The Crystal Barrel Experiment at ELSA
|
|
- Madeleine Sharp
- 5 years ago
- Views:
Transcription
1 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 1 The Crystal Barrel at ELSA Friedemann Zenke HISKP, University of Bonn Bonn Cologne Graduate School of and Astronomy Funded by DFG with SFB/TR16 June 18, 2008
2 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 2 Outline 1 2 3
3 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 3 Hadron spectroscopy atom nucleon Ba Ca
4 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 4 Missing Resonances N* resonances, Löring, Metsch, Petry, EPJA 10, 395(2001)
5 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 5 Overlapping Resonances A resonance might be hidden beneath another γ + N N N + π γ + N N N + η
6 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 6 Polarization Variables Can be disentangled with help of Polarization Variables More in Jan s talk
7 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 7 Outline 1 2 3
8 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 8 ELectron Stretcher Figure: University of Bonn, CW polarized electron accelerator
9 al Area Overview The Crystal Barrel at ELSA HISKP, Friedemann Zenke 9
10 The Bonn Frozen Spin Polarized Figure: Schematic of Polarized Cryostat Butanol frozen spin target Polarization up to 90% Decay times > 200h Ch. Bradtke et al. NIM A436 p. 430 (1999) The Crystal Barrel at ELSA HISKP, Friedemann Zenke 10
11 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 11 Tagging Photons e - Bremsstrahlung Radiator magnet 600 MeV Counts Scintillator bars E [MeV]
12 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 12 Crystal Barrel - Full Assembly
13 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 13 Outline 1 2 3
14 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 14 Current Status and Intended Current deficits No good charge particle tracking No time information from single CsI crystal Main calorimeter not in first level trigger
15 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 14 Current Status and Intended Current deficits No good charge particle tracking No time information from single CsI crystal Main calorimeter not in first level trigger Intended changes New time projection chamber (TPC) in combination with new superconducting solenoid and existing iron return yoke New single crystal readout, new first level trigger
16 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 15 Upgrade: Planned upgrades Insert TPC into calorimeter Add superconducting magnet to setup Track and momentum reconstruction on charged particles
17 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 16 Upgrade: Light 1 Speed up crystal light readout to gain trigger opportunity on Barrel 2 Replacing current QDCs by Flash-ADCs to increase both readout rates and energy resolution Currently testing new Light with two Large Area Avalanche Photo Diodes my thesis Energy Time Figure: Crystal end cap with new APD readout
18 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 17 Figure: Array of CsI(Tl) crystals with new APD readout for testing purposes
19 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 18 First Performance Results: Energy Resolution for reference: Figure: Low E energy spectrum recorded with new APD readout kept at 20 o C Figure: Reference spectrum taken with PMT currently σ π0 = 8MeV
20 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 19 First Performance Results: Time Resolution Figure: Time resolution measurement with tagged photon beam
21 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 20 and On-The-Fly FPGA Based Feature Extraction Extraction of Energy Pedestal Tail Further information Extraction of Time via Constant fraction or via optimized risetime compensating scheme Generation of a fast signal for trigger Risetime compensating timing extraction Fast time over threshold output for trigger
22 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 21 Exciting hadron spectroscopy is happening at Bonn Capabilities for double polarization experiments Several improvements planned Charged particle identification planned: TPC, magnetic field More efficient readout: more efficient trigger, better energy/time resolution
23 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 22 Acknowledgments
24 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 23
25 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 24 Risetime compensating timing extraction Fast time over threshold output for trigger
26 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 25 Energy resolution σ(m π0 ) = 8MeV Overall energy resolution like 2.5% 4 E[GeV ] Approximate energy resolution [%] E [MeV]
27 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 26 The Crystal Barrel Detector Inner detector A high precision calorimeter 513 scintillating fibres in 3 layers Charged particle identification 1280 CsI(Tl) crystals Read out by photo diodes θ coverage 30 o to 156 o
28 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 27 Detection in Forward Direction Forward plug Mini TAPS 90 CsI(Tl) crystals 180 front side plastic scintillators 12 o - 30 o coverage in θ 216 BaF 2 crystals 2 o - 12 o in θ
29 The Crystal Barrel at ELSA HISKP, Friedemann Zenke 28 Upgrade: Return Yoke and Magnet Superconducting solenoid (2.5 T) Use of existing return yoke from
