Wittgenstein's Lectures, Cambridge, 1932-1935: From the by Ludwig Wittgenstein

By Ludwig Wittgenstein

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Example text

As is demonstrated in Fig. 6 the determination of kmin is different. In case 18 2. /_ L _ _ _ L , I I Eo 0 6g 6~ 5~ I I i go I 6~ Fig. 6a,b. 23), as a measure of the deviation from perfect backscattering. There is no truly backscattered beam within the scattering range defined by 6g in case (a), in contrast to case (b) where it is part of the allowed range I O LU w 05. Fig. 7. The influence of the scattering geometry on the energy resolution is shown as a function of the deviation of the scattering angle from perfect backscattering.

4. Beam trajectories and emission patterns for bending magnet (a), wavelength shifter (b), undulator (c) and wiggler (d). of the spectra of several bending magnets. The brightness is increased by a factor corresponding to twice the number of periods. The horizontal opening angle and, therefore, the beam divergence is larger for the wiggler than for the undulator. Special magnetic structures can also be defined to generate circularly polarized radiation. One possibility is to install a crossed undulator (Moissev, Nikitin and Fedorov 1978) to obtain the desired polarization by the interference between two crossed sections.

4d). Such multipole wigglers produce a complicated spectrum, which on the high energy side resembles the simple addition 30 {o} 3. X-ray Sources ~ ~ (b) Fig. 4. Beam trajectories and emission patterns for bending magnet (a), wavelength shifter (b), undulator (c) and wiggler (d). of the spectra of several bending magnets. The brightness is increased by a factor corresponding to twice the number of periods. The horizontal opening angle and, therefore, the beam divergence is larger for the wiggler than for the undulator.

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