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21: 26.13 Permutations: Cycle Notation
26.13.2 [ 1 2 3 4 5 6 7 8 3 5 2 4 7 8 1 6 ]
Cycles of length one are fixed points. … An element of 𝔖 n with a 1 fixed points, a 2 cycles of length 2 , , a n cycles of length n , where n = a 1 + 2 a 2 + + n a n , is said to have cycle type ( a 1 , a 2 , , a n ) . … A derangement is a permutation with no fixed points. The derangement number, d ( n ) , is the number of elements of 𝔖 n with no fixed points: …
22: 2.1 Definitions and Elementary Properties
Let 𝐗 be a point set with a limit point c . As x c in 𝐗 If c is a finite limit point of 𝐗 , then … Similarly for finite limit point c in place of . … where c is a finite, or infinite, limit point of 𝐗 . …
23: 13.27 Mathematical Applications
For applications of Whittaker functions to the uniform asymptotic theory of differential equations with a coalescing turning point and simple pole see §§2.8(vi) and 18.15(i). …
24: Mark J. Ablowitz
ODEs which do not have moveable branch point singularities. …
25: 7.20 Mathematical Applications
For applications of the complementary error function in uniform asymptotic approximations of integrals—saddle point coalescing with a pole or saddle point coalescing with an endpoint—see Wong (1989, Chapter 7), Olver (1997b, Chapter 9), and van der Waerden (1951). … Let P ( t ) = P ( x ( t ) , y ( t ) ) be any point on the projected spiral. …
26: 21.7 Riemann Surfaces
Consider the set of points in 2 that satisfy the equation …Equation (21.7.1) determines a plane algebraic curve in 2 , which is made compact by adding its points at infinity. …This compact curve may have singular points, that is, points at which the gradient of P ~ vanishes. … The zeros λ j , j = 1 , 2 , , 2 g + 1 of Q ( λ ) specify the finite branch points P j , that is, points at which μ j = 0 , on the Riemann surface. Denote the set of all branch points by B = { P 1 , P 2 , , P 2 g + 1 , P } . …
27: 10.20 Uniform Asymptotic Expansions for Large Order
Corresponding points of the mapping are shown in Figures 10.20.1 and 10.20.2. … The points P 1 , P 2 where these curves intersect the imaginary axis are ± i c , where …
See accompanying text
Figure 10.20.1: z -plane. P 1 and P 2 are the points ± i c . … Magnify
See accompanying text
Figure 10.20.2: ζ -plane. E 1 and E 2 are the points e π i / 3 ( 3 π / 2 ) 2 / 3 . Magnify
28: 10.41 Asymptotic Expansions for Large Order
Figures 10.41.1 and 10.41.2 show corresponding points of the mapping of the z -plane and the η -plane. …Thus B is the point z = c , where c is given by (10.20.18). …
29: Bibliography O
  • F. W. J. Olver (1964b) Error bounds for asymptotic expansions in turning-point problems. J. Soc. Indust. Appl. Math. 12 (1), pp. 200–214.
  • F. W. J. Olver (1975a) Second-order linear differential equations with two turning points. Philos. Trans. Roy. Soc. London Ser. A 278, pp. 137–174.
  • F. W. J. Olver (1976) Improved error bounds for second-order differential equations with two turning points. J. Res. Nat. Bur. Standards Sect. B 80B (4), pp. 437–440.
  • F. W. J. Olver (1977a) Connection formulas for second-order differential equations with multiple turning points. SIAM J. Math. Anal. 8 (1), pp. 127–154.
  • F. W. J. Olver (1977c) Second-order differential equations with fractional transition points. Trans. Amer. Math. Soc. 226, pp. 227–241.
  • 30: 2.9 Difference Equations
    For discussions of turning points, transition points, and uniform asymptotic expansions for solutions of linear difference equations of the second order see Wang and Wong (2003, 2005). …