Readout Board Design for Gas Electron Multiplier Detectors for Use in a Proposed Upgrade of the CMS Hadron Calorimeter Elizabeth Starling Marcus Hohlmann.

Slides:



Advertisements
Similar presentations
Muon EDR: Chamber design M2/3 R1/2 16/04/20031T.Schneider/LHCb Muon EDR 1.General description - AW read out -Cathode pad read out -HV supply 2.Details.
Advertisements

LC Calorimeter Testbeam Requirements Sufficient data for Energy Flow algorithm development Provide data for calorimeter tracking algorithms  Help setting.
Large-area GEM Detector with Zigzag Strip Readout Aiwu Zhang, Marcus Hohlmann, Vallary Bhopatkar, Jessie Twigger, Elizabeth Starling, Michael Phipps, Eric.
SQUARE PAD PCB DESIGN Elizabeth Starling, Jerry Collins Florida Institute of Technology High Energy Physics Lab A January 26 th, 2015.
CMS GEM Workshop III, April 20, 2012
W. Clarida, HCAL Meeting, Fermilab Oct. 06 Quartz Plate Calorimeter Prototype Geant4 Simulation Progress W. Clarida The University of Iowa.
Interactions of hadrons in the SiW ECAL (CAN-025) Philippe Doublet - LAL Roman Pöschl, François Richard - LAL CALICE Meeting at Casablanca, September 22nd.
1 Study of the Tail Catcher Muon Tracker (TCMT) Scintillator Strips and Leakage with Simulated Coil Rick Salcido Northern Illinois University For CALICE.
Fiberless Coupled Tiles for a High Granularity Scintillator-SiPM Calorimeter Rick Salcido Northern Illinois University November 14, 2009 Prairie Section.
Ionization. Measuring Ions A beam of charged particles will ionize gas. –Particle energy E –Chamber area A An applied field will cause ions and electrons.
Detectors. Measuring Ions  A beam of charged particles will ionize gas. Particle energy E Chamber area A  An applied field will cause ions and electrons.
PFA Development – Definitions and Preparation 0) Generate some events w/G4 in proper format 1)Check Sampling Fractions ECAL, HCAL separately How? Photons,
ZEUS Calorimeter (1) At HERA high energetic electrons (e) collide with high energetic protons (P). The ZEUS detector measures the properties of the particles.
GEM Foil Stretching Using a Low-Cost Infrared Heating Array GEM Foil Stretching Using a Low-Cost Infrared Heating Array Elizabeth Esposito Erik Maki Undergraduate.
1 Tianchi Zhao University of Washington Concept of an Active Absorber Calorimeter A Summary of LCRD 2006 Proposal A Calorimeter Based on Scintillator and.
The SLHC and the Challenges of the CMS Upgrade William Ferguson First year seminar March 2 nd
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.
Rate and Gain Measurements of the 1-m long GEM detector Aiwu Zhang EIC tracking R&D weekly meeting.
David Attié Club ‘ILC Physics Case’ CEA Saclay June 23, 2013 ILD & SiD concepts and R&D.
Gain measurements of Triple Gas Electron Multiplier (GEM) detector with zigzag readout strips V. BHOPATKAR, E. ESPOSITO, E. HANSEN, J. TWIGGER M. HOHLMANN.
Development of Particle Flow Calorimetry José Repond Argonne National Laboratory DPF meeting, Providence, RI August 8 – 13, 2011.
Construct two layers of hadron calorimeter and test Makoto Harada High Energy Physics Laboratory Faculty of Physics Department of Science Shinshu University.
Part II: Using PCB Layout Software – Custom Component Libraries
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.
HV connection for a Common GEM foil design Aiwu Zhang
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.
Detector R&D for Muon Chamber Anand K. Dubey For VECC group.
Design of a readout system for RPCs Olu Amoda2 The LODEN Group The group is an association of Fermilab scientists who teamed up to build a cosmic ray.
Experimental Particle Physics PHYS6011 Joel Goldstein, RAL 1.Introduction & Accelerators 2.Particle Interactions and Detectors (2/2) 3.Collider Experiments.
75 th Annual Meeting March 2011 Imaging with, spatial resolution of, and plans for upgrading a minimal prototype muon tomography station J. LOCKE, W. BITTNER,
