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31: 1.3 Determinants, Linear Operators, and Spectral Expansions
The adjoint of a matrix 𝐀 is the matrix 𝐀 such that 𝐀 𝐚 , 𝐛 = 𝐚 , 𝐀 𝐛 for all 𝐚 , 𝐛 𝐄 n . …
1.3.20 𝐮 = i = 1 n c i 𝐚 i , c i = 𝐮 , 𝐚 i .
32: 33.22 Particle Scattering and Atomic and Molecular Spectra
With e denoting here the elementary charge, the Coulomb potential between two point particles with charges Z 1 e , Z 2 e and masses m 1 , m 2 separated by a distance s is V ( s ) = Z 1 Z 2 e 2 / ( 4 π ε 0 s ) = Z 1 Z 2 α c / s , where Z j are atomic numbers, ε 0 is the electric constant, α is the fine structure constant, and is the reduced Planck’s constant. The reduced mass is m = m 1 m 2 / ( m 1 + m 2 ) , and at energy of relative motion E with relative orbital angular momentum , the Schrödinger equation for the radial wave function w ( s ) is given by …
𝗄 = ( 2 m E / 2 ) 1 / 2 ,
For Z 1 Z 2 = 1 and m = m e , the electron mass, the scaling factors in (33.22.5) reduce to the Bohr radius, a 0 = / ( m e c α ) , and to a multiple of the Rydberg constant, R = m e c α 2 / ( 2 ) . …
33: 35.2 Laplace Transform
where the integration variable 𝐗 ranges over the space 𝛀 . … where the integral is taken over all 𝐙 = 𝐔 + i 𝐕 such that 𝐔 > 𝐗 0 and 𝐕 ranges over 𝓢 . …
34: 27.18 Methods of Computation: Primes
The ECPP (Elliptic Curve Primality Proving) algorithm handles primes with over 20,000 digits. …
35: Bibliography D
  • K. Dilcher, L. Skula, and I. Sh. Slavutskiǐ (1991) Bernoulli Numbers. Bibliography (1713–1990). Queen’s Papers in Pure and Applied Mathematics, Vol. 87, Queen’s University, Kingston, ON.
  • 36: Bibliography O
  • T. Oliveira e Silva (2006) Computing π ( x ) : The combinatorial method. Revista do DETUA 4 (6), pp. 759–768.
  • 37: 18.39 Applications in the Physical Sciences
    where x is a spatial coordinate, m the mass of the particle with potential energy V ( x ) , = h / ( 2 π ) is the reduced Planck’s constant, and ( a , b ) a finite or infinite interval. Here the term 2 2 m 2 x 2 represents the quantum kinetic energy of a single particle of mass m , and V ( x ) its potential energy. … and = k = m = 1 , has eigenfunctions … The eigenfunctions of L 2 are the spherical harmonics Y l , m l ( θ , ϕ ) with eigenvalues 2 l ( l + 1 ) , each with degeneracy 2 l + 1 as m l = l , l + 1 , , l . … , = m e = e 2 = 4 π ϵ 0 = 1 , Mohr and Taylor (2005, Table XXX, p. 71), where the relationship of a . u . to SI units is spelled out. …
    38: 27.6 Divisor Sums
    Sums of number-theoretic functions extended over divisors are of special interest. … Generating functions, Euler products, and Möbius inversion are used to evaluate many sums extended over divisors. …
    39: Bibliography S
  • M. J. Seaton (2002b) FGH, a code for the calculation of Coulomb radial wave functions from series expansions. Comput. Phys. Comm. 146 (2), pp. 250–253.
  • I. A. Stegun and R. Zucker (1976) Automatic computing methods for special functions. III. The sine, cosine, exponential integrals, and related functions. J. Res. Nat. Bur. Standards Sect. B 80B (2), pp. 291–311.
  • Stony Brook Algorithm Repository (website) Department of Computer Science, Stony Brook University, New York.
  • 40: 28.30 Expansions in Series of Eigenfunctions
    Then every continuous 2 π -periodic function f ( x ) whose second derivative is square-integrable over the interval [ 0 , 2 π ] can be expanded in a uniformly and absolutely convergent series …