Showermax Monte Carlo Studies

Size: px
Start display at page:

Download "Showermax Monte Carlo Studies"

Transcription

1 Showermax Monte Carlo Studies Dustin McNulty Idaho State University Thanks to: Carlos Bula, Brady Lowe, Kevin Rhine Jan 24, 2015

2 Showermax Monte Carlo Studies Outline Reproduce 2008 stack results (benchmarking MC) New Showermax Design for MOLLER Concept Light guide geometry Baseline performance (MC) Optimizing Design and Prototyping Summary Dustin McNulty Showermax Monte Carlo Studies 1

3 Detector Ring Design Concept Dustin McNulty Showermax Monte Carlo Studies 2

4 Motivation Provides additional measurement of e-e ring flux Weights flux by energy = less sensitive to low energy/low light bkgds Dustin McNulty Showermax Monte Carlo Studies 3

5 MOLLER Showermax Development Benchmark new MC: Start with 2008 stack experience Apply qsim optical MC framework to the stack Try to reproduce Jan2008 data and compare with Piotr s simulation results Create baseline showermax design Modify stack/lg/pmt geometry for MOLLER Start with Piotr s optimal stack configuration (10 pieces: 5mm quartz, 2.4mm tungsten) Apply Mainz testbeam and Peiqing s lightguide experience Optimize baseline design Study dependence on numbers and thicknesses of W and quartz, and energy, position and angles of incident particles Build prototype and test with beam (at Mainz?, SLAC) Dustin McNulty Showermax Monte Carlo Studies 4

6 2008 Showermax stack Slide from Piotr Dustin McNulty Showermax Monte Carlo Studies 5

7 2008 Stack Detector Schematic stack Al mirror PVC Schematic from Piotr Dustin McNulty Showermax Monte Carlo Studies 6

8 Jan2008 Testbeam Setup and Conditions Thin and Stack dets rigidly mounted along 45 angle; installed above rhrs focal plane (between VDC s and S1 scint. plane) E beam = 956 MeV, 5-50µA, 100mg/cm 2 Ta target rhrs at 19, using VDC s and s0 trigger (removable) Counting rates 10 Hz/µA Dustin McNulty Showermax Monte Carlo Studies 7

9 Jan2008 Testbeam Pulse Height Dists Thin Det (Raw, 3686, trig s0) hthin_raw Entries Mean RMS Stack Det (Raw, 3686, trig s0) hstk_raw Entries Mean RMS Thin Det (ped sub, 3686, trig s0) hthin 400 Entries 8915 Mean RMS χ / ndf / Lwidth 1.9 ± MPV ± 0.13 Integral 8381 ± GSigma ± Stack Det (ped sub, 3686, trig s0) 90 Entries Mean RMS χ 2 / ndf / 272 Lwidth 1.69 ± MPV ± Integral 6445 ± GSigma ± hstk Sun Jul 20 22:17: Stack performance: 51.7/144 = (raw) Dustin McNulty Showermax Monte Carlo Studies 8

10 Piotr s MC: Tungsten and Quartz thickness study (for 900MeV electrons) Dustin McNulty Showermax Monte Carlo Studies 9

11 ' $ January 2008 PREx detectors tests, comparison with simulations Thin 5mm Thin 10mm exp: 50±17(34%) exp: 93±22(24%) sim: 56.8±7.7(14%) sim: 109.2±11.3(10%) Stack exp: 434±152(35%) sim: 538.3±140.5(26%) Number of Cherenkov photons reaching PM NPE=0.2Nph (<QE>=0.2) In panels below widths of gaussian fits to the simulated Nph distributions (red lines) are corrected for the PMT resolution according to the formula (for the used PMTs measured value of the δq is 0.23): exp: 0.71±0.24(34%) pc exp: 1.31±0.31(24%) pc exp: 7.74±2.71(35%) pc sim: 0.80±0.26(32%) pc sim: 1.53±0.36(24%) pc sim: 9.61±2.68(28%) pc PM output charge (pc) & Dustin McNulty Slide from Piotr Showermax Monte Carlo Studies % 10

12 Recent Stack Simulations at ISU Dustin McNulty Showermax Monte Carlo Studies 11

13 2008 Testbeam Data and Simulation Summary Results for stack detector were lack-luster: 35% relative width Why? Because energy too low? probably not Or some other reasons?...det alignment, design... more likely Both simulations give reasonable agreement with real data at 15-20% level Simulations are also in reasonable agreement with each other: Piotr found 538 Cer. photons reach PMT per electron with 28% relative width ISU found 495 photons with 32% rel width Experiment yielded 434 photons with 35% rel. width Dustin McNulty Showermax Monte Carlo Studies 12

14 MOLLER Showermax Development Benchmark new MC: Start with 2008 stack experience Apply qsim optical MC framework to the stack Try to reproduce Jan2008 data and compare with Piotr s simulation results Create baseline showermax design Modify stack/lg/pmt geometry for MOLLER Start with Piotr s optimal stack configuration (10 pieces: 5mm quartz, 2.4mm tungsten) Apply Mainz testbeam and Peiqing s lightguide experience Optimize baseline design Study dependence on numbers and thicknesses of W and quartz, and energy, position and angles of incident particles Build prototype and test with beam (at Mainz?, SLAC) Dustin McNulty Showermax Monte Carlo Studies 13

15 Crude Sketch of MOLLER Showermax Concept Dustin McNulty Showermax Monte Carlo Studies 14

16 Showermax Detector Ring Dustin McNulty Showermax Monte Carlo Studies 15

17 Showermax Quartz Spectrosil 2000 each piece has single 45 deg bevel across long end Dustin McNulty Showermax Monte Carlo Studies 16

18 Showermax Lightguide (Bad Examples) *Lightguide design non-trivial and perhaps most important feature Dustin McNulty Showermax Monte Carlo Studies 17

