1
RD51 Collaboration: RD51 Collaboration: Development of Micro-Pattern Gaseous Detectors Development of Micro-Pattern Gaseous Detectors technologies technologies Matteo Alfonsi (CERN) on behalf of RD51 Collaboration Matteo Alfonsi (CERN) on behalf of RD51 Collaboration Current Trends in MPGD: Current Trends in MPGD: Technologies Technologies Electrons Electrons Ions Ions 60 % 40 % Micromegas Micromegas GEM GEM THGEM THGEM MHSP MHSP Ingrid Ingrid 0.18 0.18 m CMOS VLSI m CMOS VLSI CMOS high density CMOS high density readout electronics readout electronics Current Trends MPGD: Current Trends MPGD: Performance Performance Tracking - Micromegas Tracking - Micromegas TPC readout - GEM TPC readout - GEM UV photon detection UV photon detection - GEM - GEM Neutron detection Neutron detection - GEM - GEM Current Trends in MPGD: Applications Current Trends in MPGD: Applications COMPASS experiment at CERN has been the first application COMPASS experiment at CERN has been the first application of GEM and Micromegas detectors and MPGD are also present of GEM and Micromegas detectors and MPGD are also present in the apparatus of LHC experiments (LHCb and TOTEM). in the apparatus of LHC experiments (LHCb and TOTEM). Actually applications range in High Energy physics Actually applications range in High Energy physics environment as well as other fields: environment as well as other fields: High-Rate Particle Tracking and Triggering High-Rate Particle Tracking and Triggering Time Projection Chamber Readout Time Projection Chamber Readout Photon Detectors for Cherenkov Imaging Counters Photon Detectors for Cherenkov Imaging Counters X-Ray Astronomy X-Ray Astronomy Neutron Detection and Low Background Experiments Neutron Detection and Low Background Experiments Cryogenic Detectors Cryogenic Detectors Medical Applications Medical Applications Homeland Security and Prevention of Planetary Disasters Homeland Security and Prevention of Planetary Disasters More than 50 institutes More than 50 institutes from 20 countries and 4 continents from 20 countries and 4 continents decided to optimize efforts and decided to optimize efforts and resourses resourses joining forces in joining forces in RD51 RD51 collaboration collaboration 3M A3 TE347-6 Scienergy-65 3M B2 Std CERN1 More Polyimide Exposed (BNL) TE349-4 Detector Technology Detector Technology Currentl Currentl y y produced produced Future Future Requirement Requirement s s cm * cm cm * cm cm * cm cm * cm GEM GEM 40 * 40 40 * 40 50 * 50 50 * 50 GEM, single mask GEM, single mask 70 * 40 70 * 40 200 * 50 200 * 50 THGEM THGEM 70 * 50 70 * 50 200 * 100 200 * 100 RTHGEM, serial graphics RTHGEM, serial graphics 20 * 10 20 * 10 100 * 50 100 * 50 RTHGEM, Kapton RTHGEM, Kapton 50 * 50 50 * 50 200 * 100 200 * 100 Micromegas, bulk Micromegas, bulk 150 * 50 150 * 50 200 * 100 200 * 100 Micromegas, microbulk Micromegas, microbulk 10 * 10 10 * 10 30 * 30 30 * 30 MHSP (Micro-Hole and Strip MHSP (Micro-Hole and Strip Plate) Plate) 3*3 3*3 10*10 10*10 The Micro-Strip Gas Chamber, introduced by Oed in 1988 The Micro-Strip Gas Chamber, introduced by Oed in 1988 (NIMA 263, 351), was the first Micro-Pattern Gaseous (NIMA 263, 351), was the first Micro-Pattern Gaseous Detector; exploiting photolithography techniques for Detector; exploiting photolithography techniques for the production of micrometric structure of electrodes, the production of micrometric structure of electrodes, this family of gaseous detectors led to significant this family of gaseous detectors led to significant improvements in terms of rate capability and spatial improvements in terms of rate capability and spatial resolution with respect to the Multi-Wire Proportional resolution with respect to the Multi-Wire Proportional Chambers. Chambers. Structure, Structure, Y. Giomataris, NIMA 419 (1998), 239), Y. Giomataris, NIMA 419 (1998), 239), other examples of current R&D on other examples of current R&D on technologies are: technologies are: Thick-GEM Thick-GEM , , Micro Hole & Strip Micro Hole & Strip Plates Plates and other hole-type detectors; and other hole-type detectors; structures with resistive electrodes; the structures with resistive electrodes; the integration of the MPGD with CMOS pixel integration of the MPGD with CMOS pixel ASICs or the production of the two in the ASICs or the production of the two in the same process as in the case of Ingrid same process as in the case of Ingrid After 20 years, MPGD technologies are well established. After 20 years, MPGD technologies are well established. Beside well-known representatives, such as Beside well-known representatives, such as GEM GEM ( ( Gas Gas Electron Multiplier Electron Multiplier , F. Sauli, NIMA A386 (1997), 531) and , F. Sauli, NIMA A386 (1997), 531) and Micromegas Micromegas ( ( Micro Mesh Gaseous Micro Mesh Gaseous Rate Capability Rate Capability High Gain High Gain Space Resolution Space Resolution Time