Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 2 Calorimetry Performance goals Electromagnetic Calorimetry (ECal)

Slides:



Advertisements
Similar presentations
1 Individual Particle Reconstruction CHEP07, Victoria, September 6, 2007 Norman Graf (SLAC) Steve Magill (ANL)
Advertisements

LC Calorimeter Testbeam Requirements Sufficient data for Energy Flow algorithm development Provide data for calorimeter tracking algorithms  Help setting.
Calorimetry Summary Dhiman Chakraborty, NIU Linear Collider Workshop UC Santa Cruz, 29-june-2002.
Testbeam Requirements for LC Calorimetry S. R. Magill for the Calorimetry Working Group Physics/Detector Goals for LC Calorimetry E-flow implications for.
Fiberless Coupled Tiles for a High Granularity Scintillator-SiPM Calorimeter Rick Salcido Northern Illinois University November 14, 2009 Prairie Section.
Dhiman ChakrabortyCal+mu+p-id+test-beam summary LC workshop, Cornell, 16 July, '03 2 Calorimetry Performance goals Electromagnetic Calorimetry (ECal)
Some early attempts at PFA Dhiman Chakraborty. LCWS05 Some early attempts at PFA Dhiman Chakraborty2 Introduction Primarily interested in exploring the.
Directional Detectors and Digital Calorimeters Ed Norbeck and Yasar Onel University of Iowa For the 25 th Winter Workshop on Nuclear Dynamics Big Sky,
 Performance Goals -> Motivation  Analog/Digital Comparisons  E-flow Algorithm Development  Readout R&D  Summary Optimization of the Hadron Calorimeter.
P. Karchin – Scintillator Based Muon System Collaboration page 1 1/8/2004 January 8, 2004 American Linear Collider Physics Group 2004 Workshop Stanford.
A preliminary analysis of the CALICE test beam data Dhiman Chakraborty, NIU for the CALICE Collaboration LCWS07, Hamburg, Germany May 29 - June 3, 2007.
30 October 2002Paul Dauncey - CALICE/PRC1 PRC – CALICE Progress Report Paul Dauncey, Imperial College London Representing the CALICE Collaboration.
PFA Development – Definitions and Preparation 0) Generate some events w/G4 in proper format 1)Check Sampling Fractions ECAL, HCAL separately How? Photons,
Andy White U.Texas at Arlington (for J.Yu, C.Han, J.Li, D.Jenkins, J.Smith, K.Parmer, A.Nozawa, V.Kaushik) 10/18/04 IEEE/NSS Digital Hadron Calorimetry.
Report from CALICE meeting CERN 9/23-23/2002 Andy White Web Site for meeting: agenda_CALICE_23090.html.
Calorimetry: a new design 2004/Sep/15 K. Kawagoe / Kobe-U.
Development of Particle Flow Calorimetry José Repond Argonne National Laboratory DPF meeting, Providence, RI August 8 – 13, 2011.
Summary of Calorimetry/Muon Sessions Burak Bilki University of Iowa Argonne National Laboratory.
Monte Carlo Comparison of RPCs and Liquid Scintillator R. Ray 5/14/04  RPCs with 1-dimensional readout (generated by RR) and liquid scintillator with.
J-C BRIENT Prague Performances studies of the calorimeter/muon det. e + e –  W + W – at  s=800 GeV Simulation SLAC-Gismo Simulation MOKKA-GEANT4.
Simulation Studies for a Digital Hadron Calorimeter Arthur Maciel NIU / NICADD Saint Malo, April 12-15, 2002 Introduction to the DHCal Project Simulation.
Shower Containment and the Size of a Test Calorimeter Adam Para, September 6, 2006.
SiD R&D on PFA and Calorimetry -> IDAG guidance. -> Present PFA situation. -> Developing a timeline for PFA development. -> Calorimetry aspects.
SiD Concept – R&D Needs Andy White U. Texas at Arlington SiD Concept Meeting LCWS06 Bangalore, India March 11, 2006.
Light Calibration System (LCS) Temperature & Voltage Dependence Option 2: Optical system Option 2: LED driver Calibration of the Hadronic Calorimeter Prototype.
Linear collider muon detector: Marcello Piccolo Amsterdam, April 2003.
Agenda for LC Muon Detector Studies Mtg Black Hole Tues. Aug. 5 12:30 – 14:00 Parts for the prototype planes. 15 min.Gene Fisk MAPMT FE electronics/cal.
GLD Calorimetry 2005/Mar/03 K. Kawagoe / Kobe-U. Introduction Current design –To be optimized for Particle Flow Algorithm (PFA) aiming at 30%/sqrt(E)
Scintillator ECAL for ILC for Calorimeter Review DESY May2007 Tohru Takeshita (CALICE-Shinshu) Idea implementation current status future mile stones.
