Recent DHCAL Developments Jos Repond and Lei Xia Argonne National - - PowerPoint PPT Presentation

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Recent DHCAL Developments Jos Repond and Lei Xia Argonne National - - PowerPoint PPT Presentation

Recent DHCAL Developments Jos Repond and Lei Xia Argonne National Laboratory Linear Collider Workshop 2013 University of Tokyo November 11 15, 2013 The DHCAL Description 54 active layers Resistive Plate Chambers with 1 x 1 cm 2 pads


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SLIDE 1

Recent DHCAL Developments

José Repond and Lei Xia Argonne National Laboratory

Linear Collider Workshop 2013 University of Tokyo November 11 – 15, 2013

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SLIDE 2
  • J. Repond - Imaging Calorimeters
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The DHCAL

Description 54 active layers Resistive Plate Chambers with 1 x 1 cm2 pads → ~500,000 readout channels Main stack and tail catcher (TCMT) Electronic readout 1 – bit (digital) Digitization embedded into calorimeter Tests at FNAL with Iron absorber in 2010 - 2011 Tests at CERN with Tungsten absorber 2012 1st time in calorimetry

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SLIDE 3 J.Repond DHCAL 3

DHCAL Construction

Fall 2008 – Spring 2011 Resistive Plate Chamber

Sprayed 700 glass sheets Over 200 RPCs assembled → Implemented gas and HV connections

Electronic Readout System

10,000 ASICs produced (FNAL) 350 Front-end boards produced → glued to pad-boards 35 Data Collectors built 6 Timing and Trigger Modules built

Assembly of Cassettes

54 cassettes assembled Each with 3 RPCs and 9,216 readout channels

350,208 channel system in first test beam Event displays 10 minutes after closing enclosure Extensive testing at every step

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SLIDE 4 J.Repond DHCAL 4

Testing in Beams

Fermilab MT6

October 2010 – November 2011 1 – 120 GeV Steel absorber (CALICE structure)

CERN PS

May 2012 1 – 10 GeV/c Tungsten absorber (structure provided by CERN)

CERN SPS

June, November 2012 10 – 300 GeV/c Tungsten absorber

Test Beam Muon events Secondary beam Fermilab 9.4 M 14.3 M CERN 4.9 M 22.1 M TOTAL 14.3 M 36.4 M

A unique data sample

RPCs flown to Geneva All survived transportation

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SLIDE 5 J.Repond: DHCAL 5

Recent developments

Improved Resistive Plate Chambers 1-glass design High-rate RPCs High voltage distribution system Gas recirculation system

Resistive paint Resistive paint Mylar 1.2mm gas gap Mylar Aluminum foil 1.1mm glass 1.1mm glass
  • HV
Signal pads G10 board

Typical RPC design

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SLIDE 6

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1-glass RPCs

Offers many advantages

Pad multiplicity close to one → easier to calibrate Better position resolution → if smaller pads are desired Thinner → t = tchamber + treadout = 2.4 + ~1.5 mm → saves on cost Higher rate capability → roughly a factor of 2

Status

Built several large chambers Tests with cosmic rays very successful → chambers ran for months without problems Both efficiency and pad multiplicity look good

Efficiency Pad multiplicity

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SLIDE 7
  • J. Repond - The DHCAL
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Rate capability of RPCs

Measurements of efficiency

With 120 GeV protons In Fermilab test beam

Rate limitation

NOT a dead time But a loss of efficiency

Theoretical curves

Excellent description of effect

Rate capability depends

Bulk resistivity Rbulk of resistive plates (Resistivity of resistive coat)

Not a problem for an HCAL at the ILC

B.Bilki et al., JINST 4 P06003(2009)

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SLIDE 8 J.Repond: DHCAL 8
  • C. Pecharromán X. Workshop on RPC and related Detectors (Darmstadt)

Here is the problem There is a gap between 10-9 and 10-3

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SLIDE 9 J.Repond: DHCAL 9

Available resistive plates

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Float glass Semi- conductive glass Ceramics

Streamer mode Warm glass

Beijing CBM Requirement

Beijing INR+CBM lip Coimbra ALICE-muon LHCb ATLAS Warsaw CMS-forward CMS-barrel CERN+Bologna CERN+Rio Dresden STAR ALICE-TOF Lip+USC

Max Counting Rate(Hz/cm

2)

Volume Resistivity(cm)

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SLIDE 10 J.Repond: DHCAL 10

Where to use high-rate RPCs

ILC – Hadron calorimeter (close to beam pipe) CLIC – Hadron calorimeter (forward direction – 2γ background) CMS – Hadron calorimeter (forward direction)