Resolution Time Resolution Energy Resolution Energy Resolution Ageing Properties Ageing Properties Ion Backflow Ion Backflow Reduction Reduction Photon Feedback Photon Feedback Reduction Reduction MPGDs can be optimize MPGDs can be optimize in order to achieve in order to achieve challenging performance challenging performance in terms of: in terms of: Rate capability Rate capability 2x10 2x10 6 p/mm p/mm 2 Spatial Spatial resolution resolution ~ 12 ~ 12 m Ar/CO2/CF4 Ar/CO2/CF4 (45/15/40) (45/15/40) Time Time resolution resolution rms = rms = 4.5ns 4.5ns GEM GEM THGEM THGEM Micromegas Micromegas GEM GEM Micromegas Micromegas Micromegas Micromegas 10 2 10 3 10 4 10 -5 10 -4 10 -3 10 -2 10 -1 F-R-M H SP/G EM /M H SP R-M HSP/G EM /M HSP E drift =0.2kV/cm Ar/C H 4 (95/5),760 Torr IBF Total gain MHSP MHSP High energy resolution High energy resolution Ion backflow Ion backflow High gain High gain Radiation hard Radiation hard WG1: Detector design WG1: Detector design optimization – Thick GEM rim optimization – Thick GEM rim example example RIM RIM 10 4 pitch = 1 mm; diameter = 0.5 mm; rim=40; 60; 80; 100; 120 mm A Thick GEM is a copper-clad fiberglass layer with a A Thick GEM is a copper-clad fiberglass layer with a matrix of holes realized by means of mechanical drilling matrix of holes realized by means of mechanical drilling and, in some cases, chemical etching. Tipical dimension and, in some cases, chemical etching. Tipical dimension are sub-millimetric. are sub-millimetric. The introduction of a rim The introduction of a rim on the two copper layers on the two copper layers is effective for the is effective for the increase of the maximum increase of the maximum achievable gain. achievable gain. On the other hand, due to On the other hand, due to the larger dielectric the larger dielectric surface exposed to the surface exposed to the charges produced in the charges produced in the avalanche, a larger rim avalanche, a larger rim shows also larger and shows also larger and longer charging-up longer charging-up effects, increasing the effects, increasing the time to arrive to a time to arrive to a stable operation stable operation WG1: Large area MPGD WG1: Large area MPGD Large GEM Large GEM detector detector exploiting single exploiting single mask technique mask technique Largest Thick GEM Largest Thick GEM Read-out board Laminated Photo- imageable cover lay frame Stretched mesh on frame Laminated Photo- imageable cover lay Raw material (50μm copper- clad kapton foil) Single side copper patterning Polyimide etching Copper reduction Bulk Micromegas Bulk Micromegas Single mask GEM Single mask GEM Limitations in MPGD size can come from the production Limitations in MPGD size can come from the production technique or the available instrumentations and raw technique or the available instrumentations and raw material. New production techniques can overcome these material. New production techniques can overcome these limitations and open the way to larger detectors, as in limitations and open the way to larger detectors, as in the case of the case of bulk micromegas bulk micromegas and and single mask GEM foils single mask GEM foils Stretched Stretched Mesh for 1x2 Mesh for 1x2 m 2 Bulk Bulk Micromegas Micromegas 60 cm 60 cm 60 cm 60 cm WG2: Charging-up and operation WG2: Charging-up and operation stability stability BAD YES ARALDITE AW 106 (Hardener HV 935 U) CERN/GDD ATLAS/TRT BAD - YES EPOTEK E905 CERN/GDD BAD - YES NORLAND NEA 123 (UV) CERN/GDD BAD - YES TECHNICOLL 8862 + (Hardener 8263) CERN/GDD BAD - YES NORLAND NEA 155 CERN/GDD CERN/GDD CERN/GDD CERN/GDD Source BAD BAD BAD Result YES YES DURALCO 4525 - YES Effect in G.D. YES HEXCEL A40 YES DURALCO 4461 Product Outgas In Use NO NO TRABOND 2115 ATLAS/TRT In Use NO NO ARALDITE AW103 (Hardener HY 991) CERN/GDD ATLAS/TRT In Use NO NO ECCOBOND 285 HERA-B/ITR CERN/GDD HERA-B/OTR CERN/GDD Source Out of production In Use Long curing time Note NO NO HEXCEL EPO 93L NO NO STYCAST 1266 (A+Catalyst 9) NO Effect in G.D. NO STYCAST 1266 (A+B) Outgas Product Due to the presence of dielectric in MPGD geometries, Due to the presence of dielectric in MPGD geometries, charging-up phenomena must be studied to understand the charging-up phenomena must be studied to understand the stability over time of the detector. stability over time of the detector. Different geometries or production process can lead to Different geometries or production process can lead to different behaviour. different behaviour. WG2: Aging and radiation hardness WG2: Aging and radiation hardness Construction components validation, such as glues and Construction components validation, such as glues and materials, is crucial for radiation hard detectors. materials, is crucial for radiation hard detectors. 