Radiation Safety issues for the PF-AR in KEK

Similar documents
Radiation Safety issues for the PF-AR in KEK

Injection with front ends open at the ESRF

Minimizing radiation and beam losses at the ESRF

SYNCHROTRON RADIATION ABSORPTION AND VACUUM ISSUES IN THE IR*

NON-DESTRUCTIVE 2-D BEAM PROFILE MONITOR USING GAS SHEET IN J-PARC LINAC -overview & hardware construction-

Performance Requirements for Monitoring Pulsed, Mixed Radiation Fields Around High-Energy Accelerators

Vacuum Quality Assurance in Practice

BESSY ventilation concept

Change History Log. Rev Revision Sections Affected Description of Change /22/08 All Initial Version

Beam Loss Position Monitoring with Optical Fibres at DELTA

ARCON/RAMSES: Current Status and Operational Risk

Goals Understand Responsibilities, Awareness, Communication. Beamline phases Design, Implementation, Commissioning, Operation

VACUUM PERFORMANCE IN THE MOST RECENT THIRD GENERATION SYNCHROTRON LIGHT SOURCES

Competency: Critically evaluate the function of the ionisation chamber in the Linear Accelerator and its importance for correct treatment delivery

Status of the PRad Experiment (E )

Today s Outline - September 12, C. Segre (IIT) PHYS Fall 2016 September 12, / 21

LCLS Instruments. Jerry Hastings June 20, 2008 LCLS

HiRadMat facility at the CERN SPS

Experimental Particle Physics PHYS6011 Joel Goldstein, RAL

NUCLEAR INDUSTRY STANDARD PROCESS Radiological Protection. Level 3 Information Use

Radiation Safety Systems

The LHCb Outer Tracker: Production & Ageing studies

Portable Survey Instruments NISP-RP-01

Safety introduction for users

Radiation Safety Systems

Vacuum requirements and Beamline interface at the VUV-FEL User Facility

THE REPUBLIC OF UGANDA ATOMIC ENERGY ACT, 2008 SCHEDULE 1 FORM 2A

The Modular System for Radioactivity Measurements FH 40 G/GL FHT 6020

The Modular System for Radioactivity Measurements FH 40 G/GL FHT 6020

LCLS DIRECTORATE Experimental Facilities Division

Aging Analysis of Micromegas Detectors for ATLAS New Small Wheel

IBL 637 Cesium-137γ-ray machine 2016

PART V: WORKING WITH LASERS

Approved by Principal Investigator: Date: Approved by Laser Safety Officer: Date:

Particle Accelerators - Their Hazards and the Perception of Safety

Applying Layer of Protection Analysis (LOPA) to Accelerator Safety Systems Design. Feng Tao

Physics Requirements for the CXI Detector Stage

Turnkey Solutions for Radiation Protection in PET Laboratories R A D I A T I O N P R O T E C T I O N

25 TEXAS ADMINISTRATIVE CODE Radiation Safety Requirements for Analytical and Other Industrial Radiation Machines

Table of Contents. Check the LCLS Project website to verify 2 of 12 that this is the correct version prior to use.

Solid State Detectors. T. Bowcock

ALPHA Radiation Safety Manual

Machine-Detector Interface

Radiation Control and Monitoring System on the HTTR

PROFILER Family IC PROFILER, IC PROFILER - MR & SRS PROFILER. Your Most Valuable QA and Dosimetry Tools

Ionisation Chambers Containing Boron as Neutron Detectors in Mixed Radiation Fields

Identify the following features and specifications for the ESP1

Engineered and Administrative Safety Systems for the Control of Prompt Radiation Hazards at Accelerator Facilities

Doc. No. SP R0. CXI Reference Laser. Prepared by: Jean-Charles Castagna Signature Date Design Engineer

Monitoring of Radiation Exposure Adjacent to a Linear Accelerator Treatment Bunker with a Highlight Window

ISIS Design Division Electrical Engineering. S Birch. September 2012.

G155PU001S. Pigtailed 14-PIN DIL Laser Diode with TEC. FLMS Min. Typ. Max.

