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A GEM Detector System for an Upgrade of the CMS Muon Endcaps

A GEM Detector System for an Upgrade of the CMS Muon Endcaps

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Notice that pivot <strong>an</strong>d feet must both be mounted with a rotation <strong>of</strong> 180 ◦ with respect to <strong>the</strong> chimney, depending<br />

on <strong>the</strong> type <strong>of</strong> SC. If better mounting precision would be needed, <strong>the</strong> central screws <strong>of</strong> <strong>the</strong> feet c<strong>an</strong> be replaced by<br />

pins. Similar solution <strong>for</strong> pivots<br />

Due to <strong>the</strong> weight <strong>of</strong> each SC, a jig could be necessary <strong>for</strong> <strong>the</strong> insertion. The one which was used <strong>for</strong> <strong>the</strong> <strong>Muon</strong><br />

chambers could probably be adapted <strong>for</strong> that purpose (Fig. 78). The rails with T-grooves, <strong>for</strong> sliding <strong>an</strong>d <strong>the</strong>n<br />

stopping (eventually rotating) <strong>the</strong> SC, are already mounted in <strong>the</strong> back-fl<strong>an</strong>ges <strong>of</strong> <strong>CMS</strong>.<br />

B.5 Preliminary considerations GE2/1<br />

Based on <strong>the</strong> work accomplished <strong>for</strong> GE1/1, we have begun studies with <strong>the</strong> purpose <strong>of</strong> also installing <strong>GEM</strong><br />

chambers in <strong>the</strong> zone ME2/1, more exactly on <strong>the</strong> backside <strong>of</strong> YE1 (compression side).<br />

This zone was in principle <strong>for</strong>eseen <strong>for</strong> containing RE2/1 chambers but <strong>the</strong>y have never being mounted <strong>the</strong>re. In<br />

fact, only RE2/2 <strong>an</strong>d RE2/3 were installed. In <strong>the</strong> following photo, <strong>the</strong> red painted circle on <strong>the</strong> yoke would be <strong>the</strong><br />

place to be used <strong>for</strong> GE2/1 chambers:<br />

In each side <strong>of</strong> <strong>the</strong> detector <strong>the</strong> set consists <strong>of</strong> 18 GE2/1 chambers, each sp<strong>an</strong>ning 20 ◦ in φ <strong>an</strong>gle. As seen in<br />

GE1/1, <strong>the</strong> GE2/1 chambers overlap to provide continuous coverage in φ. There are 2 possible geometries to be<br />

envisaged. They depend on <strong>the</strong> possibility <strong>of</strong> c<strong>an</strong>tilever a part <strong>of</strong> each chamber on top <strong>of</strong> <strong>the</strong> neutron shielding <strong>of</strong><br />

YE/1 disk (short version in blue, long version in grey). As you c<strong>an</strong> see above, <strong>the</strong> dist<strong>an</strong>ce from <strong>the</strong> beamline to<br />

<strong>the</strong> bottom side <strong>of</strong> <strong>the</strong> chamber is 1960 (short version). Hereafter its shown <strong>the</strong> dist<strong>an</strong>ce from <strong>the</strong> IP to <strong>the</strong> backside<br />

<strong>of</strong> <strong>the</strong> yoke (7869mm), but <strong>the</strong> gap between <strong>the</strong> yoke <strong>an</strong>d <strong>the</strong> chambers is not definitely determined yet.<br />

90

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