CLAS12 FTOF at USC: Time Resolution Measurements

Size: px
Start display at page:

Download "CLAS12 FTOF at USC: Time Resolution Measurements"

Transcription

1 CLAS1 FTOF at USC: Time Resolution Measurements Evan Phelps University of South Carolina Department of Physics and Astronomy November 4, 009 1

2 TOF1 Project at USC

3 TDC Differential Nonlinearity Random Start + Periodic Stop Uniform Distribution + DNL Fluctuations + Statistical Fluctuations 3

4 TDC Calibration and Resolution * 5ns cable delays 0.7 bins 5 t= ps 17.5 ps bin ns TDC Value.8 ns bin 4

5 ADC Calibration V79N testing: Single channel example sensitivity Adjustable pedestal range is insufficient to push system charge offset above the threshold. 5

6 Time Resolution Measurement Methods Coordinate method Reference counter methods One reference Two reference Three-bar cosmic ray method Independent position measurements High statistics. Requires multiple runs per counter. Energy deposit signature does not match CLAS experimental conditions. Independent position measurements. Energy deposit signature matches CLAS experimental conditions. Very to extremely low statistics. Requires multiple runs per counter. Energy deposit signature matches CLAS experimental conditions. High statistics. Requires only one data run for full bar. Does not incorporate independent position measurements. 6

7 Three-bar Method Concept B A t t t b t 1 t t 5 t 6 4tr t 3 t 4 t r t 1 t t 5 t 6 t 4 t 3 T= t m = = 4 4 t tl t tr t t= t ml t mr t m= t bl t br t b= t tl =t 1 t r t tr =t t r t ml =t 3 t r t mr =t 4 t r t bl =t 5 t r t br =t 6 t r t r =t 3 counter = pmt tb = 1= = 5 = 6 m = 3 = = tb m 4 T 1 counter = ref T 7

8 Reference Counter Resolution B A The middle counter is the one being evaluated; the top and bottom are reference counters of known resolution. 1 counter = ref T When all three counters are identical... counter = T 3 8

9 Three-bar Method Implementation 9

10 Base Resolution TDC resolution, between 30ps and 35ps, contributes to the resolution measurements. tdc=30.5 ps Total electronics resolution is measured, but does not contribute to the resolution measurements. electronics =57. ps 10

11 Three-bar System ADC Offset in-situ offset measurements σ = bins μ = bins 11

12 Full-width Trajectory Cuts via ADC Minimums Position Cuts via TDC Difference Position-specific Event Selection 1

13 Position-specific Timewalk Correction After cuts, tcorrected is distributed about a fixed value i 3 t corrected = TDC i TDC 3 ADC i ADC 3 σ TW parameters λi and λ3 are varied for each of tl, tr, bl, br, and mr to determine values leading to minimum tcorrected spreading. 13

14 Position-specific Timewalk Correction A paraboloid fit is sufficient to obtain the minimum value and corresponding TW parameters. (λ1,λ3) (1.7,1.7) 14

15 Position-dependent Resolution Left edge of scintillator The average position-restricted resolution, <σres>, Is approximately 40ps. Right edge of scintillator Resolution measurements are consistent, within statistical uncertainties, throughout the counter length. ( Scintillator edges are defined by FWHM of TDC Difference before cuts or TWC. ) 15

16 Position-dependent TW Parameters EXAMPLE Correction function for the time (t3) of the middle-left (ML) PMT 3= x x 16

17 Full-bar Resolution Event Selection Minimum ADC Cut only eliminates VERY Low ADC Values FWHM Cut on Reference Bars ADC, Arbitrary PMT 17

18 Full-bar Resolution without Vertical Cuts 86.6ps 4.6ps Timewalk Correction Functions 18

19 Recent Results 009 USC measurement of 13cm x 5cm x 5cm Panel-1A counter 1999 JLab measurement of 13cm x 5cm x 5cm Panel-1A counter 009 USC measurement (average positionspecific resolution) of 10cm x 6cm x 6cm Panel-1B prototype counter 19

Scintillation Detectors

Scintillation Detectors Scintillation Detectors Introduction Components Scintillator Light Guides Photomultiplier Tubes Formalism/Electronics Timing Resolution Elton Smith JLab 2006 Detector/Computer Summer Lecture Series Experiment

More information

Timing and Energy Response of Six Prototype Scintillators

Timing and Energy Response of Six Prototype Scintillators Timing and Energy Response of Six Prototype Scintillators CCM Kyba 1, J Glodo 2, EVD van Loef 2, JS Karp 1, KS Shah 2 1 University of Pennsylvania 2 Radiation Monitoring Devices SCINT 2007 June 7, 2007

More information

Scintillation Detectors

Scintillation Detectors Scintillation Detectors Introduction Components Scintillator Light Guides Photomultiplier Tubes Formalism/Electronics Timing Resolution Elton Smith JLab 2009 Detecto Summer Lecture Series Experiment basics

More information

9/27 JUNE 2003 SUMMER STAGE PARTICLES REVELATION THROUGH CERENKOV AND SCINTILLATION COUNTER AND THE CEBAF EXPERIMENT

9/27 JUNE 2003 SUMMER STAGE PARTICLES REVELATION THROUGH CERENKOV AND SCINTILLATION COUNTER AND THE CEBAF EXPERIMENT 9/27 JUNE 2003 SUMMER STAGE PARTICLES REVELATION THROUGH CERENKOV AND SCINTILLATION COUNTER AND THE CEBAF EXPERIMENT Students: Riccardo Falcione, Elisa Paris Liceo Scientifico Statale Farnesina Tutor:

More information

Neutron pulse height analysis (R405n)

Neutron pulse height analysis (R405n) Neutron pulse height analysis (R405n) Y. Satou April 6, 2011 Abstract A pulse height analysis was made for the neutron counter hodoscope used in R405n. By normalizing the pulse height distributions measured

More information

The Time of Flight Detector for GlueX at Jefferson Lab. Hussein Al Ghoul University of Kansas

The Time of Flight Detector for GlueX at Jefferson Lab. Hussein Al Ghoul University of Kansas The Time of Flight Detector for GlueX at Jefferson Lab Hussein Al Ghoul University of Kansas Overview The GlueX Experiment The Time of Flight Detector Pre-Construction Testing TOF Construction at Florida

More information

arxiv: v1 [physics.ins-det] 22 Dec 2013

arxiv: v1 [physics.ins-det] 22 Dec 2013 arxiv:1312.6334v1 [physics.ins-det] 22 Dec 213 Test of the prototype of electron detector for LHAASO project using cosmic rays * WANG Xu 1 XU Tongye 1 DU Yanyan 1 SHAO Ruobin 1 ZHU Chengguang 1;1) for

More information

A Measurement of Monoenergetic Neutrons from 9 Be(p,n) 9 B

A Measurement of Monoenergetic Neutrons from 9 Be(p,n) 9 B Journal of the Korean Physical Society, Vol. 32, No. 4, April 1998, pp. 462 467 A Measurement of Monoenergetic Neutrons from 9 Be(p,n) 9 B J. H. Kim, H. Bhang, J. H. Ha, J. C. Kim, M. J. Kim, Y. D. Kim

More information

Rice University Physics 332 LIFETIME OF THE MUON I. INTRODUCTION...2! II. MEASUREMENT PROCEDURES...3! III. ANALYSIS PROCEDURES...7!

Rice University Physics 332 LIFETIME OF THE MUON I. INTRODUCTION...2! II. MEASUREMENT PROCEDURES...3! III. ANALYSIS PROCEDURES...7! Rice University Physics 332 LIFETIME OF THE MUON I. INTRODUCTION...2! II. MEAUREMENT PROCEDURE...3! III. ANALYI PROCEDURE...7! Revised July 2011 I. Introduction In this experiment you will measure the

More information

Lucite Hodoscope for SANE

Lucite Hodoscope for SANE Lucite Hodoscope for SANE A. Ahmidouch, S. Danagoulian NC A&T State University Outline Cosmic Ray test of a lucite prototype bar The old result from Monte Carlo Geometry consideration Trigger Electronics

More information

Development of a fast plastic scintillation detector with time resolution of less than 10 ps

Development of a fast plastic scintillation detector with time resolution of less than 10 ps Development of a fast plastic scintillation detector with time resolution of less than 10 ps J.W. Zhao a, B.H. Sun a,b, * 1, I. Tanihata a,b, *, S. Terashima a,b, L.H. Zhu a,b, A. Enomoto c, D. Nagae d,

More information

Hands on Project: Large Photocathode PMT Characterization

Hands on Project: Large Photocathode PMT Characterization Hands on Project: Large Photocathode PMT Characterization Rickard Stroem Dept. of Physics and Astronomy, Uppsala University E-mail: rickard.strom@physics.uu.se Institute of Cosmic Ray Research, University

More information

7th International Conference on New Developments In Photodetection

7th International Conference on New Developments In Photodetection 7th International Conference on New Developments In Photodetection Development of a cylindrical tracking detector with multichannel scintillation fibers and PPD readout Yuya Akazawa Tohoku University for

More information

LXe (part B) Giovanni Signorelli. Istituto Nazionale di Fisica Nucleare, Dipartimento di Fisica and Scuola Normale Superiore, Pisa (Italy)

LXe (part B) Giovanni Signorelli. Istituto Nazionale di Fisica Nucleare, Dipartimento di Fisica and Scuola Normale Superiore, Pisa (Italy) LXe (part B) Giovanni Signorelli Istituto Nazionale di Fisica Nucleare, Dipartimento di Fisica and Scuola Normale Superiore, Pisa (Italy) PSI, February 2003 1 MEG internal meeting 2 MC: Outline shape-qe

More information

PARTICLES REVELATION THROUGH SCINTILLATION COUNTER

PARTICLES REVELATION THROUGH SCINTILLATION COUNTER 14-25 JUNE 2004 SUMMER STAGE PARTICLES REVELATION THROUGH SCINTILLATION COUNTER by Flavio Cavalli and Marcello De Vitis Liceo Scientifico Statale Farnesina Tutor: Marco Mirazita 1) COSMIC RAYS - The Muons

More information

Particle Identification at a super B Factory. FRASCATI WORKSHOP DISCUSSION ON PID

Particle Identification at a super B Factory. FRASCATI WORKSHOP DISCUSSION ON PID Particle Identification at a super B Factory. FRASCATI WORKSHOP DISCUSSION ON PID Do no harm! ( The Hippocratic oath of detector designers, especially for those outside you ). Keep a minimum thickness

More information

7. Particle identification

7. Particle identification 7. Particle identification in general, momentum of a particle measured in a spectrometer and another observable is used to identity the species velocity time-of-flight Cherenkov threshold transition radiation

More information

RESPONSE FUNCTION STUDY FOR ENERGY TO LIGHT CONVERSION IN ORGANIC LIQUID SCINTILLATORS

RESPONSE FUNCTION STUDY FOR ENERGY TO LIGHT CONVERSION IN ORGANIC LIQUID SCINTILLATORS RESPONSE FUNCTION STUDY FOR ENERGY TO LIGHT CONVERSION IN ORGANIC LIQUID SCINTILLATORS S. Prasad *, A. Enqvist, S. D. Clarke, S. A. Pozzi, E. W. Larsen 1 Department of Nuclear Engineering and Radiological