Pion Showers in Highly Granular Calorimeters Jaroslav Cvach on behalf of the CALICE Collaboration Institute of Physics of the ASCR, Na Slovance 2, CZ -
M. Chefdeville LAPP, Annecy, France. Introduction  Motivations for a Digital hadronic calorimeter Count hits instead of measuring energy deposits Reduce.
CALICE Digital Hadron Calorimeter: Calibration and Response to Pions and Positrons International Workshop on Future Linear Colliders LCWS 2013 November.
Simulation Studies for a Digital Hadron Calorimeter Arthur Maciel NIU / NICADD Saint Malo, April 12-15, 2002 Introduction to the DHCal Project Simulation.
SiD R&D tasks for the LOI - Subsystem R&D tasks - Summary of SiD R&D - Prioritization of R&D tasks -> Document for DoE/NSF ~Feb 2009 (Mainly based on Marty’s.
O R&D programme to test detector concepts being developed for neutrino factory: wrong sign muon “Golden” signature R&D Programme MIND & TASD 15 m 100 m.
UTA GEM DHCAL Simulation Jae Yu * UTA DoE Site Visit Nov. 13, 2003 (*On behalf of the UTA team; A. Brandt, K. De, S. Habib, V. Kaushik, J. Li, M. Sosebee,
R&D status of the Scintillator- strip based ECAL for the ILD Oct LCWS14 Belgrade Satoru Uozumi (KNU) For the CALICE collaboration Scintillator strips.
Development of Digital Hadron Calorimeter Using GEM Shahnoor Habib For HEP Group, UT Arlington Oct. 12, 2002 TSAPS Fall ’02, UT Brownsville Simulation.
1 ILC/SiD Muon System Progress Colorado State – D. Warner, R. Wilson Fermilab – G. Fisk, C. Milstene UC Davis – J. Lizarazo, M. Tripathi Indiana University.
1 The CALICE experiment at MTBF (FNAL) summary of a fruitful test beam experiment Erika Garutti (DESY) On behalf of CALICE.
ILC Calorimetry Test Beam Status Lei Xia ANL HEP.
Particle-flow Algorithms in America Dhiman Chakraborty N. I. Center for Accelerator & Detector Development for the International Conference.
V. Korbel, DESY1 Progress Report on the TESLA Tile HCAL Option To be filled soon.
5-9 June 2006Erika Garutti - CALOR CALICE scintillator HCAL commissioning experience and test beam program Erika Garutti On behalf of the CALICE.
LC Muon Detector Development Overview Hardware R&D Goals Hardware Configuration Design Issues Procurement, Engineering, Manpower Additional Development.
1 Progress from José Repond Argonne National Laboratory LCWS 2007, DESY, May 30 – June 3, 2007 Emphasis on test beam results.
Individual Particle Reconstruction The PFA Approach to Detector Development for the ILC Steve Magill (ANL) Norman Graf, Ron Cassell (SLAC)
Test Beam: Calorimetric Wishes… Steve Magill, Jose Repond, Andre Turcot, Jae Yu* Jan. 10, 2003 Goals for calorimeter test beam What’s needed for EFA? Requirements.
Mar. 31, 2003CAL Testbeam Discussion J. Yu 1 Calorimeter Test Beam Goals 1.Test of hardware technologies Feasibilities, properties and performances of.
Imaging Hadron Calorimeters for Future Lepton Colliders José Repond Argonne National Laboratory 13 th Vienna Conference on Instrumentation Vienna University.
Performance of Scintillator-Strip Electromagnetic Calorimeter for the ILC experiment Satoru Uozumi (Kobe University) for the CALICE collaboration Mar 12.
DHCAL Jan Blaha R&D is in framework of the CALICE collaboration CLIC08 Workshop CERN, 14 – 17 October 2008.
Durham TB R. Frey1 ECal R&D in N. America -- Test Beam Readiness/Plans Silicon-tungsten SLAC, Oregon, Brookhaven (SOB) Scintillator tiles – tungsten U.
CEPC 数字强子量能器读出电子学预研进展
SiD Calorimeter R&D Collaboration
(My personal) CALICE Report
Tao Hu, Jianbei Liu, Haijun Yang, Boxiang Yu For the CEPC-Calo Group
Calorimetry for a CLIC experiment
State-of-the-art in Hadronic Calorimetry for the Lepton Collider
GEM-based Digital Hadron Calorimetry for SiD
Vishnu V. Zutshi For the NICADD team.
   Calorimetry et al.    SUMMARY 12 contributions Tile HCAL
GEM-based Digital Hadron Calorimetry for SiD
Study of a Scintillating Digital Hadron Calorimeter Prototype
Argonne National Laboratory
Steve Magill Steve Kuhlmann ANL/SLAC Motivation
Calice Tile-HCal and Tail-catcher/Muon Tracker
LC Calorimeter Testbeam Requirements
LC Muon Detector Development Overview
Presentation transcript:

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 2 Calorimetry Performance goals Electromagnetic Calorimetry (ECal) Hadronic Calorimetry (HCal) –Digital –Analog Particle-flow algorithms (formerly energy-flow) –Simulations –Particle identification (Digi/Ana) Test Beam

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 3 Performance goals Jet energy measurement precise enough to separate Ws and Zs in hadronic decays on an event-by- event basis: ΔE = 0.3 sqrt(E [GeV]) Use track momenta for charged clusters; cal only for for neutrals: particle-flow algorithms Identify non-pointing neutral clusters Excellent hermeticity

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 4 ECal Si-W (Oregon+SLAC) Si-W-Scint (Kansas) Scint-W (Colorado) Crystal (Iowa+Caltech) Cerenkov-compensated (Iowa+Fairfield) All analog

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 5 Si-W ECal 0.5 cm x 0.5 cm 0.3 mm Si 3.5 mm/layer 30 layers R in = ~142 cm Z max = 2.1m 20X 0, 0.8λ 0 Sampling ~2% 5T field Small R m and fine segmentation aids PFAs Europe on board Design well under way Electronics rough draft complete Mechanical conceptual design started. Tests, more simulations in the offing

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 6 Si-W-Scint. & Scint.-W More affordable than Si-W Somewhat coarser segmentation – limited by fiber routing Fine sampling and timing Efficiency and uniformity need to be established – gang 3-5 tiles Choice of photodet, fiber coupling … Europe, Asia on board on scint. option Detailed simulation studies in progress

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 7 Crystal Cerenkov Inexpensive Excellent E resol. (100% sampling) No longitudinal segmentation – limitation to PFA? Still in early stage Extensive simulations needed and planned Cerenkov- compensated precision calorimetry Uses Cerenkov light to measure e,γ; ionization for hadrons, e – combine the two Not much known

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 8 HCal RPC – Digital (ANL, U. Chicago, Boston, FNAL) Scintillator – Digital (?) (NIU, UIC) GEM – Digital (U Texas - Arlington) Scintillator – Analog (Colorado) ~34 layers, ~3.5 cm thick w/ 2.5 cm thick stainless steel or similar absorber ~ 4λ 0, ~6% sampling 1-10 cm 2 cells

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 9 RPC DHCal Multiple gas gaps, glass substrate, graphite/ink resistive layer Avalanche mode operation Prototypes constructed, electronics, DAQ in place, initial studies are very encouraging Extensive testing, readout chip design in progress Backed by detailed simulation

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 10 Scintillator DHCal Proven technology Somewhat larger cells Cheap production by in-house extrusion MANY options for fiber routing, surface treatment, groove shape, transducer tested with encouraging results Cosmic ray prototype stack ~ready Bolstered by extensive simulation

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 11 GEM DHCal New technology Double-gap First prototype w/electronics assembled, operational Initial tests with CR, source at par with results shown by developers Multichannel prototypes under construction Backed up by extensive simulation

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 12 Scint. HCal (analog) Similar to Scint DHCal, but ~2.5 times larger tiles Improve lateral resolution by staggering Cell prototyping done Stack prototype next Simulation studies in progress

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 13 Particle-flow algorithms Several calorimeter groups are deeply involved in simulation and software development as well as PFA development (NIU, ANL, Colorado, UTA, …) First jet reconstruction results are most encouraging, prompting us to more realistic simulations and sophisticated reco algorithms Much effort invested

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 14 R. Wilson – CSU: Particle ID Software Infrastructure Embedding PID in the overall LCD/JAS s/w infrastructure? Fast Simulation/Reconstruction : dE/dx tool; code checks; muon fast simulation. Cross subsystem PID. Muon & PID Summary A. Maciel – NIU: Simulation Software Development Extension of generalized and universal simulation framework – new worldwide effort. Planar muon detector example with 45 o strips. Big advance! u vs. v for 2 tracks

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 15 Muon & PID Summary (cont.) C. Milstene – NIU: Muon ID Software Development Resurrection of  code. Verification of M. Piccolo’s muon ID for single particles and b-b events. G. Fisk – Fermilab: Scintillator Muon Detector Prototype Planes: Description General description of scintillator strip layout. M. Wayne – UND: Fiber Connections & Routing Discussion of fiber associated with bringing the WLS light out of the scintillator strips and onto a multi-anode photomultiplier.

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 16 Muon & PID Summary (cont.) P. Karchin – WSU: MAPMT Readout and Calibration Issues Test results on Hamamatsu M-16 multi-anode PMT. Calibration ideas. R. Wilson – CSU Geiger Photodiode Array Readout Test Description of tests performed on prototype APD (avalanche photo- diode). M. Piccolo – INFN RPC Prototype Design Issues First test results for new glass RPCs. Rate capability studies Test Beam at Frascati Plateau curve

Dhiman ChakrabortyCalorimetry + muon/p-id summary LC workshop, Cornell, 16 July, '03 17 Prototype Module Layout 2.5m 5.0 m 43 full strips 3.6m (L) x 4.1cm (W) x 1cm (T) 43 short strips 3.6m => 0m long Read out: both ends of full strips; one end of short strips (except the shortest 22). 2*( ) fibers/side =128 channels = 8 (1.2mm dia) fibers/pix * 16(4 x 4mm 2 ) pixels => Equivalent of One MAPMT/prototype plane