Electron Beamlines Safety Workshop at ELI Beamlines April 2016

Slides:



Advertisements
Similar presentations
Fast and Precise Beam Energy Measurement at the International Linear Collider Michele Viti.
Advertisements

EAR2 simulation update Collaboration board meeting Christina Weiss & Vasilis Vlachoudis.
Collimation and tagging instrumentation for the GlueX photon beamline Richard Jones Igor Senderovich, Anne-Marie Carroll University of Connecticut APS/DNP.
FLUKA radioprotection calculations Maria – Ana Popovici Politehnica University of Bucharest.
Status of the Tagger Hall Background Simulation Simulation A. Somov, Jefferson Lab Hall-D Collaboration Meeting, University of Regina September
Radiation Physics Beam Tests J. Bauer, J. Liu, L. Nicolas, S. Rokni, M. Santana ESTB Workshop 2011 March 17, 2011.
BLM review Mario Santana Leitner OUTLOOK ON FLUKA SIMULATIONS FOR UDULATOR DAMAGE AND BLM RESPONSE Mario Santana Leitner, Alberto.
PROBLEM: Radiation Dose Rate in IR2 When IR1 is Operating (and Vice Versa) Muon Dose Rate > 1 mRem/hr for 0.1% Collimated Halo.
G2p Safety Readiness Review January 17, 2012 Expected Radiation Exposure Levels from Activated Local Dump George Kharashvili, Radiation Control.
TEST BEAMS Stanford Linear Accelerator Center Ted Fieguth DoE/SLAC Program Review April & May 1, 1997.
E. Bong, SLACLCLS FAC Meeting - April 29, 2004 Linac Overview E. Bong LCLS FAC Meeting April 29, 2004 LCLS.
BDSIM simulations/results: Synchrotron Radiation and Muons Motivation and History Tracking results Synchrotron Radiation Tracking of Halo Muons News from.
BROOKHAVEN SCIENCE ASSOCIATES Radiological Design Considerations of Synchrotron Radiation Facilities P.K. Job Radiation Physicist National Synchrotron.
Radiation Environment at AWAKE Silvia Cipiccia, Eduard Feldbaumer, Helmut Vincke.
Gamma Beam Systems a simple introduction. Purpose of the machine Deliver a high performance photon beam: Variable energy Highly polarized High intensity.
HPS Test Run Setup Takashi Maruyama SLAC Heavy Photon Search Collaboration Meeting Thomas Jefferson National Accelerator Facility, May 26-27,
Radiological Aspects of ILC Hee-Seock Lee Pohang Accelerator Laboratory 2 nd Workshop of Korean ILC at PAL.
ELI-NP: the way ahead, March Anna Ferrari An overview of the shielding problems around high energy laser-accelerated beams Anna Ferrari Institute.
FUNCTIONAL SPECIFICATION Dorothea Pfeiffer Dennis Haasler GIF++ User Meeting
Radiation Monitoring at the Undulator System Heinz-Dieter Nuhn – LCLS Undulator Group Leader Presented at Wednesday, March 7, 2012.
FNAL, May 10, Introduction for Beam Diagnostics Laboratory Main Mission: R&D on charged particle beam diagnostics for e + /e - linear colliders.
First AWAKE dump calculations Helmut Vincke. Beam on dump Muon axis inside and outside CERN Distances: Beam impact point to end of West hall: ~300 m Beam.
Possible calibration methods for the final LXe calorimeter A. Papa 01/20/2004.
The Materials Test Station: An Accelerator Driven Neutron Source for Fusion Materials Testing Eric Pitcher Presented at: Sixth US-PRC Magnetic Fusion Collaboration.
Lead Fluoride Calorimeter for Deeply Virtual Compton Scattering in Hall A Alexandre Camsonne Hall A Jefferson Laboratory October 31 st 2008.
Systematic studies of neutrons produced in the Pb/U assembly irradiated by relativistic protons and deuterons. Vladimír Wagner Nuclear physics institute.
Integrated Radiation Measurement and Radiation Protection of BES Ⅲ Zhang Qingjiang, Wu protection group, accelerator center, IHEP,
Beam test possibilities at JINR and Fermilab V. Pronskikh Fermilab 02/15/2012.
October 2005 Qweak Collaboration Meeting Detailed Design of Shield House and Collimators wrt Backgrounds Yongguang Liang Just getting started – will probably.
