Monitoring of stray magnetic fields near the PROSPECT detector

Size: px
Start display at page:

Download "Monitoring of stray magnetic fields near the PROSPECT detector"

Transcription

1 Monitoring of stray magnetic fields near the PROSPECT detector Corey Gilbert On behalf of the PROSPECT Collaboration ORNL is managed by UT-Battelle, LLC for the US Department of Energy Next Talk G : Temperature Dependence studies of the 6Li-doped liquid scintillator used in PROSPECT Brennan T Hackett

2 Motivation PROSPECT is a high precision spectrum antineutrino experiment that requires a well characterized background environment because it is operating at surface level Overburden: ~1m.w.e. Challenge: Neutron scattering experiments conducted in high magnetic environments Backgrounds include: Cosmic Gammas Neutrons Magnetic fields Next Talk G : Temperature Dependence studies of the 6Li-doped liquid scintillator used in PROSPECT }Brennan T Hackett!2

3 High Flux Isotope Reactor (HFIR) Polarized Triple Axis Spectrometer Fixed-Incident- Energy Triple-Axis Spectrometer Inner/ Outer Core 85 MW Thermal Power Research Reactor ~93% enriched 235U fuel Very compact core (h=0.6m d=0.4m) ~42% duty cycle allows good background characterization Neutron Powder Diffractomete HB-1 HB-2 PROSPECT HB-3 HB-4 Cold Neutron Experiment Hall WAND Sample Environment Storage Polarized Neutron Development Neutron Residual Stress Mapping Triple axis spectrometer 4-circle Diffractomete!3

4 Magnets at HFIR Superconducting magnets ranging from 5-11 Tesla are used on various beamlines High field magnets (25-30Tesla) are being considered Mag E 8T Vertical Asymmetric Field Cryomagnet Temp Range: 1.7 to 300 K Used on beamlines : CG-2, CG-4C, HB-1, HB-1A, HB-3!4

5 PMT Configuration in PROSPECT Detector Each of the Li-loaded liquid scintillator filled optical segments holds 2 5 PMTs PMTs are known to be sensitive to magnetic fields. Relative magnetic field values over the range of the device need to be assessed Earth s magnetic field is G at ORNL - Declination: -5º 33 30, Inclination: 64º NOAA Magnetic Field Calculator!5

6 Recent Experimental Efforts to Test/Control Magnetic Environments The STEREO Experiment (Neutrino) - arxiv: v1 (2018) Magnetic shield of PMT used in a DAMPE electromagnetic calorimeter (Dark Matter) - arxiv: v4 (2013) Performances investigation and material selection of PMT magnetic shields for the space experiments with GRIS and PING-M instruments (Space) - R M Faradzhaev et al. J. Phys.675 (2016) First Observation of P-odd γ Asymmetry in Polarized Neutron Capture on Hydrogen (Fundamental Symmetries) - arxiv: v1 (2018) Magnetic field effects on the photocathode uniformity of Hamamatsu R7081 photomultiplier tubes (Industry) - NIMA 697(2013) 46!6

7 Helical Orbit Spectrometer (HeliOS) Studies of short lived isotopes Magnetic field needs to be parallel to beam within 1 mrad Monitoring magnetometers are crucial for this type of experiment!7 Wuosmaa, A. NIMA. 2007

8 PMT Sensitivity to Magnetic Field Backgrounds Low-energy electrons travel along a long path in a vacuum to reach the dynodes. Slight magnetic fields distort that trajectory, causing an anode sensitivity variation Hamamatsu PMT 127mm Hamamatsu, PMT Basics and Applications 2007!8 Boyle J., Master s SESAPS Thesis

9 PMT Module Configuration 240 Hamamatsu R6594 (127 mm ø Q.E. 25%) - 10 stage dynode of box & line configuration 68 ET9372B (130 mm ø Q.E. 28%) - 12 stage dynode of linear focused configuration PROSPECT PMTs are fitted with a Hitachi FINEMET magnetic shield - Amorphous metal composed of Nb, B, Fe, Cu!9

10 Magnetic Field Background Characterization Background B-field was measured using a Lakeshore hall probe (HMMT-6J18-VF) before placement of PROSPECT detector Results showed hotspots approaching 2 Gauss PROSPECT Gauss!10 Boyle J., Master s Thesis 2016

11 Current Magnetometer Technology GMN Earth 1fT 1pT 1nT 1µT 1mT Lenz J., Edelstein A., IEEE Sensors Journal 2006!11

12 Adafruit Triple-Axis Magnetometer Model: LSM303DLHC Selectable range: +/- 1.3 G to +/- 8.1 G Magnetic resolution: 2mG Read through Raspberry Pi I2C 20.3 mm 22.9 mm!12

13 Monitoring of Magnetic Field Rx Core triple axis magnetometers Compact LN2 TOP VIEW DAQ Rack Low cost Online monitoring Alert system 3 1 Remote control 2!13

14 Axes Shift Calibration Out of the box, sensors are not calibrated X and Y magnetic fields plotted as magnetometer is rotated about Z axis before and after axis shift is applied. Programmed in python, takes <1 minute Before After!14

15 Axis Magnitude Calibration Metrolab THM1176-LF hall probe used as known value - Range: 8.0 mt - Resolution: 2µT ± - Accuracy: 20µT or 0.2G Sensor s axes are compared to known and shifted to match!15

