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Gratings, diffraction replicas

The principle of this method is depected in Fig. 6.85. The signal pulse at the frequency co and its frequency-shifted replica 2A(o + Sa> pass with a time delay x through a beam of noble gas atoms. The high harmonics at and n(concave grating and reach the detector. [Pg.344]

The sizes and shapes are determined using transmission electron microscopy (TEM) over a diffraction grating replica. Dynamic light scattering can also be used to obtain the dimensions (see Chapter 8). [Pg.129]

See other pages where Gratings, diffraction replicas is mentioned: [Pg.232]    [Pg.95]    [Pg.10]    [Pg.11]    [Pg.495]    [Pg.94]    [Pg.343]    [Pg.703]    [Pg.3486]    [Pg.91]    [Pg.92]    [Pg.334]    [Pg.269]    [Pg.236]    [Pg.191]    [Pg.50]    [Pg.58]    [Pg.58]    [Pg.386]    [Pg.1140]    [Pg.150]   
See also in sourсe #XX -- [ Pg.66 ]



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