Nov Beam Catcher in KOPIO (H. Mikata Kaon mini worksyop1 Beam Catcher in the KOPIO experiment Hideki Morii (Kyoto Univ.) for the KOPIO.
ELECTRON MOVING AT CONSTANT VELOCITY
EAR2 Beam Line Report on the Status C. Weiss EAR2 Beam Line - Report on the Status1.
Recent Studies on ILC BDS and MERIT S. Striganov APD meeting, January 24.
Considerations for an SPL-Beamdump Thomas Otto CERN in collaboration with Elias Lebbos, Vasilis Vlachoudis (CERN) and Ekaterina Kozlova (GSI) Partly supported.
1 BROOKHAVEN SCIENCE ASSOCIATES Summary of Shielding Calculations for NSLS2 Accelerators P.K. Job Radiation Physicist Peer Review 2007 March
Status of facility design Activities of the IPNS Nuclear/Particle Physics group Basic information for the working sessions Activities of Nuclear and Particle.
Radiation Shielding Assessment for MuCool Experimental Enclosure C. Johnstone 1), I. Rakhno 2) 1) Fermi National Accelerator Laboratory, Batavia, Illinois.
M.Moll, M.Silari, H.Vincke – 3.April Mixed field irradiation -- Who answered ?  In total 36 forms filled / 34 persons answered: 38% 62% CERN:
Results From the Radphi LGD Dan Krop 12/11/03. The Radphi Experiment Radphi Experiment Took Data in Jlab Hall B From May to July Hours Of Beam.
Radiation protection and radiation safety issues for HIE-ISOLDE. FLUKA calculations Y. Romanets ISOLDE Workshop and Users meeting 2010 CERN, 8 December.
Shielding review for temporary spectrometer for RUBICON experiment, ATF beamline #2 K. Kusche, M. Fedurin RSC meeting, Jan 20, 2015.
The T506 Experiment: Electromagnetically-induced Radiation Damage to Solid-State Sensors Test Facilities Users Workshop SLAC, September Bruce Schumm.
Overview of the BNCT neutron beam line facility in NRI Rez (Prague) Most pictures taken from presentation of J.Burian/NRI – Milano09 1 NRI = Nuclear research.
Fermilab Test Beam and Irradiation Facilities Erik Ramberg 10 January, 2013.
Proton and neutron irradiation facilities in the CERN-PS East Hall Maurice Glaser and Michael Moll CERN- PH-DT2 - Geneva - Switzerland 6 th LHC Radiation.
Dark Current in ILC Main Linac N.Solyak, A.Sukhanov, I.Tropin ALCW2015, Apr.23, 2015, KEK LCWS'15, Tsukuba, 04/2015Nikolay Solyak1.
g beam test of the Liquid Xe calorimeter for the MEG experiment
Dark Current and Radiation Shielding Studies for the ILC Main Linac
A 3D design model of the apparatus for the Laser Wakefield Acceleration of electrons at ELI-NP S. Balascuta1 , R. Dinca1 1) “Horia Hulubei” National.
Measuring light elements (e. g
INDUSTRIAL HYGIENE External EHS Expert Panel Workshop
Collimation and tagging instrumentation
Conditions at a potential location of a beam dump experiment at LCLS-II Clive Field, SLAC: 4/29/16.
BUCKY Simulations of Z and RHEPP Experiments
E3 Hall layout L4f/1.5kJ/150 fs L4p/150J/150 fs – 10 ps L4n/
Revised Commissioning Strategy
Bubble Chamber Planning Meeting
Bubble Chamber – Beam Requirements
MLS (Metrology Light Source) and the Willy-Wien-Laboratory – Status Report Ralph Lange (BESSY) Titel des Kapitels: ITC Franklin Gothic LT, Bold, 11 Punkt,
Fassò, N. Nakao, H. Vincke Aug. 2, 2005
Специализированный источник синхротронного излучения Anka Характеристики и экспериментальные возможности.
Beam Dump Experiments with Photon and Electron Beams
LCLS Radiological Considerations Sayed H. Rokni, SLAC April 24, 2002
Research Activities Seminar Nuclear Physics Group
LCLS FEL Parameters Heinz-Dieter Nuhn, SLAC / SSRL April 23, 2002
T-489: Induced Activity and Residual Dose Rates
Test Beamline System Requirements and Charge to PDR Committee
Status of ELI Beamlines
Proposal for Smith-Purcell radiation experiment at SPARC_LAB
Background Simulations at Fermilab
Presentation transcript:

Electron Beamlines Safety Workshop at ELI Beamlines 11-12 April 2016 Nikhil, Gabriele, Leonel, Roberto, Anna, Alberto Safety Workshop at ELI Beamlines 11-12 April 2016

E2 - Betatron (up to 1 GeV, monochromatic or exponential spectrum) E5 - HELL (up to 10 GeV, monochromatic or flat spectrum) E5 - LUX (up to 1.2 GeV, monochromatic spectrum)

Dump Design Strategy GOAL MODULAR MATERIALS < 1 mSv/year outside experimental halls Compact, light-weight and low cost MODULAR Dump built from "bricks" of shielding materials Add/remove "bricks" if experimental parameters change MATERIALS Restrict EM cascade inside cast iron Shower absorption in concrete Moderate back scattered neutrons in polyethylene (borated if needed)

E2 - Betatron

E2 - Betatron Monochromatic (1 GeV) Exponential (40 MeV temperature) Additional magnets placed external to the experimental chamber to direct the beam on to the dump Cast iron core of the dump is 2m x 1m x 0.6m (bulky?) Exponential (40 MeV temperature) Affected by the internal magnet which disperses the beam Long concrete wall as shielding 1 GeV monochromatic DOSE RATE (mSv/year) 1 mSv/y Exponential

E5 – HELL and LUX

E5 - LUX (Laser-driven Undulator X-ray) BEAM DUMP COLLIMATOR Activation due to 500 MeV electrons on a concrete beam dump (1.2m x 1.8m x 2m) Irradiation schedule (12 times per year) 5 consecutive days with 20 hours of operation per day 25 consecutive days with 2 hours of operation per day

E5 – HELL (High-energy Electron-acceleration by Laser) User Station Spectrometer 10 GeV beam Spectrum: 0-500 MeV flat Irradiation of samples Up to 10 Hz Low noise Low radiation damage Minimize backscattering No dedicated dump Spectrum: 0-3 GeV flat 1 T x 60 cm magnetic field Electron accelerator characterization Variable charge Variable spectrum Muon production Spectrum: 10 GeV Increase of beam energy with time Goals 10 GeV, 50 GeV Variable charge Variable spectrum Muon production Biolab downstream

E5 – HELL (High-energy Electron-acceleration by Laser) User Station Spectrometer 10 GeV beam Spectrum: 0-500 MeV flat Irradiation of samples Up to 10 Hz Low noise Low radiation damage Minimize backscattering No dedicated dump Spectrum: 0-3 GeV flat 1 T x 60 cm magnetic field Electron accelerator characterization Variable charge Variable spectrum Muon production Spectrum: 10 GeV Increase of beam energy with time Goals 10 GeV, 50 GeV Variable charge Variable spectrum Muon production Biolab downstream

E5 – HELL (High-energy Electron-acceleration by Laser) User Station Spectrometer 10 GeV beam Spectrum: 0-500 MeV flat Irradiation of samples Up to 10 Hz Low noise Low radiation damage Minimize backscattering No dedicated dump Spectrum: 0-3 GeV flat 1 T x 60 cm magnetic field Electron accelerator characterization Variable charge Variable spectrum Muon production Spectrum: 10 GeV Increase of beam energy with time Goals 10 GeV, 50 GeV Variable charge Variable spectrum Muon production Biolab downstream

E5 – HELL (High-energy Electron-acceleration by Laser) User Station Spectrometer 10 GeV beam Spectrum: 0-500 MeV flat Irradiation of samples Up to 10 Hz Low noise Low radiation damage Minimize backscattering No dedicated dump Spectrum: 0-3 GeV flat 1 T x 60 cm magnetic field Electron accelerator characterization Variable charge Variable spectrum Muon production Spectrum: 10 GeV Increase of beam energy with time Goals 10 GeV, 50 GeV Variable charge Variable spectrum Muon production Biolab downstream

Thank you!