7 WG4: Charging-up simulation WG4: Charging-up simulation Discrepancies in GEM detectors Discrepancies in GEM detectors simulation with respect to measurements simulation with respect to measurements can be explained by the charging-up of can be explained by the charging-up of the dielectric. Studies are under way the dielectric. Studies are under way to include this dynamic process in the to include this dynamic process in the simulation. simulation. WG4: Simulation improvements WG4: Simulation improvements New features have been introduced or are under way in New features have been introduced or are under way in Garfield, the main software for gas detector simulation, Garfield, the main software for gas detector simulation, in order to take into account the smaller scale of MPGD in order to take into account the smaller scale of MPGD technologies: technologies: a new algorithm for microscopic electron tracking and a new algorithm for microscopic electron tracking and avalanche avalanche the introduction of Penning transfer mechanism the introduction of Penning transfer mechanism the introduction of a Boundary Element Solver (NeBEM) the introduction of a Boundary Element Solver (NeBEM) for field calculations for field calculations the integration of Garfield in common platforms such as the integration of Garfield in common platforms such as ROOT and Geant4 ROOT and Geant4 organization in 7 Working organization in 7 Working Group Group WG3: Tracking and triggering WG3: Tracking and triggering applications applications A. Delbart, TIPP09 A. Delbart, TIPP09 T2K Micromegas TPC T2K Micromegas TPC WG7: Common test beam facility WG7: Common test beam facility Electron drift lines at Electron drift lines at t=0 t=0 no charges on kapton no charges on kapton surface surface Electron drift lines Electron drift lines modify when charges are modify when charges are accumulated on kapton accumulated on kapton surface surface RD51 is building up a semi-permanent test setup on RD51 is building up a semi-permanent test setup on the SPS/H4 beam line at CERN. Common infrastructures the SPS/H4 beam line at CERN. Common infrastructures such as cables, gas pipes, gas mixing system, as well such as cables, gas pipes, gas mixing system, as well as common devices for trigger and tracking telescope, as common devices for trigger and tracking telescope, common DAQ and analysis software will reduce common DAQ and analysis software will reduce installation dead times and will avoid duplication of installation dead times and will avoid duplication of efforts and resourses. efforts and resourses. Gas panel Setup A no magnet electr . rack for setup A Removable cable tray for setup A electr . rack for setup B Removable cable tray for setup B Setup B with magnet DAQ PC Height = 1.06 m R = 1.70 m Front opening = 2.40 m SPS/H4 beam line has been SPS/H4 beam line has been chosen for the chosen for the availability of the large availability of the large “Goliath” dipole magnet, “Goliath” dipole magnet, and for the large amount and for the large amount of space of the of space of the experimental zone, that experimental zone, that allows two setup at the allows two setup at the same time, one upstream same time, one upstream and the other inside the and the other inside the magnet magnet WG6: Common Production WG6: Common Production facilities facilities One of the main WG6 task is to promote the upgrade One of the main WG6 task is to promote the upgrade of the production facilities according to the of the production facilities according to the requirements of the future applications requirements of the future applications WG5: Multi-channel Readout WG5: Multi-channel Readout System System The development of a multi-channel scalable (from The development of a multi-channel scalable (from small test system to very large LHC-like system) are small test system to very large LHC-like system) are under way. A special effort is dedicated to make it under way. A special effort is dedicated to make it compatible to the largest possible set of current compatible to the largest possible set of current Front-End Electronics used in gaseous detectors Front-End Electronics used in gaseous detectors Corresponding author: [email protected] Corresponding author: [email protected] 1st EIROforum School on Instrumentation, CERN (Geneva, Switzerland), 11-15 May 2009 1st EIROforum School on Instrumentation, CERN (Geneva, Switzerland), 11-15 May 2009 Conferences and Workshops: Conferences and Workshops: Micro Pattern Gas Detectors. Towards an R&D Collaboration. Micro Pattern Gas Detectors. Towards an R&D Collaboration. (CERN, September 10-11, 2007) (CERN, September 10-11, 2007) Micro-Pattern Gas Detectors Workshop (Nikhef, April 16-18, Micro-Pattern Gas Detectors Workshop (Nikhef, April 16-18, 2008) 2008) 2nd RD51 Collaboration meeting (Paris, October 13-15, 2nd RD51 Collaboration meeting (Paris, October 13-15, 2008) 2008) MPGD2009 and MPGD2009 and 3rd RD51 Collaboration Meeting (Crete, 3rd RD51 Collaboration Meeting (Crete, June June 12-15, 2009) 12-15, 2009)

