2. June 1 Verification of Monte Carlo Transport Codes FLUKA, MARS and SHIELD-A Vera Chetvertkova, E. Mustafin, I.Strasik (GSI,

Slides:



Advertisements
Similar presentations
Neutron-induced Reactions
Advertisements

? Nuclear Reactions Categorization of Nuclear Reactions
Accelerator Physics, JU, First Semester, (Saed Dababneh).
Basic Nuclear Properties
PWI Modelling Meeting – EFDA C. J. OrtizCulham, Sept. 7 th - 8 th, /8 Defect formation and evolution in W under irradiation Christophe J. Ortiz Laboratorio.
M. Mayer SEWG Fuel Retention June Sample Analysis for TS, AUG and JET: Depth Profiling of Deuterium M. Mayer Max-Planck-Institut für Plasmaphysik,
Plateforme de Calcul pour les Sciences du Vivant Lydia Maigne GATE/G4 meeting collaboration - 12/09/07 - Hebden Bridge 1 Electron.
Radiation Levels in ALICE Andreas Morsch Meeting on ALICE Radiation Tolerance 30/8/2004.
SNS Spallation Neutrino Source 1 SNS layout GeV proton linear accelerator Accumulator ring Main target Stripping foil.
Partial Products. Category 1 1 x 3-digit problems.
A proposal for a polarized 3 He ++ ion source with the EBIS ionizer for RHIC. A.Zelenski, J,Alessi, E.Beebe, A.Pikin BNL M.Farkhondeh, W.Franklin, A. Kocoloski,
Measurements of Angular and Energy Distributions of Prompt Neutron Emission from Thermal Induced Fission Vorobyev A.S., Shcherbakov O.A., Gagarski A.M.,
Short-range, high-LET recoil tracks in CR-39 plastic nuclear track detector E. R. Benton 1, C. E. Johnson 1, J. DeWitt 1, N. Yasuda 2, and E. V. Benton.
Stefan Roesler SC-RP/CERN on behalf of the CERN-SLAC RP Collaboration
P HI T S Exercise ( II ) : How to stop , ,  -rays and neutrons? Multi-Purpose Particle and Heavy Ion Transport code System title1 Feb revised.
Advanced GAmma Tracking Array
1 Activation problems S.Agosteo (1), M.Magistris (1,2), Th.Otto (2), M.Silari (2) (1) Politecnico di Milano; (2) CERN.
PIGE experience in IPPE Institute of Physics and Power Engineering, Obninsk, Russia A.F. Gurbich.
Estimation of the effects of a lead vest on dose reduction for NPP workers using Monte Carlo calculations KIM JEONG-IN.
OVERVIEW NEDA Introduction to the Simulations – Geometry The Simulations Conclusions 3.7% This work summarizes the introduction to the simulations of.
Setup for large area low-fluence irradiations with quasi-monoenergetic 0.1−5 MeV light ions M. Laitinen 1, T. Sajavaara 1, M. Santala 2 and Harry J. Whitlow.
P HI T S Advanced Lecture (II): variance reduction techniques to improve efficiency of calculation Multi-Purpose Particle and Heavy Ion Transport code.
Cross section measurements for analysis of D and T in thicker films Liqun Shi Institute of Modern Physics, Fudan University, Shanghai, , People’s.
1 Induced radioactivity in the target station and in the decay tunnel from a 4 MW proton beam S.Agosteo (1), M.Magistris (1,2), Th.Otto (2), M.Silari (2)
Workshop on Physics on Nuclei at Extremes, Tokyo Institute of Technology, Institute for Nuclear Research and Nuclear Energy Bulgarian Academy.
1 JASMIN Activation Experiments (T-972/993/994) Yoshimi Kasugai on behalf of JASMIN Activation team JASMIN Activation team Y. Kasugai, K. Oishi, H. Matsumura,
ELI-NP: the way ahead, March Anna Ferrari An overview of the shielding problems around high energy laser-accelerated beams Anna Ferrari Institute.
G. Bartesaghi, 11° ICATPP, Como, 5-9 October 2009 MONTE CARLO SIMULATIONS ON NEUTRON TRANSPORT AND ABSORBED DOSE IN TISSUE-EQUIVALENT PHANTOMS EXPOSED.
I. Strasik et al. ● Halo Collimation of Proton and Ion Beams in FAIR Synchrotron SIS 100 ● CERN Halo Collimation of Proton and Ion Beams in.
Study of Pion Capture Solenoids for PRISM H.Ohnishi AB M. Aoki C, Y. Ajima A, N. Fukasawa AD, K. Ishibashi B, Y. Kuno C, T. Miura A, K. Nakahara C, T.
Proposal for Experiment S291: " Residual radioactivity induced by U ions - experimental investigation and longtime predictions" GSI, Darmstadt: G.Fehrenbacher,
Estimation of temperature increase in the dump through Monte – Carlo simulations and rough calculations N. Charitonidis (EN/MEF)