HEALTH AND SAFETY MANUAL

MD456: Monitoring of abort gap population with diamond particle detectors at the BGI in IP 4

A CONCEPT FOR CANCELLING THE LEAKAGE FIELD INSIDE THE STORED BEAM CHAMBER OF A SEPTUM MAGNET*

Special Aspects in Designing High - Frequency Betatron

Gaseous detectors. 1

PORTABLE ISOTOPE IDENTIFIER Search Tool / Sample Counting System

I Seminario Nazionale Rivelatori Innovativi

Lessons Learned Events at SLAC. Mike Woods, SLAC National Accelerator Laboratory

Maximize safety and productivity. Thermo Scientific Nuclear Power Radiation Detection and Monitoring Solutions

Abstract. 1 NSRRC, 101 Hsin-Ann Road, Hsinchu 300, Taiwan 2 Dept. of Biomedical Engineering & Environmental Sciences, NTHU, Hsinchu 300, Taiwan

Laboratory Impex Systems Ltd

Radiation Safety for AREAL Phase 1

Status Report about the TPC Detector and Module at CEPC

The use of NEG pumps and coatings in large vacuum systems: experience and limitations

DISCONTINUED PRODUCT. For reference only SMOKE DETECTOR WITH INTERCONNECT FEATURES. ABSOLUTE MAXIMUM RATINGS (Voltages are referenced to V SS

dewar or an electrically powered cooler. The sensitive detector surfaces are thus protected from moisture and condensable contaminants.

AIR or STACK MONITOR NOBLE GAS, GROSS BETA-GAMMA PARTICULATE, & IODINE. Optional Alpha, Tritium, Carbon-14

Local Rules for the Use of the Raman Spectroscopy Lab

Battery-operated, hand-held alarm and measuring instruments for radiation protection

APES- Environmental Effects of Radiation Laboratory Activity. Purpose: To see the effect of the seed irradiation on germination and plant growth

Laser Standard Operating Procedure

Plant Performance 2017 User Symposium

ESTB Proposal from the Stony Brook University: Test of a RICH-Prototype Based on CsI-GEMs

DART-Thermo LTQ/Orbitrap Interface Manual

Customized MCPs for Analytical Instruments. An MCP for every application

WG Container & Cargo X-Ray Scanning Portal

EU Diagnostics: Recent progress & near-term opportunities. Frederic Le Guern on behalf of Glenn F. Counsell Programme Manager. 18 th September 2018

The system can be easily relocated by a standard container truck., and re-commissioned by trained engineers typically within a 72-hour period

Commissioning of the ASTA Photoinjector Laser System

WG Entire Truck & Cargo X-Ray Scanning Portal

NEXT GENERATION DRINKING WATER RADIATION SAFETY MONITOR

X-ray Inspection System Discover What You've Been Missing... DETECTION PERFECTION

Micromegas detectors for the upgrade of the ATLAS Muon Spectrometer

Document Preparation Profile (DPP)

Heavy Ion Beam Characteristics of ICCHIBAN 7 and 8 Experiments and Brief Summary of the ICCHIBAN Experiments

IntegraTorr Sputtered Non-Evaporable Getter. We support your innovation

Gas System for GIF in EHN1

Active Scanning Beam 2: Controlling Delivery

Maximizing safety and productivity. Nuclear Power Radiation Detection and Monitoring Solutions

Technical Description. Ionisation Chambers

COMPANY PROFILE. DETECTION & MEASUREMENT OF IONIZING RADIATIONS RADIOLOGICAL MONITORING SYSTEMS HEALTH AND ENVIRONMENTAL SAFETY

Fireye FLAME SCANNERS

Development of a new X-ray source system using ultraviolet laser for medical treatment

Dynamic Radon Detection Over Measurement

Radiation Protection Instructions

Instrument Standards Used in Security Applications Presented by: Leticia Pibida, Ph.D.

Analytical X-Ray Safety Program

NEX-BETA-ABG FACILITY Drinking Water Safety Monitor

Transcription:

Radiation Safety issues for the PF-AR in KEK H. Nakamura, Y. Namito, K. Iijima,K. Takahashi and S. Ban High Energy Accelerator Research Organization (KEK)

Contents Present status of KEK Management of radiation for PF-AR Radiation measurements Protection Result

KEK electron accelerators KEK Tsukuba site PF-AR 3km Synchrotron light sources PF-AR(PF Advanced Ring for pulse X ray) 6.5 GeV electron for pulse X ray Photon Factory (PF) 2.5 GeV electron. PF 1km

KEK electron accelerators B-Factory (KEKB) To investigate b-meson symmetry 8 GeV electron in HER 3.5 GeV positron in LER Continuous injection

KEK electron accelerators Electron and positron LINAC 8 GeV/2.5 GeV e-, 3.5 GeV e+ typical Maximum allowable 10GeV (e-), 12.5 GeV µa 5GeV (e+), 6.25GeV µa Provide electron 3 rings Provide positron 1 ring

Simultaneous injection for 3 rings PF 2.5GeV e-, LER 3.5GeV e+, HER 8GeV e- Pulse to pulse switching injection has started since 24 th April 2009.( PF 0.5 Hz, HER 12.5 Hz, LER 25 Hz) The 3 rings can keep constant current except during PF-AR injection. This is a test operation. However it works well. PF-AR injection

Plane figure of PF-AR North West Lab. North Lab. North East Lab.