LYSO Crystal Based Shashlik Calorimeter Cell Design
LYSO Crystal Based Shashlik Calorimeter Cell Design Ren-Yuan Zhu California Institute of Technology August 30, 2012 Talk given at CMS Forward Calorimetry Taskforce Meeting Options for CMS FCAL Upgrade
More informationExploring Crystal Calorimetry for A Linear Collider Detector
Exploring Crystal Calorimetry for A Linear Collider Detector Usha Mallik (The University of Iowa)[contact person], Milind Purohit (University of South Carolina), Jack Ritchie (University of Texas at Austin),
More informationDevelopment of LYSO Crystals for CMS at SLHC. Ren-Yuan Zhu. California Institute of Technology
Development of LYSO Crystals for CMS at SLHC Ren-Yuan Zhu California Institute of Technology Crystal Degradation in situ L3 BGO: 6 7% in 7 years BaBar CsI(Tl): 1-3 % per year BGO CsI(Tl) 2 Effect of PWO
More informationRadiation Hardness Study of CsI(Tl) Crystals for the Belle II Calorimeter
Proceedings of the CERN-BINP Workshop for Young Scientists in e + e Colliders, Geneva, Switzerland, 22 25 August 2016, edited by V. Brancolini ans L. Linssen, CERN Proceedings, Vol. 1/2017, CERN-Proceedings-2017-001
More informationThe production of radiation tolerant vacuum phototriodes and their HV filters for the CMS endcap electromagnetic calorimeter
The production of radiation tolerant vacuum phototriodes and their HV filters for the CMS endcap electromagnetic calorimeter Peter R Hobson* On behalf of the Group *School of Engineering & Design, Brunel
More informationProton Induced Radiation Damage in Fast Crystal Scintillators
Proton Induced Radiation Damage in Fast Crystal Scintillators Fan Yang, Liyuan Zhang, Ren-Yuan Zhu California Institute of Technology Jon S. Kapustinsky, Daniel C. Poulson, Jeff Wang Los Alamos National
More informationScintillating Optical Fibers
Scintillating Optical Fibers CRYSTALS Plastic Scintillating Fibers Saint-Gobain Crystals manufactures a variety of plastic scintillating, wavelength-shifting and lighttransmitting fibers used for research
More informationThe CMS calorimeter in 2007: Performance and physics goals
Geo Magazine, May 2007 The CMS calorimeter in 2007: Performance and physics goals Paul Lecoq CERN, Geneva On behalf of the CMS-ECAL group P. Lecoq CERN 1 Outline General considerations Crystals Photodetectors
More informationPerformance of Lead Tungstate Crystals for the CMS Electromagnetic Calorimeter
Performance of Lead Tungstate Crystals for the CMS Electromagnetic Calorimeter Ioan Dafinei I.N.F.N. Sezione di Roma, Rome ITALY (on behalf of CMS ECAL Collaboration) Index 1. PWO general properties 2.
More informationNews on PbWO 4 Crystals
June 16, 2015 Jlab - R. W. Novotny News on PbWO 4 Crystals R. W. Novotny II.Physics Institute, University Giessen, Germany and for the PANDA collaboration The PANDA requirements Some comments on radiation
More informationStatus of the GERDA experiment NOW2008 JJ
Status of the GERDA experiment J. Janicskó-Csáthy NOW2008 JJ GERDA GErmanium Detector Array Double β decay The GERDA experiment (Phase I) Phase II R&D NOW2008 JJ 1/18 Double β decay 2ν2β 2ν2β + 0ν2β spectrum
More informationCMS combined Ecal-Hcal testbeam
CMS combined Ecal-Hcal testbeam Lisa Berntzon, Texas Tech. University, on behalf of the CMS Collaboration IPRD06 Siena 1-5 Oct 2006 Siena 2006 Lisa Berntzon 1 CMS calorimeter system HCAL : HB - Hcal Barrel
More informationDevelopment of a Dose Profiler for range monitoring in particle therapy
Università degli studi di Roma La Sapienza Dottorato di ricerca in Fisica, Development of a Dose Profiler for range monitoring in particle therapy Ph.D. candidate: Giacomo Traini Supervisor: Prof. Riccardo
More informationSearch for Scintillation in Doped Lead Fluoride Crystals
Search for Scintillation in Doped Lead Fluoride Crystals Rihua Mao, Liyuan Zhang, Ren-yuan Zhu California Institute of Technology October 29, 2009 Paper N40-2, 2009 NSS/MIC at Orlando, USA Introduction
More informationBacksplash study. Alex Moiseev 05/22/2001
Backsplash study Alex Moiseev 05/22/2001 1 Purpose High energy particle instruments which contain a heavy calorimeter to measure the energy of detected particles produce radiation emitted backward from
More informationDetector Solenoid and Iron Structure
Chapter 11 Detector Solenoid and Iron Structure 11.1 Iron Yoke TheironstructureoftheBelledetector servesasthereturnpathofmagneticfluxandanabsorber material for KLM. It also provides the overall support
More informationReport from Turku. Scanditronix Cyclotron Workshop Uppsala 23-25th May Stefan Johansson
Report from Turku Stefan Johansson Åbo Akademi University Accelerator laboratory Turku Finland Scanditronix Cyclotron Workshop Uppsala 23-25th May 2018 Turku PET Centre University of Turku Åbo Akademi
More informationRen-Yuan Zhu California Institute of Technology
Investigation on GSO:Ce Crystals Ren-Yuan Zhu California Institute of Technology October 30, 2012 Talk at CMS Forward Calorimetry Task Force Meeting CMS Forward Calorimeter Upgrade Issues: Radiation hardness
More informationQuality of Long LSO/LYSO Crystals
Home Search Collections Journals About Contact us My IOPscience Quality of Long LSO/LYSO Crystals This article has been downloaded from IOPscience. Please scroll down to see the full text article. 22 J.