RD51 Collaboration: Development of Micro-Pattern Gaseous Detectors technologies

Embed Size (px)

DESCRIPTION

0.18 m m CMOS VLSI. 3M A3. 3M B2. Height = 1.06 m. Gas panel. electr. rack for setup B. electr. rack for setup A. DAQ PC. 10 4. Removable cable tray for setup B. Ions. TE347-6. R = 1.70 m. Removable cable tray for setup A. 40 %. 60 %. Electrons. Setup B with magnet. - PowerPoint PPT Presentation

Citation preview

Page 1: RD51 Collaboration: Development of Micro-Pattern Gaseous Detectors technologies

RD51 Collaboration:RD51 Collaboration:Development of Micro-Pattern Gaseous Detectors technologiesDevelopment of Micro-Pattern Gaseous Detectors technologies

Matteo Alfonsi (CERN) on behalf of RD51 CollaborationMatteo Alfonsi (CERN) on behalf of RD51 Collaboration

Current Trends in MPGD: TechnologiesCurrent Trends in MPGD: Technologies

ElectronsElectrons

IonsIons

60 %

40 %

MicromegasMicromegas GEMGEM THGEMTHGEM MHSPMHSP IngridIngrid

0.18 0.18 m CMOS VLSIm CMOS VLSI

CMOS high densityCMOS high densityreadout electronicsreadout electronics

Current Trends MPGD:Current Trends MPGD: PerformancePerformance

Tracking - MicromegasTracking - Micromegas TPC readout - GEMTPC readout - GEM UV photon detectionUV photon detection- GEM- GEM

Neutron detectionNeutron detection- GEM- GEM

Current Trends in MPGD: ApplicationsCurrent Trends in MPGD: Applications

COMPASS experiment at CERN has been the first application of GEM and COMPASS experiment at CERN has been the first application of GEM and Micromegas detectors and MPGD are also present in the apparatus of LHC Micromegas detectors and MPGD are also present in the apparatus of LHC experiments (LHCb and TOTEM).experiments (LHCb and TOTEM).Actually applications range in High Energy physics environment as well as Actually applications range in High Energy physics environment as well as other fields:other fields:• High-Rate Particle Tracking and TriggeringHigh-Rate Particle Tracking and Triggering• Time Projection Chamber ReadoutTime Projection Chamber Readout• Photon Detectors for Cherenkov Imaging CountersPhoton Detectors for Cherenkov Imaging Counters• X-Ray AstronomyX-Ray Astronomy• Neutron Detection and Low Background ExperimentsNeutron Detection and Low Background Experiments• Cryogenic DetectorsCryogenic Detectors• Medical ApplicationsMedical Applications• Homeland Security and Prevention of Planetary DisastersHomeland Security and Prevention of Planetary Disasters