Plane figure of experimental hall This line will be constructed in 2009

Main parameter of the PF-AR Beam energy Circumference Injection energy 6.5 GeV 377 m 3.0 GeV Typical num. of bunches 1 Initial stored current Beam lifetime (at init.cur.) 60 ma 20 hours Num. of insertion devices 6

Management of radiation safety Dose rate in the radiation controlled area: 20μSv/h Personal effective dose limit for the radiation workers: 20 msv/year for men, 6 msv/year for women Target of personal effective dose: 7mSv/year for men, 2mSv/year for women

Measurement of dose rate in the experimental hall Dose rates are measured by the area monitors. (We call them ORG monitors.) Gamma monitors: Ionization chamber ;10 liters Neutron monitors: BF 3 proportional counter; 1 inches The monitors give an alarm when the dose rate is over 20μSv/h.

Area monitor Neutron monitor Gamma monitor

Location of the area monitors (at present) ORG0508 ORG0507 ORG0503 ORG0510 ORG0509 ORG0506 ORG0502 ORG0501

Measured dose rate in the experimental hall Usual dose rate Background level Dose rate over the background level occurred when the beam lifetime decreased. Next slide shows example of this phenomenon occurred at the beam line NW12. Dose rate (μsv/h) 0.16 0.14 0.12 0.1 0.08 0.06 0.04 0.02 0 Dose rate measured by ORG0509 0:00 4:00 8:00 12:00 16:00 20:00 Time Neutron Gamma 24:00

NW12 beam line

Sudden drop of the beam lifetime and increase of dose rate Current Lifetime 500min 100min 1.8 1.6 1.4 Dose rate (μsv/h) 1.2 1 0.8 0.6 0.4 0.2 0 10:00 11:00 12:00 13:00 14:00 15:00 Time Neutron Gamma ORG0509

Positions of beam line NW12 and monitor ORG509 Radiation source was the upper of NW12. Maximum dose rate at ORG509 was 1.6μSv/h. ORG509 was at long distance from the radiation source. We tried to measure near the beam line. ORG0510 ORG0509 ORG0

Radiation measurements around the beam line NW12 ORG0509 Unit: μsv/h 6 12 230 14 Date: 10/5/2005 13:20 Detector: Ion chamber Operation: stored current 52.5mA lifetime 186minutes

Beam lifetime and dose rate at ORG0509 during the measurement 1.8 1.6 1.4 Dose rate (μsv/h) 1.2 1 0.8 0.6 0.4 0.2 0 13:20 13:30 13:40 13:50 14:00 14:10 14:20 Time Neutron Gamma ORG0509

Condition of the incident Changing the gap of NW14 insertion device narrowly often triggered the incident. The vacuum level was worse. The beam lifetime decreased. The dose rate around the beam line increased. NOT around other beam line. The dose rate returned to B.G. when the main beam shutter (MBS) was closed.

The first things what we did for safety We set up the area where people were not allowed to enter. We changed temporarily the alarm level of the monitors. (20μSv/h 1μSv/h)

Study The beam orbit was newly arranged for installing new beam line NW14. So it was suspected for the reason. However old beam orbit did not change the situation. Measurement of residual radiation from the beam duct of the ring showed the duct near the steering magnet of NW12 was activated. This phenomenon is considered bremsstrahlung due to dust trapping near the duct. Checking the log of the monitors showed similar incidents were occurred before. (not so often)

Protection Lead blocks were installed in the optic hutch of the beam line. An ionization chamber for interlock was installed out of the optic hutch. It closes MBS when the dose rate exceeds 5μSv/h and continues for 3 minutes. The area monitor was replaced to detect radiation effectively later.

Shield in the main hatch Lead

Ion chamber for interlock and replaced ORG0509 ORG0 ORG0509 ORG0510 Ion chamber ORG0509 is not seen in this picture. It replaced later.

Result The frequency of the incident around NW12 decreased. Other beam line (ex. NE3) had the incident also, but not so often. One of sources of the dust is considered distributed ion pump (DIP).The frequency of the incident has decreased since DIP- OFF operation started. More study is needed.