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Laser phase shift interferometry

Things are not quite as simple as they seem. In order for the constructive interference, which is at the core of wavepacket interferometry, to occur, not only must (t + At) = (t), but also the phases of apump and aprobe> which depend on the optical phase of the femtosecond laser rather than the molecular phase, must match. A rigorous treatment of the phase coherent pump/probe scheme using optically phase-locked pulse pairs is presented by Scherer, et al., [1990, 1991, 1992] and refined by Albrecht, et al., (1999), who discuss the distinction between and consequences of pulse envelope delays vs. carrier wave phase shifts (see Fig. 9.6). A simplified treatment, valid only for weak optical pulses is presented here. [Pg.650]

Fig 1 Optical arrangement for measuring the velocity of a moving phase object using Schlieren Interferometry of Doppler-shifted laser light. A is the Doppler-shifted beam, and B is the reference beam... [Pg.179]


See other pages where Laser phase shift interferometry is mentioned: [Pg.334]    [Pg.362]    [Pg.334]    [Pg.502]    [Pg.93]    [Pg.94]    [Pg.96]    [Pg.334]    [Pg.268]    [Pg.788]    [Pg.173]    [Pg.200]    [Pg.717]    [Pg.267]   
See also in sourсe #XX -- [ Pg.93 , Pg.109 , Pg.111 ]




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