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For a review, see the feature issue on ultrashort-laser-pulse intensity and phase measurement and applications, IEEE J. Quantum Electron. 35, 418-523 (1999), and references therein.
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4
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10
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84894020570
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note
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nU(t)|dt for n = 0, 1 is finite. The absolute integrability ensures that the Fourier transform of U and its first derivative, Ũ(ω), dŨ/dω → 0 for ω → ±∝.
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11
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D. Yelin, D. Meshulach, and Y. Silberberg, Opt. Lett. 22, 1793-1795 (1997); T. Baumert, T. Brixner, V. Setfried, M. Strehle, and G. Gerber, Appl. Phys. B 65, 779 (1997); A. Efimov, M. D. Moores, N. M. Beach, J. L. Krause, and D. H. Reitze, Opt. Lett. 23, 1915-1917 (1998).
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Baumert, T.1
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16
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0000581693
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D. Yelin, D. Meshulach, and Y. Silberberg, Opt. Lett. 22, 1793-1795 (1997); T. Baumert, T. Brixner, V. Setfried, M. Strehle, and G. Gerber, Appl. Phys. B 65, 779 (1997); A. Efimov, M. D. Moores, N. M. Beach, J. L. Krause, and D. H. Reitze, Opt. Lett. 23, 1915-1917 (1998).
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18
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84894013719
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note
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If the operator £ does not contain explicit functions of time and the boundary conditions are defined at t = ±∝, then the Green's function G(t′ , t) has the form G(t′ - t). Most, if not all, physical processes of interest satisfy these conditions.
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