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Micro MEsh GASeous Detectors (MicroMegas)

Micro MEsh GASeous Detectors (MicroMegas). RD51 Electronics school CERN 3 – 5 February 2014. What are Micromegas ?. Micromegas are parallel-plate chambers where the amplification takes place in a thin gap, separated from the conversion region by a fine metallic mesh

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Micro MEsh GASeous Detectors (MicroMegas)

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  1. Micro MEshGASeous Detectors(MicroMegas) RD51 Electronics schoolCERN 3 – 5 February 2014

  2. What are Micromegas ? • Micromegas are parallel-plate chambers where the amplification takes place in a thin gap, separated from the conversion region by a fine metallic mesh • The thin amplification gap (short drift times and fast absorption of the positive ions) makes it particularly suited for high-rate applications -800 V -550 V Conversion & drift space (few mm) Mesh Amplification Gap 128 µm The principle of operation of a MicroMegas chamber RD51 Electronics School

  3. The bulk MicroMegas technique Drift UV 5 mm Pillars (Ø ~300μm) Mask 128 µm PCB 250 µm 150 µm RD51 Electronics School

  4. Bulk MicroMegas structure • Standard configuration • Pillars every 5 (or 10) mm • Pillar diameter ≈350 µm • Dead area ≈1.5 (0.4)% • Amplification gap 128 µm • Mesh: 325 lines/inch Pillar distance on photo: 2.5 mm RD51 Electronics School

  5. MicroMegas as μTPC µ HV = -850 V HV = -550 V RD51 Electronics School

  6. Operating parameters • Chambers are operating with an Ar:CO2 (93:7) gas mixture (same gas as MDTs, safe and cheap, no flammable components) • High Voltage (moderate HV requirements) • Mesh: -500 V (amplification field 40-50 kV/cm) • Drift-electrode: -800 V (~600 V/cm) • Currents in nArange RD51 Electronics School

  7. Performance requirements • Spatial resolution: ~60 m • Angular resolution: ~0.3 mrad • Good double track resolution • Trigger capability • Efficiency:> 98% RD51 Electronics School

  8. Sparks in the chamber Mesh support pillars Mesh PCB Read-out strip Sparks between mesh and readout strips may damage the detector and readout electronics and/or lead to large dead times as a result of HV breakdown RD51 Electronics School

  9. Resistive MicroMegas chambers To avoid spark effect the readout strips were covered with the 64 µm thick insulator layer with resistive strips on top of it connected to the +HV via discharge resistor and mesh is connected to GND Resistive characteristics of the chambers Resistive strip 0.5-5 MΩ/cm PCB Read-out strip Insulator Embedded resistor 15-45 MΩ 5mm long +500V Read-out strip PCB RD51 Electronics School

  10. Resistive MicroMegas chambers -300V First 2D chambers with the “spark protection” resistive strips R16, R17, R18 Pitch: all strips – 250 µm; Width: resistive – 60 µm Y-strips – 100 µm X-strips – 200 µm 5 mm +500V GND 128 µm Y-strips X-strips RD51 Electronics School

  11. Standard chamber vs resistive MicroMegas mesh currents and HV drop in neutron beam Gas: Ar:CO2 (85:15) Neutron flux: ≈ 106 n/cm2/sec Standard MM: Large currents Large HV drops, recovery time O(1s) Chamber could not be operated stably R11: Low currents Despite discharges, but no HV drop Chamber operated stably up to max HV HV values Mesh currents RD51 Electronics School

  12. Spark signals resistive vs standard Sparks measured directly on readout strips through 50 Ohm Several spark signals plotted on top of each other to enhance the overall characteristics R12 shows 2-3 order of magnitude less signal and shorter recovery time than standard MM -600 -400 -200 0 10 µs RD51 Electronics School

  13. Equivalent scheme of resistive MicroMegas chambers -HV Mesh Induced charge C2 Resistive strip C1 C3 Amp Copper strip R1 CA C4 C1 – capacitance Mesh to ground C2 – capacitance R-strip to ground C3 – capacitance R-strip to readout strip C4 – capacitance readout strip to ground CA – input capacitance of preamplifier RD51 Electronics School

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