Geant4 and the Vanderbilt Radiation Effects Simulation Strategy, RADSAFE
|
|
- Katrina Tucker
- 5 years ago
- Views:
Transcription
1 Geant4 and the Vanderbilt Radiation Effects Simulation Strategy, RADSAFE Robert A. Weller, Robert A. Reed & Marcus H. Mendenhall Institute for Space & Defense Electronics Vanderbilt University Additional Collatorators: K. M. Warren D. R. Ball J. A. Pellish B. D. Sierawski C. L. Howe A. D. Tipton R. D. Schrimpf L. W. Massengill M. Alles L. Sternberg A. F. Witulski B. E. Templeton NASA Goddard: M. A. Xapsos K. A. LaBel NASA Marshall: J. H. Adams J. W. Watts Sponsoring Agencies: NASA, DTRA, AFOSR, AEDC Geant4 Space Users Workshop - Pasadena - 7/Nov/2006 1
2 Overview Objective - A Priori radiation effects simulation in semiconductors Motivation - Current methods are increasingly encountering problems Strategy - RADSAFE Geant4 application - MRED Details - What s in MRED and why Applications - The next talk, R. Reed 2
3 RADSAFE The Vision Predictable System Error Rates Trackable System Effects Statistical Circuit Response Functional Errors 3 Component Response Statistics Physics of Radiation Interaction
4 The RADSAFE System A system for first-principles predication of device, circuit and system response to radiation. Event-based Analysis RADSAFE is a strategy for implementing the third paradigm of scientific discovery, high fidelity computer simulation, in the field of radiation effects in semiconductor electronics and materials. 4
5 Structure of MRED MRED8 is the first generation Python/Geant4 application Target machine is a Linux cluster with!1k x86 and ppc nodes Development is with Xcode under Darwin (Mac OS 10.4) Presently using gcc 4 Python SWIG MRED C++ Geant4 5
6 MRED in RADSAFE 6
7 Python control shell MRED8 Features Standard internal data structure for radiation environments TCAD structure file parsing Constructive solid tetrahedron Now G4Tet! General voxel array input mechanism Screened Coulomb scattering and recoil tracking Custom particle gun derived from G4ParticleGun Three-level track weighting, ion selection, energy selection, hadronic interaction biasing Interpolating function or C2Function tool Detector class with multiple sensitive volumes Plug-in socket for combining sensitive volume energies HDF5 output files A WWW interface for remote control 7
8 MRED8-TCAD Interface Protons incident on an advanced CMOS integrated circuit Reactions in the metal layers increase energy deposition Proton Beam Radiation Events Device Description 8
9 MRED8 Voxel Array Processor Supplements TCAD inputs Detectors and regions defined in the input file Color by region name Supports extended applications such as medical dosimetry Image: M.H.Mendenhall 9
10 MRED8 Physics Run-time selection of custom MRED physics or any Geant4 physics list Coulomb scattering of nuclei and tracking of recoils Hadronic cross section biasing with automatic track weighting Custom particle gun Derived from G4ParticleGun class Supports random planar and isotropic flux simulation Uses C2Functions class to implement random energy from arbitrary input distributions Random energy selection from the integral distribution -oruniform or logarithmic selection and track weighting Uniform track-weight scaling for radiation environments 10
11 MRED8 Displacement Single Event 11
12 Running a Space Environment Si-Nitride 0.4!m SiO2 1.0!m Al 0.84!m SiO2 0.60!m Al 0.45!m SiO2 or W 0.6!m Al 0.45!m SiO2 0.6!m Si 0.25!m 2x2x2!m 3 Sensitive Volume 50!m 12
13 Effects of Heavy Elements Si-Nitride 0.4!m Direct SiO2 1.0!m Al 0.84!m SiO2 0.60!m Al 0.45!m SiO2 or W 0.6!m Al 0.45!m SiO2 0.6!m Si 0.25!m 50!m 2x2x2!m 3 Sensitive Volume 13
14 MRED8 Detectors & Event Selection MRED8 is basically a calorimetry tool Detector class includes rectangular and ellipsoidal sensitive volumes in arbitrary numbers. Each SV includes a validity range and invert logic flag. Collected charge model - Linear or arbitrary combinations of sensitive volume energies Hard wired filter logic implements first-level event selection to: Include nuclear reaction events Include Coulomb elastic scattering events Include hadronic elastic scattering events Include delta-ray event Include large-angle scattering events by the projectile Include events satisfying energy-based validity criteria Do boolean logic on sensitive volume and detector validity Custom histogram class with Python analog class General, programmable hit mechanism for particle/location/direction selection 14
15 Sensitive Volume Descriptions Defined as rectangular volumes Can be nested Linear combinations model charge collection Volumes represent diffusion regions of off-state transistors, High efficiency, small areas Arbitrary functions possible using plug-ins Volumes below the STI, low efficiencies, large areas 15