Current forward calorimeters inadequate for high-luminosity running PbWO4 Crystals Scintillator/Brass + Quartz fibers/Steel To start in year ~2023 Luminosity of 5 x 1034 cm-2 (> x10 higher than now)

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SLIDE 11 J.Repond: DHCAL 11

High-rate Bakelite RPCs

Bakelite does not break like glass, is laminated but changes Rbulk depending on humidity but needs to be coated with linseed oil

Gas inlet Gas outlet Gas flow direction Fishing line Sleeve around fishing line Additional spacer Use of low Rbulk Bakelite with Rbulk ~ 108 - 1010 and/or Bakelite with resistive layer close to gas gap Several chambers built at ANL Gas

Resistive layer for HV

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SLIDE 12 J.Repond: DHCAL 12

High-rate Bakelite RPCs

Bakelite does not break like glass, is laminated but changes Rbulk depending on humidity but needs to be coated with linseed oil

Gas inlet Gas outlet Gas flow direction Fishing line Sleeve around fishing line Additional spacer Use of low Rbulk Bakelite with Rbulk ~ 108 - 1010 and/or Bakelite with resistive layer close to gas gap Several chambers built at ANL Gas

Resistive layer for HV

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SLIDE 13

Noise measurement: B01

1st run at 6.4 kV Last run, also 6.4kV, RPC rotated 900 Readout area Fishing lines (incorporated resistive layers)

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SLIDE 14 J.Repond: DHCAL 14

Noise measurements

Applied additional insulation Rate 1 – 10 Hz/cm2 (acceptable) Fishing lines clearly visible Some hot channels (probably on readout board) No hot regions

Cosmic ray tests

Stack including DHCAL chambers for tracking Efficiency, multiplicity measured as function of HV High multiplicity due to Bakelite thickness (2 mm)

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SLIDE 15 J.Repond: DHCAL 15

Tests carried out by University of Michigan, USTC, Academia Sinica

GIF Setup at CERN

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SLIDE 16 J.Repond: DHCAL 16

First results from GIF

Source on Source off Background rate Absolute efficiency not yet determined Clear drop seen with source on Background rates not corrected for efficiency drop Irradiation levels still to be determined (calculated)

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SLIDE 17 J.Repond: DHCAL 17

Development of semi-conductive glass

Co-operation with COE college (Iowa) and University of Iowa World leaders in glass studies and development Vanadium based glass Resistivity tunable Procedure aimed at industrial manufacture (not expensive) First samples Very low resistivity Rbulk ~ 108 Ωcm New glass plates Rbulk ~ 1010 Ωcm produced Plates still need to be polished Production still being optimized

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SLIDE 18

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High Voltage Distribution System

Generally

Any large scale imaging calorimeter will need to distribute power in a safe and cost-effective way

HV needs

RPCs need of the order of 6 – 7 kV

Specification of distribution system

Turn on/off individual channels Tune HV value within restricted range (few 100 V) Monitor voltage and current of each channel

Status

Iowa started development First test with RPCs encouraging Work stopped due to lack of funding

Size of noise file (trigger-less acquisition)

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SLIDE 19 19

Gas Recycling System

DHCAL’s preferred gas Development of ‘Zero Pressure Containment’ System

Work done by University of Iowa/ANL

Status

First parts assembled…

Gas Fraction [%] Global warming potential (100 years, CO2 = 1) Fraction * GWP Freon R134a 94.5 1430 1351 Isobutan 5.0 3 0.15 SF6 0.5 22,800 114

Recycling mandatory for larger RPC systems

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SLIDE 20 J.Repond: DHCAL 20

Summary

After successful testing of the DHCAL at Fermi and CERN Further improvements to the active medium and its supplies Development of 1-glass RPCs (design validated!) Development of low-resistivity bakelite/glass (ongoing, but encouraging) Development of a high-voltage distribution system (stalled) Development of a gas recirculation system (new concept, being assembled)

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SLIDE 21 J.Repond: DHCAL 21

Backup

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SLIDE 22 J.Repond: DHCAL 22

CMS forward calorimeter

Driven by successful application of PFAs to CMS analysis Proposal to replace forward calorimeters with an IMAGING CALORIMETER Several members of CALICE have been contacted by CMS

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SLIDE 23 J.Repond: DHCAL 23

Formidable challenge

Charged particle flux In calorimeter volume up to 50 MHz/cm2 at shower maximum Total dose Fluences of 1016 neutrons