Practical Radiation Control at KEK

Size: px
Start display at page:

Download "Practical Radiation Control at KEK"

Transcription

1 Practical Radiation Control at KEK

2 Scope of this talk Radiation Control (1) Exposure control KEK, Government (2)Controlled area Activation of beam line 12GeV-PS and the Utilizing Facilities Extraction beam line EP1, Neutrino Beam Line, Target Station 500MeV Beam Transport Line Another speaker will give more information: Professor Satoh Maintenance scenario Professor Kawakubo Practical maintenance experience Radio-activities and radiation exposure from the maintenance

3 Proton Accelerators 45MeV Linear Acc. ~ 30mA 500MeV Synchrotron ~ 6-10mA(3-5k W) 12GeV Synchrotron ~ mA (~3-8kW) 168h/w,2186h/3m (5000~ h / y ) Experimental Hall ( 168h/w,2186h/3m (4500h/y)) 12 GeV Protons ~ 0.58mA(~7kW) North Counter Hall (EP1 and Neutrino Beam Line) East Counter Hall (EP2 Beam Line) 500 MeV Protons ~ 10mA(~5kW)

4 Electron and Positron Accelerators Linear Accelerators 10GeV 0.625mA PF-AR Synchrotron 8GeV 0.25A PF Synchrotron 3GeV 0.6 A KEKB Synchrotron 10GeV 1A 5GeV 1A 168h/w,2186h/3m ( ~7 h / y )

5

6

7

8 Area KEK Design L a w Value Site Boundary 50 S v / y 250 Sv/3 m General Area 0.2 Sv/h Warning Area 1.5 Sv/h General Radiation Controlled Restricted Controlled Radiation Area Forbidden Radiation Controlled Area 20 S v / h 1.3mSv/3m (2.6 Sv/h) 1mSv/ w <100 m S v/h >100 m S v/h Ground Water activation 10 S v/y at site boundary from drinking water

9 F o r b i d d e n > m S v / h 2 0 S v / h < R e s t r i c t e d < m S v / h 1. 5 S v / h < G e n e r a l < 2 0 S v / h 0. 2 S v / h < W a r n i n g < 1. 5 S v /h F r e e o n S i t e 0. 2 S v / h P u b l i c S i t e B o u n d a r y < 5 0 S v / y

10

11 Daily Radiation Control (1) Radiation Dose (2) Access Control (3) Radioactive Material Control (4) Exposure Control Control Scheme is di fferent during operation, during maintenance after operation

12 During Operation High energy neutrons (1 100MeV) i n t h e experimental area. Access to the beam line is strictly controlled by interlock system. Radiation controlled area, experimental hall, are monitored continuously to watch the radiation level. Radiation workers and experimentalists, who enter radiation controlled area, are recorded automatically by card system.

13 A f t e r s t o p p i n g o p e r a t i o n, M a i n t e n a n c e i n s i d e b e a m l i n e m u s t b e r e s t r i c t e d. P r o c e d u r e t o s t a r t m a i n t e n a n c e i n s i d e b e a m l i n e : 1 ) m e a s u r e r a d i a t i o n d o s e a l o n g b e a m l i n e, 2 ) w r i t e p r o p o s a l f o r m a i n t e n a n c e w h o, w h e r e, w h e n, h o w 3 ) i f t h e m a i n t e n a n c e i s a t a h i g h r a d i a t i o n p l a c e, p e r m i s s i o n f r o m r a d i a t i o n o f f i c e r, a p e r s o n i n c h a r g e o f t h e f a c i l i t y, p l a n t o p r o c e e d t h e m a i n t e n a n c e t o a v o i d h i g h e x p o s u r e, s h i e l d i n g, i n d i v i d u a l w o r k i n g t i m e, m a n y p e o p l e t o d i s t r i b u t e e x p o s u r e, k e y p e r s o n m u s t b e a w a y f r o m r a d i a t i o n w o r k t i l l n e c e s s a r y. 4 ) E v e r y o n e m u s t c a r r y a n a l a r m d o s i m e t e r, T h e r e s p o n s i b l e p e r s o n m u s t c o n t r o l a n d o r g a n i z e.

14

15 Induced Radio- activities and Radiation Field 1 2 G e V P S R i n g a n d R e l a t e d F a c i l i t i e s E x t r a c t i o n S e p t u m M a g n e t s p p s ( 5. 7 k W ) f o r E P 1 F a s t E x t r a c t i o n p p s ( 1. 9 k W ) f o r E P 1 S l o w E x t r a c t i o n C o u n t e r H a l l T 5 a n d T 6 T a r g e t ( P T 6 c m ) p p s N e u t r i n o T a r g e t s t a t i o n N e u t r i n o P r o d u c t i o n T a r g e t ( A L 6 5 c m ) p p s M e V U t i l i z i n g F a c i l i t y N e u t r o n a n d M e s o n L a b o r a t o r y ( N M L ) B e a m T r a n s p o r t L i n e P 4 L i n e f o r s l o w m u o n P r o d u c t i o n

16 12GeV-NCH(sec. 2) 12GeV-ECH (sec. 2) PS-MR (Sec. 1) PS-Linac (sec. 1) PS-BS (sec. 1) 500MeV-NML (sec. 3)

17 100mSv/h EP1:12GeV 10mSv/h 1mSv/h Injection 500MeV EP2 12GeV

18 EP1 Extraction(25/12/ 02) EP2 Extraction(25/12/ 02)

19 3 weeks cooling EP1 EP2

20 North Counter Hall (K5 and K6 Experimental Area) EP1 Beam Line, Neutrino Beam Line EP1-A, Experiment Utilizing Primary Proton Beam 12GeV; 0.16nA ( p p s) EP1-B, 1) Production of Secondary Particles, p, K Target T5(PT6cm): K5 Exp. Area Target T6(PT6cm): K6 Exp. Area 2) Transmit Proton Beam to Neutrino Target Station Neutrino -TS AL target 65cm 2cm diameter 12GeV;Max 0.576mA ( p p s,6.9kw)