More informationScintillating Optical Fibers
Scintillating Optical Fibers Plastic Scintillating Fibers Saint-Gobain Crystals manufactures a variety of plastic scintillating, wavelength-shifting and light-transmitting fibers used for research and
More informationUpdate on Inorganic Scintillator Development
Update on Inorganic Scintillator Development Ren-Yuan Zhu California Institute of Technology June 22, 2017 Talk Given in Optical Detector R&D Meeting at CERN Fast & Radiation Hard Scintillators Supported
More informationCrystal Calorimeters at Linear Collider
Crystal Calorimeters at Linear Collider Ren-yuan Zhu California Institute of Technology Outline Crystal Calorimetry for LC: Why Crystal Calorimetry at LC; Possible Crystal Technologies for LC. Recent Progress
More informationApplications of Very Fast Inorganic Crystal Scintillators in Future HEP Experiments
Applications of Very Fast Inorganic Crystal Scintillators in Future HEP Experiments Ren-Yuan Zhu California Institute of Technology May 22, 2017 Talk Given in TIPP2017 Conference, Beijing, China Challenge
More informationCHAPTER 5. ABSORPTION AND FLUORESCENCE OF CsI(Tl) AND. CsI(Tl)In CRYSTALS
CHAPTER 5 ABSORPTION AND FLUORESCENCE OF CsI(Tl) AND CsI(Tl)In CRYSTALS 93 ABSTRACT In order to obtain a laser action in doped alkali halides crystals, fluorescence measurements have been performed in
More informationScintillating Optical Fibers
Scintillating Optical Fibers Plastic Scintillating Fibers Saint-Gobain Crystals manufactures a variety of plastic scintillating, wavelength-shifting and light-transmitting fibers used for research and
More informationProgress with crystal testing and selection
Progress with crystal testing and selection Salina Ali, Marco Carmignotto, Gabriel Charles, Frédéric Georges, T. Horn, Giulia Hull, Ian Pegg, Carlos Munoz-Camacho, Arthur Mkrtchyan, Hamlet Mkrtchyan, Sean
More informationA POSITRON SOURCE USING CHANNELING IN CRYSTALS FOR LINEAR COLLIDERS
A POSITRON SOURCE USING CHANNELING IN CRYSTALS FOR LINEAR COLLIDERS R.CHEHAB, X.ARTRU, M.CHEVALLIER, IPNL/ IN2P3/CNRS, UNIVERSITE LYON 1 V.M.STRAKHOVENKO, BINP-NOVOSIBIRSK A.VARIOLA, A.VIVOLI, LAL/IN2P3/CNRS,
More informationCsI crystals for the HIgh Resolution Array uniformity of the response.
CsI crystals for the HIgh Resolution Array uniformity of the response. M.J. van Goethem, M. Wallace. B. Net., W.G. Lynch, B. Tsang NSCL R. DeSouza, A.Carley, B.Devin,S. Hudan. IUCF L. Sobotka, G. Engel,
More informationScintillator tests for SpecMAT. J. A. Swartz. ACTAR TPC Collaboration Workshop GANIL, Caen 19/11/2015
Scintillator tests for SpecMAT J. A. Swartz ACTAR TPC Collaboration Workshop GANIL, Caen 19/11/2015 Contents 1. Introduction 2. Cubic scintillators with SiPMs 3. Cylindrical scintillators with PMTs + GET
More informationCross-calibration of two automatic quality control systems for the CMS ECAL crystals
Cross-calibration of two automatic quality control systems for the CMS ECAL crystals E. Auffray, S. Baccaro, E. Bouquerel, F. Cavallari, G. Chevenier, S. Costantini, I. Dafinei, M. Diemoz, P. Lecoq, E.
