Itacil C. Gomes I.C.Gomes Consulting & Investment inc. Project X Forum on Spallation Sources for Particle Physics March 19-20, 2012 Fermi National Accelerator.

Slides:



Advertisements
Similar presentations
Yoro TALL Santiago de Compostela (Spain) June 7 – 10, Second IP EUROTRANS Internal Training Course on Nuclear Data for Transmutation: status, needs.
Advertisements

Calculation of radiation produced by dark current in the Cornell ERL Lisa Nash, University of North Carolina at Chapel Hill Advisor: Val Kostroun.
Particle Production of a Carbon/Mercury Target System for the Intensity Frontier X. Ding, UCLA H.G. Kirk, BNL K.T. McDonald, Princeton Univ MAP Spring.
Pion yield studies for proton drive beams of 2-8 GeV kinetic energy for stopped muon and low-energy muon decay experiments Sergei Striganov Fermilab Workshop.
Neutral Particles. Neutrons Neutrons are like neutral protons. –Mass is 1% larger –Interacts strongly Neutral charge complicates detection Neutron lifetime.
SPES -Thin target calculations: isotope production and power deposition (ENEA-INFN Legnaro) Carlo Petrovich (ENEA, Bologna) INFN – Legnaro, 24 th January.
FETS-HIPSTER (Front End Test Stand – High Intensity Proton Source for Testing Effects of Radiation) Proposal for a new high-intensity proton irradiation.
Measurements of cross-sections of neutron threshold reactions and their usage in high energy neutron measurements Ondřej Svoboda Nuclear Physics Institute,
Studies of ADS by means of JINR Nuclotron Martin Suchopár Nuclear Physics Institute, Academy of Sciences of the Czech Republic Department of Nuclear Reactors,
High-Power Density Target Design and Analyses for Accelerator Production of Isotopes W. David Pointer Argonne National Laboratory Nuclear Engineering Division.
Nuclear Energy Options and Project-X Shekhar Mishra Fermilab Yousry Gohar ANL June 7 th 2010.
Study of a new high power spallation target concept
Future usage of quasi-infinite depleted uranium target (BURAN) for benchmark studies Pavel Tichý Future usage of quasi-infinite depleted uranium target.
Isotope R&D Facility A proposed addition to the HRIBF driver upgrade Mike Saltmarsh HRIBF Users’ Meeting Nov 13 th 2009.
1 Dr. Sandro Sandri (President of Italian Association of Radiation Protection, AIRP) Head, Radiation Protection Laboratory, IRP FUAC Frascati ENEA – Radiation.
European Physical Society 19 th Nuclear Physics Divisional Conference New Trends in Nuclear Physics Applications and Technology Pavia (Italy) September.
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.
If the Coordinates system is. R r b (impact parameter.
Proposal for Experiment S291: " Residual radioactivity induced by U ions - experimental investigation and longtime predictions" GSI, Darmstadt: G.Fehrenbacher,
Experimental studies of spatial distribution of neutron production around thick lead target irradiated by 0.9 GeV protons Antonín Krása&Vladimír Wagner.
Simulations on “Energy plus Transmutation” setup, 1.5 GeV Mitja Majerle
Modeling Production, Interactions and Transport Fermilab November 14, 2005 Fermilab ILC-CAL Nikolai Mokhov, Fermilab.
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.
Monte Carlo methods in ADS experiments Study for state exam 2008 Mitja Majerle “Phasotron” and “Energy Plus Transmutation” setups (schematic drawings)
Systematic studies of neutrons produced in the Pb/U assembly irradiated by relativistic protons and deuterons. Vladimír Wagner Nuclear physics institute.
PSB dump: proposal of a new design EN – STI technical meeting on Booster dumps Friday 11 May 2012 BE Auditorium Prevessin Alba SARRIÓ MARTÍNEZ.
Francis H. Burr Proton Therapy Center Massachusetts General Hospital December 2005 CRONUS Annual Meeting Irradiations at LANSCE May 2 – Flight.
Cross-sections of Neutron Threshold Reactions Studied by Activation Method Nuclear Physics Institute, Academy of Sciences of Czech Republic Department.
August 7, 2003K. Chow, LHC Luminosity Detector Thermal Analysis1 Analysis cases Approach: Start simple to get information— with speed with confidence that.
Neutron production study with the thick lead target and uranium blanket irradiated by 1.5 GeV protons Filip Křížek, ÚJF AV ČR.
Applications of Monte Carlo Code for a Gamma Resonance System Analysis L. Wielopolski, A. Hanson, I. Dioszegi, M. Todosow, Brookhaven National Laboratory,