16 MRED8 Available Outputs Primary output based on HDF5 data model MRED8 can pass full G4Event objects to Python Sensitive volume histograms A validity map - a histogram implemented as an STL map indexed by a key constructed from the validity bools of all SVs Mathematica output for backward compatibility 16
17 HDF5 File Example 17
18 Writing the HDF5 Tables 18
19 Conclusion The heavy fragment distributions from ion-ion collisions must be modeled for SEE Fe on anything is essential Xe on anything is almost as important Super-heavy intermediate nuclei must not crash Geant4 Good physics is important; limits are essential The e-h pair distribution around single trajectories must be modeled for ULSI. (This overlaps biophysics, cells, DNA, etc.) Little issues (suggestions): Add energy categories, ionization, phonons, displacement, radiation, etc., (in G4Step?) for processes that wish to use them. Total deposited energy is not sufficient. Require as policy that all variables be accessible to derived classes unless doing so breaks functionality. Finally, (far out) Define membranes (zero-volume, surface-only objects with unique surface normal at each point) for parallel worlds. Not for material world. Purpose: Event metrology. 19
NASA - 2: MRED. Robert A. Weller
NASA - 2: MRED Robert A. Weller Vanderbilt: R. A. Reed M. H. Mendenhall B. D. Sierawski K. M. Warren R. D. Schrimpf L. W. Massengill A. F. Witulski D. R. Ball J. A. Pellish C. L. Howe A. D. Tipton M. L.
More informationApplication of the RADSAFE Concept
Application of the RADSAFE Concept Vanderbilt University R.A. Reed, R.A. Weller, R.D. Schrimpf, L.W. Massengill, M.H. Mendenhall, K. M. Warren, D.R. Ball, C.L. Howe, J.A. Pellish, E. Montez, A. Kalavagunta,
More informationImpact of Ion Energy and Species on Single Event Effect Analysis
Impact of Ion Energy and Species on Single Event Effect Analysis Vanderbilt University Institute for Space & Defense Electronics R. A. Reed, R. A. Weller, M. H. Mendenhall K. M. Warren D. R. Ball, J. A.
More informationVirtual Irradiation: Single Event Rate Prediction for Advanced Technologies
Virtual Irradiation: Single Event Rate Prediction for Advanced Technologies Kevin Warren 1, Andrew Sternberg 1, Brian Sierawski 1, Robert Reed 2, Robert Weller 2, Carl Carmichael 3, Gary Swift 3, JL DeJong
More informationSingle Event Latchup in 65 nm CMOS SRAMs
Single Event Latchup in 65 nm CMOS SRAMs J. M. Hutson 1, A. D. Tipton 1, J. A. Pellish 1, G. Boselli 2, M. A. Xapsos 3, H. Kim 3, M. Friendlich 3, M. Campola 3, S. Seidleck 3, K. LaBel 3, A. Marshall 2,
More informationNew Features under Development - 1. Makoto Asai On behalf of the SLAC Geant4 team
New Features under Development - 1 Makoto Asai On behalf of the SLAC Geant4 team Contents Semiconductor energy transport Phonon Electron/hole drift Activation of material We expect to deliver first implementation
More informationGeneralized SiGe HBT Event Rate Predictions Using MRED
Generalized SiGe HBT Event Rate Predictions Using MRED Jonathan A. Pellish, R. A. Reed, A. K. Sutton, R.!A.!Weller, M. A. Carts, P. W. Marshall, C.!J.!Marshall, R. Krithivasan, J. D. Cressler, M.!H.!Mendenhall,
More informationFinal Report Advanced Modeling and Test Methods for Radiation Effects on Microelectronic Devices
Final Report Advanced Modeling and Test Methods for Radiation Effects on Microelectronic Devices Dr. Robert A. Reed and Dr. Robert A. Weller Electrical Engineering and Computer Science Department Institute
More informationHans-Herbert Fischer and Klaus Thiel
A simulation tool for the calculation of NIEL in arbitrary materials using GEANT4 - Some new results - Hans-Herbert Fischer and Klaus Thiel Nuclear Chemistry Dept. University of Köln, FRG ESA GSP 2005
More informationProbabilistic Modeling for Solar Energetic Particle Events
for Solar Energetic Particle Events Space Environment Engineering and Science Applications Workshop (SEESAW) Authors: Zachary Robinson (zachary@5thgait.com), James Adams Jr., Jonathan Fisher, Joseph Nonnast
More informationJames Michael Trippe. Thesis. Submitted to the Faculty of the. Graduate School of Vanderbilt University. in partial fulfillment of the requirements
A TECHNIQUE FOR PREDICTING THE MUON INDUCED UPSET CROSS SECTION IN SUBMICRON MOS DEVICES USING PROTON TESTS AND SIMULATION By James Michael Trippe Thesis Submitted to the Faculty of the Graduate School
More informationUser Documentation and Examples (II) in GEANT p01
User Documentation and Examples (II) in GEANT 4.9.3-p01 Michael H. Kelsey SLAC National Accelerator Laboratory GEANT4 Tutorial, BUAF Puebla, Mexico 14 Jun 2010 Advanced User Documentation Toolkit developers
More informationON THE IMPACT OF DEVICE ORIENTATION ON THE MULTIPLE CELL UPSET RADIATION RESPONSE IN NANOSCALE INTEGRATED CIRCUITS. Alan Douglas Tipton.