More informationtillator for which mass-production capability is presently available.
IEEE TRANSACTIONS ON NUCLEAR SCIENCE 1 Quality of a 28 cm Long LYSO Crystal and Progress on Optical and Scintillation Properties Rihua Mao, Member, IEEE, Liyuan Zhang, Member, IEEE, and Ren-Yuan Zhu, Senior
More informationDetectors for CEνNS Neutrinos in nuclear physics workshop, July 2016 J.I. Collar, UC
Detectors for CEνNS Neutrinos in nuclear physics workshop, July 2016 J.I. Collar, UC Tendons 30 mwe Everyone needs a hobby San Onofre Unit 3 core 20m that way BaDAss (Background Detector Assembly) LN2
More informationRadiation Rules at KEK
2013 5 29 2013 5 29 Radiation Rules at KEK Normal operation 0.2 µsv/h for Non-designated area (K1) 1.5 µsv/h for Supervised area (K2) experimental hall 20 µsv/h for Simple controlled area (K3) 100mSv/h
More informationMeasuring Ytterbium Neutron Cross Section at 2.5 MeV. Norbert Hugger
Project Number DM3 - AA9R Measuring Ytterbium Neutron Cross Section at 2.5 MeV A Major Qualifying Project Submitted to the Faculty of WORCESTER POLYTECHNIC INSTITUTE in partial fulfillment of the requirements
More informationThinking ahead: a new era in terahertz research
Thinking ahead: a new era in terahertz research Dedicated researchers across the world are studying the terahertz (THz) frequency range and the wide range of benefits it offers. THz has the potential to
More informationFNAL-NICADD NICADD extruded scintillator
FERMILAB FNAL-NICADD NICADD extruded scintillator Presented by Victor Rykalin Rome 1, October 24 1 FNAL-NICADD EXTRUSION FACILITY POLYMER FEEDER POLYMER DRYER DOPANT FEEDER EXTRUDER MELT PUMP DIE OUTPUT:
More informationCalculation of Water Activity in Point 7
Calculation of Water Activity in Point 7 SC/RP, M. Brugger, S. Roesler joachim.vollaire@cern.ch Calculation of Water Activity in Point 7 Production of radioactive nuclei in water Production on Oxygen atom
More informationProgress on Single Crystals for Detection of High-Energy Particles. Jindřich Houžvička
Progress on Single Crystals for Detection of High-Energy Particles Jindřich Houžvička houzvicka@crytur.cz CRYTUR Crytur is one of the world leading companies in synthetic crystal manufacturing with history
More informationIEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 57, NO. 6, DECEMBER
IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 57, NO. 6, DECEMBER 2010 3841 A Search for Scintillation in Doped Cubic Lead Fluoride Crystals Rihua Mao, Member, IEEE, Liyuan Zhang, Member, IEEE, and Ren-Yuan
More informationA Survey of Laser Types. Gas Lasers
Mihail Pivtoraiko Andrei Rozhkov Applied Optics Winter 2003 A Survey of Laser Types Laser technology is available to us since 1960 s, and since then has been quite well developed. Currently, there is a
More informationJuhee Lee KIMS collaboration For Giessen University MEASUREMENT OF QUENCHING AND CHANNELING IN CSI(TL)
Juhee Lee KIMS collaboration For SCINT2011 @ Giessen University MEASUREMENT OF QUENCHING AND CHANNELING IN CSI(TL) 2011-11-15 SCINT2011 1 CONTENTS 1. 2. 3. 4. Motivation Channeling effect & Dark Matter
More informationThe Influence of Chemical and Color Quenching on the Shape of Energy Spectrum for Beta Particles of 90 Sr 90 Y by Using Liquid Scintillation Cocktail