19 Showermax Lightguide (Good) Dustin McNulty Showermax Monte Carlo Studies 18

20 Showermax Lightguide Development Dustin McNulty Showermax Monte Carlo Studies 19

21 Showermax Lightguide Development Dustin McNulty Showermax Monte Carlo Studies 20

22 Showermax MC LG Study 2 GeV electron beam centered on quartz face; normal incidence Dustin McNulty Showermax Monte Carlo Studies 21

23 Baseline Showermax MC Results: Lightguide C 2, 5, and 8 GeV e uniformly sampled over quartz face; normal Dustin McNulty Showermax Monte Carlo Studies 22

24 What if thickness of W is halved? 2, 5, and 8 GeV e uniformly sampled over quartz face; normal Dustin McNulty Showermax Monte Carlo Studies 23

25 What if just use single piece of W and Quartz? Answer: Doesn t work well at low energy (but way cheaper!) Dustin McNulty Showermax Monte Carlo Studies 24

26 Single piece Design versus Baseline Design at 2GeV Dustin McNulty Showermax Monte Carlo Studies 25

27 Single piece Design versus Baseline Design at 8GeV Dustin McNulty Showermax Monte Carlo Studies 26

28 MOLLER Showermax Development Benchmark new MC: Start with 2008 stack experience Apply qsim optical MC framework to the stack Try to reproduce Jan2008 data and compare with Piotr s simulation results Create baseline showermax design Modify stack/lg/pmt geometry for MOLLER Start with Piotr s optimal stack configuration (10 pieces: 5mm quartz, 2.4mm tungsten) Apply Mainz testbeam and Peiqing s lightguide experience Optimize baseline design Study dependence on numbers and thicknesses of W and quartz, and energy, position and angles of incident particles Build prototype and test with beam (at Mainz?, SLAC) Dustin McNulty Showermax Monte Carlo Studies 27

29 Prel. Prototype design using 2008 Stack pieces MC studies needed to understand potential benefits of beamtest Dustin McNulty Showermax Monte Carlo Studies 28

30 Summary and Future Work Optical MC framework for showermax R&D established Reasonable/good agreement with 2008 beamtest data and Piotr s simulations Baseline MOLLER showermax detector design established Gives strong energy dependent light yields with 25% relative width Optimization of baseline design underway Build prototype based on optimized design and test with beam Other questions/considerations: 90 LG or 135 (or 45 ) LG (Need to decide) Need to worry about sensitivity to neutrons, pions PE uniformity/edge effects due to transv. shower leakage Stray electrons, splashback,...need optical MC in remoll Dustin McNulty Showermax Monte Carlo Studies 29

Shower Max Detector Plans for MOLLER

Shower Max Detector Plans for MOLLER Shower Max Detector Plans for MOLLER Dustin McNulty Idaho State University mcnulty@jlab.org May 8, 14 MOLLER Shower Max Detector Outline Conceptual Design and Motivation Review 8 prototype stack Design

More information

MOLLER/PREX Detector Development

MOLLER/PREX Detector Development MOLLER/PREX Detector Development Dustin McNulty Idaho State University mcnulty@jlab.org October 31, 2015 Introduction: Integrating detectors for PVeS PVES expts measure tiny asymmetries and require large

More information

Main Detectors for PREX and CREX

Main Detectors for PREX and CREX Main Detectors for PREX and CREX Dustin McNulty Idaho State University mcnulty@jlab.org February 27, 2016 Main Detectors for PREX and CREX Outline Detector design ( finalized) Optical simulation ( benchmarked)

More information

HRS Detector Package for PREX-II/CREX. Dustin McNulty Idaho State University Oct 1, 2017

HRS Detector Package for PREX-II/CREX. Dustin McNulty Idaho State University Oct 1, 2017 HRS Detector Package for PREX-II/CREX Dustin McNulty Idaho State University mcnulty@jlaborg Oct 1, 2017 Dustin McNulty HRS Detector Package for PREX-II/CREX 1 Dustin McNulty HRS Detector Package for PREX-II/CREX

More information

PREX/CREX Main Detectors and GEM Trackers. Dustin McNulty Idaho State University March 4, 2017

PREX/CREX Main Detectors and GEM Trackers. Dustin McNulty Idaho State University March 4, 2017 PREX/CREX Main Detectors and GEM Trackers Dustin McNulty Idaho State University mcnulty@jlaborg March 4, 2017 Dustin McNulty PREX/CREX Main Detectors and GEM Trackers 1 PREX/CREX Main Detectors and GEM

More information

Performance of 8-stage Multianode Photomultipliers

Performance of 8-stage Multianode Photomultipliers Performance of 8-stage Multianode Photomultipliers Introduction requirements by LHCb MaPMT characteristics System integration Test beam and Lab results Conclusions MaPMT Beetle1.2 9 th Topical Seminar

More information

AMS-02 Anticounter. Philip von Doetinchem I. Physics Institute B, RWTH Aachen Bad Honnef, August 2007

AMS-02 Anticounter. Philip von Doetinchem I. Physics Institute B, RWTH Aachen Bad Honnef, August 2007 AMS-02 Anticounter Philip von Doetinchem philip.doetinchem@rwth-aachen.de I. Physics Institute B, RWTH Aachen Bad Honnef, August 2007 Michael Griffin, NASA Head AMS does not have a shuttle flight! Philip

More information

Pixel hybrid photon detectors

Pixel hybrid photon detectors Pixel hybrid photon detectors for the LHCb-RICH system Ken Wyllie On behalf of the LHCb-RICH group CERN, Geneva, Switzerland 1 Outline of the talk Introduction The LHCb detector The RICH 2 counter Overall

More information

MCP-PMT status. Samo Korpar. University of Maribor and Jožef Stefan Institute, Ljubljana Super KEKB - 3st Open Meeting, 7-9 July 2009

MCP-PMT status. Samo Korpar. University of Maribor and Jožef Stefan Institute, Ljubljana Super KEKB - 3st Open Meeting, 7-9 July 2009 , Ljubljana, 7-9 July 2009 Outline: MCP aging waveform readout (MPPC) summary (slide 1) Aging preliminary news from Photonis Old information: Current performance (no Al protection layer): 50% drop of efficiency

More information

MOLLER Update. Dustin McNulty Idaho State University for the MOLLER Collaboration June 8, 2012

MOLLER Update. Dustin McNulty Idaho State University for the MOLLER Collaboration June 8, 2012 MOLLER Update Dustin McNulty Idaho State University mcnulty@jlab.org for the June 8, 2012 Outline Introduction MOLLER Update Motivation (Indirect search for new physics) Search for new contact interactions

More information

PID summary. J. Va vra, SLAC. - Barrel PID - Forward PID

PID summary. J. Va vra, SLAC. - Barrel PID - Forward PID PID summary J. Va vra, SLAC - Barrel PID - Forward PID Barrel PID FDIRC progress (SLAC, Maryland, Hawaii, Orsay, Padova) New FDIRC optics ordered. FDIRC mechanical design for the CRT test is in progress.

