A cluster counting drift chamber for central tracking at ILC Roberto Perrino INFN Lecce INSTR08 Novosibirsk Mar 1, 2008.

Slides:



Advertisements
Similar presentations
1 A CLUster COUnting Drift Chamber for ILC F.Grancagnolo, INFN – Lecce.
Advertisements

H1 SILICON DETECTORS PRESENT STATUS By Wolfgang Lange, DESY Zeuthen.
Electronics for large LAr TPC’s F. Pietropaolo (ICARUS Collaboration) CRYODET Workshop LNGS, March 2006.
Micromegas studies using cosmic rays Franck Sabatié May 7th 2009 Saclay cosmic ray bench Data acquisition system and analysis tools MIP detection Position.
Bulk Micromegas Our Micromegas detectors are fabricated using the Bulk technology The fabrication consists in the lamination of a steel woven mesh and.
The Silicon Track Trigger (STT) at DØ Beauty 2005 in Assisi, June 2005 Sascha Caron for the DØ collaboration Tag beauty fast …
Using the EUDET pixel telescope for resolution studies on silicon strip sensors with fine pitch Thomas Bergauer for the SiLC R&D collaboration 21. May.
RPC Update José Repond Argonne National Laboratory American Working Group On Linear Collider Calorimetry 16 September 2003 What’s new since Cornell…
1 F. GrancagnoloILC Workshop Valencia, ILC Workshop - ECFA and GDE Joint Meeting Valencia, 5-13 November 2006 F. Grancagnolo, INFN - Lecce.
The BTeV Tracking Systems David Christian Fermilab f January 11, 2001.
LBNE R&D Briefing May 12, 2014 LBNE R&D Briefing May 12, 2014 LArIAT and LBNE Jim Stewart LArIAT EPAG Chair BNL LBNE LARIAT-EPAG J. Stewart BNL T. Junk.
1 Conceptual design adopts state-of-the-art silicon sensor techniques (compare ATLAS/CMS/ALICE inner tracker layers, BaBar tracking of B mesons). Design.
Tobias Haas DESY 7 November 2006 A Pixel Telescope for Detector R&D for an ILC Introduction: EUDET Introduction: EUDET Pixel Telescope Pixel Telescope.
Sept. 24, Status of GEM DHCAL Jae Yu For GEM-TGEM/DHCAL Group Sept. 24, 2010 CALICE Collaboration Meeting Univ. Hassan II, Casablanca Introduction.
Ivan Vitev & E906 Muon Identifier Status Patrick McGaughey and the muon radiography team E866 Meeting at FNAL June 20-21, 2007 Large Muon Tracker at LANSCE.
VC Feb 2010Slide 1 EMR Construction Status o General Design o Electronics o Cosmics test Jean-Sebastien Graulich, Geneva.
QUPID Readout and Application in Future Noble Liquid Detectors Kevin Lung, UCLA TIPP 2011 June 11, 2011.
Pixel hybrid status & issues Outline Pixel hybrid overview ALICE1 readout chip Readout options at PHENIX Other issues Plans and activities K. Tanida (RIKEN)
21-Aug-06DoE Site Review / Harvard(1) Front End Electronics for the NOvA Neutrino Detector John Oliver Long baseline neutrino experiment Fermilab (Chicago)
NanoPHYS’12 – December 17-19, 2012 K. Nakano, S. Miyasaka, K. Nagai and S. Obata (Department of Physics, Tokyo Institute of Technology) Drift Chambers.
The AFTER electronics from a user’s point of view D. Attié, P. Colas Mamma meeting,CERN Feb T2K electronics.
Design and development of micro-strip stacked module prototypes for tracking at S-LHC Motivations Tracking detectors at future hadron colliders will operate.
Fine Pixel CCD for ILC Vertex Detector ‘08 7/31 Y. Takubo (Tohoku U.) for ILC-FPCCD vertex group ILC vertex detector Fine Pixel CCD (FPCCD) Test-sample.
The detection of single electrons using the MediPix2/Micromegas assembly as direct pixel segmented anode NIKHEF: A. Fornaini, H. van der Graaf, P. Kluit,
PHASE-1B ACTIVITIES L. Demaria – INFN Torino. Introduction  The inner layer of the Phase 1 Pixel detector is exposed to very high level of irradiation.
Tevatron II: the world’s highest energy collider What’s new?  Data will be collected from 5 to 15 fb -1 at  s=1.96 TeV  Instantaneous luminosity will.
Valerio Re, Massimo Manghisoni Università di Bergamo and INFN, Pavia, Italy Jim Hoff, Abderrezak Mekkaoui, Raymond Yarema Fermi National Accelerator Laboratory.
9 September 2004The Straw Tube Chamber1 The CDC Curtis A. Meyer Carnegie Mellon University Physics Requirements and Specifications Prototype Construction.
- Performance Studies & Production of the LHCb Silicon Tracker Stefan Koestner (University Zurich) on behalf of the Silicon Tracker Collaboration IT -
Test of the GEM Front Tracker for the SBS Spectrometer at Jefferson Lab F. Mammoliti, V. Bellini, M. Capogni, E. Cisbani, E. Jensen, P. Musico, F. Noto,
