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Muon-Muon and Other High Energy Colliders

1997, Techniques and Concepts of High-Energy Physics IX

BACKGROUND AND DETECTOR Design of the Intersection Region The design of the Intersection Regionistumer is driven by the desire to reduce the background from muon decays in the detector as much as possible. For this study a 130 m final focus section (iuliu1) which included four final quadrupoles, three toroids, a 2 T solenoidal field for the detector and the connecting beam pipe and shielding was modeled in GEANT with all the appropriate magnetic fields and shielding materials. The parameters used were taken from ffref29. Trajectories of particles with and without decay are shown later in Figs.fg.iuliu6 and fg.iuliu7. Studies of the effects of high energy electrons hitting specific edges and surfaces were carried out and the shielding adjusted or augmented to mitigate the apparent effects of particular background problems. Effects due to electrons, photons, neutrons and charged hadrons and muons were considered in turn to try to optimized the design. While the current design is not fully optimized, it is a marked improvement over a much simpler design which had been used in the past. More importantly, it helped develop the tools and strategy to do such an optimization as the lattice is further developed. A second studymokhovov d eteusingasomewhatdif f erentf inalf ocusdesignandselectingshieldingparametershasgivenresults figure[htb!] file=mumuniceall.ai,width=15in,height=5in [Region around the Intersection Region modeled in GEANT. ] Region around the Intersection Region modeled in GEANT. The black regions represent tungsten shielding. The final quadrupoles (Q) and toroids (T) on one side of the detector enclosure are shown. The shaded areas around the intersection point represent the various detector volumes used in calculating particle fluences. fg.iuliu1

BACKGROUND Design of the Intersection AND DETECTOR Region The design of the Intersection Regionistumer is driven by the desire to reduce the background from muon decays in the detector as much as possible. For this study a 130 m final focus section (iuliu1) which included four final quadrupoles, three toroids, a 2 T solenoidal field for the detector and the connecting beam pipe and shielding was modeled in GEANT with all the appropriate magnetic fields and shielding materials. The parameters used were taken from ffref29. Trajectories of particles with and without decay are shown later in Figs.fg.iuliu6 and fg.iuliu7. Studies of the effects of high energy electrons hitting specific edges and surfaces were carried out and the shielding adjusted or augmented to mitigate the apparent effects of particular background problems. Effects due to electrons, photons, neutrons and charged hadrons and muons were considered in turn to try to optimized the design. While the current design is not fully optimized, it is a marked improvement over a much simpler design which had been used in the past. More importantly, it helped develop the tools and strategy to do such an optimization as the lattice is further developed. A second studymokhovovdeteusingasomewhatdif f erentf inalf ocusdesignandselectingshieldingparametershasgivenresults figure[htb!] file=mumuniceall.ai,width=15in,height=5in [Region around the Intersection Region modeled in GEANT. ] Region around the Intersection Region modeled in GEANT. The black regions represent tungsten shielding. The final quadrupoles (Q) and toroids (T) on one side of the detector enclosure are shown. The shaded areas around the intersection point represent the various detector volumes used in calculating particle fluences. fg.iuliu1 1