16 Magnetic Field Magnitude Around PROSPECT Reactor Core 0.6 Scan using Metrolab hall probe DAQ Rack Gauss Varying magnetic field from 0.15 G to 0.6 G Scanned at sensor height (16cm) Hot spot near DAQ 0.1!16

17 Operation of Sensors since Oct 31 Spike correlated to testing ramp up and down of Mag-E (8 T) on HB-2A!17

18 Magnets Used Since Deployment of PROSPECT Detector MAG-B (5T) MAG-A (5T) MAG-H (5T) MAG-E (8T) MAG-G (11T) MAG-D (11T) HB-1A HB-1 HB-2A HB-2C HB-3 CG-2 CG-4C 3/9/18 4/8/18 5/9/18 6/8/18 7/9/18 8/8/18 9/8/18 10/8/18 11/8/18 Reactor ON Reactor OFF!18

19 Conclusions A compact, low cost magnetic monitoring system has been deployed surrounding the PROSPECT detector at HFIR. Sensors show very good stability and sensitivity to background events Me!19

20 Backup Slides!20

21 Effects of various shielding positions!21 Leo, W.R. Techniques for Nuclear and Particle Physics Experiments. 1994

22 Calibration accuracy Metrolab probe average values plotted with sensor data Sensors values are within 0.2 G of Metrolab probe after calibration Solid lines: Adafruit Sensors Dashed lines: Metrolab probe!22

Measuring the neutrino mass hierarchy with atmospheric neutrinos in IceCube(-Gen2)

Measuring the neutrino mass hierarchy with atmospheric neutrinos in IceCube(-Gen2) Measuring the neutrino mass hierarchy with atmospheric neutrinos in IceCube(-Gen2) Beyond the Standard Model with Neutrinos and Nuclear Physics Solvay Workshop November 30, 2017 Darren R Grant The atmospheric

More information

Search for Sterile Neutrinos with the Borexino Detector

Search for Sterile Neutrinos with the Borexino Detector Search for Sterile Neutrinos with the Borexino Detector PANIC 2014 Hamburg on behalf of the BOREXINO Collaboration Institut für Experimentalphysik (Universität Hamburg) Borexino Detector Site 1400 m of

More information

Neutron facilities and generation. Rob McQueeney, Ames Laboratory and Iowa State University

Neutron facilities and generation. Rob McQueeney, Ames Laboratory and Iowa State University Neutron facilities and generation Rob McQueeney, Ames Laboratory and Iowa State University September 12, 2018 19-Sep-18 Physics 502 2 Neutrons compared to other probes of matter Bulk probe Interacts with

More information

Direct WIMP Detection in Double-Phase Xenon TPCs

Direct WIMP Detection in Double-Phase Xenon TPCs Outline PMTs in the XENON dark matter experiment XENON100 and the weekly gain calibration XENON1T and candidates for the light sensors Tests of Hamamatsu R11410 2 Direct WIMP Detection in Double-Phase

More information

PoS(ICHEP2016)474. SoLid: Search for Oscillations with a Lithium-6 Detector at the SCK CEN BR2 reactor

PoS(ICHEP2016)474. SoLid: Search for Oscillations with a Lithium-6 Detector at the SCK CEN BR2 reactor SoLid: Search for Oscillations with a Lithium-6 Detector at the SCK CEN BR2 reactor University of Bristol E-mail: dan.saunders@bristol.ac.uk The disappearance of reactor antineutrinos into a new neutral

More information

Status of 13 measurement in reactor experiments

Status of 13 measurement in reactor experiments Status of 13 measurement in reactor experiments Kwong Lau University of Houston, Houston, TX 7704, USA The status of 13 measurements from Daya Bay, RENO and Double Chooz experiments is reviewed. 1. INTRODUCTION

More information

An Underground Laboratory for a Multi-Detector Experiment. Karsten Heeger Lawrence Berkeley National Laboratory

An Underground Laboratory for a Multi-Detector Experiment. Karsten Heeger Lawrence Berkeley National Laboratory Measuring sin 2 2θ 13 with Reactor Antineutrinos at Daya Bay An Underground Laboratory for a Multi-Detector Experiment Karsten Heeger Lawrence Berkeley National Laboratory On behalf of the Daya Bay collaboration

More information

Daya Bay and joint reactor neutrino analysis

Daya Bay and joint reactor neutrino analysis Daya Bay and joint reactor neutrino analysis Logan Lebanowski (Tsinghua University) on behalf of the Daya Bay collaboration 2016/11/4 - NNN16, Beijing 1 Contents Daya Bay Reactor Neutrino Experiment Introduction

More information

XMASS: a large single-phase liquid-xenon detector

XMASS: a large single-phase liquid-xenon detector XMASS: a large single-phase liquid-xenon detector Katsuki Hiraide, the university of Tokyo for the XMASS Collaboration October 3 rd, 2016 IPRD16@Siena, Italy 1 XMASS project XMASS: a multi purpose experiment

More information

The Nucifer Experiment: Non-Proliferation with Reactor Antineutrinos

The Nucifer Experiment: Non-Proliferation with Reactor Antineutrinos The Nucifer Experiment: Non-Proliferation with Reactor Antineutrinos Andi S. Cucoanes1 for the Nucifer Collaboration* * V.M.Bui2, M.Cribier1, A.S.Cucoanes1, M.Fallot2, M.Fechner1, J.Gaffiot1, L.Giot2,

