Nuclear Data in Radiation Protection Dosimetry 2011 Symposium on Nuclear Data Daiki SATOH Japan Atomic Energy Agency 1. Dosimetry calculations powered.

Slides:



Advertisements
Similar presentations
Stefan Roesler SC-RP/CERN on behalf of the CERN-SLAC RP Collaboration
Advertisements

NE Introduction to Nuclear Science Spring 2012 Classroom Session 9: Radiation Interaction with Matter  Absorbed Dose (D), Kerma (K) Gray (Gy) =
P HI T S Exercise ( II ) : How to stop , ,  -rays and neutrons? Multi-Purpose Particle and Heavy Ion Transport code System title1 Feb revised.
NE Introduction to Nuclear Science Spring 2012
Interaction of radiation with matter - 5
EMERALD1: A Systematic Study of Cross Section Library Based Discrepancies in LWR Criticality Calculations Jaakko Leppänen Technical Research Centre of.
1 Activation problems S.Agosteo (1), M.Magistris (1,2), Th.Otto (2), M.Silari (2) (1) Politecnico di Milano; (2) CERN.
Radiation Units & Quantities
Title Nuclear Reaction Models in Particle and Heavy Ion Transport code System PHITS Koji Niita: RIST, Japan Tatsuhiko Sato, JAEA, Japan Hiroshi Iwase:
Estimation of the effects of a lead vest on dose reduction for NPP workers using Monte Carlo calculations KIM JEONG-IN.
Shielding Studies using MARS Monte Carlo code Noriaki Nakao (SLAC) Jan. 6, 2005, WORKSHOP Machine-Detector Interface at ILC, SLAC.
Dose. Energy Gained Particles lose energy in matter. Eventually energy loss is due to ionization. An important measure is the amount of energy gained.
Chapter 4 Radioactivity and Medicine A CT scan (computed tomography) of the brain using X-ray beams.
Quantities and Measurements - 2 Dosimetric Quantities
IAEA Quantities and Measurements - 3 Radiation Protection Quantities Day 3 – Lecture 1 1.
Radiation Dosimetry Dose Calculations D, LET & H can frequently be obtained reliably by calculations: Alpha & low – Energy Beta Emitters Distributed in.
Title Koji Niita: RIST, Japan Hiroshi Iwase: GSI, Germany Tatsuhiko Sato, JAEA, Japan Yousuke Iwamoto, Norihito Matsuda, Yukio Sakamoto, Hiroshi Nakashima:
Alexander Brandl ERHS 630 Exposure and Dose Environmental and Radiological Health Sciences.
Radiology is concerned with the application of radiation to the human body for diagnostically and therapeutically purposes. This requires an understanding.
Photon and Energy Fluence
Radiation therapy is based on the exposure of malign tumor cells to significant but well localized doses of radiation to destroy the tumor cells. The.
Chalmers University of Technology, Sweden
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,
Nuclear _____________of atom is changed Particles or energy is absorbed or emitted from nucleus Can involve one atom or multiple atoms New elements can.
UKRNDC Activity on Nuclear Data Support to Meet the Requirements Connected with Fundamental Science and Applications Olena Gritzay, Oleksandr Kalchenko.
Internal Radiation Dosimetry Lab 9. Radiation Measurement We use different terms depending on whether: 1.The radiation is coming from a radioactive source.
The Status of Nuclear Data above 20 MeV Masayoshi SUGIMOTO, Tokio FUKAHORI Japan Atomic Energy Agency IAEA’s Technical Meeting on Nuclear Data Libraries.
NUCLEAR VS. CHEMICAL CHEMICAL reactions involve rearranging of atoms: e.g., H 2 +O 2  H 2 O No new atoms are created. Chemistry involves electrons only.
Chapter 9 Nuclear Radiation
10 CFR 835 Amendment Peter V. O’Connell, CHP U.S. Department of Energy Accelerator Safety Workshop August 8, 2007 Argonne National Laboratory.
Intervention for Chronic and Emergency Exposure Situations Assessment and Response during Radiological Emergency Dose Assessment Overview Lecture IAEA.