ON THE IMPACT OF DEVICE ORIENTATION ON THE MULTIPLE CELL UPSET RADIATION RESPONSE IN NANOSCALE INTEGRATED CIRCUITS By Alan Douglas Tipton Dissertation Submitted to the Faculty of the Graduate School of
More informationUser Documents and Examples II
User Documents and Examples II John Apostolakis Most slides from Dennis Wright s talk at SLAC Geant4 Tutorial, May 2007 Geant4 V8.3 Outline User Documents Toolkit Developers' Guide Physics Reference Manual
More informationAtmospheric radiation environment analyses based-on CCD camera at various mountain altitudes and underground sites
Atmospheric radiation environment analyses based-on CCD camera at various mountain altitudes and underground sites Pierre Li Cavoli 1,2,a, Guillaume Hubert 1,b, and José Busto 2,c 1 The French Aerospace
More informationSimulation of Radiation Effects on NGST. Bryan Fodness, Thomas Jordan, Jim Pickel, Robert Reed, Paul Marshall, Ray Ladbury
Simulation of Radiation Effects on NGST Bryan Fodness, Thomas Jordan, Jim Pickel, Robert Reed, Paul Marshall, Ray Ladbury 1 Outline Introduction to Project Goals and Challenges Approach Preliminary Results
More informationCHARGE GENERATION BY SECONDARY PARTICLES FROM NUCLEAR REACTIONS IN BACK END OF LINE MATERIALS. Nathaniel Anson Dodds. Thesis
CHARGE GENERATION BY SECONDARY PARTICLES FROM NUCLEAR REACTIONS IN BACK END OF LINE MATERIALS By Nathaniel Anson Dodds Thesis Submitted to the Faculty of the Graduate School of Vanderbilt University in
More informationNeutron Interactions Part I. Rebecca M. Howell, Ph.D. Radiation Physics Y2.5321
Neutron Interactions Part I Rebecca M. Howell, Ph.D. Radiation Physics rhowell@mdanderson.org Y2.5321 Why do we as Medical Physicists care about neutrons? Neutrons in Radiation Therapy Neutron Therapy
More informationNonionizing Energy Loss (NIEL) for Protons
Nonionizing Energy Loss (NIEL) for Protons I. Jun', M. A. Xapsos2, S. R. Messenger3,E. A. Burke3,R. J. Walters4,and T. Jordans Jet Propulsion Laboratory, Califomia Institute of Technology, Pasadena CA
More informationToday, I will present the first of two lectures on neutron interactions.
Today, I will present the first of two lectures on neutron interactions. I first need to acknowledge that these two lectures were based on lectures presented previously in Med Phys I by Dr Howell. 1 Before
More informationRadiation Effect Modeling
Radiation Effect Modeling The design of electrical systems for military and space applications requires a consideration of the effects of transient and total dose radiation on system performance. Simulation
More informationChapter V: Interactions of neutrons with matter
Chapter V: Interactions of neutrons with matter 1 Content of the chapter Introduction Interaction processes Interaction cross sections Moderation and neutrons path For more details see «Physique des Réacteurs
More informationInteraction of ion beams with matter
Interaction of ion beams with matter Introduction Nuclear and electronic energy loss Radiation damage process Displacements by nuclear stopping Defects by electronic energy loss Defect-free irradiation
More informationAtmospheric Radiation Environment Analyses Based-on CCD Camera at Various Mountain Altitudes and Underground sites
Atmospheric Radiation Environment Analyses Based-on CCD Camera at Various Mountain Altitudes and Underground sites P. Li Cavoli, G. Hubert, J. Busto To cite this version: P. Li Cavoli, G. Hubert, J. Busto.