5-9 June 2006Erika Garutti - CALOR CALICE scintillator HCAL commissioning experience and test beam program Erika Garutti On behalf of the CALICE.
Readout Architecture for MuCh Introduction of MuCh Layout of Much ( proposed several schemes) Read ASIC’s Key features Basic Readout chain ROC Block Diagram.
Detailed description of the algorithm used for the simulation of the cluster counting For the studies of CluCou we have used standard programs like MAGBOLTZ,
1 A CLUster COUnting Drift Chamber for ILC …and… can we adapt this chamber to SuperB ? F.Grancagnolo, INFN – Lecce, Italy.
Quality control for large volume production GEM detectors Christopher Armaingaud On behalf of the collaboration GEMs for CMS.
WG3 – STRIP R&D ITS - COMSATS P. Riedler, G. Contin, A. Rivetti – WG3 conveners.
CP violation in B decays: prospects for LHCb Werner Ruckstuhl, NIKHEF, 3 July 1998.
CGEM-IT project and beam test program G. Felici for the FE-LNF-TO team Partially supported by the Italian Ministry of Foreign Affairs under the Program.
DØ Beauty Physics in Run II Rick Jesik Imperial College BEACH 2002 V International Conference on Hyperons, Charm and Beauty Hadrons Vancouver, BC, June.
RD51 GEM Telescope: results from June 2010 test beam and work in progress Matteo Alfonsi on behalf of CERN GDD group and Siena/PISA INFN group.
Tracking at the Fermilab Test Beam Facility Matthew Jones, Lorenzo Uplegger April 29 th Infieri Workshop.
Villa Olmo, Como October 2001F.Giordano1 SiTRD R & D The Silicon-TRD: Beam Test Results M.Brigida a, C.Favuzzi a, P.Fusco a, F.Gargano a, N.Giglietto.
Juan Valls - LECC03 Amsterdam 1 Recent System Test Results from the CMS TOB Detector  Introduction  ROD System Test Setup  ROD Electrical and Optical.
Siena, May A.Tonazzo –Performance of ATLAS MDT chambers /1 Performance of BIL tracking chambers for the ATLAS muon spectrometer A.Baroncelli,
Rutherford Appleton Laboratory September 1999Fifth Workshop on Electronics for LHC Presented by S. Quinton.
Upgrade with Silicon Vertex Tracker Rachid Nouicer Brookhaven National Laboratory (BNL) For the PHENIX Collaboration Stripixel VTX Review October 1, 2008.
TRIUMF laboratory studies Christopher Hearty University of British Columbia/IPP 27-Sep-2010.
14/02/2008 Michele Bianco 1 G.Chiodini & E.Gorini ATLAS RPC certification with cosmic rays Università del Salento Facoltà di Scienze MM.FF.NN.
G.F. Tassielli - SuperB Workshop XI LNF1/11 02/12/2009 Status report on CLUster COUnting activities G. F. Tassielli on behalf of CLUCOU group SuperB Workshop.
Overview of TPC Front-end electronics I.Konorov Outline:  TPC prototype development  Readout scheme of the final TPC detector and further developments.
A. Calcaterra, R. de Sangro, G. Felici, G. Finocchiaro, P. Patteri, M. Piccolo INFN LNF XIV SuperB General Meeting DCH-I parallel session LNF, 27 September.
A. Calcaterra, R. de Sangro, G. Felici, G. Finocchiaro, P. Patteri, M. Piccolo INFN LNF XIII SuperB General Meeting DCH-I parallel session Elba, 30 May.
Trigger & Tracking detector for CMS
MICROMEGAS per l’upgrade delle Muon Chambers di ATLAS per SLHC Arizona, Athens (U, NTU, Demokritos), Brookhaven, CERN, Harvard, Istanbul (Bogaziçi, Doğuş),
High Energy Physics experiments.
DCH FEE STATUS Level 1 Triggered Data Flow FEE Implementation &
A General Purpose Charge Readout Chip for TPC Applications
DCH FEE 28 chs DCH prototype FEE &
Silicon Pixel Detector for the PHENIX experiment at the BNL RHIC
Tassielli G.F. INFN Lecce & Università del Salento
Update on Cluster Counting Technique
The Silicon Track Trigger (STT) at DØ
PID electronics for FDIRC (Focusing Detector of Internally Reflected Cherenkov light) and FTOF (Forward Time of Flight) Christophe Beigbeder and Dominique.
Simulation study for Forward Calorimeter in LHC-ALICE experiment
Perugia – IX SuperB General Meeting G. Finocchiaro INFN-LNF
PID meeting Mechanical implementation Electronics architecture
Cluster Counting Drift Chamber as high precision tracker for ILC experiments G.F. Tassielli(1,2) (1) Dipartimento di Fisica dell’Universita’ del Salento,
SVT detector electronics
The LHCb Front-end Electronics System Status and Future Development
Perugia SuperB Workshop June 16-19, 2009
Presentation transcript:

A cluster counting drift chamber for central tracking at ILC Roberto Perrino INFN Lecce INSTR08 Novosibirsk Mar 1, 2008

Outline Tracking requirements at the ILC Low density DCH + Cluster counting Expectations for the CluCou DCH (ILC 4 th Concept) CluCouCluCou R&D Program Status of the Experimental Tools Summary and outlook INSTR08 Novosibirsk

A golden channel for SM Higgs:  Z decay is tagged by clean l + l _ decays H-mass measured independent of decay channel, because of constrained kinematics LHC machine for discovery machine for precision measurements [ ILC-Reference Design Report - Vol.I ] Which precision? Unbiased benchmark case:Higgs detection at the ILC

How to meet P T resolution requirements? ILC-type TPC + 5 layers of Si pixels KLOE-type DCH  m New DCH with potential  m [G. Tassielli, Doctoral Dissertation, Feb 2008] We can operate on both arms of Light-mass DCH He+wires Higher position resolution track sampling 0.5 % X 0 Greatly Improves p T <25 GeV/c  m Greatly Improves p T >25 GeV/c

[C. Grupen - Particle Detectors - Cambridge U. Press] He-based mixture Low drift velocity (  2.5 times less than Ar) Low ionization density along track (  5 times less than Ar) Read-out elx Risetime  ns Sampling rate  Gsa/s 0.4 ns/chan mip crossing 2 cm radius drift tube He+iC 4 H 10 (90/10) With lesson learned from e.g. KLOE and BaBar

A cluster counting central DCH for future experiments at ILC (4 th Concept proposal) Design and construction of such type of chamber relying on robust engineering calculations and consolidated carbon fiber technology (e.g. KLOE, Novosibirsk DCH) KLOE-like DCH  CluCou (≥1GHz; ≥2 GSa/s; 8 bit)  1.5 m track-length; ~125 points/track;  = 60  m  He-based mix ⇒ contribution to m.s.~0.15% X 0  60K Hex cm cells in 20 s_layers  Full stereo U-V ±72-180mrad  60K 20  m sense wires; 120K 80  m Ewires  Uniform sampling over >90% of volume  Position resolutions:  b  = 60  m ;  z  = 300  m  PID resolution ~2% through dN cl /dx

Expectations for CluCou ILC 4th Concept Simulation in the ILCRoot framework: √s= fb -1 [G. Tassielli, Doctoral Dissertation, Feb 2008] e + e - → HZ → X + µ + µ -

The CluCou R&D Program Software simulations (Garfield, Magboltz): control of the gas transport parameters electrical characterization of drift cell measurability of single electron FE elx transfer function Simple cosmic ray experimental setup (drift tubes, trigger, fast digital scope) Development of fast FE VLSI ASIC (preamp, shaper, ADC, buffer) Precision  strip tracker for detailed study DCH small scale prototype construction CR-test and beam-test of DCH prototype Waveform analysis and cluster counting algorithms

CLUCOU Simulation: Gas parameters He-iC 4 H 10 90%-10%85%-15%80%-20% n cl /cm n el /n cl Based on packages: HEED, MAGBOLTZ, GARFIELD9 and ROOT Number of clusters/cm and e - /cluster Clusters Poisson ionization statistics He-iC 4 H 10 Working Point Electron Landau ionization statistics [G. Chiodini - SuperB Detector R&D - Slac Feb 2008]