More information

SiPMs as detectors of Cherenkov photons

SiPMs as detectors of Cherenkov photons SiPMs as detectors of Cherenkov photons Peter Križan University of Ljubljana and J. Stefan Institute Light07, September 26, 2007 Contents Photon detection for Ring Imaging CHerenkov counters Can G-APDs

More information

CALICE AHCAL overview

CALICE AHCAL overview International Workshop on the High Energy Circular Electron-Positron Collider in 2018 CALICE AHCAL overview Yong Liu (IHEP), on behalf of the CALICE collaboration Nov. 13, 2018 CALICE-AHCAL Progress, CEPC

More information

Monte Carlo Simulation of the PRad Experiment at JLab 1

Monte Carlo Simulation of the PRad Experiment at JLab 1 Monte Carlo Simulation of the PRad Experiment at JLab 1 Li Ye Mississippi State University for the PRad collaboration 1.This work is supported in part by NSF MRI award PHY-1229153, the U.S. Department

More information

Micromegas for muography, the Annecy station and detectors

Micromegas for muography, the Annecy station and detectors Micromegas for muography, the Annecy station and detectors M. Chefdeville, C. Drancourt, C. Goy, J. Jacquemier, Y. Karyotakis, G. Vouters 21/12/2015, Arche meeting, AUTH Overview The station Technical

More information

The HERA-B Ring Imaging Cerenkov ˇ Detector

The HERA-B Ring Imaging Cerenkov ˇ Detector The HERA-B Ring Imaging Cerenkov ˇ Detector Requirements Physics Genova, July 3, 1998 Jörg Pyrlik University of Houston HERA-B Collaboration Space Limitations Rate Capabilities and Aging Design Radiator

More information

Seminar. BELLE II Particle Identification Detector and readout system. Andrej Seljak advisor: Prof. Samo Korpar October 2010

Seminar. BELLE II Particle Identification Detector and readout system. Andrej Seljak advisor: Prof. Samo Korpar October 2010 Seminar BELLE II Particle Identification Detector and readout system Andrej Seljak advisor: Prof. Samo Korpar October 2010 Outline Motivation BELLE experiment and future upgrade plans RICH proximity focusing

More information

Investigation of a Cs137 and Ba133 runs. Michael Dugger and Robert Lee

Investigation of a Cs137 and Ba133 runs. Michael Dugger and Robert Lee Investigation of a Cs137 and Ba133 runs Michael Dugger and Robert Lee 1 Cs137 Using run 149 One million triggers Doing a quick analysis with fits: Not using Kei s noise corrections at the moment 2 ADC

More information

1.1 The Muon Veto Detector (MUV)

1.1 The Muon Veto Detector (MUV) 1.1 The Muon Veto Detector (MUV) 1.1 The Muon Veto Detector (MUV) 1.1.1 Introduction 1.1.1.1 Physics Requirements and General Layout In addition to the straw chambers and the RICH detector, further muon

More information

Spectrometer cavern background

Spectrometer cavern background ATLAS ATLAS Muon Muon Spectrometer Spectrometer cavern cavern background background LPCC Simulation Workshop 19 March 2014 Jochen Meyer (CERN) for the ATLAS Collaboration Outline ATLAS Muon Spectrometer

More information

Stato del progetto RICH di LHCb. CSN1 Lecce, 24 settembre 2003

Stato del progetto RICH di LHCb. CSN1 Lecce, 24 settembre 2003 Stato del progetto RICH di LHCb CSN1 Lecce, 24 settembre 2003 LHCb RICH detectors Particle ID over 1 100 GeV/c provided by 2 RICH detectors RICH2: No major changes since RICH TDR PRR in february 2003 Superstructure

More information

PoS(LHCP2018)031. ATLAS Forward Proton Detector

PoS(LHCP2018)031. ATLAS Forward Proton Detector . Institut de Física d Altes Energies (IFAE) Barcelona Edifici CN UAB Campus, 08193 Bellaterra (Barcelona), Spain E-mail: cgrieco@ifae.es The purpose of the ATLAS Forward Proton (AFP) detector is to measure

More information

Timing Measurement in the CALICE Analogue Hadronic Calorimeter.

Timing Measurement in the CALICE Analogue Hadronic Calorimeter. Timing Measurement in the CALICE Analogue Hadronic Calorimeter. AHCAL Main Meeting Motivation SPS CERN Testbeam setup Timing Calibration Results and Conclusion Eldwan Brianne Hamburg 16/12/16 Motivation

More information

Micromegas calorimetry R&D

Micromegas calorimetry R&D Micromegas calorimetry R&D June 1, 214 The Micromegas R&D pursued at LAPP is primarily intended for Particle Flow calorimetry at future linear colliders. It focuses on hadron calorimetry with large-area

More information

Precision Measurement of the Proton Elastic Cross Section at High Q 2

Precision Measurement of the Proton Elastic Cross Section at High Q 2 Precision Measurement of the Proton Elastic Cross Section at High Q 2 Longwu Ou (MIT) for the E12-07-108 Collaboration Hall A Collaboration Meeting December 8, 2014 Nucleon Form Factors The EM form factors