More informationElectron-induced Single-Event Upsets in integrated memory device
Electron-induced Single-Event Upsets in integrated memory device Pablo Caron 2 nd année DPHY Christophe Inguimbert, ONERA, DPHY Laurent Artola, ONERA, DPHY Guillaume Hubert, ONERA, DPHY Robert Ecoffet,
More informationRadiation Effect Modeling
Radiation Effect Modeling The design of electrical systems for military and space applications requires a consideration of the effects of transient and total dose radiation on system performance. Simulation
More informationScience Curriculum Matrix
Science Curriculum Matrix Physics Version 1.0 beta June 2, 2008 This curriculum (core matrix) document will eventually become part of the Science Curriculum Matrix. We envision the Science Curriculum Matrix
More informationSENSITIVE VOLUME MODELS FOR SINGLE EVENT UPSET ANALYSIS AND RATE PREDICTION FOR SPACE, ATMOSPHERIC, AND TERRESTRIAL RADIATION ENVIRONMENTS
SENSITIVE VOLUME MODELS FOR SINGLE EVENT UPSET ANALYSIS AND RATE PREDICTION FOR SPACE, ATMOSPHERIC, AND TERRESTRIAL RADIATION ENVIRONMENTS By Kevin M. Warren Dissertation Submitted to the Faculty of the
More informationOutline. Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter. Photon interactions. Photoelectric effect
Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter Radiation Dosimetry I Text: H.E Johns and J.R. Cunningham, The physics of radiology, 4 th ed. http://www.utoledo.edu/med/depts/radther
More informationRadiation Transport Tools for Space Applications: A Review
Radiation Transport Tools for Space Applications: A Review Insoo Jun, Shawn Kang, Robin Evans, Michael Cherng, and Randall Swimm Mission Environments Group, February 16, 2008 5 th Geant4 Space Users Workshop
More informationDario Barberis Evaluation of GEANT4 electromagnetic physics in ATLAS
Dario Barberis Evaluation of GEANT4 electromagnetic physics in ATLAS G4 Workshop, Genova, 5 July 2001 Dario Barberis Genova University/INFN 1 The ATLAS detector G4 Workshop, Genova, 5 July 2001 Dario Barberis
More informationqq k d Chapter 16 Electric and Magnetic Forces Electric charge Electric charges Negative (electron) Positive (proton)
Chapter 16 Electric and Magnetic Forces Electric charge Electric charges Negative (electron) Positive (proton) Electrons and protons in atoms/molecules Ions: atoms/molecules with excess of charge Ions
More informationSimulation of Radiation Monitors for Future Space Missions
1 Simulation of Radiation Monitors for Future Space Missions P.Gonçalves, M. Pimenta, B. Tomé LIP - Laboratório de Instrumentação e Física Experimental de Partículas Lisboa, Portugal Space radiation environment
More informationThe ALICE Inner Tracking System Off-line Software
The ALICE Inner Tracking System Off-line Software Roberto Barbera 1;2 for the ALICE Collaboration 1 Istituto Nazionale di Fisica Nucleare, Sezione di Catania Italy 2 Dipartimento di Fisica dell Università
More informationO WILEY- MODERN NUCLEAR CHEMISTRY. WALTER D. LOVELAND Oregon State University. DAVID J. MORRISSEY Michigan State University
MODERN NUCLEAR CHEMISTRY WALTER D. LOVELAND Oregon State University DAVID J. MORRISSEY Michigan State University GLENN T. SEABORG University of California, Berkeley O WILEY- INTERSCIENCE A JOHN WILEY &
More informationDevelopment of Contactless Method of the DUT Heating during Single-Event Effect Tests
Journal of Physical Science and Application 8 (2) (2018) 22-27 doi: 10.17265/2159-5348/2018.02.004 D DAVID PUBLISHING Development of Contactless Method of the DUT Heating during Single-Event Effect Tests
More informationAn Interdigitated Pixel PIN Detector for Energetic Particle Spectroscopy in Space
An Interdigitated Pixel PIN Detector for Energetic Particle Spectroscopy in Space R. A. Mewaldt, W. R. Cook, and A. C. Cummings California Institute of Technology Pasadena, CA 91125 T. J. Cunningham, M.
