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Technical Design Report Super Fragment Separator

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DRAFT<br />

Main-<strong>Separator</strong> to the high-energy experimental area<br />

The High-Energy Branch allows experiments with fast secondary beams up to Bρmax of 20 Tm. It<br />

combines the in-flight separator with an efficient reaction setup, see Figure 2.4.1 and Figure 2.4.10.<br />

The compact design will overcome the problem of low transmission of the present FRS to the<br />

experimental areas (in the SIS18 Target Hall) caused by long transport lines and beam-line magnets<br />

designed only for primary beams with small emittances.<br />

Figure 2.4.10: Ion optical layout of the High-Energy-Branch of the Main-<strong>Separator</strong>. Shown are the envelopes<br />

of a 40 π mm mrad beam in x direction (upper half), y direction (lower half) and the dispersion for a<br />

2.5 % momentum deviation (dashed line). The main optical properties are given in Table 2.4.3.<br />

Main-<strong>Separator</strong> to the storage rings<br />

Of special importance is the Ring Branch which consists of a storage-cooler ring system. <strong>Fragment</strong><br />

pulses as short as 50 ns are injected into the Collector Ring (CR) at rigidities of up to 13 Tm. The<br />

main task of the CR is to efficiently collect and stochastically pre-cool the hot fragment beams.<br />

Figure 2.4.11: Ion optical layout of the Ring-Branch of the Main-<strong>Separator</strong>. Shown are the envelopes of a 40<br />

π mm mrad beam in x direction (upper half), y direction (lower half) and the dispersion for a 2.5 % momentum<br />

deviation (dashed line).<br />

17

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