21 Dose Rate (msv/h) GeV Protons 1.0(3.0)E+12 P/s for 30 days irradiation on PT(AL) (MARS calculation) AL-65cm PT-6cm Na Time (hours) Na-22

22 Neutron and Meson Science Laboratory, NML Beam Line 500MeV, MAX:9.6mA ( p p s) Neutron Experimental Hall Production Target W with Ta clad 2.9cm 4 Meson Experimental Hall Meson No.1 Laboratory Meson No.2 Laboratory (P-4 Beam Line)

23 Dose rate created by induced activities 12GeV-PS extraction septum magnets Dose Rate (msv/h) Beam Loss Max Average 400W W ~20 1~5 8h cooling 3w cooling Target (EP1) in 12GeV-PS Related Facilities PT (6cm) 960W 1000 Near Target 50~100 3 d cooling

24 KEK Working Level of Exposure Control C l o s e C o n t a c t 0.5 msv/d 30 minutes/d at 1mSv/h 3 minutes/d at 10mSv/h 1 msv/w 2 days/w 7 msv/y 7 weeks/y Planning maintenance 1 ~ a few hours

Estimation of Radioactivity and Residual Gamma-ray Dose around a Collimator at 3-GeV Proton Synchrotron Ring of J-PARC Facility

Estimation of Radioactivity and Residual Gamma-ray Dose around a Collimator at 3-GeV Proton Synchrotron Ring of J-PARC Facility Estimation of Radioactivity and Residual Gamma-ray Dose around a Collimator at 3-GeV Proton Synchrotron Ring of J-PARC Facility Y. Nakane 1, H. Nakano 1, T. Abe 2, H. Nakashima 1 1 Center for Proton Accelerator

More information

STATUS OF KEKB. Ryuhei Sugahara, Yasunobu Ohsawa High Energy Accelerator Research Organization (KEK) Oho 1-1, Tsukuba, Ibaraki, Japan

STATUS OF KEKB. Ryuhei Sugahara, Yasunobu Ohsawa High Energy Accelerator Research Organization (KEK) Oho 1-1, Tsukuba, Ibaraki, Japan STATUS OF KEKB Ryuhei Sugahara, Yasunobu Ohsawa High Energy Accelerator Research Organization (KEK) 1-1,, Ibaraki, Japan Hideaki Yamashita, Yuji Hirasawa Hitachi Techno Engineering Co., Ltd. Kasuga 4-1-9,,

More information

Accelerator Facility Accident Report

Accelerator Facility Accident Report Accelerator Facility Accident Report 31 May 2013 Incorporated Administrative Agency - Japan Atomic Energy Agency Inter-University Research Institute - High Energy Accelerator Research Organization Subject:

More information

Particle Size of Radioactive Aerosols Generated During Machine Operation in High-energy Proton Accelerators

Particle Size of Radioactive Aerosols Generated During Machine Operation in High-energy Proton Accelerators Particle Size of Radioactive Aerosols Generated During Machine Operation in High-energy Proton Accelerators Yuichi Oki, Akira Endo 2, Yukio Kanda and Kenjiro Kondo Radiation Science Center, High Energy

More information

Radiation Shielding of a 230 MeV Proton Cyclotron For Cancer Therapy

Radiation Shielding of a 230 MeV Proton Cyclotron For Cancer Therapy Radiation Shielding of a 230 MeV Proton Cyclotron For Cancer Therapy BHASKAR MUKHERJEE Joint DESY and University of Hamburg Accelerator Physics Seminar 27 August 2009 WPE is located within the Campus of

More information

A Beam Dump Facility (BDF) at CERN - The Concept and a First Radiological Assessment

A Beam Dump Facility (BDF) at CERN - The Concept and a First Radiological Assessment A Beam Dump Facility (BDF) at CERN - The Concept and a First Radiological Assessment M. Calviani 1, M. Casolino 1, R. Jacobsson 1, M. Lamont 1, S. Roesler 1, H. Vincke 1, C. Ahdida 2 1 CERN, 2 PSI AccApp

More information

Research Physicist Field of Nuclear physics and Detector physics. Developing detector for radiation fields around particle accelerators using:

Research Physicist Field of Nuclear physics and Detector physics. Developing detector for radiation fields around particle accelerators using: Christopher Cassell Research Physicist Field of Nuclear physics and Detector physics Developing detector for radiation fields around particle accelerators using: Experimental data Geant4 Monte Carlo Simulations

More information

Shielding Aspects of Accelerators, Targets and Irradiation Facilities SATIF 10 ISBN (print) OECD 2010 CORRIGENDUM

Shielding Aspects of Accelerators, Targets and Irradiation Facilities SATIF 10 ISBN (print) OECD 2010 CORRIGENDUM Shielding Aspects of Accelerators, Targets and Irradiation Facilities SATIF 1 ISBN 978 92 64 3467 9 (print) OECD 21 Pages 221 to 227 CORRIGENDUM Figures 1 to 14 were not printed in full. The complete figures

More information

Lab #13: MEASUREMENT OF RADIATION DOSES

Lab #13: MEASUREMENT OF RADIATION DOSES Lab #13: MEASUREMENT OF RADIATION DOSES THEORETICAL BACKGROUND In order to estimate the radiation exposure it is essential to determine the quantity of radiation. If we identify the dose of radiation to

More information

Employees Contractors

Employees Contractors Attachment Exposure Dose Distribution 1. Effective Dose from External Exposure Table 1 shows the distribution of external exposure dose of workers who were involved in radiation work at the Fukushima Daiichi