More information

Short baseline neutrino oscillation experiments at nuclear reactors

Short baseline neutrino oscillation experiments at nuclear reactors Short baseline neutrino oscillation experiments at nuclear reactors Christian Buck, MPIK Heidelberg Erice School, Sicily Sept, 17th 2017 Neutrino oscillations = 3 2 1 3 2 1 3 2 1 3 2 1 ν ν ν ν ν ν τ τ

More information

Beam Dump Experiments at JLab and SLAC

Beam Dump Experiments at JLab and SLAC Beam Dump Experiments at JLab and SLAC Brief History (E137 at SLAC) BDX at Jefferson Lab Detector and signal Backgrounds Expected Sensitivity Elton S. Smith, Jefferson Lab On behalf of the BDX Collaboration

More information

Neutrino Oscillations

Neutrino Oscillations Neutrino Oscillations Supervisor: Kai Schweda 5/18/2009 Johannes Stiller 1 Outline The Standard (Solar) Model Detecting Neutrinos The Solar Neutrino Problem Neutrino Oscillations Neutrino Interactions

More information

Lecture 16 Light transmission and optical detectors

Lecture 16 Light transmission and optical detectors Lecture 6 Light transmission and optical detectors Charged particle traversing through a material can generate signal in form of light via electromagnetic interactions with orbital electrons of the atoms

More information

Beam Dump Experiments with Photon and Electron Beams

Beam Dump Experiments with Photon and Electron Beams Beam Dump Experiments with Photon and Electron Beams Electron beams BDX at Jefferson Lab Signal and backgrounds Muon flux measurements Status Elton S. Smith, Jefferson Lab On behalf of the BDX Collaboration

More information

PoS(DIS 2010)058. ATLAS Forward Detectors. Andrew Brandt University of Texas, Arlington

PoS(DIS 2010)058. ATLAS Forward Detectors. Andrew Brandt University of Texas, Arlington University of Texas, Arlington E-mail: brandta@uta.edu A brief description of the ATLAS forward detectors is given. XVIII International Workshop on Deep-Inelastic Scattering and Related Subjects April

More information

Background Modeling and Materials Screening for the LUX and LZ Detectors. David Malling Brown University LUX Collaboration AARM Meeting February 2011

Background Modeling and Materials Screening for the LUX and LZ Detectors. David Malling Brown University LUX Collaboration AARM Meeting February 2011 Background Modeling and Materials Screening for the LUX and LZ Detectors David Malling Brown University LUX Collaboration AARM Meeting February 2011 1 Summary LUX screening program limits background contributions

More information

Oak Ridge National Laboratory, TN. K. Scholberg, Duke University On behalf of the COHERENT collaboration August 2, 2017 DPF 2017, Fermilab

Oak Ridge National Laboratory, TN. K. Scholberg, Duke University On behalf of the COHERENT collaboration August 2, 2017 DPF 2017, Fermilab Oak Ridge National Laboratory, TN K. Scholberg, Duke University On behalf of the COHERENT collaboration August 2, 2017 DPF 2017, Fermilab Coherent elastic neutrino-nucleus scattering (CEvNS) n + A n +

More information

Reactor On/Off Monitoring with a Prototype of Plastic Anti-neutrino Detector Array (PANDA)

Reactor On/Off Monitoring with a Prototype of Plastic Anti-neutrino Detector Array (PANDA) Reactor On/Off Monitoring with a Prototype of Plastic Anti-neutrino Detector Array (PANDA) Yasuhiro Kuroda A, Yo Kato A, Nozomu Tomita A, Ryoko Nakata, Shugo Oguri, Chikara Ito B, Yoshizumi Inoue C, Makoto

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

The COHERENT Experiment: Overview and Update of Results

The COHERENT Experiment: Overview and Update of Results The COHERENT Experiment: Overview and Update of Results for the COHERENT Collaboration 2016 Fall Meeting of the APS Division of Nuclear Physics, Vancouver, B.C. ORNL is managed by UT-Battelle for the US

More information

Neutron flux measurement using fast-neutron activation of 12 B and 12 N isotopes in hydrocarbonate scintillators

Neutron flux measurement using fast-neutron activation of 12 B and 12 N isotopes in hydrocarbonate scintillators Neutron flux measurement using fast-neutron activation of 12 B and 12 N isotopes in hydrocarbonate scintillators M. M. Boliev E-mail: kchkrv@rambler.ru Yu. F. Novoseltsev R. V. Novoseltseva V. B. Petkov

More information

Neutrino Physics. Neutron Detector in the Aberdeen Tunnel Underground Laboratory. The Daya Bay Experiment. Significance of θ 13

Neutrino Physics. Neutron Detector in the Aberdeen Tunnel Underground Laboratory. The Daya Bay Experiment. Significance of θ 13 Neutrino Physics Neutron Detector in the Aberdeen Tunnel Underground Laboratory John K.C. Leung Department of Physics, HKU On behalf of CUHK, LBL & IHEP Presented to HKRPS on June 21, 2007 Neutrinos have

More information

Walter C. Pettus University of Wisconsin Madison. Weak Interactions Discussion Group Yale Physics 21 Oct 2013

