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The principle of operation of a micromegas chamber

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1 The principle of operation of a micromegas chamber
The MAMMA project Large-area micromegas muon chambers for the ATLAS upgrade Arizona, Athens (U, NTU, Demokritos), Brookhaven, CERN, JINR Dubna, Harvard, USTC Hefei, Istanbul (Bogaziçi, Doğuş), LMU Munich, Naples, South Carolina, CEA Saclay, Shandong, Stony Brook, St. Petersburg, Thessaloniki, U Washington -800 V -550 V The principle of operation of a micromegas chamber Amplification Gap 128 µm Conversion & drift space (few mm) To cope with the luminosity upgrade of the Large Hadron Collider at CERN (sLHC) ATLAS prepares for an upgrade of the muon system in, at least, the highest rapidity region. The MAMMA R&D activity focuses on the development of large-area muon detectors based on the bulk-micromegas technology as candidates for such an upgrade. The detectors will combine trigger and precision tracking in a single device. Their low costs, compared to other detector technologies, and their potential for industrial production make the bulk-micromegas excellent candidates for mass-construction of large muon chambers. Excellent performance Time bins (25 ns) Charge (200 e-) Strips (250 µm pitch) R14 R13 R12 R11 Standard Ar:CO2 gas mixtures (93:7, 85:15) Safe operating point with excellent efficiency for gas gains 3–5 x 103 (standard MMs) 1 x 104 (resistive MMs) Superb spatial resolution Rate capability > 106 Hz/cm2 500 µm strip pitch σMM = 36 ± 7 µm R ≈ 45 MΩ R ≈ 85 MΩ Convoluted resolution MM + external tracker Standard MM Straight Track through four chambers, in R14 the resistive layer is not segmented into strips 5.9 keV 55Fe γ’s cosmics R12 Ar:CO2 85:15 Gain ≈ 8000 x (mm) y (mm) Inefficient area (pillars) ≈1% R11 R12 Charge (200 e-) Time bins (25 ns) Cosmics spectrum MMs with resistive strips Inclined track (40°) through R11 and R12, illustrating the µTPC capability of MMs A novel scheme to make micromegas spark insensitive: resistive strips So far, six small prototype chambers (10 x 10 cm2 active area) with 250 µm r/o strip pitch Variety of resistance values Typical spark signals in a MM with resistive strips (terminated with 50 Ω) Spark signal is reduced by a factor of 1000 compared to a standard MM 2D readout x strips: 250/150 µm r/o and resistive strips y: 250/80 µm only r/o strips R16 Readout strips (0.25 mm) Charge (200 e– ) Time (25 ns ) Readout strips (0.25 mm) Charge (200 e– ) Time (25 ns ) PCB Mesh Resistive strips x strips y strips x strips y strips R12 chamber with 2D readout 5.9 keV 55Fe photon conversion signals as measured by the x and y strips in the R16 chamber Towards large-area detectors: the 1m2 chamber 2048 circular strips Strip pitch: 0.5 mm 8 connectors with 256 contacts each Mesh: 400 lines/inch 5 mm high frame defines drift space O-ring for gas seal Closed by a 10 mm foam sandwich panel serving at the same time as drift electrode This work is carried out in close collaboration with CERN/TE-MPE (R. de Oliveira) and in the context of the RD51 Collaboration


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