More informationInteraction of Particles and Matter
MORE CHAPTER 11, #7 Interaction of Particles and Matter In this More section we will discuss briefly the main interactions of charged particles, neutrons, and photons with matter. Understanding these interactions
More informationGeant4 Simulation of Very Low Energy Electromagnetic Interactions
Geant4 Simulation of Very Low Energy Electromagnetic Interactions R. Capra 1, Z. Francis 2, S. Incerti 3, G. Montarou 2, Ph. Moretto 3, P. Nieminen 4, M. G. Pia 1 1 INFN Sezione di Genova; I-16146 Genova,
More informationIII. Energy Deposition in the Detector and Spectrum Formation
1 III. Energy Deposition in the Detector and Spectrum Formation a) charged particles Bethe-Bloch formula de 4πq 4 z2 e 2m v = NZ ( ) dx m v ln ln 1 0 2 β β I 0 2 2 2 z, v: atomic number and velocity of
More informationIAC-08-A MONTE CARLO SIMULATIONS OF ENERGY LOSSES BY SPACE PROTONS IN THE CRATER DETECTOR
IAC-08-A1.4.06 MONTE CARLO SIMULATIONS OF ENERGY LOSSES BY SPACE PROTONS IN THE CRATER DETECTOR Lawrence W. Townsend The University of Tennessee, Knoxville, Tennessee, United States of America ltownsen@tennessee.edu
More informationNuclear Physics and Astrophysics
Nuclear Physics and Astrophysics PHY-30 Dr. E. Rizvi Lecture 4 - Detectors Binding Energy Nuclear mass MN less than sum of nucleon masses Shows nucleus is a bound (lower energy) state for this configuration
More informationCHARGED PARTICLE INTERACTIONS
CHARGED PARTICLE INTERACTIONS Background Charged Particles Heavy charged particles Charged particles with Mass > m e α, proton, deuteron, heavy ion (e.g., C +, Fe + ), fission fragment, muon, etc. α is
More informationThe interaction of radiation with matter
Basic Detection Techniques 2009-2010 http://www.astro.rug.nl/~peletier/detectiontechniques.html Detection of energetic particles and gamma rays The interaction of radiation with matter Peter Dendooven
More informationLast Lecture 1) Silicon tracking detectors 2) Reconstructing track momenta
Last Lecture 1) Silicon tracking detectors 2) Reconstructing track momenta Today s Lecture: 1) Electromagnetic and hadronic showers 2) Calorimeter design Absorber Incident particle Detector Reconstructing
More informationThe Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS CR -2018/225 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 27 September 2018 (v2, 19 November
More informationRadiation Quantities and Units
Radiation Quantities and Units George Starkschall, Ph.D. Lecture Objectives Define and identify units for the following: Exposure Kerma Absorbed dose Dose equivalent Relative biological effectiveness Activity
More informationEstec final presentation days 2018
Estec final presentation days 2018 Background VESPER Facility Conclusion & Outlook Jovian environment Radiation Effects VESPER history VESPER status Overview Experimental Results External Campaign Summary
More informationUsage of GEANT 4 versions: 6, 7 & 8 in BABAR
Usage of GEANT 4 versions: 6, 7 & 8 in BABAR Swagato Banerjee Computing in High Energy and Nuclear Physics (CHEP) 4 September 27, Victoria. SLAC-Based B-Factory: PEP II & BABAR The BABAR Detector: Simulation
More informationProbing the sub-disciplines: what do we know? what do we need to know? The physics The chemistry - Modelling
Session 3: Probing the sub-disciplines: what do we know? what do we need to know? The physics The chemistry - Modelling Michael Dingfelder Department of Physics, East Carolina University Mailstop #563
More informationGEANT4 simulation of the testbeam set-up for the ALFA detector
GEANT4 simulation of the testbeam set-up for the detector V. Vorobel a and H. Stenzel b a Faculty of Mathematics and Physics, Charles University in Prague, Czech Republic b II. Physikalisches Institut,
More informationIntroduction. Neutron Effects NSEU. Neutron Testing Basics User Requirements Conclusions
Introduction Neutron Effects Displacement Damage NSEU Total Ionizing Dose Neutron Testing Basics User Requirements Conclusions 1 Neutron Effects: Displacement Damage Neutrons lose their energy in semiconducting
More informationIMPACT OF SCALING ON ENERGY DEPOSITION IN SENSITIVE VOLUMES DUE TO DIRECT IONIZATION BY SPACE RADIATION. Erik Funkhouser. Thesis
IMPACT OF SCALING ON ENERGY DEPOSITION IN SENSITIVE VOLUMES DUE TO DIRECT IONIZATION BY SPACE RADIATION By Erik Funkhouser Thesis Submitted to the Faculty of the Graduate School of Vanderbilt University