More information

A method to measure transit time spread of photomultiplier tubes with Cherenkov light

A method to measure transit time spread of photomultiplier tubes with Cherenkov light Nuclear Science and Techniques 20 (2009) 344 348 A method to measure transit time spread of photomultiplier tubes with Cherenkov light WU Chong 1 DONG Huasong 2,* SUN Zhijia 3 1 Department of Mathematics

More information

arxiv: v1 [physics.ins-det] 29 Jun 2011

arxiv: v1 [physics.ins-det] 29 Jun 2011 Performance simulation of a MRPC-based PET Imaging System arxiv:1106.5877v1 [physics.ins-det] 29 Jun 2011 A. Banerjee, S. Chattopadhyay April 16, 2018 Abstract The low cost and high resolution gas-based

More information

STUDY ON THE ENERGY RESPONSE OF PLASTIC SCINTILLATION DETECTOR TO MEV NEUTRONS ABSTRACT

STUDY ON THE ENERGY RESPONSE OF PLASTIC SCINTILLATION DETECTOR TO MEV NEUTRONS ABSTRACT STUDY ON THE ENERGY RESPONSE OF PLASTIC SCINTILLATION DETECTOR TO 0.75-14.75 MEV NEUTRONS Jianfu Zhang 1, 2, Xiaoping Ouyang 1, 2, Suizheng Qiu 1, Xichao Ruan 3, Jinlu Ruan 2 1 School of Nuclear Science

More information

Calorimetry in particle physics experiments

Calorimetry in particle physics experiments Calorimetry in particle physics experiments Unit N. 9 The NA48 ECAL example (LKR) Roberta Arcidiacono R. Arcidiacono Calorimetry 1 Lecture overview The requirements Detector layout & construction Readout

More information

G13 Update. CLAS collaboration meeting

G13 Update. CLAS collaboration meeting G13 Update CLAS collaboration meeting Newport News VA June 12 2009 Danny Martinez G13 The experiment ran between October 2006 and June 2007 Liquid Deuterium target g13a: Circularly polarized photons g13b:

More information

Development of a Time Projection Chamber with GEM technology in IMP. Herun yang Gas detector group

Development of a Time Projection Chamber with GEM technology in IMP. Herun yang Gas detector group Development of a Time Projection Chamber with GEM technology in IMP Herun yang Gas detector group Outline Introduction TPC prototype based on GEM performance test based cosmic ray Beam test Summary Gas

More information

Prospects for achieving < 100 ps FWHM coincidence resolving time in time-of-flight PET

Prospects for achieving < 100 ps FWHM coincidence resolving time in time-of-flight PET Prospects for achieving < 100 ps FWHM coincidence resolving time in time-of-flight PET, 28-Feb-2012, ICTR-PHE, Geneva, Switzerland 1 Time-of-flight PET Colon cancer, left upper quadrant peritoneal node

More information

Time of Flight measurements with MCP-PMT

Time of Flight measurements with MCP-PMT International Symposium on the Development of Detectors, 2006/4 at SLAC Time of Flight measurements with MCP-PMT - Very high resolution TOF counter - Lifetime of MCP-PMTs T.Ohshima, K.Inami, N.Kishimoto,

More information

Commissioning of the ATLAS LAr Calorimeter

Commissioning of the ATLAS LAr Calorimeter Commissioning of the ATLAS LAr Calorimeter S. Laplace (CNRS/LAPP) on behalf of the ATLAS Liquid Argon Calorimeter Group Outline: ATLAS in-situ commissioning steps Introduction to the ATLAS LAr Calorimeter

More information

1 Introduction. KOPIO charged-particle vetos. K - RARE Meeting (Frascati) May Purpose of CPV: veto Kl

1 Introduction. KOPIO charged-particle vetos. K - RARE Meeting (Frascati) May Purpose of CPV: veto Kl Introduction - Purpose of CPV: veto Kl decay modes with a real or apparent π and a pair of charged particles - Examples of background modes: (i) K l π π + π (ii) K l π π ± eν there are always (iii) K l

More information

The AMS-02 Anticoincidence Counter

The AMS-02 Anticoincidence Counter The AMS-02 Anticoincidence Counter, W. Karpinski, Th. Kirn, K. Lübelsmeyer, St. Schael, M. Wlochal on behalf of the AMS-02 Collaboration philip.doetinchem@rwth-aachen.de I. Phys. Inst. B, RWTH Aachen University

More information

TRB Developments. Michael Traxler for the TRB Collaboration. TRB Platform. Experiences and Limits. Next Step: DiRICH. Summary

TRB Developments. Michael Traxler for the TRB Collaboration. TRB Platform. Experiences and Limits. Next Step: DiRICH. Summary 2015-11-13 Outline 1 2 3 4 : Features I Versatile and meanwhile technically mature platform for TDC measurements and digital readout consists of FPGA-firmware, DAQ- and calibration-software and hardware

More information

Cherenkov Detector Simulation

Cherenkov Detector Simulation Outline E.Chudakov JLab Cherenkov Detector 1 Cherenkov Detector Simulation E.Chudakov 1 1 JLab For GLUEX Collaboration Meeting, March 2007 http://www.jlab.org/~gen/gluex/gas_cher_geom.html Outline E.Chudakov