More than 50 institutesMore than 50 institutesfrom 20 countries and 4 continentsfrom 20 countries and 4 continents

decided to optimize efforts and resoursesdecided to optimize efforts and resoursesjoining forces injoining forces in

RD51 collaborationRD51 collaboration

3M A3

TE347-6

Scienergy-65

3M B2

Std CERN1

Mor

e P

olyi

mid

e E

xpos

ed

(BNL)

TE349-4

Detector TechnologyDetector TechnologyCurrently Currently producedproduced

Future Future RequirementsRequirements

   cm * cmcm * cm cm * cmcm * cm

        

GEMGEM 40 * 4040 * 40 50 * 5050 * 50

GEM, single maskGEM, single mask 70 * 4070 * 40 200 * 50200 * 50

THGEMTHGEM 70 * 5070 * 50 200 * 100200 * 100

RTHGEM, serial graphicsRTHGEM, serial graphics 20 * 1020 * 10 100 * 50100 * 50

RTHGEM, KaptonRTHGEM, Kapton 50 * 50 50 * 50 200 * 100200 * 100

Micromegas, bulkMicromegas, bulk 150 * 50150 * 50 200 * 100200 * 100

Micromegas, microbulkMicromegas, microbulk 10 * 1010 * 10 30 * 3030 * 30

MHSP (Micro-Hole and Strip Plate)MHSP (Micro-Hole and Strip Plate) 3*33*3 10*1010*10

The Micro-Strip Gas Chamber, introduced by Oed in 1988 (NIMA 263, The Micro-Strip Gas Chamber, introduced by Oed in 1988 (NIMA 263, 351), was the first Micro-Pattern Gaseous Detector; exploiting 351), was the first Micro-Pattern Gaseous Detector; exploiting photolithography techniques for the production of micrometric structure of photolithography techniques for the production of micrometric structure of electrodes, this family of gaseous detectors led to significant improvements electrodes, this family of gaseous detectors led to significant improvements in terms of rate capability and spatial resolution with respect to the Multi-in terms of rate capability and spatial resolution with respect to the Multi-Wire Proportional Chambers.Wire Proportional Chambers.

Structure,Structure, Y. Giomataris, NIMA 419 (1998), 239), other Y. Giomataris, NIMA 419 (1998), 239), other examples of current R&D on technologies are: examples of current R&D on technologies are: Thick-GEMThick-GEM, , Micro Hole & Strip PlatesMicro Hole & Strip Plates and other hole-type detectors; and other hole-type detectors; structures with resistive electrodes; the integration of the structures with resistive electrodes; the integration of the MPGD with CMOS pixel ASICs or the production of the two MPGD with CMOS pixel ASICs or the production of the two in the same process as in the case of Ingridin the same process as in the case of Ingrid

After 20 years, MPGD technologies are well established.After 20 years, MPGD technologies are well established.Beside well-known representatives, such as Beside well-known representatives, such as GEMGEM ( (Gas Electron MultiplierGas Electron Multiplier, , F. Sauli, NIMA A386 (1997), 531) and F. Sauli, NIMA A386 (1997), 531) and MicromegasMicromegas ( (Micro Mesh GaseousMicro Mesh Gaseous

• Rate CapabilityRate Capability• High GainHigh Gain• Space ResolutionSpace Resolution• Time ResolutionTime Resolution• Energy ResolutionEnergy Resolution• Ageing PropertiesAgeing Properties• Ion Backflow ReductionIon Backflow Reduction• Photon Feedback ReductionPhoton Feedback Reduction

MPGDs can be optimize in MPGDs can be optimize in order to achieve challenging order to achieve challenging performance in terms of:performance in terms of:

Rate capabilityRate capability

2x102x1066 p/mm p/mm22

Spatial Spatial resolution resolution ~ 12 ~ 12 mm

Ar/CO2/CF4 Ar/CO2/CF4 (45/15/40)(45/15/40)Time Time resolutionresolutionrms = 4.5nsrms = 4.5ns

GEMGEM THGEMTHGEM

MicromegasMicromegas GEMGEM

MicromegasMicromegasMicromegasMicromegas

102 103 10410-5

10-4

10-3

10-2

10-1

F-R-MHSP/GEM/MHSP R-MHSP/GEM/MHSP

Edrift

=0.2kV/cm

Ar/CH4 (95/5), 760 Torr

IBF

Total gain

MHSPMHSP

High energy resolutionHigh energy resolutionIon backflowIon backflow

High gainHigh gain

Radiation hardRadiation hard

WG1: Detector design optimization WG1: Detector design optimization – Thick GEM rim example– Thick GEM rim example

RIMRIM

6 keV X-ray

104

pitch = 1 mm; diameter = 0.5 mm; rim=40; 60; 80; 100; 120 mm

A Thick GEM is a copper-clad fiberglass layer with a matrix of holes realized A Thick GEM is a copper-clad fiberglass layer with a matrix of holes realized by means of mechanical drilling and, in some cases, chemical etching. by means of mechanical drilling and, in some cases, chemical etching. Tipical dimension are sub-millimetric.Tipical dimension are sub-millimetric.

