positive definite, but the system is ill-conditioned when n is large because the lower rows of the matrix are approximately proportional to one another. … … Then the system (3.11.33) is diagonal and hence well-conditioned. … In consequence of this structure the number of operations can be reduced to n m = n log 2 n operations. …
18: 10.72 Mathematical Applications
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)). … The number m can also be replaced by any real constant λ ( > 2 ) in the sense that ( z z 0 ) λ f ( z ) is analytic and nonvanishing at z 0 ; moreover, g ( z ) is permitted to have a single or double pole at z 0 . …
19: Bibliography L
  • D. J. Leeming (1977) An asymptotic estimate for the Bernoulli and Euler numbers. Canad. Math. Bull. 20 (1), pp. 109–111.
  • D. H. Lehmer (1941) Guide to Tables in the Theory of Numbers. Bulletin of the National Research Council, No. 105, National Research Council, Washington, D.C..
  • D. N. Lehmer (1914) List of Prime Numbers from 1 to 10,006,721. Publ. No. 165, Carnegie Institution of Washington, Washington, D.C..
  • D. Lemoine (1997) Optimal cylindrical and spherical Bessel transforms satisfying bound state boundary conditions. Comput. Phys. Comm. 99 (2-3), pp. 297–306.
  • 20: 35.7 Gaussian Hypergeometric Function of Matrix Argument
    35.7.8 F 1 2 ( a , b c ; 𝐓 ) = Γ m ( c ) Γ m ( c a b ) Γ m ( c a ) Γ m ( c b ) F 1 2 ( a , b a + b c + 1 2 ( m + 1 ) ; 𝐈 𝐓 ) , 𝟎 < 𝐓 < 𝐈 ; 1 2 ( j + 1 ) a for some j = 1 , , m ; 1 2 ( j + 1 ) c and c a b 1 2 ( m j ) for all j = 1 , , m .
    Subject to the conditions (a)–(c), the function f ( 𝐓 ) = F 1 2 ( a , b ; c ; 𝐓 ) is the unique solution of each partial differential equation …