More information

arxiv: v1 [physics.ins-det] 3 Feb 2011

arxiv: v1 [physics.ins-det] 3 Feb 2011 Nuclear Instruments and Methods in Physics Research A 00 (2018) 1 5 Alogo.pdf Nuclear Instruments and Methods in Physics Research A Scintillation decay time and pulse shape discrimination in oxygenated

More information

David Gascón. Daniel Peralta. Universitat de Barcelona, ECM department. E Diagonal 647 (Barcelona) IFAE, Universitat Aut onoma de Barcelona

David Gascón. Daniel Peralta. Universitat de Barcelona, ECM department. E Diagonal 647 (Barcelona) IFAE, Universitat Aut onoma de Barcelona LHCb 2000-32, CALO 9 June 2000 Results of a tagged photon test beam for the Scintillator Pad Detector. Llu s Garrido David Gascón Ramon Miquel Daniel Peralta Universitat de Barcelona, ECM department E-08028

More information

PoS(PD07)020. Timing Properties of MCP-PMT. Kenji Inami. Nagoya university, Nagoya, Japan

PoS(PD07)020. Timing Properties of MCP-PMT. Kenji Inami. Nagoya university, Nagoya, Japan Nagoya university, Nagoya, Japan E-mail: kenji@hepl.phys.nagoya-u.ac.jp We have studied timing properties of 4 different types of micro-channel-plate photo-multiplier tubes (MCP-PMT) by irradiating with

More information

Measuring the Muon Lifetime

Measuring the Muon Lifetime WJP, PHY38 (200) Wabash Journal of Physics v4.0, p. Measuring the Muon Lifetime L.W. Lupinski, R. Paudel, and M.J. Madsen Department of Physics, Wabash College, Crawfordsville, IN 47933 (Dated: March,

More information

Time-of-Flight PET using Cherenkov Photons Produced in PbF 2

Time-of-Flight PET using Cherenkov Photons Produced in PbF 2 Photons Produced in PbF 2 R. Dolenec a, S. Korpar b,a, P. Križan c,a, R. Pestotnik a, A. Stanovnik d,a a, Ljubljana, Slovenia b Faculty of Chemistry and Chemical Engineering, University of Maribor, Slovenia

More information

Preliminary in-flight performance and calibration status of POLAR

Preliminary in-flight performance and calibration status of POLAR Preliminary in-flight performance and calibration status of POLAR Jianchao SUN Institute of High Energy Physics, CAS On behalf of the POLAR collaboration IACHEC, 2018 2018.4.9-4.12 Terni, Italy Outline

More information

Updated results of the OPERA neutrino-velocity analysis

Updated results of the OPERA neutrino-velocity analysis Updated results of the OPERA neutrino-velocity analysis Maximiliano Sioli (Bologna University and INFN) on behalf of the OPERA Collaboration LNGS Workshop, March 28 th 2012 A brief storyline September

More information

The Generalized Centroid Difference Method

The Generalized Centroid Difference Method 15th International Symposium on Capture Gamma ray Spectroscopy and Related Topics (CGS15) 26.08.2014, Technische Universität Dresden The Generalized Centroid Difference Method for lifetime measurements

More information

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS CR -2009/0 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-11 GENEVA 23, Switzerland May 2009 Calibration of the Barrel Muon

More information

arxiv: v1 [astro-ph.im] 25 Apr 2014

arxiv: v1 [astro-ph.im] 25 Apr 2014 CPC(HEP & NP), 9, 33(X): 5 Chinese Physics C Vol. 33, No. X, Xxx, 9 A linear calibration method on DNL error for energy spectrum * arxiv:44.633v [astro-ph.im] 5 Apr 4 LU Bo() ;) FU Yan-Hong(), CHEN Yong()

More information

A RICH Photon Detector Module with G-APDs

A RICH Photon Detector Module with G-APDs A RICH Photon Detector Module with G-APDs S. Korpar a,b, H. Chagani b, R. Dolenec b, P. Križan b,c, R. Pestotnik b, A. Stanovnik b,c a University of Maribor, b J. Stefan Institute, c University of Ljubljana

More information

Timing calibration of the LHAASO-KM2A electromagnetic particle detectors

Timing calibration of the LHAASO-KM2A electromagnetic particle detectors Timing calibration of the LHAASO-KMA electromagnetic particle detectors Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 149, China E-mail: lvhk@ihep.ac.cn Huihai He Institute of

More information

Beam Test Result for a Prototype PbWO 4 Calorimeter. by Matthew Reece

Beam Test Result for a Prototype PbWO 4 Calorimeter. by Matthew Reece Beam Test Result for a Prototype PbWO 4 Calorimeter by Matthew Reece PrimEx experiment The goal of the PrimEx collaboration is to determine the lifetime of the π 0 particle with greater accuracy than ever

More information

Timing resolution measurement of a 3 Lanthanum Bromide detector

Timing resolution measurement of a 3 Lanthanum Bromide detector Timing resolution measurement of a 3 Lanthanum Bromide detector L. Galli, M. De Gerone, S. Dussoni, D. Nicolò, A.Papa, F. Tenchini, G. Signorelli INFN Pisa, INFN Genova, PSI Villigen 1 th Pisa Meeting

More information

CMS ECAL status and performance with the first LHC collisions

CMS ECAL status and performance with the first LHC collisions CMS ECAL status and performance with the first LHC collisions XIV International Conference on Calorimetry in High Energy Physics (Calor 2010) Konstantinos Theofilatos (ETH Zurich) on behalf of CMS ECAL

More information

KamLAND. Introduction Data Analysis First Results Implications Future

KamLAND. Introduction Data Analysis First Results Implications Future KamLAND Introduction Data Analysis First Results Implications Future Bruce Berger 1 Tohoku University, Sendai, Japan University of Alabama University of California at Berkeley/LBNL California Institute