More information

JSNS 2 Detector Construc0on

JSNS 2 Detector Construc0on JSNS 2 Detector Construc0on Jungsic Park High Energy Accelerator Research Organiza0on (KEK) with JSNS 2 Collabora0on 27 Oct, 2017 KPS Fall 2017, HICO, Korea Jungsic Park, KEK KPS Fall 2017 1 Contents Concept

More information

ITk silicon strips detector test beam at DESY

ITk silicon strips detector test beam at DESY ITk silicon strips detector test beam at DESY Lucrezia Stella Bruni Nikhef Nikhef ATLAS outing 29/05/2015 L. S. Bruni - Nikhef 1 / 11 Qualification task I Participation at the ITk silicon strip test beams

More information

The LHCb Vertex Locator : Marina Artuso, Syracuse University for the VELO Group

The LHCb Vertex Locator : Marina Artuso, Syracuse University for the VELO Group The LHCb Vertex Locator : status and future perspectives Marina Artuso, Syracuse University for the VELO Group The LHCb Detector Mission: Expore interference of virtual new physics particle in the decays

More information

RF Time Measuring Technique With Picosecond Resolution and Its Possible Applications at JLab. A. Margaryan

RF Time Measuring Technique With Picosecond Resolution and Its Possible Applications at JLab. A. Margaryan RF Time Measuring Technique With Picosecond Resolution and Its Possible Applications at JLab A. Margaryan 1 Contents Introduction RF time measuring technique: Principles and experimental results of recent

More information

Mitigating high energy anomalous signals in the CMS barrel Electromagnetic Calorimeter

Mitigating high energy anomalous signals in the CMS barrel Electromagnetic Calorimeter Mitigating high energy anomalous signals in the CMS barrel Electromagnetic Calorimeter Summary report Ali Farzanehfar University of Southampton University of Southampton Spike mitigation May 28, 2015 1

More information

Muon Collider background rejection in ILCroot Si VXD and Tracker detectors

Muon Collider background rejection in ILCroot Si VXD and Tracker detectors Muon Collider background rejection in ILCroot Si VXD and Tracker detectors N. Terentiev (Carnegie Mellon U./Fermilab) MAP 2014 Winter Collaboration Meeting Dec. 3-7, 2014 SLAC New MARS 1.5 TeV Muon Collider

More information

The Calice Analog Scintillator-Tile Hadronic Calorimeter Prototype

The Calice Analog Scintillator-Tile Hadronic Calorimeter Prototype SNIC Symposium, Stanford, California -- 3-6 April 26 The Calice Analog Scintillator-Tile Hadronic Calorimeter Prototype M. Danilov Institute of Theoretical and Experimental Physics, Moscow, Russia and

More information

Hall C Winter Collaboration Meeting. Hall C Analyzer Update

Hall C Winter Collaboration Meeting. Hall C Analyzer Update Hall C Winter Collaboration Meeting Hall C Analyzer Update Jefferson Lab On Behalf of the Software Working Group Hall A/C Software Analysis Workshop Hall A/C software analysis workshop took place June

More information

Monte Carlo simulations for the JEDI polarimeter at COSY

Monte Carlo simulations for the JEDI polarimeter at COSY Monte Carlo simulations for the JEDI polarimeter at COSY Paul Maanen on behalf of the JEDI Collaboration JEDI Collaboration Physics Institute III B, RWTH Aachen University DPG Frühjahrstagung 216 Outline

More information

The MUSE experiment. Technical Overview. Guy Ron (for the MUSE collaboration) Hebrew University of Jerusalem

The MUSE experiment. Technical Overview. Guy Ron (for the MUSE collaboration) Hebrew University of Jerusalem The MUSE experiment Technical Overview Guy Ron (for the MUSE collaboration) Hebrew University of Jerusalem MUSE is not your garden variety scattering experiment Low beam flux Large angle, non-magnetic

More information

The Silicon TPC System

The Silicon TPC System The Silicon TPC System EUDET Annual Meeting 20 October 2009 Jan Timmermans NIKHEF 1 JRA2 activity/task Silicon TPC readout ( SITPC ) - development TimePix chip - development diagnostic endplate module

More information

SCINTILLATOR / WLS FIBER OPTION FOR BABAR MUON DETECTOR UPGRADE

SCINTILLATOR / WLS FIBER OPTION FOR BABAR MUON DETECTOR UPGRADE SCINTILLATOR / WLS FIBER OPTION FOR BABAR MUON DETECTOR UPGRADE PETER KIM SLAC HAWAII SUPER B FACTORY WORKSHOP JAN 19-22, 2004 BABAR BARELL RPC MUON SYSTEM DETERIORATING RAPIDLY WE NEED REPLACEMENT IN

More information

SiD and CLIC CDR preparations

SiD and CLIC CDR preparations SiD and CLIC CDR preparations Outline: Introduction Description of SiD detector R&D in software/hardware for SiD Preparations for the CLIC CDR Conclusions 1 Introduction In several aspects the CLIC detector

More information

Plans for RPC DHCAL Prototype. David Underwood Argonne National Laboratory

Plans for RPC DHCAL Prototype. David Underwood Argonne National Laboratory Plans for RPC DHCAL Prototype David Underwood Argonne National Laboratory Linear Collider Meeting, SLAC 7-10 January 2004 Outline Collaborators Goals Motivation Mechanical Structure Chamber Description

More information

Characterization of GEM Chambers Using 13bit KPiX Readout System

Characterization of GEM Chambers Using 13bit KPiX Readout System Characterization of GEM Chambers Using bit KPiX Readout System Safat Khaled and High Energy Physics Group Physics Department, University of Texas at Arlington (Dated: February, ) The High Energy Physics

More information

HAMC = Hall A Monte Carlo

HAMC = Hall A Monte Carlo HAMC = Hall A Monte Carlo Bob Michaels Hall A Jefferson Lab, Dec 3, 28 Software Workshop p.1 Two Previous Monte Carlos SAMC genercone (A. Deur, V. Sulkosky) (D. Lhuillier, K. Paschke, B. Moffit) much was