The introduction of a rim on the The introduction of a rim on the two copper layers is effective for two copper layers is effective for the increase of the maximum the increase of the maximum achievable gain.achievable gain.On the other hand, due to the On the other hand, due to the larger dielectric surface exposed larger dielectric surface exposed to the charges produced in the to the charges produced in the avalanche, a larger rim shows avalanche, a larger rim shows also larger and longer charging-up also larger and longer charging-up effects, increasing the time to effects, increasing the time to arrive to a stable operationarrive to a stable operation

WG1: Large area MPGDWG1: Large area MPGD

Large GEM detector Large GEM detector exploiting single mask exploiting single mask techniquetechnique

Largest Thick GEMLargest Thick GEM

Read-out board

Laminated Photo-imageable cover lay

frame

Stretched mesh on frame

Laminated Photo-imageable cover lay

Raw material(50μm copper-clad kapton foil)

Single side copper patterning

Polyimide etching

Copper reduction

Bu

lk M

icro

me

ga

sB

ulk

Mic

rom

eg

as

Sin

gle

ma

sk G

EM

Sin

gle

ma

sk G

EM

Limitations in MPGD size can come from the production technique or the Limitations in MPGD size can come from the production technique or the available instrumentations and raw material. New production techniques can available instrumentations and raw material. New production techniques can overcome these limitations and open the way to larger detectors, as in the overcome these limitations and open the way to larger detectors, as in the case of case of bulk micromegasbulk micromegas and and single mask GEM foilssingle mask GEM foils

Stretched Mesh Stretched Mesh for 1x2 mfor 1x2 m22 Bulk Bulk MicromegasMicromegas

60 cm60 cm

60 cm60 cm

WG2: Charging-up and operation stabilityWG2: Charging-up and operation stability

BADYESARALDITE AW 106

(Hardener HV 935 U)CERN/GDD

ATLAS/TRT

BAD-YESEPOTEK E905CERN/GDD

BAD-YESNORLAND NEA 123 (UV)CERN/GDD

BAD-YESTECHNICOLL 8862

+ (Hardener 8263)CERN/GDD

BAD-YESNORLAND NEA 155CERN/GDD

CERN/GDD

CERN/GDD

CERN/GDD

Source

BAD

BAD

BAD

Result

YESYESDURALCO 4525

-

YES

Effectin G.D.

YESHEXCEL A40

YESDURALCO 4461

Product Outgas

In UseNONOTRABOND 2115ATLAS/TRT

In UseNONOARALDITE AW103(Hardener HY 991)

CERN/GDD

ATLAS/TRT

In UseNONOECCOBOND 285HERA-B/ITR

CERN/GDD

HERA-B/OTR

CERN/GDD

Source

Out ofproduction

In Use

Longcuring time

Note

NONOHEXCEL EPO 93L

NONOSTYCAST 1266(A+Catalyst 9)

NO

Effect inG.D.

NOSTYCAST 1266(A+B)

OutgasProduct

Due to the presence of dielectric in MPGD geometries, charging-up phenomena Due to the presence of dielectric in MPGD geometries, charging-up phenomena must be studied to understand the stability over time of the detector.must be studied to understand the stability over time of the detector.Different geometries or production process can lead to different behaviour.Different geometries or production process can lead to different behaviour.

WG2: Aging and radiation hardnessWG2: Aging and radiation hardnessConstruction components validation, such as glues and materials, is crucial for Construction components validation, such as glues and materials, is crucial for radiation hard detectors.radiation hard detectors.

7

WG4: Charging-up simulationWG4: Charging-up simulation

Discrepancies in GEM detectors simulation with Discrepancies in GEM detectors simulation with respect to measurements can be explained by the respect to measurements can be explained by the charging-up of the dielectric. Studies are under way charging-up of the dielectric. Studies are under way to include this dynamic process in the simulation.to include this dynamic process in the simulation.