More information

Dual Isotope Imaging with LaBr3:Ce Crystal and H8500 PSPMT

Dual Isotope Imaging with LaBr3:Ce Crystal and H8500 PSPMT Dual Isotope Imaging with LaBr3:Ce Crystal and H8500 PSPMT Dr. Andrea Fabbri, University of Rome Roma Tre I.N.F.N. (National Institue of Nuclear Physics) γ-ray imaging with scintillator and PSPMT γ-ray

More information

The First Large Application of MPPC: T2K Neutrino Beam Monitor INGRID

The First Large Application of MPPC: T2K Neutrino Beam Monitor INGRID The First Large Application of MPPC: T2K Neutrino Beam Monitor INGRID Kyoto University, Japan E-mail: masashi.o@scphys.kyoto-u.ac.jp We report design and performance of T2K neutrino beam monitor INGRID.

More information

Equalisation of the PMT response to charge particles for the Lucid detector of the ATLAS experiment

Equalisation of the PMT response to charge particles for the Lucid detector of the ATLAS experiment Equalisation of the PMT response to charge particles for the Lucid detector of the ATLAS experiment Camilla Vittori Department of Physics, University of Bologna, Italy Summer Student Program 2014 Supervisor

More information

II. 5. Study for NaI(Tl) and Scintillation Fiber with 80 MeV Proton Beam Toward ESPRI Experiment at NIRS-HIMAC, RIKEN-RIBF

II. 5. Study for NaI(Tl) and Scintillation Fiber with 80 MeV Proton Beam Toward ESPRI Experiment at NIRS-HIMAC, RIKEN-RIBF CYRIC Annual Report 2005 II. 5. Study for NaI(Tl) and Scintillation Fiber with 80 MeV Proton Beam Toward ESPRI Experiment at NIRS-HIMAC, RIKEN-RIBF Zenihiro J. 1, Matsuda Y. 2, Sakaguchi H. 3, Takeda H.

More information

Gamma Spectroscopy. References: Objectives:

Gamma Spectroscopy. References: Objectives: Gamma Spectroscopy References: G.F. Knoll, Radiation Detection and Measurement (John Wiley & Sons, New York, 2000) W. R. Leo, Techniques for Nuclear and Particle Physics Experiments: A How-to Approach,

More information

A New Microchannel-Plate Neutron Time-of-Flight Detector

A New Microchannel-Plate Neutron Time-of-Flight Detector A New Microchannel-Plate Neutron Time-of-Flight Detector 1 1 3 14. MCP ntof at.3 m 1. 16. 167. 17. T i ratio 1.6 1.4 1. 1..8.6.4.. T i 1.8-m ntof/ T i MCP ntof Average = 1. rms =.% 1 1 Shot number V. Yu.

More information

GEANT4 Simulations of. the LAXPC Performance. H. M. Antia. Tata Institute of Fundamental Research

GEANT4 Simulations of. the LAXPC Performance. H. M. Antia. Tata Institute of Fundamental Research GEANT4 Simulations of the LAXPC Performance H. M. Antia Tata Institute of Fundamental Research GEANT4 simulations of LAXPC detector were used to estimate Efficiency of background rejection Efficiency and

More information

Nuclear Lifetimes. = (Eq. 1) (Eq. 2)

Nuclear Lifetimes. = (Eq. 1) (Eq. 2) Nuclear Lifetimes Theory The measurement of the lifetimes of excited nuclear states constitutes an important experimental technique in nuclear physics. The lifetime of a nuclear state is related to its

More information

Developing Zero-Suppression Schemes for the Deep Underground Neutrino Experiment. Maggie Beheler-Amass August 4, 2017

Developing Zero-Suppression Schemes for the Deep Underground Neutrino Experiment. Maggie Beheler-Amass August 4, 2017 Developing Zero-Suppression Schemes for the Deep Underground Neutrino Experiment Maggie Beheler-Amass August 4, 2017 1 Outline: Introduction DUNE Rare Event Searches Zero Suppression Methods and Studies

More information

PoS(ICRC2017)168. PSD performance and charge reconstruction with DAMPE

PoS(ICRC2017)168. PSD performance and charge reconstruction with DAMPE PSD performance and charge reconstruction with DAMPE 1 Yongjie Zhang 1,2, Tiekuang Dong 3, Pengxiong Ma 2,3, Yuhong Yu 1, Paolo Bernardini 4,5, for the DAMPE collaboration 1 Institute of Modern Physics,

More information

Cosmic Ray Detector Software

Cosmic Ray Detector Software Cosmic Ray Detector Software Studying cosmic rays has never been easier Matthew Jones Purdue University 2012 QuarkNet Summer Workshop 1 Brief History First cosmic ray detector built at Purdue in about

More information

29th Monitoring Research Review: Ground-Based Nuclear Explosion Monitoring Technologies

29th Monitoring Research Review: Ground-Based Nuclear Explosion Monitoring Technologies CHARACTERIZATION OF PHOSWICH WELL DETECTORS FOR RADIOXENON MONITORING Wolfgang Hennig 1, Hui Tan 1, William K. Warburton 1, Anthony Fallu-Labruyere 1, Konstantin Sabourov 1, Justin I. McIntyre 2, Matthew

More information

LNS. Tagging the EMC effect in d(e, e N) reactions using the BAND and LAD detectors at JLab12. Axel Schmidt MIT. July 5, 2017