Walter C. Pettus University of Wisconsin Madison. Weak Interactions Discussion Group Yale Physics 21 Oct 2013 Walter C. Pettus University of Wisconsin Madison Weak Interactions Discussion Group Yale Physics 21 Oct 2013 Dark Matter and DM- ICE Cosmogenic Activation in DM- ICE O(50 1000 kev ee ) Calibration Pulse

More information

Dark Matter Searches with AMS-02. AMS: Alpha Magnetic Spectrometer

Dark Matter Searches with AMS-02. AMS: Alpha Magnetic Spectrometer Dark Matter Searches with AMS-02 AMS: Alpha Magnetic Spectrometer 2007/2008 Wim de Boer on behalf of the AMS collaboration University of Karlsruhe July, 20. 2004 COSPAR, Paris, W. de Boer, Univ. Karlsruhe

More information

Correction for PMT temperature dependence of the LHCf calorimeters

Correction for PMT temperature dependence of the LHCf calorimeters Journal of Physics: Conference Series OPEN ACCESS Correction for PMT temperature dependence of the LHCf calorimeters To cite this article: Eri Matsubayashi and the LHCf collaboration 2015 J. Phys.: Conf.

More information

The Hyper-Kamiodande Project A New Adventure in n Physics

The Hyper-Kamiodande Project A New Adventure in n Physics http://hyperk.org The Hyper-Kamiodande Project A New Adventure in n Physics ICNFP2017 Kolymbari, Crete August 26, 17 Alessandro Bravar on behalf of the HK Proto-Collaboration Hyper-K Physics Overview 2

More information

After LUX: The LZ Program. David Malling, Simon Fiorucci Brown University APS DPF Conference August 10, 2011

After LUX: The LZ Program. David Malling, Simon Fiorucci Brown University APS DPF Conference August 10, 2011 After LUX: The LZ Program David Malling, Simon Fiorucci Brown University APS DPF Conference August 10, 2011 The LZ Program LZ LUX-ZEPLIN LUX (14 U.S. institutions) + new collaborators from ZEPLIN, other

More information

arxiv:hep-ex/ v1 15 Aug 2006

arxiv:hep-ex/ v1 15 Aug 2006 The Double Chooz Experiment 1 Daniel M. Kaplan (for the Double Chooz Collaboration) Illinois Institute of Technology, 3101 South Dearborn Street, Chicago, Illinois, USA arxiv:hep-ex/0608040v1 15 Aug 2006

More information

arxiv: v1 [physics.ins-det] 9 Apr 2018

arxiv: v1 [physics.ins-det] 9 Apr 2018 arxiv:1804.02889v1 [physics.ins-det] 9 Apr 2018 Study of neutron shielding collimators for curved beamlines at the European Spallation Source 1. Introduction V. Santoro 1,2, D. D. DiJulio 1,2, S. Ansell

More information

Chemistry Instrumental Analysis Lecture 19 Chapter 12. Chem 4631

Chemistry Instrumental Analysis Lecture 19 Chapter 12. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 19 Chapter 12 There are three major techniques used for elemental analysis: Optical spectrometry Mass spectrometry X-ray spectrometry X-ray Techniques include:

More information

Neutron Instruments I & II. Ken Andersen ESS Instruments Division

Neutron Instruments I & II. Ken Andersen ESS Instruments Division Neutron Instruments I & II ESS Instruments Division Neutron Instruments I & II Overview of source characteristics Bragg s Law Elastic scattering: diffractometers Continuous sources Pulsed sources Inelastic

More information

Measurement of nuclear recoil responses of NaI(Tl) crystal for dark matter search

Measurement of nuclear recoil responses of NaI(Tl) crystal for dark matter search Measurement of nuclear recoil responses of NaI(Tl) crystal for dark matter search Hanwool Joo on behalf of the KIMS-NaI collaboration Department of Physics and Astronomy, 1 Gwanak-ro, Gwanak-gu, Seoul

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

Directional Measurement of Anti-Neutrinos with KamLAND

Directional Measurement of Anti-Neutrinos with KamLAND Directional Measurement of Anti-Neutrinos with KamLAND Research Center for Neutrino Science, Tohoku University Aoba-ku aramaki aza aoba, Sendai, Miyagi, Japan E-mail: shingo@awa.tohoku.ac.jp I show possibility

More information

Monte Carlo Simulations for Future Geoneutrino Detectors

Monte Carlo Simulations for Future Geoneutrino Detectors Monte Carlo Simulations for Future Geoneutrino Detectors Morgan Askins Abstract The main contribution of heat in the earth s mantle is thought to be the radioactive decays of 238 U, 232 T h, and 40 K.

More information

Appendix A2. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France.

Appendix A2. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France. Appendix A. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France. Prepared by: Arash Akbari-Sharbaf Why Build Accelerators? Probe deeper From

More information

arxiv: v1 [physics.ins-det] 27 Jun 2017

arxiv: v1 [physics.ins-det] 27 Jun 2017 Double Calorimetry System in JUNO Miao He on behalf of the JUNO collaboration arxiv:1706.08761v1 [physics.ins-det] 27 Jun 2017 Institute of High Energy Physics, Beijing hem@ihep.ac.cn Abstract. The Jiangmen

More information

New Search for Mirror Neutrons at HFIR

New Search for Mirror Neutrons at HFIR New Search for Mirror Neutrons at HFIR Leah Broussard Oak Ridge National Laboratory October 24, 2017 Neutron-Antineutron Oscillations: Appearance, Disappearance, and Baryogenesis (October 23-27, 2017)