Bulg. J. Phys. 35 (2008) 142 150 The Influence of Chemical and Color Quenching on the Shape of Energy Spectrum for Beta Particles of 90 Sr 90 Y by Using Liquid Scintillation Cocktail M.W.M. Al-Badrani
More informationPoS(ICHEP2012)382. Status of the Gadolinium project for Super-Kamiokande. Takatomi Yano for The Super-Kamiokande Collaboration
Status of the Gadolinium project for Super-Kamiokande for The Super-Kamiokande Collaboration Okayama University E-mail: tyano@fphy.hep.okayama-u.ac.jp EGADS (Evaluating Gadolinium s Action on Detector
More informationEnergy Spectrum of Cosmic-Ray Photons Observed at the Ground Level in Japan
Energy Spectrum of Cosmic-Ray Photons Observed at the Ground Level in Japan H.Sagawa and I.Urabe Fukuyama University, Hiroshima 729-0292, Japan INTRODUCTION The public was exposed to terrestrial gamma-rays,
More informationPhotoluminescence Spectroscopy on Chemically Synthesized Nanoparticles
Photoluminescence Spectroscopy on Chemically Synthesized Nanoparticles Torben Menke 1 Institut für Angewandte Physik und Zentrum für Mikrostrukturforschung Universität Hamburg Diploma Talk, 18.12.27 1
More informationCrystal Calorimeters for Future HEP Experiments
Crystal Calorimeters for Future HEP Experiments Ren-Yuan Zhu California Institute of Technology January 11, 2013 Talk at the Joint CPAD and Instrumentation Frontier Community Meeting, ANL Why Crystal Calorimeter
More informationATTACHMENTES FOR APD 2000 PRO POWDER X-RAY DIFFRACTOMETER. Monochromators
Monochromators Secondary graphite monochromator Johansson Ka 1 monochromator Parabolic monochromator Secondary flat and curved graphite monochromators suitable for Ag, Cr, Fe, Cu, Co and Mo radiations
More informationProgress Status of SBS GEMs
Progress Status of SBS GEMs Kondo Gnanvo Hall A/C Summer Collaboration Meeting 06/22/2017 Outline Production Status of SBS GEM Modules GEM Readout and DAQ Preparation for GMn Experiment Why GEMs for Super
More informationSBDUV-APD Solar-Blind Deep UV APDs
SBDUV-APD Solar-Blind Deep UV APDs Industry Day Dr. Y. K. Chen DARPA 9/18/2018 Distribution Statement A (Approved for Public Release, Distribution Unlimited) 1 SBDUV-APD Technical Background Distribution
More informationIrradiation Studies on Inorganic Scintillators (LYSO & BaF 2 )
Irradiation Studies on Inorganic Scintillators (LYSO & BaF 2 ) Ren-Yuan Zhu California Institute of Technology November 8, 2017 Talk in the CMS MTD - Barrel Sensors Meeting Fast & Radiation Hard Scintillators
More informationMeasurement Probe Brochures
Measurement Probe Brochures Papers Cryogenic News March 2012 World s first 18 Tesla Cryogen Free VSM Measurement system with sample rotating He-3 insert Cryocooled Cryostat For Use With Ccc/Josephson Array
More informationNPS Calorimeter Curing System
NPS Calorimeter Curing System All known crystals suffer from radiation damage. The most common damage phenomenon is radiation-induced absorption (reduction in crystal s light attenuation length). Studies
More informationThe New Engine Exhaust CPC
The New Engine Exhaust CPC Model 3790 EECPC Mark Crooks Regional Sales Manager TSI Instruments Ltd Schematic Diagram New design of the saturator and condenser: - Anti-spill - Water removal - Improved temperature
More informationPhosphor Screens. Applications. Features. Taper and glass substrates with phosphor layer.