Experimental Studies of Spatial Distributions of Neutrons Produced by Set-ups with Thick Lead Target Irradiated by Relativistic Protons Vladimír Wagner.
Solid Targets for Neutron Spallation Sources Eric Pitcher Los Alamos National Laboratory Presented to: AHIPA Workshop October 20, 2009.
Ondřej Svoboda Nuclear Physics Institute, Academy of Sciences of Czech Republic Department of Nuclear Reactors, Faculty of Nuclear Sciences and Physical.
A. Zelenski a, G. Atoian a *, A. Bogdanov b, D.Raparia a, M.Runtso b, D. Steski a, V. Zajic a a Brookhaven National Laboratory, Upton, NY, 11973, USA b.
Jet Fuel Vaporization and Condensation: Modeling and Validation Robert Ochs and C.E. Polymeropoulos Rutgers, The State University of New Jersey International.
Experimental and Theoretical Study of Energy Deposition and Residual Activation Induced by Uranium Ions to Model the Beam Loss Hazards in the GSI Future.
EURISOL – Task 11 meeting 2007S. Chabod 1 OUR CONTRIBUTION INSIDE EURISOL TASK 11 OPTIMIZATION OF IN-TARGET NUCLEI YIELDS Target parameters: material (Al.
Investigating the Feasibility of a Small Scale Transmuter – Part II Roger Sit NCHPS Meeting March 4-5, 2010.
Ondřej Svoboda Nuclear Physics Institute, Academy of Sciences of Czech Republic Department of Nuclear Reactors, Faculty of Nuclear Sciences and Physical.
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.
Update on radiation estimates for the CLIC Main and Drive beams Sophie Mallows, Thomas Otto CLIC OMPWG.
Pion-Induced Fission- A Review Zafar Yasin Pakistan Institute of Engineering and Applied Sciences (PIEAS) Islamabad, Pakistan.
Simulations on “Energy plus Transmutation” setup, 1.5 GeV Mitja Majerle, V Wagner, A Krása, F Křížek This document can be downloaded.
Neutron production in Pb/U assembly irradiated by 1.26 AGeV deuterons. First experimental results Ondřej Svoboda Neutron production in Pb/U assembly irradiated.
Summary of radiation shielding studies for MTA Muon production at the MiniBooNE target Igor Rakhno August 24, 2006.
Validation of Geant4 Bertini cascade nuclide production Aatos Heikkinen Helsinki Institute of Physics FrontierScience, Milano, September 12-17, 2005.
1 BROOKHAVEN SCIENCE ASSOCIATES NSLS-II Shielding Workshop R. Casey Activation Issues for NSLS-II March 28, 2007.
Simulation of heat load at JHF decay pipe and beam dump KEK Yoshinari Hayato.
Systematical Analysis of Fast Neutron Induced Alpha Particle Emission Reaction Cross Sections Jigmeddorj Badamsambuu, Nuclear Research Center, National.
Present status of production target and Room design Takashi Hashimoto, IBS/RISP 2015, February.
ADS Activities at Argonne National Laboratory Yousry Gohar Argonne National Laboratory Proton Accelerators for Science and Innovation Workshop FERMILAB,
Alternative Methods for Production of Ac225 James Harvey 1, Jerry A. Nolen 3, Thomas Kroc 4, Itacil Gomes 5, E. Philip. Horwitz 2, Daniel R. McAlister.
Neutron production and iodide transmutation studies using intensive beam of Dubna Phasotron Mitja Majerle Nuclear Physics Institute of CAS Řež, Czech republic.
Ali Ahmad FLUKA code validation of nuclear data required for the spallation target design in Accelerator Driven Subcritical Reactors ThorEA Meeting – Daresbury.
Transmutation of 129 I with high energy neutrons produced in spallation reactions induced by protons in massive target V.HENZL Nuclear Physics Institute.
EURISOL, TASK#5, Bucuresti, November 1 Preliminary shielding assessment of EURISOL Post Accelerator D. Ene, D. Ridikas. B. Rapp.
Monte Carlo methods in spallation experiments Defense of the phD thesis Mitja Majerle “Phasotron” and “Energy Plus Transmutation” setups (schematic drawings)
Investigation of the proton-induced reactions on natural molybdenum.
The BLAIRR Irradiation Facility Hybrid Spallation Target Optimization
Inter-comparison of Particle production (2)
Transmutation of 129I with high energy neutrons produced in spallation reactions induced by protons in massive target V. HENZL1,*, D. HENZLOVA1, A. KUGLER1,
GAMOS tutorial Shielding Exercises
for collaboration “Energy plus transmutation”
Susan Hogle, Julie G. Ezold
BEAM INTENSITIES WITH EURISOL
The experiment on JINR Dubna Nuclotron
Performed experiments Nuclotron – set up ENERGY PLUS TRANSMUTATION
Neutron production in Pb/U assembly irradiated by p+, d+ at 0. 7 – 2
LAHET code simulations in comparison with bare Pb spallation target experiment Daniela Henzlova.
Presentation transcript:

Itacil C. Gomes I.C.Gomes Consulting & Investment inc. Project X Forum on Spallation Sources for Particle Physics March 19-20, 2012 Fermi National Accelerator Laboratory, Batavia, IL, USA I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

 Calculations Presented in the AHIPA’09 Targets for Comparison Actinides Production and Decay  Ac-225 Experiment Design of the Experiment Results  Conclusions I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

 This study compares Thorium and Uranium target bombarded by Protons 200MeV and 2GeV with the same total beam power (500kW).  The 200 MeV Thorium target was modeled with 2-cm radius and 4.1cm thick.  The 200 MeV Uranium target was modeled with 2-cm radius and 2.5-cm thick.  The 2GeV Thorium and Uranium targets were modeled with 2-cm radius and 30-cm thick.  Natural densities were used in all cases.  The P-beam uniform over a 0.7-cm radius I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

 This analysis concentrated on high Z alpha-emitters but similar results are available for fission products.  The production rates were calculated using the MCNPX code with the CEM03.3 event generator.  The Thorium target have a higher production rate than the Uranium target in all alpha-emitters with Z<90.  The in the curves of production rate are considered all isotopes created and no consideration is given for the decay of the produced isotopes.  The CINDER 07.4 code was used to analyze post- production activity in the target. I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

Experimental Validation: Irradiation of a Thorium Target with a 8GeV Proton Beam In August, 2009 an Invention Report was filled by I.C.Gomes Consulting & Investment Inc and the Physics Division of the Argonne National Laboratory about the production of Ac-225 for medical applications by Th irradiated by HE protons and subsequently a patent application was filed. In the beginning of 2010 DOE granted NorthStar Medical Radioisotopes, LLC a project to perform experimental validation of the “ Production of Actinium-225 via High Energy Proton Induced Spallation of Thorium-232” The irradiation was set to be performed in the Fermilab’s 8-GeV booster synchrotron at the beam dump entrance. I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

The design of the experiment was performed by I.C.Gomes C&I Inc and Argonne. Calculations indicated that a beam current of 1.32x10 11 protons per second (total of 8x10 16 protons, 1wk irradiation) was appropriate. Th target with Cu cover: Initial estimation of the activity (Ci) of actinium for a 2cm 3 Th target was: Estimated activity of all alpha emitters after 10 days of irradiation was : Actinium IsotopesAll Alpha Emitters (including Ac) 10 days after EOI1.88x x days after EOI6.33x x I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

The impact of the presence of the target on the beam dump entrance : Concerns about heating the target: Beam Power: ~170W Calculated heating deposition: ~1W Estimated maximum temperature just by radiation cooling: ~220 o C Estimated very slow temp. raise: >>10 minutes from 25 o C to 220 o C Fraction of DOE CAT-3 threshold : Neutron Current With the Target Present Surface180 o to 150 o 150 o to 120 o to 90 o 90 o to 60 o 60 o to 30 o 30 o to 0 o Entrance Target8.80E E E Exit Target5.75E E E E E E-01 Tunnel Entrance6.50E E E E E E-01 Neutron Current Without the Presence of any Target Material Entrance Target3.51E E E Exit Target5.73E E E Tunnel Entrance6.44E E E E E E-06 After 7 days of Irradiation10 days after the EOI30 days after the EOI 2x1x1cm 3 Target1.43x x x I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

The Experimental Results – the volume of the irradiated target was 2.95cm 3 not 2cm 3 : Beam Profile on the Copper Cover Plate: Activity was measured at several points Y-direction: FWHM = 0.6cm, Center = -0.2cm X-direction: FWHM = 2.4cm, center = -0.5cm I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

Beam Intensity on Target - Temporal Profile : DateEvent 13Event 15Event 16Event 17Event 1CTotal June E E E E+16–1.07E+16 June E E E E E E+16 June E E E E E E+16 June E E E E+16–8.64E+16 June 5 ≤ 8AM 5.24E+13–5.74E E+15–9.60E+16 June 5 > 8 AM 1.24E E E+12––9.64E+16 June E E E+12––9.73E+16 June E E E+12––9.77E+16 Totals 1.00E E E E E+14 Ac-225Ac-227Ra-225Th-227Ra-223 Calculated Activity Measured (±1σ TPU)2.08± ± ± ± ±0.09 Table: Activities of actinium and related radioisotopes in millicuries The calculated beam profile was input in MCNPX model and the irradiation temporal profile was input in the CINDER code for calculating production rates. I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

Ra-223Ra-225Ac-225Ac-227Th-227 Calculated x-sec LANL5.0±0.63.0± ± ± ±1.0 This Work (±1σ TPU)4.5±0.54.2± ± ±3.49.8±1.3 Table : Comparison of calculated and measured cross sections for selected isotopes Be-7Sc-46V-48Cr-51Mn-54Fe-59Co-56Co-57Co-58Co-60 Production x-sec (mb) Published X-Sec 6.22± ± ± ± ± ± ± ± ± 0.53 Table : Production “cross section” extracted from the MCNPX calculated production rate for the spallation products in the copper front plate of the target. Also MCNPX calculated spallation products cross sections of the copper were compared with published values. I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab

 There a considerable production of highly desirable alpha- emitters by HE protons on thorium targets.  The design performed for the irradiation experiment at Fermilab has been shown as highly reliable.  The simulation by MCNPX/CINDER of spallation product production/decay by 8GeV proton beam are in good agreement with experimental results (remember TFTR).  Performing a careful modeling of an experimental setup can provide valuable insight of the expect outcome of the irradiation.  As an old conclusion (from AHIPA’09): Thorium has a higher production rate of alpha-emitters with Z<90 than uranium. I.C.Gomes Consulting & Investment Inc. Project-X – March 19-20, Fermilab