More information

Polarimetry Concept Based on Heavy Crystal Hadron Calorimeter

Polarimetry Concept Based on Heavy Crystal Hadron Calorimeter Polarimetry Concept Based on Heavy Crystal Hadron Calorimeter for the JEDI Collaboration CALOR 216 May 17, 216 Irakli Keshelashvili Introduction JEDI Polarimetry Concept MC Simulations Laboratory and Beam

More information

Development of TOP counter for Super B factory

Development of TOP counter for Super B factory 2009/5/11-13 Workshop on fast Cherenkov detectors - Photon detection, DIRC design and DAQ Development of TOP counter for Super B factory - Introduction - Design study - Focusing system - Prototype development

More information

Trigger Rate Dependence and Gas Mixture of MRPC for the LEPS2 Experiment at SPring-8

Trigger Rate Dependence and Gas Mixture of MRPC for the LEPS2 Experiment at SPring-8 Trigger Rate Dependence and Gas Mixture of MRPC for the LEPS2 Experiment at SPring-8 1 Institite of Physics, Academia Sinica 128 Sec. 2, Academia Rd., Nankang, Taipei 11529, Taiwan cyhsieh0531@gmail.com

More information

Beam Loss Monitoring (BLM) System for ESS

Beam Loss Monitoring (BLM) System for ESS Beam Loss Monitoring (BLM) System for ESS Lali Tchelidze European Spallation Source ESS AB lali.tchelidze@esss.se March 2, 2011 Outline 1. BLM Types; 2. BLM Positioning and Calibration; 3. BLMs as part

More information

Backgrounds in DMTPC. Thomas Caldwell. Massachusetts Institute of Technology DMTPC Collaboration

Backgrounds in DMTPC. Thomas Caldwell. Massachusetts Institute of Technology DMTPC Collaboration Backgrounds in DMTPC Thomas Caldwell Massachusetts Institute of Technology DMTPC Collaboration Cygnus 2009 June 12, 2009 Outline Expected backgrounds for surface run Detector operation Characteristics

More information

arxiv: v2 [physics.ins-det] 14 Jan 2009

arxiv: v2 [physics.ins-det] 14 Jan 2009 Study of Solid State Photon Detectors Read Out of Scintillator Tiles arxiv:.v2 [physics.ins-det] 4 Jan 2 A. Calcaterra, R. de Sangro [], G. Finocchiaro, E. Kuznetsova 2, P. Patteri and M. Piccolo - INFN,

More information

Contents. Why waveform? Waveform digitizer : Domino Ring Sampler CEX Beam test autumn 04. Summary

Contents. Why waveform? Waveform digitizer : Domino Ring Sampler CEX Beam test autumn 04. Summary Contents Why waveform? Waveform digitizer : Domino Ring Sampler CEX Beam test data @PSI autumn 04 Templates and time resolution Pulse Shape Discrimination Pile-up rejection Summary 2 In the MEG experiment

More information

DHCAL Prototype Construction José Repond Argonne National Laboratory

DHCAL Prototype Construction José Repond Argonne National Laboratory DHCAL Prototype Construction José Repond Argonne National Laboratory Linear Collider Workshop Stanford University March 18 22, 2005 Digital Hadron Calorimeter Fact Particle Flow Algorithms improve energy

More information

Multianode Photo Multiplier Tubes as Photo Detectors for Ring Imaging Cherenkov Detectors

Multianode Photo Multiplier Tubes as Photo Detectors for Ring Imaging Cherenkov Detectors Multianode Photo Multiplier Tubes as Photo Detectors for Ring Imaging Cherenkov Detectors F. Muheim a edin]department of Physics and Astronomy, University of Edinburgh Mayfield Road, Edinburgh EH9 3JZ,

More information

arxiv: v1 [physics.ins-det] 28 Feb 2018

arxiv: v1 [physics.ins-det] 28 Feb 2018 Development of GEM Detectors at Hampton University arxiv:18.12v1 [physics.ins-det] 28 Feb 218, Michael Kohl, Jesmin Nazeer, and Tanvi Patel Department of Physics, Hampton University, Hampton, VA 2668,

More information

Study the Compact Photon Source Radiation Using FLUKA

Study the Compact Photon Source Radiation Using FLUKA Study the Compact Photon Source Radiation Using FLUKA Jixie Zhang, Donal Day, Rolf Ent Nov 30, 2017 This is a summary of radiation studies done for both the UVa target alone (for electron and photon beams)

More information

Wavelength-shifting Optical Module (WOM)

Wavelength-shifting Optical Module (WOM) Wavelength-shifting Optical Module (WOM) Vincenzo Di Lorenzo HAP Workshop: Advanced Technologies Mainz 2016-02-02 Cherenkov light Increase the energy resolution decreasing the energy threshold Cherenkov

More information

Performance of the MCP-PMTs of the TOP counter in the first beam operation of the Belle II experiment

Performance of the MCP-PMTs of the TOP counter in the first beam operation of the Belle II experiment Performance of the MCP-PMTs of the TOP counter in the first beam operation of the Belle II experiment K. Matsuoka (KMI, Nagoya Univ.) on behalf of the Belle II TOP group 5th International Workshop on New

More information

A Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers

A Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers A Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers APS Division of Nuclear Physics Meeting October 25, 2008 GlueX Photon Spectrum Bremsstrahlung in diamond

More information

SCINTILLATOR DETECTORS FOR THE ESS HIGH ENERGY WIRE SCANNER

SCINTILLATOR DETECTORS FOR THE ESS HIGH ENERGY WIRE SCANNER MOPL8 Proceedings of HB6, Malmö, Sweden SCINTILLATOR DETECTORS FOR THE ESS HIGH ENERGY WIRE SCANNER B. Cheymol, European Spallation Source, Lund, Sweden Abstract In the ESS linac [], during commissioning

More information

Construction and first beam-tests of silicon-tungsten prototype modules for the CMS High Granularity Calorimeter for HL-LHC