Phosphor Screens Taper and glass substrates with phosphor layer. Structure of a phosphor screen with ITO base coating, chromium ring, phosphor layer and aluminium reflection layer. Applications Electron
More informationECE 440 Lecture 27 : Equilibrium P-N Junctions I Class Outline:
ECE 440 Lecture 27 : Equilibrium P-N Junctions I Class Outline: Fabrication of p-n junctions Contact Potential Things you should know when you leave Key Questions What are the necessary steps to fabricate
More informationCrystals for the Homogeneous Hadron Calorimeter Detector Concept
Crystals for the Homogeneous Hadron Calorimeter Detector Concept Ren-yuan Zhu California Institute of Technology October 20, 2010 International Workshop on Linear Colliders 2010, CERN Homogeneous Hadron
More informationBuilding better baffles. R. Holmes SoLID collaboration meeting 5/14/15
Building better baffles R. Holmes SoLID collaboration meeting 5/14/15 1 Zigzag, lead (π 0 generator) Baffle Total in baffles Total all z_v 1 2 3 4 5 6 7 8 9 10 11 p > 1 p > 10 standard zigzag % diff standard
More informationGEOLOGY 333 LAB 14. Lab Final Exam See information sheet for details
GEOLOGY 333 LAB 14 X-RAY DIFFRACTION OF EVERYDAY MATERIALS Lab Final Exam See information sheet for details! Next week during Lab (10 am - noon, May 2, 69 CAB).! 25% of Lab grade, out of 65 points plus
More informationIllinois Accelerator Research Center
FERMILAB-CONF-16-639-AD-DI ACCEPTED Conference on the Application of Accelerators in Research and Industry, CAARI 2016, 30 October 4 November 2016, Ft. Worth, TX, USA Illinois Accelerator Research Center
More information1420 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 55, NO. 3, JUNE 2008
1420 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 55, NO. 3, JUNE 2008 Development of Low Background CsI(Tl) Crystals and Search for WIMP H. J. Kim, H. S. Lee, H. C. Bhang, J. H. Choi, H. Dao, I. S. Hahn,
More informationRunaway Electron Transport & Disruption Mitigation Optimization on Alcator C-Mod
Runaway Electron Transport & Disruption Mitigation Optimization on Alcator C-Mod D.G. Whyte 1, R. Granetz 1, V. Izzo 2, M. Reinke 1, G. Olynyk 1 & Alcator C-Mod team 1 MIT Plasma Science & Fusion Center
More informationUltrafast and Radiation Hard Inorganic Scintillators for Future HEP Experiments
Ultrafast and Radiation Hard Inorganic Scintillators for Future HEP Experiments Ren-Yuan Zhu California Institute of Technology May 24, 2018 Talk in the XVIII International Conference on Calorimetry in
More informationExtruded Plastic Scintillation Detectors
Extruded Plastic Scintillation Detectors Anna Pla-Dalmau, Alan D. Bross and Kerry L. Mellott Fermi National Accelerator Laboratory P. O. Box 500, Batavia, IL 60510, USA As a way to lower the cost of plastic
More informationStructure Design of SciBar Tracker
Structure Design of SciBar Tracker H. Maesaka Kyoto University July 26, 2002 Abstract A SciBar tracker will be constracted as a new near detector for the KEK-to-Kamioka long-baseline neutrino oscillation
More informationEMC in BESIII Experiment
EMC in BESIII Experiment Weiguo Li Representing BESIII Collaboration Calor2010 May 10, 2010 IHEP, Beijing 1 Outline BEPCII /BESIII EMC Design and Construction EMC Performances Summary 2 n2.5m8sbepc II
More informationTechnical Proposal. A UV Laser Setup for Thinning Radiator Diamonds for GlueX
Technical Proposal A UV Laser Setup for Thinning Radiator Diamonds for GlueX Richard T. Jones (University of Connecticut) August 10, 2009 Executive Summary The GlueX experiment at Jefferson lab is a driving
More informationLiquid scintillator R&D in Europe
Liquid scintillator R&D in Europe, NNN08 Paris, September, 2008 Overview Introduction Scintillator components Energy transfers Metal loaded scintillators onclusions Liquid scintillator past and present
More informationFabrication and testing of Resistive Plate Chambers
Fabrication and testing of Resistive Plate Chambers 1 Aim 1. Coating graphite paint on electrodes and measuing the surface resistivity. 2. Measuring the bulk resistivity of bakelite/glass electrodes. 3.
More informationEach question may have MULTIPLE correct answers. Select all that are correct.
Knowledge Assessment Flow Cytometry Workshop, Part 1 April 20, 2015 Each question may have MULTIPLE correct answers. Select all that are correct. 1. Tandem dyes are a. highly stable fluorophores after
More informationGLAST Large Area Telescope:
Gamma-ray Large Area Space Telescope GLAST Large Area Telescope: Calorimeter (CAL) Subsystem WBS: 4.1.5 W. Neil Johnson Naval Research Lab, Washington DC Calorimeter Subsystem Manager neil.johnson@nrl.navy.mil
More informationRen-Yuan Zhu. 1 st Report on Twenty Mu2e BaF 2 Crystals from SIC. California Institute of Technology. June 25, 2014
1 st Report on Twenty Mu2e BaF 2 Crystals from SIC Ren-Yuan Zhu California Institute of Technology June 25, 2014 Mu2e Calorimeter Collaboration Meeting 1 Crystal Samples and Experiment SIC-1 SIC-2 SIC-3
More information9. VACUUM TANK 9. VACUUM TANK
9. VACUUM TANK This system constitutes the external part of the solenoid cryostat. The vacuum tank, made of stainless steel, is cantilevered from the central ring of the barrel yoke. It houses and supports
More informationCMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS NOTE 98/038 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland May 19, 1998 SPECIFICATIONS FOR LEAD TUNGSTATE
More informationNanophotonics with the Scanning Electron Microscope
Nanophotonics with the Scanning Electron Microscope Fredrik Jonsson, Andrey Denisyuk, Bruno Soares, Max Bashevoy, Zsolt Samson, Kevin MacDonald, Nikolay Zheludev EPSRC Nanophotonics Portfolio Centre Optoelectronics
More informationShort Minutes of the BVR 44
Short Minutes of the BVR 44 Meetings of January 14 16, 2013 1 Meetings of the Committee closed meetings: Tuesday, January 15, from 9:00 12:30 Wednesday, January 16, from 8:30 12:00 present: beam time coordinator:
More informationTopics Fukushima 15 September 2015 No.70
Topics Fukushima 15 September 2015 No.70 Examination of reactor cores using laser Analysis of elemental composition in fuel debris became possible How is the present situation of the reactor cores inside
More informationTRACE: silicon-detector array for direct and binary reaction at SPES
TRACE: silicon-detector array for direct and binary reaction at SPES Daniele Mengoni for the GHT collaboration Università and INFN - Padova SPES meeting, Milano 09-10 Dicembre 2013 Daniele Mengoni (Univ.
