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Bibliography Bibliography 1. Abe, T.j Mitsunaga, Y.j Koga, H.: Novel measurement method for axial residual stress in optical fibre. Electron Lett. 21, 4-5 (1985) 2. Abe, T.j Mitsunaga, Y.j Koga, H.: Photoe1astic computer tomography: a nove1 measure­ ment method for axial residual stress profile in optical fibers. J. Opt. Soc. Am. 3A, 133-138 (1986) 3. Aben, H.: Zur Anwendung des Verfahrens der schiefen Durchstrahlung in der Spannung­ soptik. Proc. Internat. Symp. Photoelasticity, Berlin 1961. Berlin: Akademie-Verlag 1962, pp. 7-23 4. Aben, H.: Phase plates in the measurement of phase difference. Optika Spektrosk. 14, 124-129 (1963) 5. Aben, H.: Optical phenomena in photoelastic models by the rotation of principal axes. Exp. Mech. 6, 13-22 (1966) 6. Aben, H.: Magnetophotoelasticity - photoelasticity in a magnetic field. Exp. Mech. 10, 97-105 (1970) 7. Aben, H.: Integrated photoelasticity. New York, etc.: McGraw-Hill1979 8. Aben, H.: Integrated photoelasticity ofaxisymmetric cubic single crystals. In: Paipetis, S.A.j Holister, G.S. (eds.): Photoelasticity in engineering practice. London: Elsevier Ap­ plied Science 1985, pp. 103-132 9. Aben, H.: Characteristic directions in optics of twisted birefringent media. J. Opt. Soc. Am. A3, 1414-1421 (1986) 10. Aben, H.: Integrated photoelasticity as tensor field tomography. Proc. Internat. Symp. Photoe1asticity, Tokyo 1986. Tokyo: Springer 1986, pp. 243-250 11. Aben, H.: Tomographie optique des champs de contraintes. Rev. Fran!;. Mec. N°1, 121-130 (1989) 12. Aben, H.: Integrated photoelasticity for stress analysis ofbottles. Proc. CSME Mechanical Engineering Forum, Toronto, 1990, pp. 143-146 13. Aben, H.: Una tecnica fotoelastica avanzata per la misura delle tensioni nei contenitori in vetro. Vetro Informazione W65, 26-31 (1991) 14. Aben, H.j Brosman, E.: Integrated photoe1asticity of cubic single crystals. VDI-Ber. W313, 45-50 (1978) 15. Aben, H.K.j Brosman, E.Lj Saar, A.J.: The method of nonmatching immersion in in­ tegrated photoelastieity. Proc. Eighth All-Union Conf. on Photoelastieity Tallinn 1979. Tallinn: Acad. Sei. Estonian SSR 1979, 2, pp. 12-15 230 Bibliography 16. Aben, H.; Idnurm, S.: Stress concentration in bent plates by magnetophotoelasticity. Proc. Fifth Internat. Conf. Exp. Stress Anal., Udine 1974, pp. 4.5-4.10 17. Aben, H.; Idnurm, S.; Puro, A.: Integrated photoelasticity in case of weak birefringence. Proc. 9th Internat. Conf. Exp. Mech., Copenhagen 1990, 2, pp. 867-875 18. Aben, H.K.; Josepson, J.I.: On the investigation ofaxisymmetric dielectric tensor fields by integrated photoelasticity. In: Paipetis, S.A.; Holister, G.S. (eds.): Photoelasticity in engineering practice. London: Elsevier Applied Science 1985, pp. 133-155 19. Aben, H.K.; Josepson, J .1.; Keil, K.-J.E.: The case of weak birefringence in integrated photoelasticity. Optics and Lasers in Eng. 11, 145-157 (1989) 20. Aben, H.K.; Keil, K.-J .E.: Integrated gradientphotoelasticity ofaxisymmetric bodies. Prik­ lad. Mekh. 21, 11-15 (1985) 21. Aben, H., Keil, K.