More information

CANDLES Experiment Current Status and Future Plan. X. Li for the CANDLES Collaboration

CANDLES Experiment Current Status and Future Plan. X. Li for the CANDLES Collaboration CANDLES Experiment Current Status and Future Plan X. Li for the CANDLES Collaboration 1 Neutrinoless Double Beta Decay (0νββ) 2νββ decay 0νββ decay (A, Z) => (A, Z+2) + 2e - process beyond Standard Model

More information

Neutron Calibration System for the MiniCLEAN Experiment. Lu Feng for the MiniCLEAN collaboration APS April Meeting May 2, 2011

Neutron Calibration System for the MiniCLEAN Experiment. Lu Feng for the MiniCLEAN collaboration APS April Meeting May 2, 2011 Neutron Calibration System for the MiniCLEAN Experiment Lu Feng for the MiniCLEAN collaboration APS April Meeting May 2, 2011 The MiniCLEAN Experiment Mini Cryogenic Low Energy Astrophysics with Noble

More information

Recent T2K results on CP violation in the lepton sector

Recent T2K results on CP violation in the lepton sector Recent T2K results on CP violation in the lepton sector presented by Per Jonsson Imperial College London On Behalf of the T2K Collaboration, December 14-20 2016, Fort Lauderdale, USA. Outline Neutrino

More information

Y2 Neutrino Physics (spring term 2017)

Y2 Neutrino Physics (spring term 2017) Y2 Neutrino Physics (spring term 2017) Lecture 5 Discoveries of the leptons Dr E Goudzovski eg@hep.ph.bham.ac.uk http://epweb2.ph.bham.ac.uk/user/goudzovski/y2neutrino Previous lecture In 1940s, nuclear

More information

Background Neutron Studies for Coherent Elastic Neutrino-Nucleus Scattering Measurements at the SNS

Background Neutron Studies for Coherent Elastic Neutrino-Nucleus Scattering Measurements at the SNS Background Neutron Studies for Coherent Elastic Neutrino-Nucleus Scattering Measurements at the SNS D. Markoff (NC Central University, Triangle Universities Nuclear Laboratory) For the COHERENT Collaboration

More information

Detectors for astroparticle physics

Detectors for astroparticle physics Detectors for astroparticle physics Teresa Marrodán Undagoitia marrodan@physik.uzh.ch Universität Zürich Kern und Teilchenphysik II, Zürich 07.05.2010 Teresa Marrodán Undagoitia (UZH) Detectors for astroparticle

More information

New Search for Mirror Neutrons at HFIR

New Search for Mirror Neutrons at HFIR New Search for Mirror Neutrons at HFIR L. J. Broussard Oak Ridge National Laboratory May 17, 2017 2017 International Workshop on Baryon and Lepton Number Violation Search for neutron disappearance Neutron

More information

The Daya Bay Reactor Neutrino Oscillation Experiment

The Daya Bay Reactor Neutrino Oscillation Experiment The Daya Bay Reactor Neutrino Oscillation Experiment Measurement of θ 13 Mixing Parameter Viktor Pěč for the Daya Bay Experiment Collaboration Charles University in Prague EPS HEP09, Neutrino Physics,

More information

New results from RENO and prospects with RENO-50

New results from RENO and prospects with RENO-50 New results from RENO and prospects with RENO-50 Soo-Bong Kim KNRC, Department of Physics and Astronomy, Seoul National University, Seoul 151-742, South Korea Abstract RENO (Reactor Experiment for Neutrino

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

arxiv:physics/ v1 3 Aug 2006

arxiv:physics/ v1 3 Aug 2006 Gamma Ray Spectroscopy with Scintillation Light in Liquid Xenon arxiv:physics/6834 v1 3 Aug 26 K. Ni, E. Aprile, K.L. Giboni, P. Majewski, M. Yamashita Physics Department and Columbia Astrophysics Laboratory

More information

Neutrino oscillation physics potential of Hyper-Kamiokande

Neutrino oscillation physics potential of Hyper-Kamiokande Neutrino oscillation physics potential of Hyper-Kamiokande on behalf of the Hyper-Kamiokande Collaboration Queen Mary University of London E-mail: l.cremonesi@qmul.ac.uk Hyper-Kamiokande (Hyper-K) is a

More information

The XENON1T experiment

The XENON1T experiment The XENON1T experiment Ranny Budnik Weizmann Institute of Science For the XENON collaboration 1 The XENON1T experiment Direct detection with xenon The XENON project XENON1T/nT 2 Quick introduction and

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

Current status of LUX Dark Matter Experiment

Current status of LUX Dark Matter Experiment Current status of LUX Dark Matter Experiment by A. Lyashenko Yale University On behalf of LUX collaboration LUX Large Underground Xenon experiment LUX Collaboration: Yale, CWRU, UC Santa Barbara, Brown,

More information

Cosmic Ray Physics with the Alpha Magnetic Spectrometer

Cosmic Ray Physics with the Alpha Magnetic Spectrometer Cosmic Ray Physics with the Alpha Magnetic Spectrometer Università di Roma La Sapienza, INFN on behalf of AMS Collaboration Outline Introduction AMS02 Spectrometer Cosmic Rays: origin & propagations: Dominant