Experimental part: Measurement the energy deposition profile for U ions with energies E=100 MeV/u - 1 GeV/u in iron and copper. Measurement the residual.
Radiation damage calculation in PHITS
Systematic studies of neutrons produced in the Pb/U assembly irradiated by relativistic protons and deuterons. Vladimír Wagner Nuclear physics institute.
Experimental and Theoretical Study of Energy Deposition and Residual Activation Induced by Uranium Ions to Model the Beam Loss Hazards in the GSI Future.
Precision analysis of Geant4 condensed transport effects on energy deposition in detectors M. Batič 1,2, G. Hoff 1,3, M. G. Pia 1 1 INFN Sezione di Genova,
Neutron production study with the thick lead target and uranium blanket irradiated by 1.5 GeV protons Filip Křížek, ÚJF AV ČR.
LAL, Orsay IDEA meeting Validation of excitation functions of 60 Co and 68 Ge production on germanium isotopes V.F. Batyaev, I.V. Kirpichnikov,
Experimental Studies of Spatial Distributions of Neutrons Produced by Set-ups with Thick Lead Target Irradiated by Relativistic Protons Vladimír Wagner.
The energy deposition profile for 238U ions with energies 500 and 950 MeV/u in iron and copper. A.A.Golubev 1, A.V.Kantsyrev 1, V.E.Luckjashin 1, A.D.Fertman.
O FF - LINE TECHNIQUE FOR DEUTERON BEAM PARAMETERS DETERMINATION USING SOLID STATE NUCLEAR TRACK DETECTORS E XPERIMENTS AT THE QUINTA TARGET (D UBNA, R.
Neutron measurement with nuclear emulsion Mitsu KIMURA 27th Feb 2013.
Neutron production in Pb/U assembly irradiated by deuterons at 1.6 and 2.52 GeV Ondřej Svoboda Nuclear Physics Institute, Academy of Sciences of Czech.
1 Neutron Effective Dose calculation behind Concrete Shielding of Charge Particle Accelerators with Energy up to 100 MeV V. E Aleinikov, L. G. Beskrovnaja,
An introduction Luisella Lari On behalf of the FLUKA collaboration CAoPAC: Computer-Aided Optimization of Particle Accelerator Workshop March 2015.
Neutron production in Pb/U assembly irradiated by 1.26 AGeV deuterons. First experimental results Ondřej Svoboda Neutron production in Pb/U assembly irradiated.
1 Activation by Medium Energy Beams V. Chetvertkova, E. Mustafin, I. Strasik (GSI, B eschleunigerphysik), L. Latysheva, N. Sobolevskiy (INR RAS), U. Ratzinger.
Neutron production and iodide transmutation studies using intensive beam of Dubna Phasotron Mitja Majerle Nuclear Physics Institute of CAS Řež, Czech republic.
Neutron double differential distributions, dose rates and specific activities from accelerator components irradiated by 50 – 400 MeV protons F. Cerutti.
Christos Lamboudis HEP April. Athens Study of MDT response to neutrons and possible ageing effects Do we really need to worry about neutrons? Do.
EURISOL, TASK#5, Bucuresti, November 1 Preliminary shielding assessment of EURISOL Post Accelerator D. Ene, D. Ridikas. B. Rapp.
Fluka Simulations: Electron spectrometer window for AWAKE Jose A. Briz and V. Vlachoudis.
VALIDATION OF THE FLUKA MONTE CARLO CODE FOR RESIDUAL PRODUCTION WITH 500 MeV/u AND 950 MeV/u URANIUM BEAM ON COPPER AND STAINLESS STEEL TARGET E. Kozlova.
Activation by Heavy-Ion Beams
INDUCED BY HEAVY-ION BEAMS IN MATTER
Nam-Suk Jung, Arim Lee, Hee-Seock Lee,
Investigation of the proton-induced reactions on natural molybdenum.
Heating and radiological
Induced-activity experiment:
at TSL high energy neutron facility
variance reduction techniques to improve efficiency of calculation A
Development and characterization of the Detectorized Phantom for research in the field of spatial fractionated radiation therapy. D. Ramazanov, V. Pugatch,
for collaboration “Energy plus transmutation”
The experiment on JINR Dubna Nuclotron
1. Introduction Secondary Heavy charged particle (fragment) production
Fragmentation cross sections of Fe26+, Si14+ and C6+ ions of 0
Performed experiments Nuclotron – set up ENERGY PLUS TRANSMUTATION
Neutron production in Pb/U assembly irradiated by p+, d+ at 0. 7 – 2
Estimation of the effects of a lead vest on dose reduction for NPP workers using Monte Carlo calculations KIM JEONG-IN.
Presentation transcript:

2. June 1 Verification of Monte Carlo Transport Codes FLUKA, MARS and SHIELD-A Vera Chetvertkova, E. Mustafin, I.Strasik (GSI, Germany) L.Latysheva, N. Sobolevskiy (INR RAS, Russia)

2. June 2 Content 1. Introduction 2. Verification of electronic stopping modules Experiment Simulations 3. Verification of isotope production modules Experiment Simulations 4. Discussion 5. Summary 6. Conclusion

2. June 3 1. Introduction Monte Carlo codes -used in estimation of radiation hazards in accelerator facilities -are being constantly developed Verification of the codes is needed Project 'Verification of MC transport codes FLUKA, MARS and SHIELD-A' -Verification of electronic stopping modules -Verification of isotope production modules

2. June 4 2. Verification of electronic stopping modules:Experiment A.A. Golubev, E. Mustafin et al, Measurement of the energy deposition profile for 238 U ions with specific energy 500 and 950 MeV/u in stainless steel and copper targets, NIM B 263 (2007) 339–344 The idea: measuring energy deposition function and stopping range using the thick target technique

2. June 5 2. Verification of electronic stopping modules:Simulations 1. Energy deposition function [GeV/mm] + range [mm] Target material equivalent thickness Stainless steel: 262 µm Copper: 235 µm Range, mm E = 500 MeV/uE = 950 MeV/u St. steelCuSt. steelCu Measurement 6.0 ± ± ± ± 0.4 ATIMA PHITS SHIELD SRIM

2. June 6 2. Verification of electronic stopping modules:Simulations 500 MeV/u U beam Stainless steel target Copper target 950 MeV/u U beam

2. June 7 2. Verification of electronic stopping modules:Simulations Measured and calculated penetration depths of 238 U ions in copper and stainless steel targets Penetration depth, mm E = 500 MeV/uE = 950 MeV/u St. steelCuSt. steelCu Measurement 5.7 ± ± ± ± 0.4 SHIELD-A MARS FLUKA

2. June 8 3. Verification of isotope production modules:Experiment Scheme of the experiment Irradiation: 500 MeV/u argon beam Measurements: HPGe detector, 20% efficiency, Energy range: 30keV – 2 MeV Energy resolution at 122 keV – 0.9 keV; at 1.33 MeV – 1.9 keV

2. June 9 3. Verification of isotope production modules:Experiment Cylinder assembled from discs Isotope distribution Depth profiles of activation 1.Simulations of the interaction of certain ions with chosen target =>Finding the stopping range 2.Assembling the target 3.Irradiation 4.Measurements of the residual activity => experimental study of the depth profiles of activity Activation foils

2. June 10 Activation of the aluminum target

2. June Verification of isotope production modules:Simulations Depth profiles of the isotopes activated by argon beam of 500 MeV/u in aluminum target Depth profiles of 7 Be Depth profiles of 22 Na

2. June Discussion How could the discrepancies be explained? ?Differences in cross sections ?Different number of simulated secondary particles ?Different models of nuclear interactions ????

2. June Summary Experiments for finding energy deposition function of uranium ions in copper and stainless steel were held, respective simulations were done Activation of aluminum by argon ions was studied, depth profiles were analyzed and respective simulations were performed

2. June Conclusion MARS and SHIELD-A – the stopping range of U ions (500 MeV/u; 1 GeV/u) in copper and stainless steel was consistent with the experimental results within the error bars – depth profiles of activity induced by argon beam (500 MeV/u) in aluminum target were different either in shape or absolute values (25%÷100% discrepancies) FLUKA –depth profiles of activity induced by argon beam in aluminum target were consistent with the experimental ones within the error bars –the stopping range of the uranium ions was overestimated by 5% for 500 MeV/u and 10% for 950 MeV/u beam