WG4: Simulation improvementsWG4: Simulation improvementsNew features have been introduced or are under way in Garfield, the main New features have been introduced or are under way in Garfield, the main software for gas detector simulation, in order to take into account the smaller software for gas detector simulation, in order to take into account the smaller scale of MPGD technologies:scale of MPGD technologies:

• a new algorithm for microscopic electron tracking and avalanchea new algorithm for microscopic electron tracking and avalanche

• the introduction of Penning transfer mechanismthe introduction of Penning transfer mechanism

• the introduction of a Boundary Element Solver (NeBEM) for field calculationsthe introduction of a Boundary Element Solver (NeBEM) for field calculations

• the integration of Garfield in common platforms such as ROOT and Geant4the integration of Garfield in common platforms such as ROOT and Geant4

organization in 7 Working Grouporganization in 7 Working Group

WG3: Tracking and triggering applicationsWG3: Tracking and triggering applications

A. Delbart, TIPP09A. Delbart, TIPP09

T2K Micromegas TPCT2K Micromegas TPC

WG7: Common test beam facilityWG7: Common test beam facility

Electron drift lines at t=0Electron drift lines at t=0no charges on kapton surface no charges on kapton surface

Electron drift lines modify when Electron drift lines modify when charges are accumulated on charges are accumulated on kapton surface kapton surface

RD51 is building up a semi-permanent test setup on the SPS/H4 beam RD51 is building up a semi-permanent test setup on the SPS/H4 beam line at CERN. Common infrastructures such as cables, gas pipes, gas line at CERN. Common infrastructures such as cables, gas pipes, gas mixing system, as well as common devices for trigger and tracking mixing system, as well as common devices for trigger and tracking telescope, common DAQ and analysis software will reduce installation telescope, common DAQ and analysis software will reduce installation dead times and will avoid duplication of efforts and resourses.dead times and will avoid duplication of efforts and resourses.

Gas panel

Setup A no magnet

electr. rack for setup A

Removable cable tray for

setup A

electr. rack for setup B

Removable cable tray for setup B

Setup Bwith magnet

DAQPC

Height = 1.06 m

R = 1.70 m

Front opening = 2.40 m

SPS/H4 beam line has been SPS/H4 beam line has been chosen for the availability of the chosen for the availability of the large “Goliath” dipole magnet, and large “Goliath” dipole magnet, and for the large amount of space of for the large amount of space of the experimental zone, that allows the experimental zone, that allows two setup at the same time, one two setup at the same time, one upstream and the other inside the upstream and the other inside the magnetmagnet

WG6: Common Production facilitiesWG6: Common Production facilitiesOne of the main WG6 task is to promote the upgrade of the production One of the main WG6 task is to promote the upgrade of the production facilities according to the requirements of the future applicationsfacilities according to the requirements of the future applications

WG5: Multi-channel Readout SystemWG5: Multi-channel Readout SystemThe development of a multi-channel scalable (from small test system to The development of a multi-channel scalable (from small test system to very large LHC-like system) are under way. A special effort is dedicated very large LHC-like system) are under way. A special effort is dedicated to make it compatible to the largest possible set of current Front-End to make it compatible to the largest possible set of current Front-End Electronics used in gaseous detectorsElectronics used in gaseous detectors

Corresponding author: [email protected] author: [email protected] 1st EIROforum School on Instrumentation, CERN (Geneva, Switzerland), 11-15 May 20091st EIROforum School on Instrumentation, CERN (Geneva, Switzerland), 11-15 May 2009

Conferences and Workshops:Conferences and Workshops:• Micro Pattern Gas Detectors. Towards an R&D Collaboration.Micro Pattern Gas Detectors. Towards an R&D Collaboration.

(CERN, September 10-11, 2007)(CERN, September 10-11, 2007)

• Micro-Pattern Gas Detectors Workshop (Nikhef, April 16-18, 2008)Micro-Pattern Gas Detectors Workshop (Nikhef, April 16-18, 2008)

• 2nd RD51 Collaboration meeting (Paris, October 13-15, 2008)2nd RD51 Collaboration meeting (Paris, October 13-15, 2008)

• MPGD2009 and MPGD2009 and 3rd RD51 Collaboration Meeting (Crete, 3rd RD51 Collaboration Meeting (Crete, June 12-15, 2009)June 12-15, 2009)