LNS. Tagging the EMC effect in d(e, e N) reactions using the BAND and LAD detectors at JLab12. Axel Schmidt MIT. July 5, 2017 Tagging the EMC effect in d(e, e N) reactions using the BAND and LAD detectors at JLab12 Axel Schmidt MIT July 5, 2017 LNS Laboratory for Nuclear Science 1 The EMC effect still puzzles. 1.2 2σ C 12σ d

More information

章飞虹 ZHANG FeiHong INTERNATIONAL SCHOOL OF SUBNUCLEAR PHYSICS Ph.D. student from Institute of High Energy Physics, Beijing

章飞虹 ZHANG FeiHong INTERNATIONAL SCHOOL OF SUBNUCLEAR PHYSICS Ph.D. student from Institute of High Energy Physics, Beijing 章飞虹 ZHANG FeiHong zhangfh@ihep.ac.cn Ph.D. student from Institute of High Energy Physics, Beijing INTERNATIONAL SCHOOL OF SUBNUCLEAR PHYSICS 2012 Erice, 23 June 2 July 2012 1 Before Hunting Introduction

More information

Module of Silicon Photomultipliers as a single photon detector of Cherenkov photons

Module of Silicon Photomultipliers as a single photon detector of Cherenkov photons Module of Silicon Photomultipliers as a single photon detector of Cherenkov photons R. Pestotnik a, H. Chagani a, R. Dolenec a, S. Korpar a,b, P. Križan a,c, A. Stanovnik a,c a J. Stefan Institute, b University

More information

The cosmic-ray energy spectrum above ev measured with the LOFAR Radboud Air Shower Array

The cosmic-ray energy spectrum above ev measured with the LOFAR Radboud Air Shower Array The cosmic-ray energy spectrum above 16 ev measured with the LOFAR Radboud Air Shower Array,1, S. Buitink, A. Corstanje 1, J.E. Enriquez 1, H. Falcke 1,,4, J.R. Hörandel 1,, A. Nelles 1,5, J.P. Rachen

More information

Single Channel Beta-Gamma Coincidence Detection of Radioactive Xenon Using Digital Pulse Shape Analysis of Phoswich Detector Signals

Single Channel Beta-Gamma Coincidence Detection of Radioactive Xenon Using Digital Pulse Shape Analysis of Phoswich Detector Signals Single Channel Beta-Gamma Coincidence Detection of Radioactive Xenon Using Digital Pulse Shape Analysis of Phoswich Detector Signals Wolfgang Hennig, Hui Tan, William K Warburton, and Justin I McIntyre

More information

Calorimeter test-beam results with APDs

Calorimeter test-beam results with APDs LCWS 05 Calorimeter test-beam results with APDs J.Cvach Institute of Physics AS CR, Prague Test set-up, APD, preamplifiers Calibration Results Future options with APDs Analog HCAL MiniCal test calorimeter

More information

Search for Antiparticles in Cosmic Rays in Space and the Earth s Atmosphere. Philip von Doetinchem I. Phys. Inst. B, RWTH Aachen University

Search for Antiparticles in Cosmic Rays in Space and the Earth s Atmosphere. Philip von Doetinchem I. Phys. Inst. B, RWTH Aachen University Search for Antiparticles in Cosmic Rays in Space and the Earth s Atmosphere Philip von Doetinchem I. Phys. Inst. B, RWTH Aachen University Hausseminar, Aachen 6th of June 008 Overview cosmic ray physics

More information

Design of a Lanthanum Bromide Detector for TOF PET

Design of a Lanthanum Bromide Detector for TOF PET Design of a Lanthanum Bromide Detector for TOF PET A. Kuhn, S. Surti, Member, IEEE, J. S. Karp, Senior Member, IEEE, P. S. Raby, K. S. Shah, A. E. Perkins, Member, IEEE, G. Muehllehner, Fellow Member,

More information

AIRFLY: Measurement of the Air Fluorescence induced by electrons

AIRFLY: Measurement of the Air Fluorescence induced by electrons AIRFLY: Measurement of the Air Fluorescence induced by electrons Valerio Verzi INFN Sezione di Roma II For the Airfly collaboration 9 th Topical Seminar on Innovative Particle and Radiation Detectors 23-26

More information

PoS(ICRC2017)326. The influence of weather effects on the reconstruction of extensive air showers at the Pierre Auger Observatory

PoS(ICRC2017)326. The influence of weather effects on the reconstruction of extensive air showers at the Pierre Auger Observatory The influence of weather effects on the reconstruction of extensive air showers at the Pierre Auger Observatory a for the Pierre Auger Collaboration b a Penn State Physics Department, State College, USA

More information

Mass of the electron m 0

Mass of the electron m 0 Mass of the electron m 0 1 Objective To determine the rest mass of the electron, m e, via γ-ray interactions (mainly Compton scattering and photoeffect) in a NaI scintillation detector. Based on the enclosed

More information

The AMIGA detector of the Pierre Auger Observatory: an overview

The AMIGA detector of the Pierre Auger Observatory: an overview The AMIGA detector of the Pierre Auger Observatory: an overview Federico Sánchez 1 for the Pierre Auger Collaboration 2 1 Instituto de Tecnologías en Detección y Astropartículas (CNEA-CONICET-UNSAM), Buenos

More information

Response curve measurement of the SiPM

Response curve measurement of the SiPM Response curve measurement of the SiPM The theoritical formula : N Fired = N pix. (1 (1 1/N pix ) Npe ) does not hold because: 1) crosstalk and afterpulses increases N Fired (by a factor 1 / (1 ε) for

More information

Scintillation Detector

Scintillation Detector Scintillation Detector Introduction The detection of ionizing radiation by the scintillation light produced in certain materials is one of the oldest techniques on record. In Geiger and Marsden s famous

More information

Simulation Results for CLAS12 From gemc

Simulation Results for CLAS12 From gemc CLAS12 Software Workshop - May 25, 20 p. 1/2 Simulation Results for CLAS12 From gemc G.P.Gilfoyle, M.Ungaro et al. CLAS12 Software Group Outline: 1. gemc Overview 2. Neutron efficiency in first TOF panel.