More information

Bulk shielding design for the MAX IV facility

Bulk shielding design for the MAX IV facility Bulk shielding design for the MAX IV facility Magnus Lundin 1, Lennart Isaksson 1, Bent Schröder 1 1 Lund University, MAX-lab, P.O. Box 118, SE-221 Lund, Sweden Abstract This paper reports on the design

More information

Employees Contractors

Employees Contractors Attachment Exposure Dose Distribution 1. Effective Dose from External Exposure Table 1 shows the distribution of external exposure dose of workers who were involved in radiation work at the Fukushima Daiichi

More information

October 2017 November Employees Contractors

October 2017 November Employees Contractors Attachment Exposure Dose Distribution 1. Effective Dose from External Exposure Table 1 shows the distribution of external exposure dose of workers who were involved in radiation work at the Fukushima Daiichi

More information

Reactor & Spallation Neutron Sources

Reactor & Spallation Neutron Sources Reactor & Spallation Neutron Sources Oxford School of Neutron Scattering Oxford, 2011-09-06 Ken Andersen ESS Instruments Division ISIS ILL Time evolution: Major neutron sources ILL BENSC (D) SINQ (CH)

More information

Proton and neutron radiation facilities in the PS East hall at CERN

Proton and neutron radiation facilities in the PS East hall at CERN Proton and neutron radiation facilities in the PS East hall at CERN http://www.cern.ch/irradiation M. Glaser, CERN Division EP-TA1-SD Introduction CERN Accelerators CERN-PS East Hall Proton irradiation

More information

Radiation Safety Considerations for the TPS Accelerators

Radiation Safety Considerations for the TPS Accelerators Radiation Safety Considerations for the TPS Accelerators R.J. Sheu, J. Liu, and J.P. Wang National Synchrotron Radiation Research Center, 101 Hsin-Ann Road, Hsinchu Science Park, Hsinchu 30076, TAIWAN

More information

Test Beams: Availability & Plans

Test Beams: Availability & Plans Gene Fisk Fermilab LCWS_2002 Jeju Do Test Beams: Availability & Plans KEK DESY CERN Fermilab SLAC Other KEK Test Beams @ 12 GeV PS Information from: yoshiaki.fujii@kek.jp KEK East Counter Hall T1 and π2

More information

Fundamental Concepts of Particle Accelerators V : Future of the High Energy Accelerators. Koji TAKATA KEK. Accelerator Course, Sokendai

Fundamental Concepts of Particle Accelerators V : Future of the High Energy Accelerators. Koji TAKATA KEK. Accelerator Course, Sokendai .... Fundamental Concepts of Particle Accelerators V : Future of the High Energy Accelerators Koji TAKATA KEK koji.takata@kek.jp http://research.kek.jp/people/takata/home.html Accelerator Course, Sokendai

More information

Advanced Storage Photon Ring Source Upgrade Project:

Advanced Storage Photon Ring Source Upgrade Project: Advanced Storage Photon Ring Source Upgrade Project: The Shielding World s for Leading the Hard X-ray Light Source Advanced Photon Source - Upgrade Bradley J. Micklich Radiation Physicist Argonne National

More information

Experiments on deflection of charged particles using silicon crystals at. Proton Synchrotron (KEK(

Experiments on deflection of charged particles using silicon crystals at. Proton Synchrotron (KEK( Experiments on deflection of charged particles using silicon crystals at REFER ring (Hiroshima( University) and Proton Synchrotron (KEK( KEK) S. Sawada KEK High Energy Accelerator Research Organization

More information

Contents. LC : Linear Collider. µ-µ Collider. Laser-Plasma Wave Accelerator. Livingston Chart 6 References

Contents. LC : Linear Collider. µ-µ Collider. Laser-Plasma Wave Accelerator. Livingston Chart 6 References .... Fundamental Concepts of Particle Accelerators V : Future of the High Energy Accelerators VI : References Koji TAKATA KEK koji.takata@kek.jp http://research.kek.jp/people/takata/home.html Accelerator

More information

Radiation Protection Considerations *

Radiation Protection Considerations * Chapter 11 Radiation Protection Considerations * C. Adorisio 1, S. Roesler 1, C. Urscheler 2 and H. Vincke 1 1 CERN, TE Department, Genève 23, CH-1211, Switzerland 2 Bundesamt fuer Gesundheit, Direktionsbereich

More information

Introduction to Accelerator Physics Part 1

Introduction to Accelerator Physics Part 1 Introduction to Accelerator Physics Part 1 Pedro Castro / Accelerator Physics Group (MPY) Introduction to Accelerator Physics DESY, 28th July 2014 Pedro Castro / MPY Accelerator Physics 28 th July 2014

More information

Fundamental Concepts of Particle Accelerators V: Future of the High Energy Accelerators VI: References. Koji TAKATA KEK. Accelerator Course, Sokendai

Fundamental Concepts of Particle Accelerators V: Future of the High Energy Accelerators VI: References. Koji TAKATA KEK. Accelerator Course, Sokendai .... Fundamental Concepts of Particle Accelerators V: Future of the High Energy Accelerators VI: References Koji TAKATA KEK koji.takata@kek.jp http://research.kek.jp/people/takata/home.html Accelerator

More information

Summary of Shielding and Activation analysis for the European Spallation Source Linac Tunnel

Summary of Shielding and Activation analysis for the European Spallation Source Linac Tunnel Summary of Shielding and Activation analysis for the European Spallation Source Linac Tunnel SHORT SUMMARY OF FINAL RESULTS by Lali Tchelidze March 21, 2013 Several different approaches were taken to estimate

More information

Review of ISOL-type Radioactive Beam Facilities

Review of ISOL-type Radioactive Beam Facilities Review of ISOL-type Radioactive Beam Facilities, CERN Map of the nuclear landscape Outline The ISOL technique History and Geography Isotope Separation On-Line Existing facilities First generation facilities

