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Technical Design Report Super Fragment Separator

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DRAFT<br />

Figure 2.4.7: Upper figures: Calculated phase space in the dispersive focal plane PF2 for a beam of 40 mm<br />

mrad and three different momenta of ∆p/p = ±2.5 % with (blue distributions) and without (red distributions)<br />

correction of image aberrations. Lower figurel: Corresponding phase space in the achromatic focal plane<br />

PF4.<br />

Main-<strong>Separator</strong><br />

The Main-<strong>Separator</strong> consists of four dipole stages with focusing elements in front and behind each<br />

dipole magnet system. The 29-degree dipole magnets are divided in 3 parts to facilitate the production<br />

of the iron-dominated superconducting magnets. The ion-optical design of the<br />

Main-<strong>Separator</strong> closely follows the concept applied for the Pre-<strong>Separator</strong>. However, the radiation<br />

level in this part of the <strong>Super</strong>-FRS is about two orders of magnitude lower because the primary<br />

beam and the non-desired fragments are deposited in the Pre-<strong>Separator</strong>. The Main-<strong>Separator</strong> has<br />

also four focal planes to accommodate an achromatic system with a degrader station in the central<br />

focal plane. The Main-<strong>Separator</strong> has three experimental branches to different experimental areas.<br />

The characteristic features are outlined for the example of the High-Energy-Branch. This branch<br />

has the advantage of a symmetrical geometry and therefore, the potential for the highest ion-optical<br />

resolution and transmission. The most relevant ion-optical properties can be deduced from the<br />

first-order ion-optical matrix elements presented in Table 2.4.3.<br />

14

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