More information

Radiation (Particle) Detection and Measurement

Radiation (Particle) Detection and Measurement Radiation (Particle) Detection and Measurement Radiation detection implies that the radiation interacts (e.g. leaves at least part of its energy) in the material. A specific material is chosen, because

More information

University of California, Los Angeles, CA 90095, USA

University of California, Los Angeles, CA 90095, USA GAPS Dark matter search using low-energy antimatter Rene A. Ong, for the GAPS Collaboration University of California, Los Angeles, CA 90095, USA Cosmic Ray Anomalies There are a variety of puzzles in cosmic

More information

arxiv: v1 [physics.ins-det] 1 Sep 2009

arxiv: v1 [physics.ins-det] 1 Sep 2009 The MEG Spectrometer at PSI Paolo Walter Cattaneo on behalf of the MEG collaboration INFN Pavia, Via Bassi 6, Pavia, I-27100, Italy arxiv:0909.0199v1 [physics.ins-det] 1 Sep 2009 The MEG experiment is

More information

Experimental Verification of a Timing Measurement Circuit With Self-Calibration

Experimental Verification of a Timing Measurement Circuit With Self-Calibration 19 th IEEE IMS3TW, Porto Alegre, Brazil Sept. 17, 2014 Experimental Verification of a Timing Measurement Circuit With Self-Calibration Kateshi Chujyo, Daiki Hirabayashi, Kentaroh Katoh Conbing Li, Yutaroh

More information

HIGH RESOLUTIO TIME-I TERVAL MEASUREME T SYSTEMS APPLIED TO FLOW MEASUREME T. Sławomir Grzelak, Marcin Kowalski, Jarosław Czoków and Marek Zieliński

HIGH RESOLUTIO TIME-I TERVAL MEASUREME T SYSTEMS APPLIED TO FLOW MEASUREME T. Sławomir Grzelak, Marcin Kowalski, Jarosław Czoków and Marek Zieliński Metrol. Meas. Syst., Vol. XXI (2014), No. 1, pp. 77 84. METROLOGY A D MEASUREME T SYSTEMS Index 330930, ISS 0860-8229 www.metrology.pg.gda.pl HIGH RESOLUTIO TIME-I TERVAL MEASUREME T SYSTEMS APPLIED TO

More information

Análisis de datos en KASCADE-Grande

Análisis de datos en KASCADE-Grande Análisis de datos en KASCADE-Grande Juan Carlos Arteaga-Velázquez for the KASCADE-Grande Collaboration Instituto de Física y Matemáticas Universidad Michoacana arteaga@ifm.umich.mx Morelia,Mich. Junio

More information

THE AMS RICH COUNTER

THE AMS RICH COUNTER THE AMS RICH COUNTER G. BOUDOUL ISN Grenoble ISN-GRENOBLE 1 The AMS RICH collaboration: Bologna, Grenoble, Lisbon, Madrid, Maryland, Mexico 2 The AMS collaboration UNAM S.C.C. TING (MIT), PI 3 AMS Scientific

More information

Development of Ring-Imaging Cherenkov Counter for Heavy Ions

Development of Ring-Imaging Cherenkov Counter for Heavy Ions Development of Ring-Imaging Cherenkov Counter for Heavy Ions Masahiro Machida Tokyo University of Science New Facilities and Instrumentation INPC 2016 Collaborators 2 Tokyo University of Science M. Machida,

More information

Timing Characterization of Helium-4 Fast Neutron Detector with EJ-309 Organic Liquid Scintillator

Timing Characterization of Helium-4 Fast Neutron Detector with EJ-309 Organic Liquid Scintillator Timing Characterization of Helium-4 Fast Neutron Detector with EJ-309 Organic Liquid Scintillator Yinong Liang 1, Ting Zhu, Andreas Enqvist Abstract Recently, the Helium-4 gas fast neutron scintillation

More information

Probability & Statistics: Introduction. Robert Leishman Mark Colton ME 363 Spring 2011

Probability & Statistics: Introduction. Robert Leishman Mark Colton ME 363 Spring 2011 Probability & Statistics: Introduction Robert Leishman Mark Colton ME 363 Spring 2011 Why do we care? Why do we care about probability and statistics in an instrumentation class? Example Measure the strength

More information

Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory

Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory Title Labr3:Ce scintillators for gamma ray spectroscopy Permalink https://escholarship.org/uc/item/38f0c7zv Authors Shah, K.S.

