X-ray small angle camera with block-collimation system an instrument of colloid research

Abstract

1. For X-ray small angle research usually a primary beam of line shaped crosssection is applied. The longest known is the three-slit-camera with two parallel diaphragms defining the primary beam and the third one limiting the parasitic scattering caused by the second one. 2. The difficulty of the correct mutual adjustment of the three diaphragms is circumvented by the block collimation system, where the primary beam is guided by three bodies (2 blocks and 1 edge). The essential principle is the exact coincidence of the extremely smooth upper surface of the first block (middle block) with the also perfectly plane bottom surface of the second block (bridge) in their mutual extension. The third diaphragm, the edge, controls the widths of the ribbon-shaped primary beam and is situated as entrance slit in front of the two blocks, this being closest to the X-ray tube. 3. The basic concept from 1954 has been maintained, however, the entire apparatus of the small angle camera has been modified. Only the earliest professional type, the building block camera, has been described in a comprehensive communication (1958); the more recently developed types are only known from short communications and from prospects of the manufacturer, A. Paar KG. The main topic of the present work is the description of the most important recent type, the compact camera. Whereas the individual parts of the building block camera are mounted on some kind of optical rail in a mutually adjustable way, all parts of the compact camera except the detector slit and the detector are accomodated in an evacuated compact rigid housing without foils or air paths to be penetrated like for the building block camera. An important feature is the support of the front end of the camera on top of the X-ray tube avoiding those minor movements between camera and X-ray tube caused by thermal and mechanical influences. As shown by experiment, practically perfect stability of the scattering intensity at medium and high resolution (above 1000 A) is obtained by these means. Moreover, the independent motion of detector slit and detector shall be mentioned, as well as the improved coincidence of surfaces of the beam — guiding blocks, operation of the vacuum surrounded entrance slit from outside etc. 4. An attempt of an optimization is made with view to obtain maximum primary intensity at a given resolution, measured by the smallest angle from which on a scattering measurement is possible. This optimization was tried to be achieved by variation of two experimental parameters: Variation of the pick-up angle of the radiation from the focus and the position of the middle-block of the collimation system which is in between the entrance slit and the bridge. The primary energy entering the collimation system in dependence of the two variables has been calculated