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ITk radiation monitoring I. Mandić et al. Jožef Stefan Institute, Ljubljana, Slovenia

ITk radiation monitoring I. Mandić et al. Jožef Stefan Institute, Ljubljana, Slovenia. Introduction: goal of radiation monitoring system is measurement of displacement damage in Si caused by energetic

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ITk radiation monitoring I. Mandić et al. Jožef Stefan Institute, Ljubljana, Slovenia

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  1. ITk radiation monitoring I. Mandić et al. Jožef Stefan Institute, Ljubljana, Slovenia SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  2. Introduction: • goal of radiation monitoring system is measurement of displacement damage in Si caused by energetic • hadrons (NIEL - 1 MeV neqfluence) and TID at several locations in the detector • to cross check radiation background simulations • online (remote) readout of sensors: •  necessary in the ITkbecause there is no access to replace passive dosimeters •  frequent measurements, up to date information about doses and fluences, better accuracy, • better control of annealingeffects… • dose monitoring more important at start of operation: •  early comparison with radiation background simulations •  doses proportional to integrated luminosity  measure dose/integrated_luminosity • accuracy less important at high doses towards the end of operation SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  3. Introduction • ITk radiation monitor system: • measure TID from ~ 1 kGy to ~100 kGy • measure Фeqfrom ~ 1013 to ~ 1015 n/cm2 • precision about ~20% • build a similar system to the one now running in ATLAS ID Results of radiation monitoring system in ATLAS ID for Run 2: SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  4. Sensors • NIEL: • OSRAM BPW34 diodes • measure forward bias at 1 mA forward current • can be used up to1e15 n/cm2 •  needs sufficiently high bias voltages • F. Ravotti et al. , IEEE TNS, VOL. 55, (2008), p 2133 • M.R. Hoeferkamp, et al., NIMA 890 (2018) 108-111, https://doi.org/10.1016/j.nima.2018.02.070 • P. Palni, et al., NIMA 735 (2014) 213–217, • http://dx.doi.org/10.1016/j.nima.2013.09.037 M.R. Hoeferkamp et al. NIMA 890 (2018) 108-111 SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  5. Sensors • TID: • RadFET(p-MOS transistors) • measure gate voltage at given drain current • need thin oxide RadFETs for high doses (above few kGy) •  not many manufacturers •  a set of devices (REM, oxide thickness 130 nm) • used in ATLAS ID available from the PS-IRRAD team •  new manufacturer: AbantIzzetBaysal University, Bolu, Turkey • (Center of Nuclear Radiation Detector Research and Application (NURDAM)) • Promising results at high doses with 65 nm oxide • thickness devices • Selection of sensors: max. response at highest doses, • minimum fading after hadron irradiation •  irradiation studies are going on NurFET See: A.H. Siedle, F. Ravotti, M.Glaser, The Dosimetric Performance of RADFETs in Radiation Test Beams 2007 IEEE Radiation Effects Data Workshop, https://doi.org/10.1109/REDW.2007.4342539 SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  6. Locations • max. fluence ~ 1e15 neq/cm2 • max. TID~ 1e5 Gy •  doses/fluences are proportional to integrated luminosity sensitivity up to maximal doses/fluences not critical, monitors can be placed also in locations with somewhat higher doses SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  7. Locations fixed on outer side of Outer Cylinder • fixed on the blades of disk 1 or disk 2 • inside tracking volume, connection goes • through the enclosure strip EC service volume, outer side of the bulkhead pixel service volume outside of the enclosure SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  8. Radiation Monitor Sensor Board (RMSB) • example from ATLAS ID shown on photos Back side ( heater for temp stabilization) Sensor side Pigtail cable • Ceramic (Al2O3) • front side: sensors • back side: resistive layer • Very similar design for ITk: • 3 RadFETs (TID) • temperature sensor (10 kOhmNTC) • 3 BPW34 diodes (NIEL) PCB ~ 2.2 cm SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  9. Radiation Monitor Sensor Board (RMSB) • hybrid fixed inside PEEK box, 3 cm x 3 cm, 0.8 cm thick, • flat cable soldered and clamped to the PCB • cable connector, 1.27 mm pitch (ERNI or 3M SN: 45110-000000) Sensor box 3 cm x 3 cm 8 mm thick • Photo of the connector on the mockup : • ERNI, 1.27 mm pitch, flat cable, 30 AWG wires • this is an example of possible connector Mockup with ~ 1 m pigtail • Connections: • monitors inside tracking volume (8 locations, 4 per side on strip EC) will be connected via PP1, • 2 RMSB in contiguous quadrants will connect to one connector at high radius in one EC tray •  connection of remaining RMSB (not entering the enclosure) to type II cables needs to be defined SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  10. Readout • measure voltage over radiation sensor at given current • current pulses ~0.1 mA (RADFET), ~ 1 mA (diode), < 1 s long, voltage from ~ 0 V to ~ 100 V after highest doses •  use voltage divider to adapt to ADC dynamic range, may be adjusted during operation to follow • large increase of voltage after exposure to large doses/fluneces •  ADC with 12 bit resolution OK • read few times per hour •  when not read out no bias (sensor contacts shorted) • temperature stabilization: DC current to heat ceramic hybrid (~2 W for ΔT = 60°C  50 mA at 40 V) • 6 radiation sensors (3 NIEL, 3 TID)+ 1 temperature sensor + return wire + temperature stabilization pair •  10 wires per RMSB • readout circuitry (current sources, ADCs …) in USA15 SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  11. Readout Read sensors one by one, few times per hour • readout based on ELMB2  same functionality as ELMB, communication with DCS via ELMB2 • similar radiation monitor readout system running now in the ID adapt firmware for ELMB2 •  build new current source unit controlled by ELMB2: • a) chose DAC compatible with ELMB2 firmware • b) output up to 100 V •  readout system must meet grounding and shielding requirements •  floating power supply referenced at the Faraday cage • design of current sources and monitoring circuits will follow the solutions described in: • ATL-IP-ES-0106 The Supply and Control system for the Opto Link of the ATLAS pixel detector SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  12. Schedule • monitors in EC volume (z ~ 160 cm, r ~ 60 cm, 8 locations) connected via PP1 •  cables/connectors up to PP1 should be ready for installation in the beginning of 2021 •  sensor boards with pigtail cable will be installed in ~ 2023 • other locations: •  installation in 2024 or 2025 •  not connected via PP1, connections to type II services to be defined • readout •  components in USA15 •  readout based on ELMB2 •  integrated in DCS by the start of HL-LHC SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

  13. Summary • radiation monitoring system for ATLAS ITk • measure NIEL (1 MeV neqfluence) and TID in Si at several locations in the detector to cross check radiation • background simulations • similar system as currently running in ATLAS ID • sensor candidates with required properties found, selection of RadFET manufacturer has to be made • locations defined • readout system will be based on ELMB2 • sensor boards and readout will be designed and manufactured by Jožef Stefan Institute SPR ITK common environmental monitoring and interlocking - radiation monitoring, 24th September 2019

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