More informationTime-dependent transformations & off-hugoniot processes
Time-dependent transformations & off-hugoniot processes The scientific understanding of the dynamics of chemical and structural transitions can be dramatically advanced through the development of time-resolved
More informationTECHNIQUES OF INDUCTIVELY COUPLED PLASMA OPTICAL EMISSION SPECTROMETER S. KARTHIKEYAN SSA CENTRAL POLLUTION CONTROL BOARD SOUTH ZONE OFFICE BANGALORE
TECHNIQUES OF INDUCTIVELY COUPLED PLASMA OPTICAL EMISSION SPECTROMETER By S. KARTHIKEYAN SSA CENTRAL POLLUTION CONTROL BOARD SOUTH ZONE OFFICE BANGALORE INTRODUCTION ICP-OES is a sophisticated instrument
More informationGrowth and scintillation properties of Ce doped Gd 2. /SiO 2 O 7. Si 2. eutectics. Journal of Physics: Conference Series.
Journal of Physics: Conference Series PAPER OPEN ACCESS Growth and scintillation properties of Ce doped Gd eutectics Related content - Spectroscopy and scintillation properties of cerium doped YAl single
More information100 Percent Screening of Cargo Containers (Session 3A: Security II)
100 Percent Screening of Cargo Containers (Session 3A: Security II) MTS R&T Coordination Conference November 16-17, 17, 2004 Washington, D.C. Victor J. Orphan Science Applications International Corporation
More informationDirect Dark Matter Search with the CRESST-III Experiment
Direct Dark Matter Search with the CRESST-III Experiment Andrea Mu nster TUM TeVPA 2017 CRESST Collaboration A.Mu nster (TUM) Direct Dark Matter Search with CRESST-III 08/08/17 2 / 18 Direct Dark Matter
More informationAddendum No 3 to Collaboration Agreement KN3774/EP for the SHiP Program at CERN. Plastic-scintillator based timing detector prototype
Addendum No 3 to Collaboration Agreement KN3774/EP for the SHiP Program at CERN Plastic-scintillator based timing detector prototype 2 Considering that: The SHiP Program is governed by Collaboration Agreement
More informationStructure in mobile discrete-particle nonlinear lattice excitations.