More information

PoS(ICRC2015)641. Cloud Monitoring using Nitrogen Laser for LHAASO Experiment. Z.D. Sun 1,Y. Zhang 2,F.R. Zhu 1 for the LHAASO Collaboration

PoS(ICRC2015)641. Cloud Monitoring using Nitrogen Laser for LHAASO Experiment. Z.D. Sun 1,Y. Zhang 2,F.R. Zhu 1 for the LHAASO Collaboration Cloud Monitoring using Nitrogen Laser for LHAASO Experiment Z.D. Sun 1,Y. Zhang 2,F.R. Zhu 1 for the LHAASO Collaboration [1]School of Physical Science and Technology, Southwest Jiaotong University, Chengdu

More information

Precision neutron flux measurement with a neutron beam monitor

Precision neutron flux measurement with a neutron beam monitor Journal of Physics: Conference Series OPEN ACCESS Precision neutron flux measurement with a neutron beam monitor To cite this article: T Ino et al 2014 J. Phys.: Conf. Ser. 528 012039 View the article

More information

Super Bigbite Spectrometer (SBS) Status

Super Bigbite Spectrometer (SBS) Status Super Bigbite Spectrometer (SBS) Status Mark Jones SBS Program manager 1/18/2017 Hall A Jan 2017 Meeting 1 Outline Status of SBS project Overview of experiments Status of SBS equipment SBS equipment covered

More information

Thin Calorimetry for Cosmic-Ray Studies Outside the Earth s Atmosphere. 1 Introduction

Thin Calorimetry for Cosmic-Ray Studies Outside the Earth s Atmosphere. 1 Introduction Thin Calorimetry for Cosmic-Ray Studies Outside the Earth s Atmosphere Richard WIGMANS Department of Physics, Texas Tech University, Lubbock TX 79409-1051, USA (wigmans@ttu.edu) Abstract Cosmic ray experiments

More information

Dark Matter Particle Explorer: The First Chinese Cosmic Ray and Hard γ-ray Detector in Space

Dark Matter Particle Explorer: The First Chinese Cosmic Ray and Hard γ-ray Detector in Space SPACE SCIENCE ACTIVITIES IN CHINA Dark Matter Particle Explorer: The First Chinese Cosmic Ray and Hard γ-ray Detector in Space AUTHORS CHANG Jin Key Laboratory of Dark Matter and Space Astronomy, Purple

More information

Measuring the Speed of Light on a Nanosecond Time Scale

Measuring the Speed of Light on a Nanosecond Time Scale WJP, PHY381 (2009) Wabash Journal of Physics v4.0, p.1 Measuring the Speed of Light on a Nanosecond Time Scale Bradley C. Vest, Thomas Warn, and M.J. Madsen Department of Physics, Wabash College, Crawfordsville,

More information

Calibration of the Modular Neutron Array (MoNA)

Calibration of the Modular Neutron Array (MoNA) Calibration of the Modular Neutron Array (MoNA) Robert Pepin Gonzaga University ~1~ Calibration of the Modular Neutron Array (MoNA): Figure 1 - A rendering of the Modular Neutron Array In recent years

More information

Progress Report on the WLRS: Getting ready for GGOS, LLR and Time Transfer

Progress Report on the WLRS: Getting ready for GGOS, LLR and Time Transfer 13-0219 Progress Report on the WLRS: Getting ready for GGOS, LLR and Time Transfer G. Herold (1), J. Eckl (1), M. Mühlbauer (1), A. Leidig (1), J. Kodet (2), U. Schreiber (2) (1) Geodetic Observatory Wettzell,

More information

Response function measurements of an NE102A organic scintillator using an 241 Am-Be source

Response function measurements of an NE102A organic scintillator using an 241 Am-Be source Nuclear Instruments and Methods m Physics Research A 345 (1994) 514-519 North-Holland NCLEAR INSTRMENTS & METHODS IN PHYSICS RESEARCH Section A Response function measurements of an NE12A organic scintillator

More information

DIGITAL PULSE SHAPE ANALYSIS WITH PHOSWICH DETECTORS TO SIMPLIFY COINCIDENCE MEASUREMENTS OF RADIOACTIVE XENON

DIGITAL PULSE SHAPE ANALYSIS WITH PHOSWICH DETECTORS TO SIMPLIFY COINCIDENCE MEASUREMENTS OF RADIOACTIVE XENON DIGITAL PULSE SHAPE ANALYSIS WITH PHOSWICH DETECTORS TO SIMPLIFY COINCIDENCE MEASUREMENTS OF RADIOACTIVE XENON W. Hennig 1, H. Tan 1, W.K. Warburton 1, and J.I. McIntyre 2 XIA LLC 1, Pacific Northwest

More information

The Versatile Array of Neutron Detectors at Low Energy

The Versatile Array of Neutron Detectors at Low Energy The Versatile Array of Neutron Detectors at Low Energy S. V. Paulauskas, R. Grzywacz, M. Madurga, D. Miller, S. Padgett, W. A. Peters, and the VANDLE Collaboration Why use the time-of-flight technique?

More information

Performance of the MCP-PMT for the Belle II TOP counter

Performance of the MCP-PMT for the Belle II TOP counter Performance of the MCP-PMT for the Belle II TOP counter a, S. Hirose b, T. Iijima ab, K. Inami b, Y. Kato a, Y. Maeda a, R. Mizuno b, Y. Sato a and K. Suzuki b a Kobayashi-Maskawa Institute, Nagoya University

More information

Measurement of Muon Lifetime

Measurement of Muon Lifetime Measurement of Muon Lifetime Noah Scandrette Physics and Astronomy Department, San Francisco State University, San Francisco, California (Dated: December 16, 2016) The average lifetime of the muon has

More information

hν' Φ e - Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous?

hν' Φ e - Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous? Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous? 2. Briefly discuss dead time in a detector. What factors are important

More information

The early days of ground-based gamma-ray astronomy in France. Gerard Fontaine - Hillas symposium Heidelberg December

The early days of ground-based gamma-ray astronomy in France. Gerard Fontaine - Hillas symposium Heidelberg December The early days of ground-based gamma-ray astronomy in France Gerard Fontaine - Hillas symposium Heidelberg December 10-12 2018 Timeline from 1986 to 2004 86 87 88 89 90 91 92 93 94 95 96 97 98 99 00 01

More information