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1: 4.37 Inverse Hyperbolic Functions
§4.37(v) Fundamental Property
2: 4.23 Inverse Trigonometric Functions
§4.23(v) Fundamental Property
3: 27.2 Functions
Functions in this section derive their properties from the fundamental theorem of arithmetic, which states that every integer n > 1 can be represented uniquely as a product of prime powers, …
4: 28.2 Definitions and Basic Properties
§28.2 Definitions and Basic Properties
(28.2.1) possesses a fundamental pair of solutions w I ( z ; a , q ) , w II ( z ; a , q ) called basic solutions with …Other properties are as follows. … A solution with the pseudoperiodic property (28.2.14) is called a Floquet solution with respect to ν . …
Change of Sign of q
5: 3.11 Approximation Techniques
They enjoy an orthogonal property with respect to integrals: …as well as an orthogonal property with respect to sums, as follows. … For these and further properties of Chebyshev polynomials, see Chapter 18, Gil et al. (2007a, Chapter 3), and Mason and Handscomb (2003). … The property …is of fundamental importance in the FFT algorithm. …
6: 28.29 Definitions and Basic Properties
§28.29 Definitions and Basic Properties
28.29.4 w I ( z + π , λ ) = w I ( π , λ ) w I ( z , λ ) + w I ( π , λ ) w II ( z , λ ) ,
Then (28.29.1) has a nontrivial solution w ( z ) with the pseudoperiodic propertyIf ν ( 0 , 1 ) is a solution of (28.29.9), then F ν ( z ) , F ν ( z ) comprise a fundamental pair of solutions of Hill’s equation. …
7: 18.38 Mathematical Applications
The monic Chebyshev polynomial 2 1 n T n ( x ) , n 1 , enjoys the ‘minimax’ property on the interval [ 1 , 1 ] , that is, | 2 1 n T n ( x ) | has the least maximum value among all monic polynomials of degree n . … Classical OP’s play a fundamental role in Gaussian quadrature. …
8: 18.39 Applications in the Physical Sciences
The fundamental quantum Schrödinger operator, also called the Hamiltonian, , is a second order differential operator of the form … The properties of V ( x ) determine whether the spectrum, this being the set of eigenvalues of , is discrete, continuous, or mixed, see §1.18. … As the Coulomb–Pollaczek OP’s are members of the Nevai-Blumenthal class, this is, for Z < 0 , a physical example of the properties of the zeros of such OP’s, and their possible accumulation at x = 1 , as discussed in §18.2(xi). …
9: Bibliography G
  • I. M. Gel’fand and G. E. Shilov (1964) Generalized Functions. Vol. 1: Properties and Operations. Academic Press, New York.
  • Z. Gong, L. Zejda, W. Dappen, and J. M. Aparicio (2001) Generalized Fermi-Dirac functions and derivatives: Properties and evaluation. Comput. Phys. Comm. 136 (3), pp. 294–309.
  • K. Gottfried and T. Yan (2004) Quantum mechanics: fundamentals. Second edition, Springer-Verlag, New York.
  • B. Grammaticos, A. Ramani, and V. Papageorgiou (1991) Do integrable mappings have the Painlevé property?. Phys. Rev. Lett. 67 (14), pp. 1825–1828.
  • P. Groeneboom and D. R. Truax (2000) A monotonicity property of the power function of multivariate tests. Indag. Math. (N.S.) 11 (2), pp. 209–218.
  • 10: 20.2 Definitions and Periodic Properties
    §20.2 Definitions and Periodic Properties
    The four points ( 0 , π , π + τ π , τ π ) are the vertices of the fundamental parallelogram in the z -plane; see Figure 20.2.1. …
    Figure 20.2.1: z -plane. Fundamental parallelogram. …