More information

Occupational Radiation Protection at Accelerator Facilities: Challenges

Occupational Radiation Protection at Accelerator Facilities: Challenges Occupational Radiation Protection at Accelerator Facilities: Challenges Haridas.G Health Physics Division Bhabha Atomic Research Centre INDIA Int. Conf. on Occupational Radiation Protection: Enhancing

More information

PoS(NuFact2017)088. EMuS in CSNS. Guang Zhao 1. Institute of High Energy Physics Beijing, China

PoS(NuFact2017)088. EMuS in CSNS. Guang Zhao 1. Institute of High Energy Physics Beijing, China 1 Institute of High Energy Physics Beijing, China E-mail: zhaog@ihep.ac.cn In this presentation, we report the recent progress in EMuS at CSNS. The following topics will be discussed: a) the base design

More information

10 GeV Synchrotron Longitudinal Dynamics

10 GeV Synchrotron Longitudinal Dynamics 0 GeV Synchrotron Longitudinal Dynamics G. Dugan Laboratory of Nuclear Studies Cornell University Ithaca, NY 483 In this note, I provide some estimates of the parameters of longitudinal dynamics in the

More information

Calculation of the Dose Equivalent Rate from Induced Radioactivity Around the CNGS Target and Magnetic Horn

Calculation of the Dose Equivalent Rate from Induced Radioactivity Around the CNGS Target and Magnetic Horn The CERN Neutrino Beam to Gran Sasso Project EDMS Document No. 599104 CERN Div./Group: 1 AB/ATB, 2 SC/RP Date: 5/15/2005 Calculation of the Dose Equivalent Rate from Induced Radioactivity Around the CNGS

More information

M d e i di l ca A pplilli t ca i ttions o f P arti ttic ti l P e h Physics Saverio Braccini INSEL

M d e i di l ca A pplilli t ca i ttions o f P arti ttic ti l P e h Physics Saverio Braccini INSEL Medical la Applications of Particle Physics Saverio Braccini INSELSPITALSPITAL Department of Medical Radiation Physics University Hospital, Berne, Switzerland Rome - 14-15.06.07 - SB - 1/5 Saverio.Braccini@cern.ch

More information

SSA Measurements with Primary Beam at J-PARC

SSA Measurements with Primary Beam at J-PARC SSA Measurements with Primary Beam at J-PARC Joint UNM/RBRC Workshop on Orbital Angular Momentum in Albuquerque February 25 th, 2006 Yuji Goto (RIKEN/RBRC) February 25, 2006 Yuji Goto (RIKEN/RBRC) 2 Introduction

More information

European Organisation for Nuclear Research European Laboratory for Particle Physics

European Organisation for Nuclear Research European Laboratory for Particle Physics European Organisation for Nuclear Research European Laboratory for Particle Physics TECHNICAL NOTE CERN-DGS-XXXX Radiological assessment of the Tungsten Powder Test (HRM10) at HiRadMat Nikolaos Charitonidis

More information

1. RADIOACTIVITY AND RADIATION PROTECTION

1. RADIOACTIVITY AND RADIATION PROTECTION 1. Radioactivity and radiation protection 1 1. RADIOACTIVITY AND RADIATION PROTECTION Revised August 2011 by S. Roesler and M. Silari (CERN). 1.1. Definitions [1,2] 1.1.1. Physical quantities: Fluence,

More information

Working Correctly & Safely with Radiation. Talia Tzahor Radiation safety officer Tel:

Working Correctly & Safely with Radiation. Talia Tzahor Radiation safety officer Tel: Working Correctly & Safely with Radiation Talia Tzahor Radiation safety officer Tel: 5196 Email: talia.tzahor@weizmann.ac.il Environmental Exposure The typical human body contains: Potassium-40 ( 40 K)

More information

Introduction to Accelerator Physics Part 1

Introduction to Accelerator Physics Part 1 Introduction to Accelerator Physics Part 1 Pedro Castro / Accelerator Physics Group (MPY) Introduction to Accelerator Physics DESY, 27th July 2015 Pedro Castro / MPY Introduction to Accelerator Physics

More information

Positron program at the Idaho Accelerator Center. Giulio Stancari Idaho State University and Jefferson Lab

Positron program at the Idaho Accelerator Center. Giulio Stancari Idaho State University and Jefferson Lab Positron program at the Idaho Accelerator Center Giulio Stancari Idaho State University and Jefferson Lab International Workshop on Positrons at Jefferson Lab Newport News, Virginia (USA), 26 March 2009

More information

Evaluation and Measurements of Radioactive Air Emission and Off-Site Doses at SLAC

Evaluation and Measurements of Radioactive Air Emission and Off-Site Doses at SLAC SLAC-PUB-15365 Evaluation and Measurements of Radioactive Air Emission and Off-Site Doses at SLAC I.Chan, J.Liu, H.Tran SLAC National Accelerator Laboratory, M.S. 48, 2575 Sand Hill Road, Menlo Park, CA,

More information

Technological Challenges for High-Intensity Proton Rings

Technological Challenges for High-Intensity Proton Rings Technological Challenges for High-Intensity Proton Rings Yoshishige Yamazaki 52 nd ICFA Advanced Beam Dynamics Workshop on High-Intensity and High-Brightness Hadron Beams Park Plaza Beijing West, September

More information

MESON AREA 1000 GeV STUDY. C. N. Brown, A. L. Read, A. A. Wehmann Fermi National Accelerator Laboratory

MESON AREA 1000 GeV STUDY. C. N. Brown, A. L. Read, A. A. Wehmann Fermi National Accelerator Laboratory -375 MESON AREA 1000 GeV STUDY C. N. Brown, A. L. Read, A. A. Wehmann Fermi National Accelerator Laboratory This report attempts to collect together preliminary thoughts on how protons from the Energy

More information

Performance Studies of the Vibration Wire Monitor on the Test Stand with Low Energy Electron Beam

