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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: 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. …
    37: 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. …
    38: 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 …
    39: Richard A. Askey
    Over his career his primary research areas were in Special Functions and Orthogonal Polynomials, but also included other topics from Classical Analysis and related areas. …
    40: 1.6 Vectors and Vector-Valued Functions
    Much vector algebra involves summation over suffices of products of vector components. In almost all cases of repeated suffices, we can suppress the summation notation entirely, if it is understood that an implicit sum is to be taken over any repeated suffix. Thus pairs of indefinite suffices in an expression are resolved by being summed over (or “traced” over). …
    §1.6(v) Surfaces and Integrals over Surfaces
    The integral of a continuous function f ( x , y , z ) over a surface S is …