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1: 36.2 Catastrophes and Canonical Integrals
Diffraction Catastrophes
36.2.10 Ψ K ( 𝐱 ; k ) = k exp ( i k Φ K ( t ; 𝐱 ) ) d t , k > 0 .
36.2.11 Ψ ( U ) ( 𝐱 ; k ) = k exp ( i k Φ ( U ) ( s , t ; 𝐱 ) ) d s d t , U = E , H ; k > 0 .
36.2.28 Ψ ( E ) ( 0 , 0 , z ) = Ψ ( E ) ( 0 , 0 , z ) ¯ = 2 π π z 27 exp ( 2 27 i z 3 ) ( J 1 / 6 ( 2 27 z 3 ) + i J 1 / 6 ( 2 27 z 3 ) ) , z 0 ,
36.2.29 Ψ ( H ) ( 0 , 0 , z ) = Ψ ( H ) ( 0 , 0 , z ) ¯ = 2 1 / 3 3 exp ( 1 27 i z 3 ) Ψ ( E ) ( 0 , 0 , z 2 2 / 3 ) , < z < .
2: Sidebar 7.SB1: Diffraction from a Straightedge
Sidebar 7.SB1: Diffraction from a Straightedge
Photograph of light diffracted by a straightedge. …The faint circular patterns are additional diffraction effects due to imperfections in the edge.
3: 7.21 Physical Applications
§7.21 Physical Applications
Fresnel integrals and Cornu’s spiral occurred originally in the analysis of the diffraction of light; see Born and Wolf (1999, §8.7). … Voigt functions 𝖴 ( x , t ) , 𝖵 ( x , t ) , can be regarded as the convolution of a Gaussian and a Lorentzian, and appear when the analysis of light (or particulate) absorption (or emission) involves thermal motion effects. These applications include astrophysics, plasma diagnostics, neutron diffraction, laser spectroscopy, and surface scattering. …
4: Bibliography N
  • D. Naylor (1989) On an integral transform involving a class of Mathieu functions. SIAM J. Math. Anal. 20 (6), pp. 1500–1513.
  • W. J. Nellis and B. C. Carlson (1966) Reduction and evaluation of elliptic integrals. Math. Comp. 20 (94), pp. 223–231.
  • H. M. Nussenzveig (1992) Diffraction Effects in Semiclassical Scattering. Montroll Memorial Lecture Series in Mathematical Physics, Cambridge University Press.
  • J. F. Nye (2006) Dislocation lines in the hyperbolic umbilic diffraction catastrophe. Proc. Roy. Soc. Lond. Ser. A 462, pp. 2299–2313.
  • J. F. Nye (2007) Dislocation lines in the swallowtail diffraction catastrophe. Proc. Roy. Soc. Lond. Ser. A 463, pp. 343–355.
  • 5: 20 Theta Functions
    Chapter 20 Theta Functions
    6: Bibliography B
  • G. Backenstoss (1970) Pionic atoms. Annual Review of Nuclear and Particle Science 20, pp. 467–508.
  • M. V. Berry and C. J. Howls (1990) Stokes surfaces of diffraction catastrophes with codimension three. Nonlinearity 3 (2), pp. 281–291.
  • M. V. Berry and C. J. Howls (2010) Axial and focal-plane diffraction catastrophe integrals. J. Phys. A 43 (37), pp. 375206, 13.
  • M. V. Berry (1980) Some Geometric Aspects of Wave Motion: Wavefront Dislocations, Diffraction Catastrophes, Diffractals. In Geometry of the Laplace Operator (Proc. Sympos. Pure Math., Univ. Hawaii, Honolulu, Hawaii, 1979), Vol. 36, pp. 13–28.
  • M. Born and E. Wolf (1999) Principles of Optics: Electromagnetic Theory of Propagation, Interference and Diffraction of Light. 7th edition, Cambridge University Press, Cambridge.
  • 7: 36.1 Special Notation
    §36.1 Special Notation
    The main functions covered in this chapter are cuspoid catastrophes Φ K ( t ; 𝐱 ) ; umbilic catastrophes with codimension three Φ ( E ) ( s , t ; 𝐱 ) , Φ ( H ) ( s , t ; 𝐱 ) ; canonical integrals Ψ K ( 𝐱 ) , Ψ ( E ) ( 𝐱 ) , Ψ ( H ) ( 𝐱 ) ; diffraction catastrophes Ψ K ( 𝐱 ; k ) , Ψ ( E ) ( 𝐱 ; k ) , Ψ ( H ) ( 𝐱 ; k ) generated by the catastrophes. …
    8: 36.5 Stokes Sets
    Stokes sets are surfaces (codimension one) in 𝐱 space, across which Ψ K ( 𝐱 ; k ) or Ψ ( U ) ( 𝐱 ; k ) acquires an exponentially-small asymptotic contribution (in k ), associated with a complex critical point of Φ K or Φ ( U ) . …
    36.5.4 80 x 5 40 x 4 55 x 3 + 5 x 2 + 20 x 1 = 0 ,
    36.5.7 X = 9 20 + 20 u 4 Y 2 20 u 2 + 6 u 2 sign ( z ) ,
    9: 7.3 Graphics
    See accompanying text
    Figure 7.3.3: Fresnel integrals C ( x ) and S ( x ) , 0 x 4 . Magnify
    10: 9.16 Physical Applications
     Airy on the intensity of light in the neighborhood of a caustic (Airy (1838, 1849)). … Examples dealing with the propagation of light and with radiation of electromagnetic waves are given in Landau and Lifshitz (1962). Extensive use is made of Airy functions in investigations in the theory of electromagnetic diffraction and radiowave propagation (Fock (1965)). …A quite different application is made in the study of the diffraction of sound pulses by a circular cylinder (Friedlander (1958)). …