Performance Studies of the Vibration Wire Monitor on the Test Stand with Low Energy Electron Beam Proc. 2nd Int. Symp. Science at J-PARC Unlocking the Mysteries of Life, Matter and the Universe http://dx.doi.org/10.7566/jpscp.8.012024 Performance Studies of the Vibration Wire Monitor on the Test Stand

More information

Electron scattering experiment off proton at ultra-low Q 2

Electron scattering experiment off proton at ultra-low Q 2 Electron scattering experiment off proton at ultra-low Q 2 Toshimi Suda Research Center for Electron-Photon Science, Tohoku University, Sendai Proton Radius Puzzle NEUROSCIENCE People Who Remember Everything

More information

STUDIES OF MATERIAL PROPERTIES UNDER IRRADIATION AT BNL LINEAR ISOTOPE PRODUCER (BLIP) N. Simos, H. Kirk, H. Ludewig; BNL

STUDIES OF MATERIAL PROPERTIES UNDER IRRADIATION AT BNL LINEAR ISOTOPE PRODUCER (BLIP) N. Simos, H. Kirk, H. Ludewig; BNL STUDIES OF MATERIAL PROPERTIES UNDER IRRADIATION AT BNL LINEAR ISOTOPE PRODUCER (BLIP) N. Simos, H. Kirk, H. Ludewig; BNL N. Mokhov, P. Hurh, J. Hylen, J. Misek, Fermilab Overview Materials & High Power

More information

Part E. Radiation monitors. Radiation Safety - JUAS 2014, X. Queralt. Part E. Radiation monitors

Part E. Radiation monitors. Radiation Safety - JUAS 2014, X. Queralt. Part E. Radiation monitors Part E. Radiation monitors 1 / 29 Part E. Radiation monitors dose rate ( Sv.h -1 ) ma 0 10 20 30 40 50 10.0 1.0 0.1 250 0 10 20 30 40 50 days since 18/01/02 200 150 100 50 0 Example: photon dose rate measurement

More information

The CNGS neutrino beam

The CNGS neutrino beam 10th Topical Seminar on Innovative Particle and Radiation Detectors (IPRD06) 1-5 October 2006 Siena, Italy ν The CNGS neutrino beam G. Sirri INFN Bologna CNGS (CERN Neutrinos to Gran Sasso) The project

More information

JHFnu at J-PARC neutrino oscillation experiment

JHFnu at J-PARC neutrino oscillation experiment @IAC Mar.0,00 JHFnu at J-PARC neutrino oscillation experiment 50 GeV PS LOI # International collaboration Recent developments in neutrino physics Readiness Summary Koichiro Nishikawa Kyoto niversity for

More information

Operational Experience with J-PARC Injection and Extraction Systems

Operational Experience with J-PARC Injection and Extraction Systems Operational Experience with J-PARC Injection and Extraction Systems Pranab Kumar Saha Japan Proton Accelerator Research Complex (J-PARC) 46th ICFA Advanced Beam Dynamics Workshop ( HB2010 ) Morschach,

More information

STATUS OF THE J-PARC FACILITY

STATUS OF THE J-PARC FACILITY STATUS OF THE J-PARC FACILITY Shoji Nagamiya, J-PARC Center, 2-4 Shirakata Shirane, Tokai-Mura, Ibaraki 319-1195, Japan Abstract J-PARC (Japan Proton Accelerator Research Complex) consists of three accelerators

More information

How J-PARC recovered from the big earthquake

How J-PARC recovered from the big earthquake How J-PARC recovered from the big earthquake KEK / Fujio Naito Outline About J-PARC The earthquake Damage on J-PARC Recovery plan Beam study results Summary J-PARC (Japan Proton Accelerator Research Complex)

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 -2018/225 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 27 September 2018 (v2, 19 November

More information

A beam line for schools

A beam line for schools A beam line for schools Great things can happen when high schools get involved with cutting edge science, and that s exactly what CERN is proposing with its new beam line for schools competition, which

More information

J-PARC Japan Proton Accelerator Research Complex. J-PARC Status after March 11. J-PARC at Tokai-mura, Ibaraki-ken

J-PARC Japan Proton Accelerator Research Complex. J-PARC Status after March 11. J-PARC at Tokai-mura, Ibaraki-ken J-PARC Japan Proton Accelerator Research Complex J-PARC Status after March 11 J-PARC at Tokai-mura, Ibaraki-ken Bird s eye photo in July 2009 J-PARC Japan Proton Accelerator Research Complex ν to SK 400MeV

More information

Reduction of Radioactive Waste by Accelerators

Reduction of Radioactive Waste by Accelerators October 9-10, 2014 International Symposium on Present Status and Future Perspective for Reducing Radioactive Waste - Aiming for Zero-Release - Reduction of Radioactive Waste by Accelerators Hiroyuki Oigawa

More information

JAPAN PROTON ACCELERATOR RESEARCH COMPLEX

JAPAN PROTON ACCELERATOR RESEARCH COMPLEX J-PARC JAPAN PROTON ACCELERATOR RESEARCH COMPLEX Facilities at J-PARC The J PARC stands for Japan Proton Accelerator Research Complex and it is a new and exciting accelerator research facility in Japan.

