Sökning: WFRF:(Phillips N) > (2005-2009) > The ATLAS semicondu...
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000 | 14398naa a2204225 4500 | |
001 | oai:DiVA.org:uu-144473 | |
003 | SwePub | |
008 | 110131s2007 | |||||||||||000 ||eng| | |
024 | 7 | a https://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-1444732 URI |
024 | 7 | a https://doi.org/10.1016/j.nima.2007.02.0192 DOI |
040 | a (SwePub)uu | |
041 | a engb eng | |
042 | 9 SwePub | |
072 | 7 | a ref2 swepub-contenttype |
072 | 7 | a art2 swepub-publicationtype |
100 | 1 | a Abdesselam, A.4 aut |
245 | 1 0 | a The ATLAS semiconductor tracker end-cap module |
264 | 1 | b Elsevier BV,c 2007 |
338 | a print2 rdacarrier | |
520 | a The challenges for the tracking detector systems at the LHC are unprecedented in terms of the number of channels, the required read-out speed and the expected radiation levels. The ATLAS Semiconductor Tracker. (SCT) end-caps have a total of about 3 million electronics channels each reading out every 25 ns into its own on-chip 3.3 mu s buffer. The highest anticipated dose after 10 years operation is 1.4x10(14) cm(-2) in units of 1 MeV neutron equivalent (assuming the damage factors scale with the non-ionising energy loss). The forward tracker has 1976 double-sided modules, mostly of area similar to 70 cm(2), each having 2 x 768 strips read out by six ASICs per side. The requirement to achieve an average perpendicular radiation length of 1.5% X-0, while coping with up to 7 W dissipation per module (after irradiation), leads to stringent constraints on the thermal design. The additional requirement of 1500e(-) equivalent noise charge (ENC) rising to only 1800e(-) ENC after irradiation, provides stringent design constraints on both the high-density Cu/Polyimide flex read-out circuit and the ABCD3TA read-out ASICs. Finally, the accuracy of module assembly must not compromise the 16 mu m (r phi) resolution perpendicular to the strip directions or 580 mu m radial resolution coming from the 40 mrad front-back stereo angle. A total of 2210 modules were built to the tight tolerances and specifications required for the SCT. This was 234 more than the 1976 required and represents a yield of 93%. The component flow was at times tight, but the module production rate of 40-50 per week was maintained despite this. The distributed production was not found to be a major logistical problem and it allowed additional flexibility to take advantage of where the effort was available, including any spare capacity, for building the end-cap modules. The collaboration that produced the ATLAS SCT end-cap modules kept in close contact at all times so that the effects of shortages or stoppages at different sites could be rapidly resolved. | |
650 | 7 | a NATURVETENSKAPx Fysik0 (SwePub)1032 hsv//swe |
650 | 7 | a NATURAL SCIENCESx Physical Sciences0 (SwePub)1032 hsv//eng |
653 | a silicon | |
653 | a module | |
653 | a microstrip | |
653 | a ATLAS | |
653 | a SCT | |
653 | a LHC | |
653 | a Physics | |
653 | a Fysik | |
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700 | 1 | a Zhu, H.4 aut |
700 | 1 | a Bingefors, Nilsu Uppsala universitet,Institutionen för kärn- och partikelfysik4 aut |
700 | 1 | a Brenner, Richardu Uppsala universitet,Institutionen för kärn- och partikelfysik4 aut |
700 | 1 | a Ekelöf, Tordu Uppsala universitet,Institutionen för kärn- och partikelfysik4 aut |
710 | 2 | a Uppsala universitetb Institutionen för kärn- och partikelfysik4 org |
773 | 0 | t Nuclear Instruments and Methods in Physics Research Section Ad : Elsevier BVg 575:3, s. 353-389q 575:3<353-389x 0168-9002x 1872-9576 |
856 | 4 8 | u https://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-144473 |
856 | 4 8 | u https://doi.org/10.1016/j.nima.2007.02.019 |
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