More information

PoS(TIPP2014)033. Upgrade of MEG Liquid Xenon Calorimeter. Ryu SAWADA. ICEPP, the University of Tokyo

PoS(TIPP2014)033. Upgrade of MEG Liquid Xenon Calorimeter. Ryu SAWADA. ICEPP, the University of Tokyo ICEPP, the University of Tokyo E-mail: sawada@icepp.s.u-tokyo.ac.jp The MEG experiment yielded the most stringent upper limit on the branching ratio of the flavorviolating muon decay µ + e + γ. A major

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

Latest Results from the OPERA Experiment (and new Charge Reconstruction)

Latest Results from the OPERA Experiment (and new Charge Reconstruction) Latest Results from the OPERA Experiment (and new Charge Reconstruction) on behalf of the OPERA Collaboration University of Hamburg Institute for Experimental Physics Overview The OPERA Experiment Oscillation

More information

Walter C. Pettus on behalf of the DM- ICE collaboration University of Wisconsin Madison. APS April Meeting Session D11: Dark Matter II 13 April 2013

Walter C. Pettus on behalf of the DM- ICE collaboration University of Wisconsin Madison. APS April Meeting Session D11: Dark Matter II 13 April 2013 Walter C. Pettus on behalf of the DM- ICE collaboration University of Wisconsin Madison APS April Meeting Session D11: Dark Matter II 13 April 2013 Before running a dark matter experiment at the South

More information

The JUNO veto detector system. Haoqi Lu Institute of High Energy physics (On Behalf of the JUNO Collaboration) TIPP2017, May22-26,Beijing

The JUNO veto detector system. Haoqi Lu Institute of High Energy physics (On Behalf of the JUNO Collaboration) TIPP2017, May22-26,Beijing The JUNO veto detector system Haoqi Lu Institute of High Energy physics (On Behalf of the JUNO Collaboration) TIPP2017, May22-26,Beijing 1 The Jiangmen Underground Neutrino Observatory (JUNO) Detector

More information

arxiv: v1 [hep-ex] 14 May 2015

arxiv: v1 [hep-ex] 14 May 2015 arxiv:1505.03641v1 [hep-ex] 14 May 2015 Recent Results from Daya Bay Reactor Neutrino Experiment B. Z. HU on behalf of the Daya Bay collaboration Department of Physics, National Taiwan University, No.

More information

PHYS 3446 Lecture #12

PHYS 3446 Lecture #12 PHYS 3446 Lecture #12 Wednesday, Oct. 18, 2006 Dr. 1. Particle Detection Ionization Detectors MWPC Scintillation Counters Time of Flight 1 Announcements Next LPCC Workshop Preparation work Each group to

More information

PREX and CREX. R N from Electroweak Asymmetry in Elastic Electron-Nucleus Scattering. Neutron Skin.

PREX and CREX.   R N from Electroweak Asymmetry in Elastic Electron-Nucleus Scattering. Neutron Skin. http://hallaweb.jlab.org/parity/prex PREX and CREX 08 Pb Horowitz 48 Ca Neutron Skin R N from Electroweak Asymmetry in Elastic Electron-Nucleus Scattering R L 4 6 A ~ 10 PV Q ~ 10 R L PRL 108 (01) 1150

More information

The next generation dark matter hunter: XENON1T status and perspective

The next generation dark matter hunter: XENON1T status and perspective The next generation dark matter hunter: XENON1T status and perspective A. Rizzo a on behalf of the XENON Collaboration Department of Astrophysics, Columbia University in the City of New York, USA Abstract.

More information

arxiv: v1 [physics.ins-det] 23 Oct 2007

arxiv: v1 [physics.ins-det] 23 Oct 2007 1 arxiv:0710.4279v1 [physics.ins-det] 23 Oct 2007 The SuperNEMO double beta decay experiment I. Nasteva on behalf of the SuperNEMO Collaboration School of Physics and Astronomy, University of Manchester,

More information

John Ellison University of California, Riverside. Quarknet 2008 at UCR

John Ellison University of California, Riverside. Quarknet 2008 at UCR Cosmic Rays John Ellison University of California, Riverside Quarknet 2008 at UCR 1 What are Cosmic Rays? Particles accelerated in astrophysical sources incident on Earth s atmosphere Possible sources

More information

NATIONAL RESEARCH NUCLEAR UNIVERSITY MEPhI (Moscow Engineering Physics Institute) Laboratory for Experimental Nuclear Physics

NATIONAL RESEARCH NUCLEAR UNIVERSITY MEPhI (Moscow Engineering Physics Institute) Laboratory for Experimental Nuclear Physics NATIONAL RESEARCH NUCLEAR UNIVERSITY MEPhI (Moscow Engineering Physics Institute) Laboratory for Experimental Nuclear Physics http://enpl.mephi.ru/ The RED-100 Search for elastic coherent neutrino scattering

More information

Update on Experiments using SoLID Spectrometer

Update on Experiments using SoLID Spectrometer Update on Experiments using SoLID Spectrometer Yi Qiang for SoLID Collaboration Hall A Collaboration Meeting Dec 16, 2011 Overview SoLID: Solenoidal Large Intensity Device High rate capability: allow for

More information

The Double Chooz Project

The Double Chooz Project The Double Chooz Project Progress and Expected Sensitivity David McKee, KSU 13 17 July 2009 TeVPA @ SLAC Outline I. Neutrino mixing and θ 13 II. Existing θ 13 measurements III. This is hard with a single