More information

Radiation Damage and Recovery in Polarized Ammonia Targets

Radiation Damage and Recovery in Polarized Ammonia Targets Radiation Damage and Recovery in Polarized Ammonia Targets James Maxwell Univ. of Virginia Polarized Target Group Polarized Sources & Targets, Ferrara, Italia, 8.9.2009 Outline Spin Physics at TJNAF (Jefferson

More information

ATL-INDET /04/2000

ATL-INDET /04/2000 Evolution of silicon micro-strip detector currents during proton irradiation at the CERN PS ATL-INDET-2000-009 17/04/2000 R.S.Harper aλ, P.P.Allport b, L.Andricek c, C.M.Buttar a, J.R.Carter d, G.Casse

More information

Radiation Protection At Synchrotron Radiation Facilities

Radiation Protection At Synchrotron Radiation Facilities 3 rd ILSF Advanced School on Synchrotron Radiation and Its Applications September 14-16, 2013 Radiation Protection At Synchrotron Radiation Facilities Ehsan Salimi Shielding and Radiation Safety Group

More information

Safety Training for Radiation Workers at ICRR, Univ. of Tokyo. April, 2017

Safety Training for Radiation Workers at ICRR, Univ. of Tokyo. April, 2017 Safety Training for Radiation Workers at ICRR, Univ. of Tokyo April, 2017 Outline What is new in this year Law, Rules at ICRR Radiation management at ICRR Rules at ICRR Safety handling Important notices

More information

3. Particle accelerators

3. Particle accelerators 3. Particle accelerators 3.1 Relativistic particles 3.2 Electrostatic accelerators 3.3 Ring accelerators Betatron // Cyclotron // Synchrotron 3.4 Linear accelerators 3.5 Collider Van-de-Graaf accelerator

More information

Benchmark Experiments of Accelerator Driven Systems (ADS) in Kyoto University Critical Assembly (KUCA)

Benchmark Experiments of Accelerator Driven Systems (ADS) in Kyoto University Critical Assembly (KUCA) Benchmark Experiments of Accelerator Driven Systems (ADS) in Kyoto University Critical Assembly (KUCA) C. H. Pyeon, T. Misawa, H. Unesaki, K. Mishima and S. Shiroya (Kyoto University Research Reactor Institute,

More information

STATUS REPORT ON SURVEY AND ALIGNMENT OF J-PARC AFTER THE EARTHQUAKE

STATUS REPORT ON SURVEY AND ALIGNMENT OF J-PARC AFTER THE EARTHQUAKE STATUS REPORT ON SURVEY AND ALIGNMENT OF J-PARC AFTER THE EARTHQUAKE N. Tani#, T. Morishita, S. Meigo, M. Harada, H. Stefanus, JAEA/J-PARC, Tokai, Japan M. Shirakata, T. Ishii, Y. Fujii, Y. Shirakabe,

More information

J-PARC (Japan Proton Accelerator Research Complex)

J-PARC (Japan Proton Accelerator Research Complex) J-PARC Tokai, Japan (Japan Proton Accelerator Research Complex) Material and Biological Science Facility 50 GeV Synchrotron (15 ma) 400 MeV Linac (350m) 3 GeV Synchrotron (333 ma) Neutrino Facility World-highest

More information

New irradiation zones at the CERN-PS

New irradiation zones at the CERN-PS Nuclear Instruments and Methods in Physics Research A 426 (1999) 72 77 New irradiation zones at the CERN-PS M. Glaser, L. Durieu, F. Lemeilleur *, M. Tavlet, C. Leroy, P. Roy ROSE/RD48 Collaboration CERN,

More information

Exam Results. Force between charges. Electric field lines. Other particles and fields

Exam Results. Force between charges. Electric field lines. Other particles and fields Exam: Exam scores posted on Learn@UW No homework due next week Exam Results F D C BC B AB A Phy107 Fall 2006 1 Particles and fields We have talked about several particles Electron,, proton, neutron, quark

More information

Nuclear and Radiation Physics

Nuclear and Radiation Physics 501503742 Nuclear and Radiation Physics Why nuclear physics? Why radiation physics? Why in Jordan? Interdisciplinary. Applied? 1 Subjects to be covered Nuclear properties. Nuclear forces. Nuclear matter.

More information

Radiation measurements around ESRF beamlines

Radiation measurements around ESRF beamlines Radiation measurements around ESRF beamlines P. Berkvens & P. Colomp European Synchrotron Radiation Facility Abstract Over the last 2 years radiation levels around a number of beamlines have been continuously

More information

Fundamentals of radiation protection

Fundamentals of radiation protection Fundamentals of radiation protection Kamel ABBAS European Commission, Joint Research Centre Institute for Transuranium Elements, Nuclear Security Unit Via E. Fermi, 2749, I-21027 Ispra, Italy tel. +39-0332-785673,

More information

Status of J-PARC Transmutation Experimental Facility

Status of J-PARC Transmutation Experimental Facility Status of J-PARC Transmutation Experimental Facility 10 th OECD/NEA Information Exchange Meeting for Actinide and Fission Product Partitioning and Transmutation 2008.10.9 Japan Atomic Energy Agency Toshinobu

More information

Radiation damage calculation in PHITS

Radiation damage calculation in PHITS Radiation Effects in Superconducting Magnet Materials (RESMM'12), 13 Feb. 15 Feb. 2012 Radiation damage calculation in PHITS Y. Iwamoto 1, K. Niita 2, T. Sawai 1, R.M. Ronningen 3, T. Baumann 3 1 JAEA,

More information

Measurement of induced radioactivity in air and water for medical accelerators

Measurement of induced radioactivity in air and water for medical accelerators Measurement of induced radioactivity in air and water for medical accelerators K. Masumoto 1, K. Takahashi 1, H. Nakamura 1, A. Toyoda 1, K. Iijima 1, K. Kosako 2, K. Oishi 2, F. Nobuhara 1 High Energy

More information

Particle Accelerators

Particle Accelerators Experimental Methods of Particle Physics Particle Accelerators Andreas Streun, PSI andreas.streun@psi.ch https://ados.web.psi.ch/empp-streun Andreas Streun, PSI 1 Particle Accelerators 1. Introduction

More information

Production target and beam dump in the slow-extraction beam line. Hadron Beam Line Group Target and Monitor Group

Production target and beam dump in the slow-extraction beam line. Hadron Beam Line Group Target and Monitor Group Production target and beam dump in the slow-extraction beam line Yoshinori Sato (KEK) On behalf of Hadron Line Group Target and Monitor Group KEK-JAERI Joint Project roduction target (T1) Requirements

