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Applicability/ intended use of method:

An X-ray beam incident at an angle on a lattice plane (hkl) obeying Bragg s law at point C will be diffracted as shown A circle centered at point C may be drawn with a radius of 1/ This is called the Ewald circle but, for a real three-dimensional crystal lattice, a three-dimensional Ewald sphere would be generated..

P1: KOA WY050-19 WY050-Ulick-v4 September 19, 2004 12:41

resonator operation compared to the shorter path in the SBS resonator only (Fig. 3.2f) [34]. In a similar, slightly different concept the light is coupled out using a quarterwave plate and a polarizer [35] (see Fig. 3.3). In the sf-SBS laser the output pulse energy can be varied by the re ectance of Mstart or a lter in front of Mstart. Here it can be done by rotating the quarter-wave plate to change the rotation angle of the intracavity eld. In the rst case solely the Q of the start resonator is varied. In the latter case the Qs of both the start resonator and the SBS resonator are changed. A fundamentally different SBS-laser concept was invented by Chandra et al. [36] (see Fig. 3.4) and was later used by others also [35, 37]. Here the SBS mirror is placed outside the resonator. The concept uses the polarization status of the light to discriminate between a start and an SBS resonator. The Q ratio of the two resonators can be adjusted by rotating the quarter-wave plate. Placing the SBS-mirror extracavity makes the alignment of the focusing lens in front of the SBS mirror uncritical compared to the intracavity telescope (see above). Also, absorbing media intracavity leading to wavefront distortions or lamentation can be used with high average output powers in this scheme. On the other hand, one gives up the threshold

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Once the x-ray beam from the x-ray tube has been filtered and collimated to produce the required number and quality (energy) of the x-rays striking the patient, a number of factors become important in producing the x-ray image: the number of x-rays and the distribution of energies; the pattern of penetration, absorption, and scatter of x-rays in the patient (ie, the image information); physical interactions in the film-screen to encode the image; and processing of the film to make it visible to the diagnostician Interactions of x-ray photons in the patient to yield diagnostic information occur primarily through the photoelectric effect and Compton scattering Coherent scattering is numerically unimportant, and pair production and photodisintegration do not occur at most diagnostic x-ray energies.

The photoelectric effect, which is dominant for low-energy photons and high-Z absorbers, generates no significant scatter radiation and produces high contrast in the x-ray image, but due to total absorption of photon energy, can contribute significantly to patient exposure This can be offset by using higher energy x-ray techniques, but Compton interactions increase at these higher energies with a reduction in radiographic image contrast due to an increase in scatter radiation Photons that are absorbed are removed from the x-ray beam and this absence will appear as information in the x-ray film; those that are scattered are deflected into a random course and no longer carry useful information because their direction is random Scattered photons darken the film creating film fog which may completely obscure the image (it is still there, but cannot be seen).

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