More informationTracking at the LAND/R B setup on 17
3 Tracking at the LAND/R B setup on 17 the example of Ne(γ,2p)15O R. Plag*, J. Marganiec 21. Januar 2011 Dedicated to the students of LAND/R3B Outline rp process and motivation coulomb dissociation as
More informationOutline. Radiation Interactions. Spurs, Blobs and Short Tracks. Introduction. Radiation Interactions 1
Outline Radiation Interactions Introduction Interaction of Heavy Charged Particles Interaction of Fast Electrons Interaction of Gamma Rays Interactions of Neutrons Radiation Exposure & Dose Sources of
More informationLaser-Induced Current Transients in Strained-Si Diodes
Laser-Induced Current Transients in Strained-Si Diodes Hyunwoo Park 1, Daniel J. Cummings 1, Rajan Arora 2, Jonathan A. Pellish 3, Robert A. Reed 2, Ronald D. Schrimpf 2, Dale McMorrow 4, Sarah Armstrong
More informationAISSCE 2016 EXPECTED (SURE SHORT) QUESTIONS WEIGHTAGE-WISE 2016
CLASS: XII AISSCE 2016 Subject: Physics EXPECTED (SURE SHORT) QUESTIONS WEIGHTAGE-WISE 2016 Q3 Section A ( 1 Mark ) A force F is acting between two charges placed some distances apart in vacuum. If a brass
More informationRadioactivity. Lecture 6 Detectors and Instrumentation
Radioactivity Lecture 6 Detectors and Instrumentation The human organs Neither humans nor animals have an organ for detecting radiation from radioactive decay! We can not hear it, smell it, feel it or
More informationTotal probability for reaction Yield
Total probability for reaction Yield If target has thickness d, and target material has # nuclei/volume: n 0 [part./cm 3 ] Y=σ n 0 d The yield gives the intensity of the characteristic signal from the
More informationAIM AIM. Study of Rare Interactions. Discovery of New High Mass Particles. Energy 500GeV High precision Lots of events (high luminosity) Requirements
AIM AIM Discovery of New High Mass Particles Requirements Centre-of-Mass energy > 1000GeV High Coverage Study of Rare Interactions Requirements Energy 500GeV High precision Lots of events (high luminosity)
More informationAbstract: J. Urbar [1], J. Scheirich [2], J. Jakubek [3] MEDIPIX CR tracking device flown on ESA BEXUS-7 stratospheric balloon flight
[1] Department of Space Science, LTU, Kiruna, Sweden [2] Faculty of Electrical Engineering, Czech Technical University in Prague [3] Institute of Experimental and Applied Physics, CTU Prague, Czech Rep.
More informationLecture 14 (11/1/06) Charged-Particle Interactions: Stopping Power, Collisions and Ionization
22.101 Applied Nuclear Physics (Fall 2006) Lecture 14 (11/1/06) Charged-Particle Interactions: Stopping Power, Collisions and Ionization References: R. D. Evans, The Atomic Nucleus (McGraw-Hill, New York,
More informationPreliminary results from gamma-ray observations with the CALorimeteric Electron Telescope (CALET)
Preliminary results from gamma-ray observations with the CALorimeteric Electron Telescope (CALET) Y.Asaoka for the CALET Collaboration RISE, Waseda University 2016/12/15 CTA-Japan Workshop The extreme
More informationHEAVY ION-INDUCED SINGLE PARTICLE DISPLACEMENT DAMAGE IN SILICON. Elizabeth C. Auden. Dissertation. Submitted to the Faculty of the
HEAVY ION-INDUCED SINGLE PARTICLE DISPLACEMENT DAMAGE IN SILICON By Elizabeth C. Auden Dissertation Submitted to the Faculty of the Graduate School of Vanderbilt University in partial fulfillment of the
More informationSelected Topics in Physics a lecture course for 1st year students by W.B. von Schlippe Spring Semester 2007
Selected Topics in Physics a lecture course for 1st year students by W.B. von Schlippe Spring Semester 2007 Lecture 11 1.) Determination of parameters of the SEMF 2.) α decay 3.) Nuclear energy levels
More informationTracking. Witold Pokorski, Alberto Ribon CERN PH/SFT
Tracking Witold Pokorski, Alberto Ribon CERN PH/SFT ESIPAP, Archamps, 8-9 February 2016 Geant4 User Guides geant4.web.cern.ch/geant4/support/userdocuments.shtm User's Guide: For Application Developers
More informationDetekce a spektrometrie neutronů. neutron detection and spectroscopy
Detekce a spektrometrie neutronů neutron detection and spectroscopy 1. Slow neutrons 2. Fast neutrons 1 1. Slow neutrons neutron kinetic energy E a) charged particles are produced, protons, α particle,