Construction and first beam-tests of silicon-tungsten prototype modules for the CMS High Granularity Calorimeter for HL-LHC TIPP - 22-26 May 2017, Beijing Construction and first beam-tests of silicon-tungsten prototype modules for the CMS High Granularity Calorimeter for HL-LHC Francesco Romeo On behalf of the CMS collaboration

More information

CALICE Software. Data handling, prototype reconstruction, and physics analysis. Niels Meyer, DESY DESY DV Seminar June 29, 2009

CALICE Software. Data handling, prototype reconstruction, and physics analysis. Niels Meyer, DESY DESY DV Seminar June 29, 2009 CALICE Software Data handling, prototype reconstruction, and physics analysis Niels Meyer, DESY DESY DV Seminar June 29, 2009 The ILC Well, the next kid around the block (hopefully...) Precision physics

More information

Investigation of a Transmission-Line Readout for Building PET Detector Modules

Investigation of a Transmission-Line Readout for Building PET Detector Modules Investigation of a Transmission-Line Readout for Building PET Detector Modules Contents 1. Introduction 2. Simulation Setup 3. Results 4.Summary and Plans Heejong Kim, Univ. of Chicago Pico-Second Workshop

More information

Development of Personal Dosimeter Using Electronic Dose Conversion Method

Development of Personal Dosimeter Using Electronic Dose Conversion Method Proceedings of the Korean Nuclear Spring Meeting Gyeong ju, Korea, May 2003 Development of Personal Dosimeter Using Electronic Dose Conversion Method Wanno Lee, Bong Jae Lee, and Chang Woo Lee Korea Atomic

More information

Spatially Resolved Backscatter Ceilometer

Spatially Resolved Backscatter Ceilometer Spatially Resolved Backscatter Ceilometer Design Team Hiba Fareed, Nicholas Paradiso, Evan Perillo, Michael Tahan Design Advisor Prof. Gregory Kowalski Sponsor, Spectral Sciences Inc. Steve Richstmeier,

More information

HAPD Status. S. Nishida KEK. Dec 11, st Open Meeting of the SuperKEKB collaboration. HAPD Status. 1st SuperKEKB Meeting 1

HAPD Status. S. Nishida KEK. Dec 11, st Open Meeting of the SuperKEKB collaboration. HAPD Status. 1st SuperKEKB Meeting 1 S. Nishida KEK 1st Open Meeting of the SuperKEKB collaboration Dec 11, 2008 1 Contents 144ch HAPD Key Issues Summary I. Adachia, R. Dolenecb, K. Harac, T. Iijimac, H. Ikedad, Y. Ishiie, H. Kawaie, S. Korparb,f,

More information

The LHCb Silicon Tracker

The LHCb Silicon Tracker Journal of Instrumentation OPEN ACCESS The LHCb Silicon Tracker To cite this article: C Elsasser 214 JINST 9 C9 View the article online for updates and enhancements. Related content - Heavy-flavour production

More information

UV Light Shower Simulator for Fluorescence and Cerenkov Radiation Studies

UV Light Shower Simulator for Fluorescence and Cerenkov Radiation Studies UV Light Shower Simulator for Fluorescence and Cerenkov Radiation Studies P. Gorodetzky, J. Dolbeau, T. Patzak, J. Waisbard, C. Boutonnet To cite this version: P. Gorodetzky, J. Dolbeau, T. Patzak, J.

More information

A tracking detector to study O(1 GeV) ν μ CC interactions

A tracking detector to study O(1 GeV) ν μ CC interactions A tracking detector to study O(1 GeV) ν μ CC interactions Laura Pasqualini on behalf of the mm-tracker Collaboration IPRD16, 3-6 October 2016, Siena Motivations ν/μ Tracking system for a light magnetic

More information

R & D for Aerogel RICH

R & D for Aerogel RICH 1 R & D for Aerogel RICH Ichiro Adachi KEK Proto-Collaboration Meeting March 20, 2008 2 1 st Cherenkov Image detected by 3 hybrid avalanche photon detectors from a beam test About 3:00 AM TODAY Clear image

More information

X-Ray Transport, Diagnostic, & Commissioning Plans. LCLS Diagnostics and Commissioning Workshop

X-Ray Transport, Diagnostic, & Commissioning Plans. LCLS Diagnostics and Commissioning Workshop X-Ray Transport, Diagnostic, & Commissioning Plans LCLS Diagnostics and Commissioning Workshop *This work was performed under the auspices of the U.S. Department of Energy by the University of California,

More information

LCLS Injector Diagnostics. Henrik Loos. Diagnostics overview Transverse Beam Properties Longitudinal Beam Properties

LCLS Injector Diagnostics. Henrik Loos. Diagnostics overview Transverse Beam Properties Longitudinal Beam Properties Diagnostics overview Transverse Beam Properties Longitudinal Beam Properties LCLS Diagnostics Tasks Charge Toroids (Gun, Inj, BC, Und) Faraday cups (Gun & Inj) Trajectory & energy Stripline BPMs (Gun,

More information

The CMS Outer HCAL SiPM Upgrade.

The CMS Outer HCAL SiPM Upgrade. The CMS Outer HCAL SiPM Upgrade. Artur Lobanov on behalf of the CMS collaboration DESY Hamburg CALOR 2014, Gießen, 7th April 2014 Outline > CMS Hadron Outer Calorimeter > Commissioning > Cosmic data Artur

More information

Attenuation length in strip scintillators. Jonathan Button, William McGrew, Y.-W. Lui, D. H. Youngblood

Attenuation length in strip scintillators. Jonathan Button, William McGrew, Y.-W. Lui, D. H. Youngblood Attenuation length in strip scintillators Jonathan Button, William McGrew, Y.-W. Lui, D. H. Youngblood I. Introduction The ΔE-ΔE-E decay detector as described in [1] is composed of thin strip scintillators,

More information

Performance of Microchannel Plates Fabricated Using Atomic Layer Deposition

Performance of Microchannel Plates Fabricated Using Atomic Layer Deposition Performance of Microchannel Plates Fabricated Using Atomic Layer Deposition Andrey Elagin on behalf of the LAPPD collaboration Introduction Performance (timing) Conclusions Large Area Picosecond Photo

