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Technical Design Report Super Fragment Separator

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DRAFT<br />

Figure 2.4.43: Front, side, and back view of a normal conducting radiation resistant quadrupole having a<br />

pole tip radius of 210 mm for the 1 st stage of the Pre-<strong>Separator</strong>. Dimensions are given in mm.<br />

2.4.2.2.2 <strong>Super</strong>ferric quadrupole magnets<br />

Each dipole stage of the <strong>Super</strong>-FRS is equipped with a quadrupole triplet in front and behind the<br />

dipole magnet. The standard quadrupole triplet consists of 3 cold-iron, superferric quadrupole<br />

magnets with warm aperture radius of ± 190 mm. Their lengths is 800 mm, 1200 mm, and 800 mm<br />

and provide a maximum field gradient of 10.0 T/m. The distance between two quadrupoles is 1000<br />

mm. Octupole correction coils are embedded in the 800 mm long quadrupole magnets to allow<br />

corrections of image aberration. The three quadrupole magnets will be assembled in one common<br />

cryostat together with up to three 500 mm long superferric hexapole magnets and 500 mm long<br />

superferric steering dipoles. One example for such a multiplet consisting of three quadrupoles and<br />

two hexapoles is schematically illustrated in Figure 2.4.44. All magnets in the cryostat are cooled<br />

with liquid helium in a common helium bath. The same principle is used for the A1900 quadrupole<br />

triplet [16] and the quadrupole triplet for the BigRIPS [17].<br />

Figure 2.4.44: Schematic view of a <strong>Super</strong>-FRS multiplet structure consisting of a quadrupole triplet with<br />

octupole correction coils and two hexapole magnets. All magnets are located in a common cryostat. Hexapole<br />

magnets can also be inserted between two quadrupoles (indicated with dashed lines).<br />

45

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