More information

Commissioning of the Beta Secondary Standard (BSS2)

Commissioning of the Beta Secondary Standard (BSS2) Commissioning of the Beta Secondary Standard (BSS2) Speaker / Author: R.W. Thoka* Co-author: S. Jozela* * National Metrology Institute of South Africa (NMISA), Private Bag X 34, Lynnwood Ridge, Pretoria,

More information

H. Koshiishi, H. Matsumoto, A. Chishiki, T. Goka, and T. Omodaka. Japan Aerospace Exploration Agency

H. Koshiishi, H. Matsumoto, A. Chishiki, T. Goka, and T. Omodaka. Japan Aerospace Exploration Agency 9 th Workshop on Radiation Monitoring for the International Space Station Evaluation of Neutron Radiation Environment inside the International Space Station based on the Bonner Ball Neutron Detector Experiment

More information

MAGNET INSTALLATION AND ALIGNMENT FOR THE FUJI TEST BEAM LINE AT KEKB

MAGNET INSTALLATION AND ALIGNMENT FOR THE FUJI TEST BEAM LINE AT KEKB MAGNET INSTALLATION AND ALIGNMENT FOR THE FUJI TEST BEAM LINE AT KEKB M. Masuzawa, K.Egawa and Y. Ohsawa, KEK, Tsukuba, Japan Abstract Since the 12 GeV Proton Synchrotron ended its operation in March 2006,

More information

Planning and preparation approaches for non-nuclear waste disposal

Planning and preparation approaches for non-nuclear waste disposal Planning and preparation approaches for non-nuclear waste disposal Lucia Sarchiapone Laboratori Nazionali di Legnaro (Pd) Istituto Nazionale di Fisica Nucleare INFN Lucia.Sarchiapone@lnl.infn.it +39 049

More information

Department of Radiation Protection, Nuclear Science Research Institute, Japan Atomic Energy Agency

Department of Radiation Protection, Nuclear Science Research Institute, Japan Atomic Energy Agency Department of Radiation Protection, Nuclear Science Research Institute, Japan Atomic Energy Agency Facility of Radiation Standards It is important that radiation measuring instruments are calibrated by

More information

ICALEPCS Oct. 6-11, 2013

ICALEPCS Oct. 6-11, 2013 Outline 2 SOHO (ESA & NASA) 3 SOHO (ESA & NASA) 4 SOHO (ESA & NASA) EGRET Team 5 Heavy Ions Charged Ionizing Radiation Outer-Space is full of them Figures reproduced from: 1.Mewaldt, R.A., "Elemental Composition

More information

The residual radioactivity of a water-copper beam dump for the TESLA Test Facility

The residual radioactivity of a water-copper beam dump for the TESLA Test Facility Internal Report DESY D3-92 November 1998 The residual radioactivity of a water-copper beam dump for the TESLA Test Facility A. Leuschner and K. Tesch Internal Report DESY D3-92 November 1998 The residual

More information

Physics 736. Experimental Methods in Nuclear-, Particle-, and Astrophysics. - Accelerator Techniques: Introduction and History -

Physics 736. Experimental Methods in Nuclear-, Particle-, and Astrophysics. - Accelerator Techniques: Introduction and History - Physics 736 Experimental Methods in Nuclear-, Particle-, and Astrophysics - Accelerator Techniques: Introduction and History - Karsten Heeger heeger@wisc.edu Homework #8 Karsten Heeger, Univ. of Wisconsin

More information

Energy response for high-energy neutrons of multi-functional electronic personal dosemeter

Energy response for high-energy neutrons of multi-functional electronic personal dosemeter Energy response for high-energy neutrons of multi-functional electronic personal dosemeter T. Nunomiya 1, T. Ishikura 1, O. Ueda 1, N. Tsujimura 2,, M. Sasaki 2,, T. Nakamura 1,2 1 Fuji Electric Systems

More information

Spectral Correction Factors for Conventional Neutron Dose Meters Used in High-Energy Neutron Environments

Spectral Correction Factors for Conventional Neutron Dose Meters Used in High-Energy Neutron Environments Spectral Correction Factors for Conventional Neutron Dose Meters Used in High-Energy Neutron Environments A complete survey of all neutron spectra in IAEA-TRS-403 RadSynch2015, DESY Hamburg, Germany (June

More information

PERSPECTIVES OF PERSONNEL EXTERNAL DOSIMETRY AT STANFORD LINEAR ACCELERATOR CENTER

PERSPECTIVES OF PERSONNEL EXTERNAL DOSIMETRY AT STANFORD LINEAR ACCELERATOR CENTER SLAC-PUB-95-6749 (March 1995) PERSPECTIVES OF PERSONNEL EXTERNAL DOSIMETRY AT STANFORD LINEAR ACCELERATOR CENTER J. C. Liu, D. Busick 1, K. R. Kase, R. C. McCall 2, R. Sit and H. Tran 3 Stanford Linear

More information

PULSE-TO-PULSE TRANSVERSE BEAM EMITTANCE CONTROLLING FOR MLF AND MR IN THE 3-GeV RCS OF J-PARC

PULSE-TO-PULSE TRANSVERSE BEAM EMITTANCE CONTROLLING FOR MLF AND MR IN THE 3-GeV RCS OF J-PARC THO3AB3 Proceedings of HB, East-Lansing, MI, USA PULSE-TO-PULSE TRANSVERSE BEAM EMITTANCE CONTROLLING FOR MLF AND MR IN THE 3-GeV RCS OF J-PARC P.K. Saha, H. Harada, H. Hotchi and T. Takayanagi J-PARC

More information

New and accelerator research facility, using MW-class high power proton beams at both 3 GeV and 30 GeV. J-PARC Tokai KEK Tsukuba LINAC 400 MeV Rapid Cycle Synchrotron Energy : 3 GeV Repetition : 25 Hz