Performance of a Large-Area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System Vallary Bhopatkar M. Hohlmann, M. Phipps, J. Twigger,
16-Nov-2002Konstantin Beloous1 Digital Hadron Calorimeter Energy Resolution.
GEM Foil Stretching Using a Low-Cost Infrared Heating Array Elizabeth Esposito, Erik Maki Faculty Advisor: Dr. Marcus Hohlmann, Dept. of Physics and Space.
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,
Update on the Triple GEM Detectors for Muon Tomography K. Gnanvo, M. Hohlmann, L. Grasso, A. Quintero Florida Institute of Technology, Melbourne, FL.
R&D status of the Scintillator- strip based ECAL for the ILD Oct LCWS14 Belgrade Satoru Uozumi (KNU) For the CALICE collaboration Scintillator strips.
Developing Imaging Calorimeters for a SiD-Flavor Lepton Collider Jacob Smith Linear Collider Physics School Ambleside,England 2009.
M. Staib, M. Abercrombie, B. Benson, K. Gnanvo, M. Hohlmann Department of Physics and Space Sciences Florida Institute of Technology.
Bennett Marsh UM CERN REU 2014 Upgrades to the CMS HCAL Run Control System.
 The zigzag readout board is divided into eight η-sectors; each sector has a length of ~12 cm and comprises 128 zigzag strips; zigzag strips run in radial.
CaTS and Dual Readout. CaTS – Calorimeter and Tracker Simulation Describe detector in gdml file (xml like) Define.
Cost Reduction for Gas Electron Multiplier Detector Readout Boards Using Zigzag Strips Elizabeth Starling Marcus Hohlmann Kimberley Walton, Aiwu Zhang.
Abstract Beam Test of a Large-area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System V. Bhopatkar, M. Hohlmann, M. Phipps, J. Twigger,
1 Hadronic calorimeter simulation S.Itoh, T.Takeshita ( Shinshu Univ.) GLC calorimeter group Contents - Comparison between Scintillator and Gas - Digital.
Beam Test of a Large-Area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System Vallary Bhopatkar M. Hohlmann, M. Phipps, J. Twigger, A.
Construction and beam test analysis of GE1/1 prototype III gaseous electron multiplier (GEM) detector V. BHOPATKAR, E. HANSEN, M. HOHLMANN, M. PHIPPS,
Learning Objectives Calorimetry and Showers
Imaging Hadron Calorimeters for Future Lepton Colliders José Repond Argonne National Laboratory 13 th Vienna Conference on Instrumentation Vienna University.
Lattice Multiplication. Step 1 1)Draw a set of 2 by 2 boxes. 46 x 79 2) Cut the boxes in half diagonally. 3) Place the numbers on the outside of the boxes.
Detecting shielded nuclear contraband using muon tomography Judson Locke, William Bittner, Leonard Grasso, Dr. Kondo Gnanvo; Adviser: Dr. Marcus Hohlmann.
FNAL beam test data analysis A Hands-on session at CMS Upgrade School Aiwu Zhang Florida Institute of Technology On behalf of the CMS GEM collaboration.
1 Micromegas for sampling calorimetry Chronology & people  Initiated by LAPP LC-group in 2006 (C. Adloff, M. Chefdeville, Y. Karyotakis, I. Koletsou)
1 Update on the project - selected topics - Valeria Bartsch, Martin Postranecky, Matthew Warren, Matthew Wing University College London.
PPAC Jonathan Olson University of Iowa Thesis Defense 8 April 2005.
CEPC 数字强子量能器读出电子学预研进展
The Hadron Calorimeter (HCAL)
Dual Readout Clustering and Jet Finding
Matthew Bomberger1, Francisco Izquierdo1, Aiwu Zhang2
The Compact Muon Solenoid Detector
State-of-the-art in Hadronic Calorimetry for the Lepton Collider
   Calorimetry et al.    SUMMARY 12 contributions Tile HCAL
Development of Gas Electron Multiplier Detectors for Muon Tomography
ILC Detector Technology
J. Twigger, V. Bhopatkar, E. Hansen, M. Hohlmann, J.B. Locke, M. Staib
Rick Salcido Northern Illinois University For CALICE Collaboration
Event Monitor and Display for Muon Tomography Station
Steve Magill Steve Kuhlmann ANL/SLAC Motivation
LC Calorimeter Testbeam Requirements
A DLC μRWELL with 2-D Readout
Presentation transcript:

Readout Board Design for Gas Electron Multiplier Detectors for Use in a Proposed Upgrade of the CMS Hadron Calorimeter Elizabeth Starling Marcus Hohlmann Kimberley Walton, Aiwu Zhang [March 7 th, 2014]

Introduction Each layer of the CMS detector is designed to stop/measure a different kind of particle. The hadron calorimeter (HCAL) is one of these layers. 1)Hadrons enter HCAL 2)They interact with the brass absorber material and create showers 3)The energy of the shower, which we can measure, is proportional to the energy of the particle! March 7th, 2014Florida Academy of Sciences2

The Problem However, HCAL has its limits. Can: measure the scintillation energy of the particles, Cannot: measure their position or movement within the detector. If we want more data, we need to upgrade the calorimeter such that it can see particle flow as well as energies – from a hadron calorimeter (HCAL) to a particle flow calorimeter (PFCAL). March 7th, 2014Florida Academy of Sciences3

The Solution! Unlike HCAL’s current design, GEM detectors can easily detect the location of particle hits – we’ve used this fact to our advantage for our muon tomography station. We need to design a readout board that will be capable of accurately measuring the location of each particle hit on the GEM detector. The solution: a segmented pad readout board! March 7th, 2014Florida Academy of Sciences4

Design – Basics March 7th, 2014Florida Academy of Sciences5 Hadron showers are large! They can be several centimeters across, so the pads can be wider than the strips from previous readout boards! Detectors will be “sandwiched” in-between brass absorber plates – these plates cause the showers that the GEM detectors can then pick up.

Design – Square Pads 10 cm x 10 cm active area 11 rows of 11 square pads: 121 total. Each pad is: mm x mm March 7th, 2014Florida Academy of Sciences6

Design – Square Pads All read-out components are routed to a single APV: 2 ground connections (top left, bottom right) 121 pad connections 5 auxiliary connectors – to allow for easier “plug-and- play” access when testing the boards March 7th, 2014Florida Academy of Sciences7 Panasonic footprint

Design – Square Pads March 7th, 2014Florida Academy of Sciences8 All pads are routed underneath each other on a mid-layer. Does cross-talk make a measureable difference? To find out, we routed three rows all the way across!

Design – Chevrons 10 cm x 10 cm active area “Zig-zag”-style chevrons! Chevron pads give us different information than the square pads, and improves upon the shower descriptions. Because of the different horizontal segmentation, the charge sharing between adjacent pads can tell us more about the particles and their positions! March 7th, 2014Florida Academy of Sciences9

Design – Chevrons In order to maintain the square shape of the active area and keep to a single Panasonic connector, we used three types of pads: 110 full-chevron pads – formed by cutting the square pads diagonally in half and flipping one half. 12 half-chevron pads to “fill in” the main square! 5 merged half-chevron pads, to fit to a single APV March 7th, 2014Florida Academy of Sciences10

What’s Next Have the boards produced by outside industry Test the boards: – Do they accomplish our goals? – What differences do we see between the square and chevron pads? Make a square “pixel” style board, with 9 square pixels for every 1 square pad. – Is this possible at the 10x10 scale? Routing? March 7th, 2014Florida Academy of Sciences11

What’s Next March 7th, 2014Florida Academy of Sciences square pads1,089 square pixels

References Image on slides #2, 5: March 7th, 2014Florida Academy of Sciences13