NA2: Thin actinide targets optimized for high intensity beams Purpose: Optimize the high power capability and durability of thin actinide targets (“thin”

Slides:



Advertisements
Similar presentations
Report from: the High Intensity Stable Beam Working Group HISB-WG Marie-Helene Moscatello (GANIL) Annamaria Porcellato (Legnaro) Uli Ratzinger (GSI) Faical.
Advertisements

Perspectives of Croatian experimental nuclear physics Neven Soić Division of experimental physics Ruđer Bošković Institute NuPECC meeting 13. Jun 2008.
Expected counting rates. FRS experimental setup Total load is limited by SC1 and MUSIC1.
The fission of a heavy fissile nucleus ( A, Z ) is the splitting of this nucleus into 2 fragments, called primary fragments A’ 1 and A’ 2. They are excited.
Development of novel Silicon detectors for next generation nuclear physics experiments (SIDET) O. Kiselev University of Mainz JRA21/JRA22.
Contributions to Nuclear Data by Radiochemistry Division, BARC
1 Andreas Görgen EURISOL – EURONS Town Meeting, Helsinki,
Nuclear Physics Atomic Physics Chemistry Theoretical Physics Theoretical Chemistry ShERN Superheavy Element Research Network.
The need for cross section measurements for neutron- induced reactions If no cross section measurement exists, alternative strategies are: The cross section.
Accelerator technique FYSN 430 Fall Syllabus Task: determine all possible parameters for a new accelerator project Known: Scope of physics done.
FETS-HIPSTER (Front End Test Stand – High Intensity Proton Source for Testing Effects of Radiation) Proposal for a new high-intensity proton irradiation.
Radiation Detection and Measurement, JU, 1st Semester, (Saed Dababneh). 1 Radiation Sources Heavy nuclei are unstable against spontaneous emission.
Martin Freer Materials Irradiation at University of Birmingham.
NEEP 541 Radiation Interactions Fall 2003 Jake Blanchard.
A facility for Nuclear, Atomic, Material and Radiobiology Sciences. Delivering stable (from C to U) and radioactive ions (from He to Xe) in the energy.
Heavy Element Research at Dubna (current status and future trends) Yuri Oganessian Flerov Laboratory of Nuclear Reactions Joint Institute for Nuclear Research.
Nuclear Energy Options and Project-X Shekhar Mishra Fermilab Yousry Gohar ANL June 7 th 2010.
G. Bartesaghi, 11° ICATPP, Como, 5-9 October 2009 MONTE CARLO SIMULATIONS ON NEUTRON TRANSPORT AND ABSORBED DOSE IN TISSUE-EQUIVALENT PHANTOMS EXPOSED.
Ion Beam Analysis Dolly Langa Physics Department, University of Pretoria, South Africa Blane Lomberg Physics Department, University of the Western Cape,
Simulating fusion neutron damage using protons in ODS steels Jack Haley.
Interactions of Neutrons
CERN NuPAC meeting Dec 2005 The future of ISOLDE: accelerated radioactive beams Peter Butler 1.HIE-ISOLDE 2.EURISOL.
Simulations of Accelerator Driven Systems (ADS) Aleksander Polanski Joint Institute for Nuclear Research, Dubna, Russia. The Andrzej Soltan Institute for.
Radiation Test Facilities G. Spiezia. Engineering Department ENEN Radiation tests facilities  Radiation test in the accelerator sector  External facilities.
Facilities at the Nuclear Physics Institute Academy of Sciences of the Czech Rep., Řež.
If the Coordinates system is. R r b (impact parameter.
abrasion ablation  σ f [cm 2 ] for projectile fragmentation + fission  luminosity [atoms cm -2 s -1 ]  70% transmission SIS – FRS  ε trans transmission.
Duncan Weathers Department of Physics University of North Texas.
Proposal for uranium micro-beam linac at the APS for reactor fuel and structural materials studies 1 MeV/u heavy ions up to uranium includes “fission fragments”
VIEW on RAD HARDNESS TESTS of STS FEE IN MEPHI. Simakov A.B. – Head of “Special Microelectronics” Lab.
1 Beam and Target Issues Chris Booth 5 th May 2004.
European Isotope Separation On-Line Radioactive Nuclear Beam Facility A preliminary design study of the next- generation European ISOL RNB facility GANIL,
Applications of Demokritos TANDEM Accelerator in Fusion Technology Research TANDEM Lab I.N.P.P M. Andrianis S. Harisopoulos A. Lagoyianis G. Provatas National.
Experimental and Theoretical Study of Energy Deposition and Residual Activation Induced by Uranium Ions to Model the Beam Loss Hazards in the GSI Future.
Nuclear Astrophysics ARUNA Workshop, Notre Dame, IN Carl R. Brune Ohio University, Athens Ohio June 12-13, 2014.
1 Cost Room Availability Passive Shielding Detector spheres for accelerators Radiation Detection and Measurement, JU, First Semester, (Saed Dababneh).
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.
SECONDARY-BEAM PRODUCTION: PROTONS VERSUS HEAVY IONS A. Kelić, S. Lukić, M. V. Ricciardi, K.-H. Schmidt GSI, Darmstadt, Germany  Present knowledge on.
Energy recovery linacs for commercial radioisotope production A. Sy, G. Krafft, V. S. Morozov, R. P. Johnson, T. Roberts, C. Boulware, J. Hollister May.
June , RD50 Workshop1 Jan B o hm, Jan Brož, Zdeněk Doležal, Peter Kodyš, Petr Kubík, Marcela Mikeštíková Neutron irradiation program in Prague Charles.
Antonio C.C. Villari - GANILMoriond-2003 Radioactive beam research notches up 50 years Otto Kofoed-Hansen and Karl Ove Nielsen were the authors of NBI's.
1 Activation by Medium Energy Beams V. Chetvertkova, E. Mustafin, I. Strasik (GSI, B eschleunigerphysik), L. Latysheva, N. Sobolevskiy (INR RAS), U. Ratzinger.
The 14 MeV Frascati Neutron Generator (FNG)
Measurement of the 240 Pu(n,f) reaction cross-section at the CERN n_TOF facility EAR-2 47 th Meeting of the INTC CERN, June 25, 2014 A. Tsinganis 1, N.
HEBT Design Considerations Jingyu Tang, Xiangqi Wang, Hao Hao, Jiajia Tian IHEP, USTC International Review Meeting on Accelerator Physics Design of C-ADS,
Overview of Tandem Accelerator Facility and related R&D Work at NCP Ishaq Ahmad
Joint LIA COLL-AGAIN, COPIGAL and POLITA workshop Catania, April 2016 Outline - Motivations - Description - Experiments The Neutrons for Science.
Seite 1 Coordination of European efforts to exploit up-to-date neutron beam technology novel research on advanced concepts for nuclear fission reactors.
High Energy Neutron and Proton Irradiation Facilities at TSL Alexander Prokofiev, , 6th LHC Radiation Workshop 1.
12 C fragmentation measurements for hadrontherapy applications Introduction Status French program Japanese-French collaboration.
STATUS REPORT ON THE “MASHA” SET-UP A.M.Rodin, A.V.Belozerov, S.N.Dmitriev, Yu.Ts.Oganessian, R.N.Sagaidak, V.S.Salamatin, S.V.Stepantsov, D.V.Vanin PAC.
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.
MSc-Student Activities at Institut Laue-Langevin
Lecture at the MEDICIS-PROMED Summer School
Discussions on preparations for future (joint) research projects
Measuring light elements (e. g
Coatings for neutron conversion for n_TOF
“hot spots” SIS100 internal beam dump Super-FRS production target
for the EURISOL Steering Committee
for the LNL-Ganil collaboration
Cross-section Measurements of (n,xn) Threshold Reactions
Solving CARIBU Open Source Contamination Problems
Presentation of the transverse thematic Nuclear Energy
Susan Hogle, Julie G. Ezold
Ming Tang, Los Alamos National Laboratory, USA Eric R. Vance,
Prototype Diamond-like Carbon (DLC) Stripper Foils for NPAs
JOINT INSTITUTE FOR NUCLEAR RESEARCH
The need for cross section measurements for neutron-induced reactions
Uppsala University Goals, Visions and Novelties - Research - Education.
Scientific collaboration: 50 physicists, 15 laboratories
Presentation transcript:

NA2: Thin actinide targets optimized for high intensity beams Purpose: Optimize the high power capability and durability of thin actinide targets (“thin” means 0.1 to few mg/cm 2, i.e. not ISOL targets) for neutron and charged-particle induced reactions. Benefits: Extended target lifetimes and increased primary/secondary beam intensities at existing European user facilities Organisation: Coordinated production and test of fissile and non-fissile actinide targets under reproducible conditions. Comparison of different target preparation techniques, backings and covers. Training activities: Workshop on thin actinide targets. Permanent link between target producers and target users. Hands-on experience for students and postdocs.

NA2 Participant Institutions 1. Institut Laue Langevin & LPSC Grenoble, F target production by electrolysis, electrodeposition and painting on-line target tests under intense neutron flux to measure temperature, fission product intensity and energy distribution 2. IRMM Geel, B target production by spray-painting, electrodeposition (and evaporation) 3. LMU Munich, D target production by evaporation (and sputtering) 4. IPN Orsay, F target production by electrodeposition, spray painting target characterization by RBS, alpha, gamma spectroscopy future: CACAO project: joint CNRS-IN2P3/CEA hot lab 5. GANIL Caen, F heavy ion irradiation for validation of dpa-lifetime-relation Target production in collaboration with Nuclear Chemistry Institute Mainz, LBL Berkeley and Radium Institute St. Peterburg. Open to other collaborators.

RBS cartography (1.5 mm step) 235 U target NA2: Actinide target production and characterization LMU IPNO IRMM

target thickness monitored on-line via width of fission product energy distribution target temperature distribution monitored by pyrometer and IR camera longterm studies (several weeks) possible NA2: On-line test of high power actinide targets  Additional losses due to: sputtering by fission products evaporation (e.g. for UF 4 ) diffusion into backing or cover loss of adhesion to backing Burnup of 235 U target in 5.5E14 n/cm 2 /s neutron flux n/cm 2 /s ≈ 88 p  A/cm 2 comparison to accelerator beams: simulate at LOHENGRIN long exposition to intense HI beams

NA2: Synergies with other NA or JRA “survival training” for actinide targets at ILL: very high neutron flux: 5.5E14 n/cm 2 /s nuclear heating up to ca °C extremely high radiation damage: ca. 50 dpa/day, equivalent to damage by 3  A/cm 2 340MeV 48 Ca beam on 238 U target, i.e. 100 times more intense than present accelerator beams We identified overlap/possible synergies with the following other LoIs: ShERN (NA12) ECOS (NA4 or JRA11) ISOL-AT (JRA1) We are ready to merge our LoI and contribute with our capabilities to any of these. We leave the decision to the EURONS2-proposal management team to select the best option for fitting it into the overall EURONS2 proposal.

mass-separated fission fragments, up to 10 5 per second, T 1/2 ≥ microsec. The LOHENGRIN fission fragment separator flux 5.5·10 14 n./cm 2 /s few mg fission target (0.1-1 mg/cm 2, few cm 2 ) several fissions/s