APHY398C 6/4/ Dosimetry   Quantifying the incidence of various biological changes as a function of the radiation dose.   Exposure Ratio of total.
Lecture 26 Atomic Structure and Radioactivity Chapter 29.1  29.4 Outline Properties of the Atomic Nucleus Binding Energy Radioactivity and Radioactive.
3/2003 Rev 1 II.2.8 – slide 1 of 42 IAEA Post Graduate Educational Course Radiation Protection and Safe Use of Radiation Sources Part IIQuantities and.
What is Radiation? The transfer of energy in the form of particles or waves from one object to another though a medium. Module #2.
JAERI nuclear analyses for IFMIF T. Umetsu, M. Yamauchi and M. Sugimoto Presented by Takeo NISHITANI Japan Atomic Energy Agency (JAEA) IAEA Technical Meeting.
Radiation damage calculation in PHITS
1 Chapter 9 Nuclear Radiation 9.1 Natural Radioactivity Copyright © 2009 by Pearson Education, Inc.
3/2003 Rev 1 II.1.2 – slide 1 of 32 IAEA Post Graduate Educational Course Radiation Protection and Safe Use of Radiation Sources Session II.1.2 Part IIQuantities.
Cosmic rays at sea level. There is in nearby interstellar space a flux of particles—mostly protons and atomic nuclei— travelling at almost the speed of.
P HI T S Melt a snowman by proton beam Multi-Purpose Particle and Heavy Ion Transport code System title1 Aug revised.
P HI T S Shielding exercise Multi-Purpose Particle and Heavy Ion Transport code System title1 Last revised 2015/10.
3/2003 Rev 1 I.2.0 – slide 1 of 12 Session I.2.0 Part I Review of Fundamentals Module 2Introduction Session 0Part I Table of Contents IAEA Post Graduate.
Investigating the Feasibility of a Small Scale Transmuter – Part II Roger Sit NCHPS Meeting March 4-5, 2010.
Neutron measurement with nuclear emulsion Mitsu KIMURA 27th Feb 2013.
Authorization and Inspection of Cyclotron Facilities Radiation Fields.
Radiological Assessment - of effects from - Fukushima Daiichi Nuclear Power Plant April 18, 2011.
1 Neutron Effective Dose calculation behind Concrete Shielding of Charge Particle Accelerators with Energy up to 100 MeV V. E Aleinikov, L. G. Beskrovnaja,
Review of Fundamentals
Pavel Oblozinsky NSDD’07, St. Petersburg June 11-15, 2007 ENDF/B-VII.0 Library and Use of ENSDF Pavel Oblozinsky National Nuclear Data Center Brookhaven.
1 BROOKHAVEN SCIENCE ASSOCIATES NSLS-II Shielding Workshop R. Casey Activation Issues for NSLS-II March 28, 2007.
SACE Stage 2 Physics The Structure of the Nucleus.
Ma zhongjian Ding yadong Wang qingbin Wu qingbiao Radiation Protection Group/IHEP.
Course : Inorganic Pharmacy II Course code: PHR 107 Course Teacher : Zara Sheikh Radioactivity and Radiopharmaceuticals.
EURISOL, TASK#5, Bucuresti, November 1 Preliminary shielding assessment of EURISOL Post Accelerator D. Ene, D. Ridikas. B. Rapp.
Jiaxin Wang and Robin P. Gardner Oct 6 th 2011, CEAR at NC State University, Raleigh, NC.
Louisiana State University Radiation Safety Office
Primary Radiation Calculation for Sun Yat-Sen Proton Hospital
Heating and radiological
INTERCOMPARISON P3. Dose distribution of a proton beam
IONIZING RADIATION IN MEDICINE.
Gas Detectors for Neutron Dosimetry and Monitoring
A Brachytherapy Treatment Planning Software Based on Monte Carlo Simulations and Artificial Neural Network Algorithm Amir Moghadam.
Multi-Purpose Particle and Heavy Ion Transport code System
Electromagnetic Radiation
What is an isotope? Agenda for Tuesday Feb 8th Percent composition
Ryuji Hosoyamada2, Hiroshi Iwase3, Hiroshi Nakashima1, and Koji Niita2
Witold Matysiak (University of Florida Proton Therapy Institute)
Presentation transcript:

Nuclear Data in Radiation Protection Dosimetry 2011 Symposium on Nuclear Data Daiki SATOH Japan Atomic Energy Agency 1. Dosimetry calculations powered by Nuclear Data. 2. Abnormalities of kerma coefficients in JENDL Neutron production cross sections at zero degrees in JENDL/HE. Contents 1

1. Dosimetry Calculations Powered by Nuclear Data Calculation of Dose Conversion Coefficients (DCC) for external exposure to radionuclides in air, water, and soil. Radioactive plume Fukushima Dai-ichi Nuclear Power Plant Submersion in a contaminated atmospheric cloud (air submersion) Immersion in contaminated water (water immersion) Exposure to contamination on or in the ground (ground exposure) 2

3 Calculation method Radiation transport in the environment DCC for monoenergetic photons or electrons DCC from radionuclides in the environment Radiation fields from … ENDF EPDL97 ENSDF semi-infinite cloud source, infinite water source, contaminated soil source. Radius = 5×MFP(E) (e.g. 1.0MeV photon; MFP = 130 m, Radius = 650 m ) PHITS Photo-atomic data library (mcplib04) Electron data library (el03) Publ Publ Publ Reference phantom Decay data

Organ absorbed doses from the contaminated soil source DCC for monoenergetic photons from the contaminated soil 4

Development of a Calculation system for Decontamination Effect (CDE). 5

Response matrix Simulation geometry of semi-infinite soil and atmosphere Scoring mesh Soil Atmosphere Source ( 137 Cs, 134 Cs) 1005m Calculation method Use of PHITS and Nuclear Data Library for dose contribution simulation from contaminated soil Including sky-shine and ground-shine effects. Construction of Response Matrix on the basis of the PHITS calculation. Response matrix: Dose contribution per unit activity from the central source region to the peripheral area. Estimation of the dose rate distribution from the activity map on the contaminated environment by using the response matrix. The forest and steep slope effect to dose rate is taken into account. 6

PHITS (3D)CDE (2D) A1 A2 B1 B2 C D A1A2B1B2CD CDE PHITS Unit:  Sv/h 7

Short summary Thanks to the great works of nuclear data communities, results of dosimetry calculation are maintaining high precision. The photo-atomic data library mcplib04 (official released in 2002 based on ENDF/B-VI) will be upgraded to mcplib05 in the next MCNP6 to take the complete form-factor data available in ENDF/ B-VII into account. What does JENDL do? 8

2. Abnormalities of kerma coefficients in JENDL-4 Kerma (Kinetic energy released per unit mass) The sum of the initial kinetic energies of all the charged particles liberated by uncharged particles in a mass of material. (ICRU Report 60, 1998) j: nuclide type, i: reaction type, Evaluated Nuclear Data Kerma Coefficients Evaluation Calculation NJOY 9

HCNONaPSClK Wt % Elemental composition of muscle tissue. (ICRP Publ. 110, 2009) ENDF/B-VII.0; Chadwick MB, “A consistent set of neutron kerma coefficients from thermal to 150 MeV for biologically important materials”, Med. Phys., 26(6), , HONC NaPSK Cl 10

Neutron flux ( MeV) Tissue equivalent sphere (diameter = 30 cm) Calculation of the HEAT inside a tissue equivalent sphere with kerma approximation. (H, C, N, O, Na, P, S, Cl, K) JENDL-4.0 ENDF/B-VII.0 11

Short summary Who has the responsibility for the evaluation of kerma coefficients? Evaluated Nuclear Data Kerma Coefficients JENDL-4 overestimates the kerma coefficients of Cl. This leads to the overestimation of absorbed doses inside a human body. 12

3. Neutron production cross sections at zero degrees in JENDL/HE Proton therapy center of Fukui prefectural hospital Synchrotron 235-MeV proton beam Horizontal irradiation room : 1 Gantry room : 2 13

Concrete wall (385 cm) JAM JENDL/HE 14

Neutron production double differential cross sections 15

Short summary We plan to measure the neutron-production double-differential cross sections in most- forward direction. Please wait for a little while longer. JENDL/HE would be suitable to use in shielding design at accelerator facilities. But, JENDL/HE and theoretical modes fail to reproduce the neutron-production double differential cross sections at zero degrees. To overcome this bad situation, systematic data set of the cross sections are required… 16

Summary Various kinds of nuclear data are utilized in the study of radiation protection dosimetry. Nuclear data are essential for dosimetry calculations to ensure the accuracy of the results. Some problems would be remained in the current nuclear data and the subset of the libraries. I believe… Collaborations across the fields of nuclear data and radiation protection would solve these problems, and lead us to the better future! 17

Development of the calculation system for decontamination effect. Kensuke Kojima, Akito Ohizumi, Norihiro Matsuda, Hiroki Iwamoto, Teruhiko Kugo, Yukio Sakamoto, Akira Endo, and Shigeaki Okajima. Calculation of the dose conversion coefficients for external photon exposure from the contaminated environment. Akira Endo Yuji Tameshige, Yoshikazu Maeda, Shuichi Tsuda, Akira Endo, Hiroshi Nakashima, Tokushi Shibata. Measurement of the neutron doses at the proton therapy center of Fukui prefectural hospital. Collaborators 18