Elmaddin Guliyev LLR-Ecole Polytechnique, CNRS/IN2P3 Palaiseau, France ASIC readout for Electomagnetic Calorimeter for future Linear Collider Experiment
Jun 19, 2015
Elmaddin Guliyev
LLR-Ecole Polytechnique, CNRS/IN2P3Palaiseau, France
ASIC readout for Electomagnetic Calorimeter for future
Linear Collider Experiment
Higgs particle predicted by the Standard Model – 1964
LHC started to exploration of this particle at TeV scale with proton beam...
Question?
Is the Higgs boson fundamentalparticle or composite?
Is it part of a more complicated electroweak sector?
Does it universally couple to all matter proportionally to mass?
The LHC can only partiallyanswer these questions.
How we will explore the answers of that questions?
Physics motivation
International Linear Collider (ILC) experiment will explore the depth answer ofquestions related with Higgs boson.
ILC menu:
Detailed study of Higgs boson
Search super-symmetric particles
Study of physics:W, Z particles
Top quark .....
ILC – different approach than LHC
Electron-positron collision at TeV scale
Clean environment – low QCD background compre to LHC
Precise measurements
ILC tunnels [http://www.linearcollider.org]
Physics menu
Hadron process resultining in final states containing many jets.four componenets: charged particles, photons, neutral hadrons and neutrinos
the jet energy is carried:60% by charged particles (hadrons),30% by photons 10% by neutral hadrons
Developed technique – Particle Flow (PF)reconstruction of the four-vectors
of all visible particles in an event
To measure the : momenta of charged particles ==> tracking detectors Photon energy ==> electromagnetic calorimeter (ECAL) neutral hadrons ==> hadron calorimeter (HCAL)
Particle Flow Calorimetery – new Concept of CALORIMETER
Particle Flow Method
International Detector (ILD)
e-e+ collision at TeV scaleHigh luminosity – low rate
Tracking system:Vertex Pixel (or TPC) detector
Calorimetery: ECAL – tungsten Absorber, silicon pixel Sensor detector material
HCAL – tungsten/steel absorber, gaseous resistive plate chamber (RPC) detector
Whole system will be placed 5 T solenoid magnetic field
ILD Detector
Electromagnetic Calorimeter for ILC
Very good jet resolution > Fine granularity > Silicon wafer
Compact > sandwich (sampling) calorimeter > W (tungsten) plate as absorber
Dynamic range ~ few 100 MeV – 500 GeV / 1 TeV
Readout electronics integration to active elements of ECAL > ASIC (Application Specific Integrated Circuit)
Prototype for ECAL
Prototype of Si-W ECAL
ASIC+Si Wafer
Tested with electron beam (DESY)
Tested with pulse generator at LLR
Tested with cosmic muon at LLR
6 layer
1 layer
ASIC readout – concept developed due to requirement of physics program. The requirements are:
* Small size* Low noise* Low power* Large dynamic range * Large number readout channels
Prototype SKIROC
64 channelDual gainDynamic range:0.5 – 2000 MIP (minimum ionizing particle)
ASIC chip – has been designed to match the ILC beam structure. The complete readout process needs at least 3 different steps:
a. acquisition phaseb. conversion phasec. readout phased. possibly idle phase
Implemented Technique:
POWER PULSING >
-high channel density-high power dissipation
NoisePedestal (baseline)
En
egy
(ch
arg
e)
Analog output of ASIC
Signal processing for ASICSKIROC
- analog waveform at the output
of the pre-amplifier andthat at the output of the shaping amplifierwere observed using the monitor linesby injecting a charge.
For the charge (energy)information thegenerated signalfalling edge positionedin to the maximum ofsignal out of shaper unit.The hold signal can help to digitize thethe amplitude of analog waveform as a energy information, baselineto study the noise level.
Pedestal (baseline) distribution
Less noise valueNegligible baseline fluctuations
Verification of ASIC work abilityWith injected charge:
LinearityHold (delay)Gain
Setup with electron beam
e- beam
6 x [ silicon wafer + FEV8 + 4xSKIROC+DIF] W plate
e- beam
Performance study with electron beam:Energy of electron beam was 1-5 GeVRate 1 kHz6 detector layer
Pedestal
First MIP position
Second MIP position
Third MIP position
1st MIP = 356 +- 6.5 ADC Count2nd MIP = 426 +- 16.2 ADC Count3rd MIP = 498 +- 24.3 ADC Count
Hit map for 1 GeV electron beam
Shower radius developmentfor different radiation length
1. ASIC readout concept developed for ECAL.
2. It verified using high energy electron beams.
3. Parameters of ASIC; delay, gain, trigger threshold, time constant etc. performed with pulse generator and electron beam.
4. The chain of readout electronics based on ASIC is almost completed.
SUMMARY