[1]Balian R, Bloch C. Distribution of eigenfrequencies for the wave equation in a finite domain.I. Three-dimensional problem with smooth boundary surface. Annal Phys, 1970, 60: 401-447
[2]Baltes H P, Hilf E R. Spectra of finite system. B I Wissenschafts Verlag, Mannheim, 1976
[3]Berry M V. Some geometric aspects of the wave motion: wave front dislocations, diffraction catastrophes,diffractals, geometry of the Laplace operator. Proc Sympos Pure Math, 36, Amer Math Soc; Providence,1980, 13-38
[4]Brossard J, Carmona R. Can one hear the dimension of a fractal? Comm Math Phys, 1986, 104: 103-122
[5]Chen H, Sleeman B D. Fractal drums and n-dimensional modified Weyl-Berry conjecture. Comm MathPhys, 1995, 168: 581-601
[6]Gordon C, Webb D L, Wolpert S. One can not hear the shape of a drum. Bull Amer Math Soc, 1992, 27:134-138
[7]Gottlieb H P W. Eigenvalues of the Laplacian with Neumann boundary conditions. J Austral Math Soc,1985,26B: 293-309
[8]Gutierrez G, Yanez J M. Can an ideal gas feel the shape of its container? Amer J Phys, 1997, 65: 739-743
[9]Hsu P. On the -function of a Riemannian manifold with boundary. Trans Amer Math Soc, 1992, 333:643-671
[10]Kac M. Can one hear the shape of a drum? Amer Math Monthly, 1966,73: 1-23
[11]Lapidus M L. Fractal drum, Inverse spectral problems for elliptic operators and a partial resolution of the Weyl-Berry conjecture. Transa Amer Math Soc, 1991, 325: 465-529
[12]McKean H P, Singer I M. Curvature and the eigenvalues of the Laplacian. J Diff Geom, 1967,1: 43-69
[13]Pathria R K. An ideal quantum gas in a finite-sized container. Amer J Phys, 1998, 66: 1080-1085
[14]Pathria R K. Similarities and differences between Bose and Fermi gases. Phys Rev E, 1998, 57: 2697-2702
[15]Pleijel A. A study of certain Green’s functions with applications in the theory of vibrating membranes.Ark Mat, 1954, 2: 553-569
[16]Pleijel A. On Green’s functions and the eigenvalue distribution of the the three-dimensional membrane equation. Skand Mat Konger, 1954, 12: 222-
[17]Robinett R W. Visualizing classical periodic orbits from the quantum energy spectrum via the Fourier transforms: Simple infinite well examples. Amer J Phys, 1997,65: 1167-1175
[18]Sleeman B D, Zayed E M E. An inverse eigenvalue problem for a general convex domain. J Math Anal Appl, 1983,94: 78-95
[19]Sridhar S, Kudrolli A. Experiments on Not hearing the shape of drums. Phys Rev Lett, 1994,72: 2175-2178
[20]Stewartson K, Waechter R T. On hearing the shape of a drum: Further results. Proc Camb Philos Soc,1971,69: 353-363
[21]Waechter R T. On hearing the shape of a drum: An extension to higher dimensions. Proc Camb Philos Soc, 1972,72: 439-447
[22]Zayed E M E, Ibrahim S F M. An inverse problem for an arbitrary annular bounded domain in R3 with positive smooth functions in the boundary conditions. Pan Amer Math J, 2000, 10: 87-100
[23]Zayed E M E, Younis A I. An inverse problem for a general convex domain with impedance boundary conditions. Quart Appl Math, 1990, 48: 181-188
[24]Zayed E M E. An inverse eigenvalue problem for a general convex domain: An extension to higher dimen- sions. J Math Anal Appl, 1985, 112: 455-470
[25]Zayed E M E. Heat equation for an arbitrary doubly-connected region in R2 with mixed boundary condi-tions. J Applied Math Phys (ZAMP), 1989,40: 339-355
[26]Zayed E M E. On hearing the shape of an arbitrary doubly-connected region in R2. J Austral Math Soc,1990, 31B: 472-483
[27]Zayed E M E. Heat equation for an arbitrary multiply connected region in R2 with impedance boundary conditions. IMAJ Appl Math, 1990,45: 233-241
[28]Zayed E M E. Hearing the shape of a general doubly connected region in R3 with impedance boundary conditions. J Math Phys, 1990, 31: 2361-2365
[29]Zayed E M E. An inverse eigenvalue problem for an arbitrary multiply connected bounded region in R2.Internat J Math Math Sci, 1991, 14: 571-580
[30]Zayed E M E. Hearing the shape of a general doubly-connected region in R3 with mixed boundary condi-tions. Z Angew Math Phys, 1991, 42: 547-564
[31]Zayed E M E. An inverse eigenvalue problem for an arbitrary multiply connected bounded domain in R3 with impedance boundary conditions. SIAM J Appl Math, 1992, 52: 725-729
[32]Zayed E M E. An inverse eigenvalue problem for an arbitrary multiply connected bounded region: An extentsion to higher dimensions. Internat J Math Math Sci, 1993, 16: 485-492
[33]Zayed E M E. An inverse problem for a general multiply connected bounded domain. Appl Anal, 1995,59: 121-145
[34]Zayed E M E. Short-time asymptotics of the heat kernel of the Laplacian of a bounded domain with Robin boundary conditions. Houston J Math, 1998,24: 377-385
[35]Zayed E M E. An inverse problem for a general multiply connected bounded domain: An extension to higher dimensions. Appl Anal, 1999, 72: 27-41
[36]Zayed E M E. On hearing the shape of a bounded domain with Robin boundary conditions. IMAJ Appl Math, 2000, 64: 95-108
[37]Zayed E M E. An inverse problem for a general annular drum with positive smooth functions in the Robin boundary conditions. Collect Math, 2000, 51(3): 261-275
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