More informationDario Barberis Evaluation of GEANT4 Electromagnetic and Hadronic Physics in ATLAS
Dario Barberis Evaluation of GEANT4 Electromagnetic and Hadronic Physics in ATLAS LC Workshop, CERN, 15 Nov 2001 Dario Barberis Genova University/INFN 1 The ATLAS detector LC Workshop, CERN, 15 Nov 2001
More informationGeant4 simulation of SOI microdosimetry for radiation protection in space and aviation environments
Geant4 simulation of SOI microdosimetry for radiation protection in space and aviation environments Dale A. Prokopovich,2, Mark I. Reinhard, Iwan M. Cornelius 3 and Anatoly B. Rosenfeld 2 Australian Nuclear
More informationSIMULATION OF THE LIQUID TARGETS FOR MOLYBDENUM-99 PRODUCTION
SIMULATION OF THE LIQUID TARGETS FOR MOLYBDENUM- PRODUCTION Y.V. Rudychev, D.V. Fedorchenko, M.A. Khazhmuradov National Science Center Kharkov Institute of Physics and Technology Kharkov, Ukraine Simulation
More informationThe next three lectures will address interactions of charged particles with matter. In today s lecture, we will talk about energy transfer through
The next three lectures will address interactions of charged particles with matter. In today s lecture, we will talk about energy transfer through the property known as stopping power. In the second lecture,
More informationENERGETIC ELECTRON-INDUCED SINGLE EVENT UPSETS IN STATIC RANDOM ACCESS MEMORY. Michael Patrick King. Dissertation. Submitted to the Faculty of the
ENERGETIC ELECTRON-INDUCED SINGLE EVENT UPSETS IN STATIC RANDOM ACCESS MEMORY By Michael Patrick King Dissertation Submitted to the Faculty of the Graduate School of Vanderbilt University in partial fulfillment
More informationNuclear contribution into single-event upset in 3D on-board electronics at moderate energy cosmic proton impact
Nuclear contribution into single-event upset in 3D on-board electronics at moderate energy cosmic proton impact N. G. Chechenin, T. V. Chuvilskaya and A. A. Shirokova Skobeltsyn Institute of Nuclear Physics,
More informationIon-ion Physics in Geant4. Dennis Wright (SLAC) 5 th Geant4 Space Users' Workshop 14 February 2008
Ion-ion Physics in Geant4 Dennis Wright (SLAC) 5 th Geant4 Space Users' Workshop 14 February 2008 Outline Introduction and Motivation Cross sections Existing models New Models Interfaces to external models
More informationGeant4 version 10.0.p01. Hadronic Physics I. Geant4 Tutorial: version 10.0.p01. Michael Kelsey, Wed 5 Mar 2014
Michael Kelsey, Wed 5 Mar 2014 Hadronic Physics I Geant4 Tutorial: version 10.0.p01 Hadronic Physics I What is Hadronic Physics? The Hadronic Framework - Processes vs. Models - Cross sections and process
More informationPhysics of particles. H. Paganetti PhD Massachusetts General Hospital & Harvard Medical School
Physics of particles H. Paganetti PhD Massachusetts General Hospital & Harvard Medical School Introduction Dose The ideal dose distribution ideal Dose: Energy deposited Energy/Mass Depth [J/kg] [Gy] Introduction
More informationDisplacement Damage Characterization of Electron Radiation in. Triple-Junction GaAs Solar Cells
Displacement Damage Characterization of Electron Radiation in Triple-Junction GaAs Solar Cells Sheng-sheng Yang, Xin Gao, Yun-fei Wang,Zhan-zu Feng 2syang@sina.com National key Lab. of Vacuum & Cryogenics
More informationPhysics of Radiotherapy. Lecture II: Interaction of Ionizing Radiation With Matter
Physics of Radiotherapy Lecture II: Interaction of Ionizing Radiation With Matter Charge Particle Interaction Energetic charged particles interact with matter by electrical forces and lose kinetic energy
More informationAnalysis distribution of galactic cosmic rays particle energy with polar orbit satellite for Geant4 application
Journal of Physics: Conference Series OPEN ACCESS Analysis distribution of galactic cosmic rays particle energy with polar orbit satellite for Geant4 application To cite this article: W Suparta and W S
More informationA MONTE CARLO SIMULATION OF COMPTON SUPPRESSION FOR NEUTRON ACTIVATION ANALYSIS. Joshua Frye Adviser Chris Grant 8/24/2012 ABSTRACT
A MONTE CARLO SIMULATION OF COMPTON SUPPRESSION FOR NEUTRON ACTIVATION ANALYSIS Joshua Frye Adviser Chris Grant 8/24/2012 ABSTRACT A Monte Carlo simulation has been developed using the Geant4 software
More informationENERGY DEPOSITION MECHANISMS FOR PROTON- AND NEUTRON-INDUCED SINGLE EVENT UPSETS IN MODERN ELECTRONIC DEVICES. Michael Andrew Clemens.