-J.: Development of a nondestructive method for the determination of the stress distribution in cylindrical glass specimens. Institute of Cybernetics, Estonian Acad. Sci. Tallinn, 1988 22. Aben, H.K.; Krasnowski, B.R.; Pindera, J.T.: Nonrectilinear light propagation in inte­ grated photoelasticity ofaxisymmetric bodies. Trans. CSME 8, 195-200 (1984) 23. Aben, H.; et al.: Integrated photoelasticity for stress analysis in glass specimens of compli­ cated shape. In: Ponter, A.R.S.; Cocks, A.C.F. (eds.): Applied solid mechanics - 4. London and New York: Elsevier Applied Science 1991, pp. 326-340 24. Aben, H.; et al.: Integrated photoelasticity for residual stresses in glass specimens of com­ plicated shape. In: Chiang, F.-P. (ed.): Speckle techniques, birefringence methods, and applications to solid mechanics. Bellingham: SPIE 1991, pp. 298-309 25. Acloque, P.: Etude experimentale de l'effet de certains traitements thermiques sur le verre et de leur influence sur les contraintes mecaniques internes. Verres Refract. 4, 10-19 (1950) 26. Acloque, P.: Le probleme de la determination du sens et de l'intensite des contraintes dans le verre auto-contraint. VerresRefract. 9,3-12 (1955) 27. Acloque, P.: Methode et appareil pour la separation immediate des contraintes en lumiere polarisee oblique. Rev. Optique 34, 553-574 (1955) 28. Acloque, P.; Guillemet, C.: Methode pour la mesure par voie photoeIastique des contraintes "equilibrees dans l'epaisseur" d'une plaque. Verres Refract. 14, 3-10 (1960) 29. Acloque, P.; Guiilemet, C.: Spannungsmessung durch ein "Spiegelungs" - Verfahren. Si­ likattechnik 11, 502-506 (1960) 30. Adams, L.H.; Williamson, E.D.: Annealing of glass. J. Franklln Inst. 190,597 (1920) 31. Akeyoshi, K; Kanai, E.; Yamamoto, K.: Study on the physical tempering of glass plates. Res. Lab. Asahi Glass, Rep. 17,23-26,1967 32. Apati, A.: Spannungsoptische Bestimmung der Kühlspannungen in der Glaskugel. Tungsram Techn. Mitteilungen N°14, 3-7 (1964) 33. Apati, A.: Spannungsoptische Bestimmung von Glasspannungen, die durch kugelförmige feste Einschlüsse entstehen. Strojnicky Casop. 22, 307-318 (1971) 34. Appel, A.V.; Betz, H.T.; Pontarelli, D.A.: Infrared polariscope for photoelastic measure­ ment of semiconductors. Appl. Opt. 4, 1475-1478 (1965) Bibliography 231 35. Arora, A.; Ma.rshall, D.B.; Lawn, B.R.: Indentation deformation/fracture of normal and anomalous glasses. J. Non-Cryst. Solids 31, 415-428 (1979) 36. Augustsson, B.O.; Wasylyk, J.S.; Southwick, R.D.: Computer modelled internal pressure strength predictions for refillable glass containers. Glastech. Ber. 59, 121-131 (1986) 37. Azzam, R.M.: Generalized ellipsometry based on azimuth measurements alone. J. Opt. Soc. Am. 68, 514-518 (1978) 38. Azzam, R.M.A.; Basha.ra, N.M.: Ellipsometry and pola.rized light. Amsterdam, New York, Oxford: North-Holland 1977 39. Bachmann, P.K.; et al.: Stress in optical waveguides. 2: Fibers. Appl. Opt. 26, 1175-1182 (1987) 40. Badoz, J.: Mesures photoeIectriques de faibles birefringences et de tres petits pouvoirs rotatoires. J. Phys. Radium 17, 143A-149A (1956) 41. Ballantyne, E.R.: Fracture of toughened glass wall cladding. CSIRO Report N°06, Mel­ bourne 1961 42. Balmforth, W.j Holland, A.J.: The stress-optical coefficient of glasses. J. Soc. Glass Tech­ nol. 29, 111-123 (1945) 43. Banerjee, K.R.: Theory of photoelasticity. Indian J. Phys. 2, 195-242 (1927) 44. Bartenev, G.: On the theory of mechanical strengthening of glass by tempering. Dokl. Akad. Nauk SSSR 60, 257-260 (1948) 45. Ba.rtenev, G .M.: The structure and mechanical properties of inorganic glasses. Groningen: Wolters-Nordhoff