More information

Fast-Neutron Production via Break-Up of Deuterons and Fast-Neutron Dosimetry

Fast-Neutron Production via Break-Up of Deuterons and Fast-Neutron Dosimetry Fast-Neutron Production via Break-Up of Deuterons and Fast-Neutron Dosimetry F. Gutermuth *, S. Beceiro, H. Emling, G. Fehrenbacher, E. Kozlova, T. Radon, T. Aumann, T. Le Bleis, K. Boretzky, H. Johansson,

More information

ACCUMULATION OF ACTIVATION PRODUCTS IN PB-BI, TANTALUM, AND TUNGSTEN TARGETS OF ADS

ACCUMULATION OF ACTIVATION PRODUCTS IN PB-BI, TANTALUM, AND TUNGSTEN TARGETS OF ADS ACCUMULATION OF ACTIVATION PRODUCTS IN PB-BI, TANTALUM, AND TUNGSTEN TARGETS OF ADS A.S. Gerasimov, G.V. Kiselev, A.I. Volovik State Scientific Centre of the Russian Federation Institute of Theoretical

More information

Radiation Safety Assessment of the CLS Beamlines Using FLUKA Monte-Carlo Code

Radiation Safety Assessment of the CLS Beamlines Using FLUKA Monte-Carlo Code Radiation Safety Assessment of the CLS Beamlines Using FLUKA Monte-Carlo Code Mo Benmerrouche Fluka Advanced Workshop - Oct 07, 2010 Ericeira, Portugal M. Benmerrouche, HSE Manager http://www.lightsource.ca

More information

Electromagnetic characterization of big aperture magnet used in particle beam cancer therapy

Electromagnetic characterization of big aperture magnet used in particle beam cancer therapy Electromagnetic characterization of big aperture magnet used in particle beam cancer therapy Jhonnatan Osorio Moreno M.Pullia, C.Priano Presented at Comsol conference 2012 Milan Milan 10 th October 2012

More information

Secondary Particles Produced by Hadron Therapy

Secondary Particles Produced by Hadron Therapy Iranian Journal of Medical Physics Vol. 12, No. 2, Spring 2015, 1-8 Received: March 10, 2015; Accepted: July 07, 2015 Original Article Secondary Particles Produced by Hadron Therapy Abdolkazem Ansarinejad

More information

Radiological Implications of Top-up Operation at Canadian Light Source: Dose Computations and Measurements at the Vulnerable Points

Radiological Implications of Top-up Operation at Canadian Light Source: Dose Computations and Measurements at the Vulnerable Points Radiological Implications of Top-up Operation at Canadian Light Source: Dose Computations and Measurements at the Vulnerable Points P. Chowdhury 1 and G. Cubbon 1 1 Canadian Light Source Inc., 44 Inovation

More information

FOOD IRRADIATION TECHNOLOGY. BAEN-625- Advances in Food Engineering

FOOD IRRADIATION TECHNOLOGY. BAEN-625- Advances in Food Engineering FOOD IRRADIATION TECHNOLOGY BAEN-625- Advances in Food Engineering Food irradiation KE produced by accelerators system is limited by regulation to 10 MeV for direct electron irradiation 5 or 7.5 MeV for

More information

MockTime.com. Ans: (b) Q6. Curie is a unit of [1989] (a) energy of gamma-rays (b) half-life (c) radioactivity (d) intensity of gamma-rays Ans: (c)

MockTime.com. Ans: (b) Q6. Curie is a unit of [1989] (a) energy of gamma-rays (b) half-life (c) radioactivity (d) intensity of gamma-rays Ans: (c) Chapter Nuclei Q1. A radioactive sample with a half life of 1 month has the label: Activity = 2 micro curies on 1 8 1991. What would be its activity two months earlier? [1988] 1.0 micro curie 0.5 micro

More information

A Project to convert TLS Booster to hadron accelerator 1. Basic design. 2. The injection systems:

A Project to convert TLS Booster to hadron accelerator 1. Basic design. 2. The injection systems: A Project to convert TLS Booster to hadron accelerator 1. Basic design TLS is made of a 50 MeV electron linac, a booster from 50 MeV to 1.5 GeV, and a storage ring. The TLS storage ring is currently operating

More information

Concepts and R&D for beta beam facilities

Concepts and R&D for beta beam facilities Concepts and R&D for beta beam facilities, CERN on behalf of the EURISOL Beta Beam Study Group 1 Outline Beta Beam Concepts and Options The EURISOL Beta Beam Scenario Ion Production Loss Management Improvements

More information

Neutrino Factory in Japan: based on FFAG

Neutrino Factory in Japan: based on FFAG Neutrino Factory in Japan: based on FFAG Yoshiharu Mori (KEK) 1. Introduction 2. Scenario of muon acceleration 3. Neutrino Factory based on FFAG 4. Summary Introduction What is Neutrino Factory? High-intensity

More information

Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders

Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders Explanation of the Basic Principles and Goals Visit to the CTF3 Installation Roger Ruber Collider History p p hadron collider

More information

Propagation in the Galaxy 2: electrons, positrons, antiprotons

Propagation in the Galaxy 2: electrons, positrons, antiprotons Propagation in the Galaxy 2: electrons, positrons, antiprotons As we mentioned in the previous lecture the results of the propagation in the Galaxy depend on the particle interaction cross section. If

More information

Final Exam, Part A. December 12, Score:

Final Exam, Part A. December 12, Score: Physics 152 December 12, 2005 Final Exam, Part A Roster No.: Score: Exam time limit: 2 hours. You may use a calculator and both sides of TWO sheets of notes, handwritten only. Closed book; no collaboration.

More information

PREX Background Simulation Update

PREX Background Simulation Update PREX Background Simulation Update Rakitha Beminiwattha Syracuse University rakithab@jlab.org 1 Outline PREX-II Collimator Plastic Shielding for Neutrons PREX-II Background Radiation Activation Studies

More information