Structure in mobile discrete-particle nonlinear lattice excitations. F M Russell, Heriot-Watt University. 15 February 2012 Mica as a detector of events at the atomic level. The discovery that natural crystals
More informationAging research of the LAB-based liquid scintillator in stainless. steel container *
Aging research of the LAB-based liquid scintillator in stainless steel container * CHEN Hai-tao 1,2;1) YU Bo-xiang 2,3;2) SHAN Qing 1 DING Ya-yun 2,3 DU Bing 2,3 Liu Shu-tong 2 ZHANG Xuan 2,3 ZHOU Li 2,3
More informationGeneral Fusion CNS
General Fusion CNS 2013 1 Fusion Technologies $ Cost of Confinement $ Cost of Driver Plasma Energy 1.00E+11 Driver Power 1.00E+15 GJ ITER $20B NIF $6B TW 1.00E+08 1.00E+12 MJ GF $150M GW 1.00E+05 1.00E+09
More informationTracking POG Kickoff. Joint DPG-POG Tracking Meeting October 27, Kevin Burkett (FNAL), Boris Mangano (UCSD)
Tracking POG Kickoff Joint DPG-POG Tracking Meeting October 27, 2008 Kevin Burkett (FNAL), Boris Mangano (UCSD) Welcome! First joint meeting between Tracker DPG and Tracking POG Tracking POG announced
More informationExperiences from First Top-Off Injection At The Stanford Synchrotron Radiation Lightsource
SLAC-PUB-13825 October 2009 Experiences from First Top-Off Injection At The Stanford Synchrotron Radiation Lightsource J.M. Bauer *, J.C. Liu, A.A. Prinz, and S.H. Rokni Radiation Protection Department,
More informationLSO/LYSO Crystals for Calorimeters in Future HEP Experiments
IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 61, NO. 1, FEBRUARY 2014 483 LSO/LYSO Crystals for Calorimeters in Future HEP Experiments Liyuan Zhang, Member, IEEE, Rihua Mao, Member, IEEE, Fang Yang, Member,
More informationAdvanced Reservoir Monitoring
Advanced Reservoir Monitoring Water Oil Overview Following topics will be addressed in this course: Saturations of Water (Sw), oil (So) and gas (Sg) are likely to change with time. This is caused by fluid
More informationLSO/LYSO Crystals for Calorimeters in Future HEP Experiments
IEEE TRANSACTIONS ON NUCLEAR SCIENCE 1 LSO/LYSO Crystals for Calorimeters in Future HEP Experiments Liyuan Zhang, Member, IEEE, Rihua Mao, Member, IEEE, Fang Yang, Member, IEEE, and Ren-Yuan Zhu, SeniorMember,IEEE
More informationWhat is a positron moderator?
What is a positron moderator? The advent of slow positron beams has resulted in nondestructive depth profiling of defects in surfaces and interfaces, low energy positron diffraction and positron remission
More informationNONDESTRUCTIVE QUANTIFICATION OF INDUCED SURFACE TREATMENT AND RELAXATION EFFECTS IN METALS
NONDESTRUCTIVE QUANTIFICATION OF INDUCED SURFACE TREATMENT AND RELAXATION EFFECTS IN METALS D. Akers and C. Rideout Positron Systems, Inc., Boise, Idaho, USA Abstract: Photon Induced Positron Annihilation
More informationIvan Bazarov Physics Department, Cornell University. Fundamental processes in III-V photocathodes; application for high-brightness photoinjectors
Ivan Bazarov Physics Department, Cornell University Fundamental processes in III-V photocathodes; application for high-brightness photoinjectors 07/21/09 I.V. Bazarov, III-V Photocathodes, ERL09 2 Contents
More informationMeasurements of conversion coefficients using a Si(Li) detector. V. Horvat, J.C. Hardy, N. Nica, and V.E. Iacob
Measurements of conversion coefficients using a Si(Li) detector V. Horvat, J.C. Hardy, N. Nica, and V.E. Iacob As part of our program to make precise measurements of internal conversion coefficients (ICCs)
More informationAIMING at the best jet-mass resolution, inorganic crystal
IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 61, NO. 1, FEBRUARY 2014 489 Doped Lead Fluoride Chloride Crystals for the HHCAL Detector Concept Fan Yang, Member, IEEE, Guoqing Zhang, Guohao Ren, Rihua Mao,Member,IEEE,
More informationPart 3 Oral Exam Content Guide
Initial Certification in Medical Physics Part 3 Oral Exam Content Guide The oral examination is designed to test your knowledge and fitness to practice applied medical physics in the specified specialty(ies).
More informationMössbauer Spectroscopy Part 2
Mössbauer Spectroscopy Part 2 D.H. Ryan Centre for the Physics of Materials and Physics Department, McGill University, Montreal, Quebec ISU Physics-590B 25/27 Feb 2019 1 Instant Mössbauer 2 Typical spectrometer
More informationHigh Power Operation of Cryogenic Yb:YAG. K. F. Wall, B. Pati, and P. F. Moulton Photonics West 2007 San Jose, CA January 23, 2007
High Power Operation of Cryogenic Yb:YAG K. F. Wall, B. Pati, and P. F. Moulton Photonics West 2007 San Jose, CA January 23, 2007 Outline Early work on cryogenic lasers MPS laser technology Recent program
More informationPerformance of the Micro Photon Devices PDM 50CT SPAD detector with PicoQuant TCSPC systems
Technical Note Performance of the Micro Photon Devices PDM 5CT SPAD detector with PicoQuant TCSPC systems Rolf Krahl, Andreas Bülter, Felix Koberling, PicoQuant GmbH These measurements were performed to
More information