Publ. 1970 46. Bartholomew, R.F.j Ga.rfinkel, H.M.: Chemical strengthening of glass. In: Uhlmann, D.R.j Kreidl, N.J. (eds.): Elasticity and strength in glasses. New York: Academic Press 1980, pp. 217-263 47. Bar-Ziv, E.j et al.: Temperature mappingin Hames by moire deHectometry. Appl. Opt. 22, 698-705 (1983) 48. Bateson, S.j et al.: Birefringence in glass measured by the scattered-light technique with a laser. Appl. Opt. 3, 902 (1964) 49. Bateson, S.; et al.: Stress measurement in tempered glass plates by scattered light method with a laser source. J. Am. Ceram. Soc. 49, 193-198 (1966) 50. Batteh, J .H.: Effect of surface relaxation on stress failure in laser-irradiated glass. J. Appl. Phys. 54, 3769-3776 (1983) 51. Belousov, J.L.; et al.: Optimization of the annealing of the bottles of champagne. Steklo Keram. 47, N°l, 17-19 (1990) 52. Berezina, E.E.: Photoelasticproperties of catalog glasses. Sov. J. Opt. Technol. 41, 429-430 (1974) 53. Berezina, E.E.j Golynja, V.S.: Dispersion in optical stress coefficients. Sov. J. Opt. Technol. 40, 370-371 (1972) 54. Berghaus, D.G.: Simplifications for scattered-light photoelasticity when using the unpo­ la.rized incident beam. Exp. Mech. 21, 394-400 (1981) 55. Berghaus, D.G.j Cannon, J .P.: Obtaining derivatives from experimental data using smoothed-spline functions. Exp. Mech. 13, 38-42 (1973) 232 Bibliography 56. Bestimmung des spannungsoptischen Koeffizienten im Zugversuch. DIN 52 314: 1977 57. Bickel, P.J.j Doksum, K.A.: Mathematical statistics. San Francisco: Holden-Ray 1977 58. Birger, LA.: Circular plates and shells of revolution. Moscow: Gos. Izdat. Teoret.-Tekh. Lit. 1961 59. Boguslavskii, LA.: Investigation of the superstrength of glasses strengthened by the ther­ mophysical method. Steklo Kera.m. 21, N°lO, 4-9 (1964) 60. Boguslavskii, I.A.j Vitman, F.F.j Puhlik, 0.1.: Further hardening of glass by increased quenching stress. Sov. Phys. Dokl. 9, 587-589 (1965) 61. Boguslavskii, I.A.j et al.: The strength of industrial sheet glass hardened by the ion ex­ change method. Sov. Phys. Dokl. 21, 44-46 (1976) 62. Boileau, H.j et al.: Photoelasticimetrie infrarouge assistee par ordinateur. Mater. et techno 74,443-445 (1986) 63. Bokshtein, M.F.: On the resolving power of the polarizing system for stress investigations. Zh. Tekh. Fiz. 19,1103-1109 (1949) 64. Bokshtein, M.F.: Investigation of stresses using scattered light. In: Polarization-optical method of stress investigation, Moscow: Akad. Nauk SSSR 1956, pp. 138-181 65. Bokshtein, M.F.: Determination of the optical anisotropy using the scattered light method for investigating stresses and strains. In: Methods of investigating stresses in structures. Moscow: Nauka 1976, pp. 72-84 66. Boley, B.A.; Weiner, J.H.: Theory ofthermal stresses. New York: John Wiley & Sons 1960 67. Born, M.j Wolf, E.: Principles of optics. Oxford: Perga.mon Press 1959 68. Borelli, N .F.j Miller, R.A.: Determination of the individual strain-optic coefficients of glass by an ultrasonic technique. Appl. Opt. 7, 745-750 (1968) 69. Botvinkin, O.K.j Ananich, N.!.: Anomalous birefringence and structure of glass. Steklo Kera.m. 16, W9, 6-11 (1959) 70. Bradshaw, W.: Stress profile determination in chemically strengthened glass using scat­ tered light. J. Mater. Sci. 14,2981-2988 (1979) 71.
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