More information

On the possible construction of a Mu2e calibration linac built around a spare Project-X or ILC cryomodule

On the possible construction of a Mu2e calibration linac built around a spare Project-X or ILC cryomodule On the possible construction of a Mu2e calibration linac built around a spare Project-X or ILC cryomodule George Gollin a Department of Physics University of Illinois at Urbana-Champaign 1110 West Green

More information

The KATRIN experiment

The KATRIN experiment The KATRIN experiment Status and SDS comissioning Philipp Chung-On Ranitzsch for the KATRIN collaboration Insitute for Nuclear Physics, Westfälische Wilhelms-Universität, Münster The KATRIN experiment

More information

The GERmanium Detector Array

The GERmanium Detector Array The GERmanium Detector Array n n ν=v p e - e - p Outline: Exp. issues of 0νββ-decay of 76 Ge Concept of GERDA Status of the experiment Summary and conclusions Kevin Kröninger (Max-Planck-Institut für Physik,

More information

Neutron Scattering under Extreme Conditions at the Spallation Neutron Source

Neutron Scattering under Extreme Conditions at the Spallation Neutron Source Neutron Scattering under Extreme Conditions at the Spallation Neutron Source Jamie Molaison Oak Ridge National Laboratory International Workshop on Synchrotron High Pressure Mineral Physics and Materials

More information

Chung-Yao Fellowship 2016 interview

Chung-Yao Fellowship 2016 interview 1/12 Chung-Yao Fellowship 2016 interview Hiroki KUSANO Department of Physics and Astronomy, Shanghai Jiao Tong University May 8, 2016 Resume 1 2/12 Personal data Name: Hiroki Kusano Date of birth: Nov

More information

Temperature Dependence Calibration and Correction of the DAMPE BGO Electromagnetic Calorimeter

Temperature Dependence Calibration and Correction of the DAMPE BGO Electromagnetic Calorimeter Temperature Dependence Calibration and Correction of the DAMPE BGO Electromagnetic Calorimeter Yifeng Wei, Zhiyong Zhang, Yunlong Zhang*, Sicheng Wen, Chi Wang, Zhiying Li, Changqing Feng, Xiaolian Wang,

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

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

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. First Physics at CMS Available on CMS information server CMS CR -2009/034 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 04 February 2009 First Physics at CMS

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

DUSEL Theory Workshop, OSU April 4, Yuri Kamyshkov/ University of Tennessee

DUSEL Theory Workshop, OSU April 4, Yuri Kamyshkov/ University of Tennessee DUSEL Theory Workshop, OSU April 4, 2008 Yuri Kamyshkov/ University of Tennessee email: kamyshkov@utk.edu τ N N 8 10 sec (in vacuum) Sensitivity for free neutron search (observation probability) t obs

More information

The Daya Bay Reactor Neutrino Experiment

The Daya Bay Reactor Neutrino Experiment The Daya Bay Reactor Neutrino Experiment Ming-chung Chu The Chinese University of Hong Kong, Hong Kong On behalf of the Daya Bay Collaboration Partial support: CUHK VC Discretionary Fund, RGC CUHK3/CRF/10R

More information

Neutrinos. Why measure them? Why are they difficult to observe?

Neutrinos. Why measure them? Why are they difficult to observe? Outline What is a neutrino? Why do we want to study them? Building a detector to detect the undetectable What does a neutrino detector see? How do you seperate a neutrino signal from the background? Neutrinos

More information

The relevance of XENON10 constraints in this low-mass region has been questioned [15] C.E. Aalseth et al. arxiv: v1

The relevance of XENON10 constraints in this low-mass region has been questioned [15] C.E. Aalseth et al. arxiv: v1 The relevance of XENON10 constraints in this low-mass region has been questioned [15] C.E. Aalseth et al. arxiv:1001.2834v1 Peter Sorensen LLNL on behalf of the XENON10 Collaboration at UC Davis HEFTI

More information

Solid Xenon Detector R&D

Solid Xenon Detector R&D Solid Xenon Detector R&D Jonghee Yoo Fermilab 24 Feb 2012 UCLA Dark Matter Symposium Solid Xenon Scintillation ~100 ev/γ Phonons ~100 mev/ph Ionization ~10 ev/el Why Xenon? No long-lived Xe radio isotope

More information

AMoRE 0 experiment using low temperature 40 Ca 100 MoO 4 calorimeters

AMoRE 0 experiment using low temperature 40 Ca 100 MoO 4 calorimeters AMoRE 0 experiment using low temperature 40 Ca 100 MoO 4 calorimeters Yong-Hamb Kim On behalf of AMoRE collaboration Institute for Basic Science (IBS) Korea Research Institute for Standards and Science

More information

Detectors for the COHERENT neutrino experiment R. Tayloe Indiana U. for the COHERENT collaboration

Detectors for the COHERENT neutrino experiment R. Tayloe Indiana U. for the COHERENT collaboration Detectors for the COHERENT neutrino experiment R. Tayloe Indiana U. for the COHERENT collaboration Outline Physics motivation Experimental overview detectors: CsI NaI LAr Ge LAr CsI Coherent Elastic n-nucleus

More information

PHY326/426 Dark Matter and the Universe. Dr. Vitaly Kudryavtsev F9b, Tel.:

