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A Digital Hadron Calorimeter ?

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Title: Towards a Digital Hadron Calorimeter Author: Vishnu V. Zutshi Last modified by: Vishnu V. Zutshi Created Date: 3/20/2002 10:58:59 PM Document presentation format – PowerPoint PPT presentation

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Title: A Digital Hadron Calorimeter ?


1
A Digital Hadron Calorimeter ?
  • Vishnu V. Zutshi
  • NIU/NICADD

2
The proposal
  • Development of New Hadronic Calorimetery
    Technology
  • G. Blazey, D. Chakraborty, A. Dyshkant, M.
    Martin,
  • V. Rykalin, V. Zutshi
  • NIU/NICADD
  • A. Brandt, K. De, A. White, J. Yu
  • UTA

Arrive at a realistic cost estimate for one of
these devices
3
From analog to digital
  • Eflow seems to be a promising option for
    improving jet resolutions significantly
  • ALEPH and CDF have successfully used it
  • Requires a high granularity calorimeter
  • Digital hadron calorimeters high granularity at
    affordable price ?

4
General Considerations
  • Granularity (energy and resolving power)
  • MIP recognition
  • Absorber density (optimize shower lateral size)
  • Depth
  • Matching to EM calorimeter
  • Readout (2d preferred to strip type)
  • Minimal intrusions

5
Energy and position
6
Too much of a good thing?
7
Analog and Digital
20 GeV pions in SD
8
Single Particle Resolutions
9
On the software side of things
  • Prototype simulations
  • try out different cell shapes
  • parameterized losses from test stand
  • hoping to do this in GEANT4 framework
  • Event generation and LC detector simulation
  • Eflow algorithm development
  • starting with the EM section

10
The Algorithm (cal-seeded)
  • Layer-by-layer clustering based on a search for
    local maxima
  • Cluster definition based on nearest neighbour
  • Track extrapolation through the calorimeter
    picking clusters in its path
  • EM/HAD. Charged/neutral discrimination
  • Understanding of errors involved with the
    tracking and calorimetric measurements

11
Sanity Checks
clusters
hits
12
Initial concept (scintillator-based)
Four concentric layers of towers (7 stacks of
6-12 cells to a tower) formed with hexagonal
cells. Start with 9cm2 cell.
13
Initial concept (scintillator-based)
  • Conversion to current
  • VLPCs
  • APDs
  • MRSs
  • PMTs
  • Cost per channel v/s S/N

14
Test stand
Cell with WLS fiber irradiated by a radioactive
or LED WLS fiber connected to clear fiber which
is connected to a photodetector (PMTs, VLPCs
etc.) Output measured by a Pico ammeter
15
Test goals
Find minimum area/thickness of cell Find minimum
length of WLSF
Measure signal losses at the WLSF to clear fiber
transition
16
MIP signal
With VLPC readout
9mm thickness,0.5mm fiber,2optical connectors
17
Initial concept (gas-based)
  • GEM approach
  • Developed initially for MSGCs
  • Can be used with printed circuit readout
  • GEMs with gains above 104 and spark
    probabilities lt 10-10 have been developed
  • Reasonably fast operation
  • Relatively low HV

18
Initial concept (gas-based)
19
Issues/concerns (gas-based)
  • Cost of GEM layers
  • Lifetime/damage to layers
  • Effects of highly ionizing particles
  • Gas(es) ?
  • Mechanical stability of GEM gaps/supports
  • Cross-talk
  • ..

20
Summary
  • Single cell characterization studies have begun
  • GEM based feasibility studies starting soon
  • Event generation and simulation server ready
  • Setting up for GEANT4 based prototype simulation
    studies
  • Eflow algorithm development underway
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