More information

P ILC A. Calcaterra (Resp.), L. Daniello (Tecn.), R. de Sangro, G. Finocchiaro, P. Patteri, M. Piccolo, M. Rama

P ILC A. Calcaterra (Resp.), L. Daniello (Tecn.), R. de Sangro, G. Finocchiaro, P. Patteri, M. Piccolo, M. Rama P ILC A. Calcaterra (Resp.), L. Daniello (Tecn.), R. de Sangro, G. Finocchiaro, P. Patteri, M. Piccolo, M. Rama Introduction and motivation for this study Silicon photomultipliers ), often called SiPM

More information

Readout ASICs and Electronics for the 144-channel HAPDs for the Aerogel RICH at Belle II

Readout ASICs and Electronics for the 144-channel HAPDs for the Aerogel RICH at Belle II Available online at www.sciencedirect.com Physics Procedia 37 (2012 ) 1730 1735 TIPP 2011 - Technology and Instrumentation in Particle Physics 2011 Readout ASICs and Electronics for the 144-channel HAPDs

More information

Testing the Electronics for the MicroBooNE Light Collection System

Testing the Electronics for the MicroBooNE Light Collection System Testing the Electronics for the MicroBooNE Light Collection System Kathleen V. Tatem Nevis Labs, Columbia University & Fermi National Accelerator Laboratory August 3, 2012 Abstract This paper discusses

More information

Particle identification at Belle-II

Particle identification at Belle-II Particle identification at Belle-II Matthew Barrett University of Hawaiʻi at Mānoa University of Oxford seminar Outline The B factories Belle II and superkekb The TOP subdetector The Belle II sub-detectors

More information

A TUNGSTEN PIN CUSHION PHOTON BEAM MONITOR* Guthrie Miller Department of Physics University of Washington, Seattle, Washington 98105, USA

A TUNGSTEN PIN CUSHION PHOTON BEAM MONITOR* Guthrie Miller Department of Physics University of Washington, Seattle, Washington 98105, USA SLAC-PUB-1297 (I/A) August 1973 A TUNGSTEN PIN CUSHION PHOTON BEAM MONITOR* Guthrie Miller Department of Physics University of Washington, Seattle, Washington 98105, USA Dieter R. Walz Stanford Linear

More information

Proximity focusing RICH with flat pannel PMTs as photon detector

Proximity focusing RICH with flat pannel PMTs as photon detector Proximity focusing RICH with flat pannel PMTs as photon detector Peter Križan University of Ljubljana and J. Stefan Institute For Belle Aerogel RICH R&D group Contents Motivation and requirements Beam

More information

Production of HPDs for the LHCb RICH Detectors

Production of HPDs for the LHCb RICH Detectors Production of HPDs for the LHCb RICH Detectors LHCb RICH Detectors Hybrid Photon Detector Production Photo Detector Test Facilities Test Results Conclusions IEEE Nuclear Science Symposium Wyndham, 24 th

More information

STUDY OF NEW FNAL-NICADD EXTRUDED SCINTILLATOR AS ACTIVE MEDIA OF LARGE EMCAL OF ALICE AT LHC

STUDY OF NEW FNAL-NICADD EXTRUDED SCINTILLATOR AS ACTIVE MEDIA OF LARGE EMCAL OF ALICE AT LHC STUDY OF NEW FNAL-NICADD EXTRUDED SCINTILLATOR AS ACTIVE MEDIA OF LARGE EMCAL OF ALICE AT LHC O. A. GRACHOV Department of Physics and Astronomy, Wayne State University, Detroit, MI 48201, USA T.M.CORMIER

More information

Beam Loss Calibration Studies at the LHC Collimator in LSS5

Beam Loss Calibration Studies at the LHC Collimator in LSS5 Beam Loss Calibration Studies at the LHC Collimator in LSS5 Experiment and Simulation BLM Team Till Böhlen 1 Outline Project Introduction Purpose, Aims & Related Work Experiment @ SPS Simulations Measurements,

More information

SAM (Swift Analogue Memory): a new GHz sampling ASIC for the HESS-II Front-End Electronics.

SAM (Swift Analogue Memory): a new GHz sampling ASIC for the HESS-II Front-End Electronics. SAM (Swift Analogue Memory): a new GHz sampling ASIC for the HESS-II Front-End Electronics. E. Delagnes 1, Y. Degerli 1, P. Goret 1, P. Nayman 2, F. Toussenel 2, P. Vincent 2 1 DAPNIA, CEA/Saclay 2 IN2P3/LPNHE

More information

Development of an atmospheric Cherenkov era for the CANGAROO-III experiment

Development of an atmospheric Cherenkov era for the CANGAROO-III experiment The Universe Viewed in Gamma-Rays 1 imaging cam- Development of an atmospheric Cherenkov era for the CANGAROO-III experiment S. Kabuki, K. Tsuchiya, K. Okumura, R. Enomoto, T. Uchida, and H. Tsunoo Institute

More information

TOP R&D status. Noriaki Sato (Nagoya Univ.) Super B-Factory Workshop in Hawaii. Status MCP-PMT R&D Summary

TOP R&D status. Noriaki Sato (Nagoya Univ.) Super B-Factory Workshop in Hawaii. Status MCP-PMT R&D Summary TOP R&D status Noriaki Sato (Nagoya Univ.) 2005.04.20 Super B-Factory Workshop in Hawaii Status MCP-PMT R&D Summary Status of TOP Counter, 2005.04.20 Super B-Factory Workshop p.1/22 TOP Counter Ring Imaging

More information

Photon sandwich detectors with WLS fiber readout

Photon sandwich detectors with WLS fiber readout Photon sandwich detectors with WLS fiber readout arxiv:physics/0207033v1 [physics.ins-det] 9 Jul 2002 O. Mineev a,, E. Garber b, J. Frank b, A. Ivashkin a, S. Kettell b, M. Khabibullin a, Yu. Kudenko a,