PHY326/426 Dark Matter and the Universe. Dr. Vitaly Kudryavtsev F9b, Tel.: PHY326/426 Dark Matter and the Universe Dr. Vitaly Kudryavtsev F9b, Tel.: 0114 2224531 v.kudryavtsev@sheffield.ac.uk Indirect searches for dark matter WIMPs Dr. Vitaly Kudryavtsev Dark Matter and the Universe

More information

Solar Neutrinos in Large Liquid Scintillator Detectors

Solar Neutrinos in Large Liquid Scintillator Detectors Solar Neutrinos in Large Liquid Scintillator Detectors M. Chen Queen s University DOANOW March 24, 2007 Low Energy Solar Neutrinos complete our understanding of neutrinos from the Sun pep, CNO, 7 Be, pp

More information

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

arxiv: v1 [physics.ins-det] 29 Jun 2011 Investigation of Large LGB Detectors for Antineutrino Detection P. Nelson a,, N. S. Bowden b, a Department of Physics, Naval Postgraduate School, Monterey, CA 99, USA b Lawrence Livermore National Laboratory,

More information

Vacuum System of Synchrotron radiation sources

Vacuum System of Synchrotron radiation sources 3 rd ILSF Advanced School on Synchrotron Radiation and Its Applications September 14-16, 2013 Vacuum System of Synchrotron radiation sources Prepared by: Omid Seify, Vacuum group, ILSF project Institute

More information

Particle Detectors Tools of High Energy and Nuclear Physics Detection of Individual Elementary Particles

Particle Detectors Tools of High Energy and Nuclear Physics Detection of Individual Elementary Particles Particle Detectors Tools of High Energy and Nuclear Physics Detection of Individual Elementary Particles Howard Fenker Jefferson Lab May 31, 2006 Outline of Talk Interactions of Particles with Matter Atomic

More information

x Contents Segmented Mirror Telescopes Metal and Lightweight Mirrors Mirror Polishing

x Contents Segmented Mirror Telescopes Metal and Lightweight Mirrors Mirror Polishing Contents 1 Fundamentals of Optical Telescopes... 1 1.1 A Brief History of Optical Telescopes.................... 1 1.2 General Astronomical Requirements..................... 6 1.2.1 Angular Resolution.............................

More information

Studies of the XENON100 Electromagnetic Background

Studies of the XENON100 Electromagnetic Background Studies of the XENON100 Electromagnetic Background Daniel Mayani Physik-Institut University of Zurich PhD Seminar PSI, August 26-27, 2015 Searching for elusive particles The main challenge for experiments

More information

DOE SBIR & STTR FY 2019 Phase 1, Release 1 Topics

DOE SBIR & STTR FY 2019 Phase 1, Release 1 Topics Source: InternetCoast BUSINESS OPPORTUNITIES web page>>> Letter of Intent Deadline: September 4, 2018 Application Deadline: October 15, 2018 Download Solicitation Topic Details>>> 1. TECHNOLOGIES FOR MANAGING

More information

Publications of Francesco Arneodo: journal articles

Publications of Francesco Arneodo: journal articles Publications of Francesco Arneodo: journal articles Figure 1: Citation report from ISI Web of Science (IF=31.0) [1] E. Aprile et al., First Axion Results from the XENON100 Experiment, arxiv.org (submitted

More information

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

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. Commissioning of the CMS Detector Available on CMS information server CMS CR -2009/113 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 15 May 2009 Commissioning of the CMS

More information

(a) (i) State the proton number and the nucleon number of X.

(a) (i) State the proton number and the nucleon number of X. PhysicsAndMathsTutor.com 1 1. Nuclei of 218 84Po decay by the emission of an particle to form a stable isotope of an element X. You may assume that no emission accompanies the decay. (a) (i) State the

More information

The Daya Bay Anti-neutrino Experiment

The Daya Bay Anti-neutrino Experiment The Daya Bay Anti-neutrino Experiment On behalf on the Daya Bay Collaboration Jianglai Liu Shanghai Jiao Tong University KPS-CPS joint session, KPS annual meeting, Busan, 2011-10-20 1 13 in PMNS Matrix

More information

UCN supersource at PNPI and fundamental physics program А.P. Serebrov

UCN supersource at PNPI and fundamental physics program А.P. Serebrov UCN supersource at PNPI and fundamental physics program А.P. Serebrov 8 th UCN Workshop Ultra Cold & Cold Neutrons Physics & Sources 11-21 June 2011 1 Content 1. UCN sources at PNPI 2. Ultracold neutron

More information

P.M. King Ohio University for the MOLLER Collaboration

P.M. King Ohio University for the MOLLER Collaboration Parity violating electron scattering at JLab: the MOLLER experiment P.M. King Ohio University for the MOLLER Collaboration SESAPS, 10 November 2016; University of Virginia, Charlottesville, VA The Standard

More information

THE CRYOGENIC UNDERGROUND OBSERVATORY FOR RARE EVENTS: STATUS AND PROSPECTS

THE CRYOGENIC UNDERGROUND OBSERVATORY FOR RARE EVENTS: STATUS AND PROSPECTS THE CRYOGENIC UNDERGROUND OBSERVATORY FOR RARE EVENTS: STATUS AND PROSPECTS Eric B. Norman Dept. of Nuclear Engineering Univ. of California, Berkeley, CA U. S. A. Recent results in n physics Neutrinos

More information