CLUCOU simulations: Peak Finder after Front-End Atlas internal note MUON-NO-105 (1995) and PS-SPICE Gain Phase ~1MHz ~3GHz [G. Tassielli, Doctoral Dissertation, Feb 2008] FE response

CluCou Measurements Scintillator trigger Drift tube: r = 1.4 cm L=30 cm He 90% + iC 4 H 10 10% Sense wire 25  m ∅ HV  V 10 × bw=500 MHz 2.5 Gsa/s 4GHz bw digital scope Slow control parameters continuosly monitored (HV, Temp, Press, GasFlow) t dr tt t FIRST t LAST

“Confidence gaining” results R=1.2 cm R=2.0 cm  t=900 ns High # of peaks Short arrival time Little Impact Parameter DriftTime “white” spectrum Look forward to select impact parameter with micrometric tracker

A precision tracking telescope

CLUCOU measurements: Si-Telescope (I) Linux OS FNAL PTA card FNAL Mezzanine PCI bus XILINX FPGA ALTERA FPGA ILLINOIS adapter board Daisy-Chain 6 CDF Run2b modules Module~4x18 cm 2 = 1 hybrid+ 2 Si sensor: 8 bit ADC p+/n sensors 75um readout pitch with intermediate floating strips HV caen LV Power Supply TTL Trigger In Hardware ready Firmware ready Software to finalize for: tracking analysis Two Si-modules already readout in daisy chain External trigger readout 6 modules + 4 spare available Mechanical assembly and HV ready. Drift tube Under test Many thanks Fermilab ESE department and Thomas Junk (IL Urbana University) !!! [G. Chiodini - SuperB Detector R&D - Slac Feb 2008]

Si - telescope and Device Under Test. Only one Si plane shown out of 6. 6 plane microStrip-Si telescope Next: Tracking on cosmics - X 0 Material not optimized yet CLUCOU measurements: Si-Telescope (II) Full adjustable angles step Easy to upgrade to more planes [G. Chiodini - SuperB Detector R&D - Slac Feb 2008]

The CluCou Chip Technology = 0.13 µm CMOS Core area = 2.4 mm 2 ADC: Resolution = 6 bits Sample rate = 1 GSa/s FS input range = 160 mV Preamp: Programmable DC-gain 0-20 dB BW dB Input-referred noise = 52  V rms wrt drift tube output noise of 100  V rms [S. D’Amico - Proc. IWASI Bari June 26-27, 2007] Design specs

CluCou FE Chip test plan Last Word from TESTS ON DETECTOR’s FE BENCH TESTS: Polarization: control of absorbed current and output voltages Characterization of variable gain amplifier prior to ADC Frequency response for different gains Noise and linearity Characterization of the ADC S/N ratio evaluation + distorsion Feb 18th 2008: 70 chips delivered Feb 22nd 2008: Test boards delivered In the course of setting-up bench tests (electrical, general functionality)

Summary & Outlook  The CluCou Collaboration is exploring the introduction of a very light He-based DCH with cluster counting capabilities  Exploration of new light materials for wiring (carbon, polyester, as thin as 10  m)  Solution applicable to ILC for pushing to extreme resolution on momentum measurements (or to SuperB Factories for PID with ionization density measurement)  MC computational tools developed for exploring the improvement of single point position resolution to 50  m  VLSI ASIC designed for 1 GHz bw and 1 Gsa/s 6 bit waveform sampling; first 70 out of foundry ready for testing  Experimental tools for consistency check of simulations with drift tubes and cosmic rays INSTR08 Novosibirsk In progress this year:  Bench tests of the 70 pre-production CluCou chips; get conclusions within 2008  Further development of peak-counting algorithms for efficient waveform analysis  Setting-up microstrip telescope for detailed study of the ionization statistics, r-t relation and resolution  Event-by-event measurements on drift tubes with the CluCou chip and a commercial board (National Semiconductors) for performance comparison On the longer run (2009)  Design and build a prototype DCH w/ 50 cells fully equipped with FE elx  Test of the prototype DCH with cosmics  Test of the prototype DCH in a testbeam

Credits The CluCou Collaboration F. Grancagnolo [1], A. Baschirotto [2,1], G. Chiodini [1], P. Creti [1], S. D’Amico [2,1], M. De Matteis [2,1], M. Panareo [2,1], R. Perrino [1], S. Spagnolo [3,1], G.F. Tassielli [3,1] 1) INFN Lecce 2) Università del Salento, Dipartimento di Ingegneria dell’Innovazione, Lecce 3) Università del Salento, Dipartimento di Fisica, Lecce INSTR08 Novosibirsk