More information

Monte Carlo study on a new concept of a scanning photon beam system for IMRT

Monte Carlo study on a new concept of a scanning photon beam system for IMRT NUKLEONIKA 2011;56(4):291 297 ORIGINAL PAPER Monte Carlo study on a new concept of a scanning photon beam system for IMRT Anna M. Wysocka-Rabin, Günter H. Hartmann Abstract. Intensity-modulated radiation

More information

The DIRC-like TOF : a time-of-flight Cherenkov detector for particle identification at SuperB

The DIRC-like TOF : a time-of-flight Cherenkov detector for particle identification at SuperB The DIRC-like TOF : a time-of-flight Cherenkov detector for particle identification at SuperB Laboratoire de l Accélérateur Linéaire (CNRS/IN2P3), Université Paris-Sud 11 N. Arnaud, D. Breton, L. Burmistrov,

More information

BaBar and PEP II. Physics

BaBar and PEP II. Physics BaBar and PEP II BaBar SVT DCH DIRC ECAL IFR Trigger Carsten Hast LAL Orsay December 8th 2000 Physics Main Goal: CP Violation sin2β,sin2α PEP II Performance Backgrounds December 8th 2000 Carsten Hast PEP

More information

Digitization of PMT signals with FADCs: comparison of simulation and measurement

Digitization of PMT signals with FADCs: comparison of simulation and measurement Digitization of PMT signals with FADCs: comparison of simulation and measurement Arno Gadola General, 10. 12.05.2010 Outline Summary of previous presentations Impact of sampling rate Verification of simulation

More information

Monolithic Pixel Sensors in SOI technology R&D activities at LBNL

Monolithic Pixel Sensors in SOI technology R&D activities at LBNL Monolithic Pixel Sensors in SOI technology R&D activities at LBNL Lawrence Berkeley National Laboratory M. Battaglia, L. Glesener (UC Berkeley & LBNL), D. Bisello, P. Giubilato (LBNL & INFN Padova), P.

More information

Progress on development of the new FDIRC PID detector

Progress on development of the new FDIRC PID detector Progress on development of the new FDIRC PID detector N. Arnaud c, A.Yu. Barnyakov a, M.Yu. Barnyakov a,c. Beigbeder c, M. Benettoni j, M. El Berni c, M. Borsato c, D. Breton c, L.Burmistrov c, G. Collazuol

More information

The HPD DETECTOR. Michele Giunta. VLVnT Workshop "Technical Aspects of a Very Large Volume Neutrino Telescope in the Mediterranean Sea"

The HPD DETECTOR. Michele Giunta. VLVnT Workshop Technical Aspects of a Very Large Volume Neutrino Telescope in the Mediterranean Sea The HPD DETECTOR VLVnT Workshop "Technical Aspects of a Very Large Volume Neutrino Telescope in the Mediterranean Sea" In this presentation: The HPD working principles The HPD production CLUE Experiment

More information

The Scintillator HCAL Testbeam Prototype

The Scintillator HCAL Testbeam Prototype 2005 International Linear Collider Workshop - Stanford, U.S.A. The Scintillator HCAL Testbeam Prototype F. Sefkow DESY, Hamburg, Germany CALICE Collaboration The CALICE tile HCAL group has completed the

More information

PREX- 2 Issues. April 11, Kent Paschke

PREX- 2 Issues. April 11, Kent Paschke PREX- 2 Issues April 11, 2014 Kent Paschke What We Learned in PREX-I What Worked: New Septum We now know how to tune it to optimize FOM A T false asymmetry A T is small (

More information

HPS ECal & Trigger Simulation. HPS Collaboration Meeting.

HPS ECal & Trigger Simulation. HPS Collaboration Meeting. HPS ECal & Trigger Simulation HPS Collaboration Meeting. May 7, 11 HPS Electromagnetic Calorimeter HPS Experiment needs the calorimeter to identify the electron/ positron pair and to construct the trigger.

More information

HERA-B RICH. Samo Korpar

HERA-B RICH. Samo Korpar HERA- RICH 1. Introduction 2. The design of the RICH 3. Measured parameters of the RICH 4. Particle identification 5. Conclusions HERA- RICH (page 1) HERA- RICH group P. Križan 1, A. Gorišek 1, S. Korpar

More information

Electron Beam Properties and Instrumentation MOLLER Director s Review, Jan. 14, 2010 Mark Pitt, Virginia Tech

Electron Beam Properties and Instrumentation MOLLER Director s Review, Jan. 14, 2010 Mark Pitt, Virginia Tech Electron Beam Properties and Instrumentation MOLLER Director s Review, Jan. 14, 2010 Mark Pitt, Virginia Tech This talk will focus on the electron beam properties and beam instrumentation requirements

More information

Summer Student project report

Summer Student project report Summer Student project report Mika Väänänen September 1, 2017 Abstract In this report I give a brief overview of my activities during the summer student project. I worked on the scintillating fibre (SciFi)

More information

Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning

Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning Technology and Instrumentation in Particle Physics 2011 Chicago, June 11 Jacqueline Yan, M.Oroku, Y. Yamaguchi T. Yamanaka, Y. Kamiya, T.

More information

Fragment Mass Analyzer Argonne N.L.

Fragment Mass Analyzer Argonne N.L. Fragment Mass Analyzer (FMA) @ Argonne N.L. Version 9.10.177 from 09/11/2015 Link: Separator FMA @ ANL FMA extended configuration Documentation FMA files location Optics Optimization Angular Acceptance

More information

MEASUREMENT OF BEAM LOSSES USING OPTICAL FIBRES AT THE AUSTRALIAN SYNCHROTRON

MEASUREMENT OF BEAM LOSSES USING OPTICAL FIBRES AT THE AUSTRALIAN SYNCHROTRON MEASUREMENT OF BEAM LOSSES USING OPTICAL FIBRES AT THE AUSTRALIAN SYNCHROTRON E. Nebot del Busto (1,2), M. J. Boland (3,4), E. B. Holzer (1), P. D. Jackson (5), M. Kastriotou (1,2), R. P. Rasool (4), J.

More information