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642 ReferencesHajj-Boutros, J.(1985).On hypersurface-homogeneous space-times.JMP 26, 2297.See§14.3.Hajj-Boutros, J.(1986).New cosmological models.CQG 3, 311.See §14.3.Hajj-Boutros, J.(1989).Radiation equilibrium in general relativity: general solution.Mod. Phys. Lett. A 4, 427.See §16.1.Hajj-Boutros, J.and Léauté, B.(1985).Solutions of Einstein’s field equations withplane symmetry.Lett. Nuovo Cim. 43, 140.See §15.6.Hajj-Boutros, J.and Sfeila, J.(1987).Zero-curvature FRW models and Bianchi I spacetimeas solutions of the same equation.Int. J. Theor. Phys. 26, 97.See §14.3.Hajj-Boutros, J.and Sfeila, J.(1989).Radiating regime to matter dominated regime.Phys. Lett. A 136, 274.See §14.3.Halford, W.D. (1979). Petrov type N vacuum metrics and homothetic motions. JMP20, 1115.See §29.3.Halford, W.D. (1980). Einstein spaces and homothetic motions. II. JMP 21, 129. See§§11.4, 29.2.Halford, W.D. and Kerr, R.P. (1980).Einstein spaces and homothetic motions. I. JMP21, 120.See §11.4.Halford, W.D., McIntosh, C.B.G. and Van Leeuwen, E.H. (1980). Curvaturecollineations of non-expanding and twist-free vacuum type-N metrics in generalrelativity.J. Phys. A 13, 2995.See §35.4.Halilsoy, M.(1985).A class of transcendent solutions to the Ernst system.Lett. NuovoCim. 44, 88.See §21.1.Halilsoy, M.(1988a).Colliding electromagnetic shock waves in general relativity.PRD37, 2121.See §25.5.Halilsoy, M.(1988b).Cross-polarized cylindrical gravitational waves of Einstein andRosen.Nuovo Cim. B 102, 563.See §22.3.Halilsoy, M.(1988c).Distinct family of colliding gravitational waves in generalrelativity.PRD 38, 2979.See §25.4.Halilsoy, M.(1989).Colliding superposed waves in the Einstein–Maxwell theory.PRD39, 2172.See §25.5.Halilsoy, M.(1990a).Colliding impulsive waves in succession.PRD 42, 2922. See§25.3.Halilsoy, M.(1990b).Large family of colliding waves in the Einstein–Maxwell theory.JMP 31, 2694.See §25.5.Halilsoy, M.(1990c).Separable wave equation in the space of colliding waves.Phys.Lett. A 151, 205.See §25.4.Halilsoy, M.(1992).New metrics for spinning spheroids in general relativity.JMP 33,4225.See §20.3.Halilsoy, M.(1993a). Interpolation of the Schwarzschild and Bertotti–Robinsonsolutions.GRG 25, 275.See §21.1.Halilsoy, M.(1993b).Note on ‘Large family of colliding waves in the Einstein–Maxwelltheory’.JMP 34, 3553.See §25.5.Halilsoy, M.and Al-Badawi, A.(1998).Modified Reissner–Nordström metric in anexternal electrostatic field.Nuovo Cim. B 13, 761.See §21.2.Halilsoy, M.and El-Said, M.(1993).The physical interpretation of a Painlevétranscendent spacetime.GRG 25, 81.See §20.6.Halilsoy, M.and Gürtuĝ, Ö.(1994).On some properties of the nut–Curzon space-time.Nuovo Cim. B 109, 963.See §20.3.Hall, G.S. (1973). On the Petrov classification of gravitational fields. J. Phys. A 6, 619.See §4.3.Hall, G.S. (1976a). The classification of the Ricci tensor in general relativity theory. J.Phys. A 9, 541.See §5.1.Hall, G.S. (1976b).Ricci recurrent space times.Phys. Lett. A 56, 17.See §35.2.

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