ENERGY DEPOSITION MECHANISMS FOR PROTON- AND NEUTRON-INDUCED SINGLE EVENT UPSETS IN MODERN ELECTRONIC DEVICES By Michael Andrew Clemens Dissertation Submitted to the Faculty of the Graduate School of Vanderbilt
More informationSimulating Gamma-Ray Telescopes in Space Radiation Environments with Geant4: Detector Activation
Simulating Gamma-Ray Telescopes in Space Radiation Environments with Geant4: Detector Activation Andreas Zoglauer University of California at Berkeley, Space Sciences Laboratory, Berkeley, USA Georg Weidenspointner
More informationA detailed FLUKA-2005 Monte-Carlo simulation for the ATIC detector
Available online at www.sciencedirect.com Advances in Space Research (8) 7 www.elsevier.com/locate/asr A detailed FLUKA- Monte-Carlo simulation for the ATIC detector R.M. Gunasingha a, *, A.R. Fazely a,
More informationSecondary beam production with fragment separators
Secondary beam production with fragment separators Introduction Application Statistics Monte Carlo calculation of fragment transmission EBSS tutorial The code operates under MS Windows environment and
More informationTHE LHC, currently under construction at the European Organization
IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 53, NO. 5, OCTOBER 2006 2907 Background Radiation Studies at LHCb Using Geant4 G. G. Daquino, G. Corti, and G. Folger Abstract This paper aims to describe the
More informationDevelopment of a Radiation Hard CMOS Monolithic Pixel Sensor
Development of a Radiation Hard CMOS Monolithic Pixel Sensor M. Battaglia 1,2, D. Bisello 3, D. Contarato 2, P. Denes 2, D. Doering 2, P. Giubilato 2,3, T.S. Kim 2, Z. Lee 2, S. Mattiazzo 3, V. Radmilovic
More informationGeant Hadronic Physics I. Geant4 Tutorial at Lund University. 6 September 2018 Dennis Wright
Geant4 10.4 Hadronic Physics I Geant4 Tutorial at Lund University 6 September 2018 Dennis Wright Outline Overview of hadronic physics Precompoundand de-excitation models Cascade models 2 Hadronic Processes,
More informationEmphasis on what happens to emitted particle (if no nuclear reaction and MEDIUM (i.e., atomic effects)
LECTURE 5: INTERACTION OF RADIATION WITH MATTER All radiation is detected through its interaction with matter! INTRODUCTION: What happens when radiation passes through matter? Emphasis on what happens
More informationConcepts of Event Reconstruction
August 3, 2007 Directly Detectable Particles electrons, positrons: e ±, lightest charged lepton photons: γ, gauge boson for electromagnetic force pions: π ±, lightest mesons kaons: K ±, K L, lightest strange
More informationUSING CAPACITANCE TO RADIATION HARDEN FLIP-FLOPS AT ADVANCED TECHNOLOGY NODES. Zachary J. Diggins. Thesis. Submitted to the Faculty of the
USING CAPACITANCE TO RADIATION HARDEN FLIP-FLOPS AT ADVANCED TECHNOLOGY NODES By Zachary J. Diggins Thesis Submitted to the Faculty of the Graduate School of Vanderbilt University in partial fulfilment
More informationExternal MC code : PHITS
External MC code : PHITS Particle and Heavy Ion Transport code System Koji. Niita 1, Tatsuhiko Sato 2, Hiroshi Iwase 3, Yosuke Iwamoto 2, Norihiro Matsuda 2, Yukio Sakamoto 2, Hiroshi Nakashima 2, Davide
More informationEE 5211 Analog Integrated Circuit Design. Hua Tang Fall 2012
EE 5211 Analog Integrated Circuit Design Hua Tang Fall 2012 Today s topic: 1. Introduction to Analog IC 2. IC Manufacturing (Chapter 2) Introduction What is Integrated Circuit (IC) vs discrete circuits?
More informationParticle Interactions in Detectors
Particle Interactions in Detectors Dr Peter R Hobson C.Phys M.Inst.P. Department of Electronic and Computer Engineering Brunel University, Uxbridge Peter.Hobson@brunel.ac.uk http://www.brunel.ac.uk/~eestprh/
More informationExperimental Methods of Particle Physics
Experimental Methods of Particle Physics PHYS 7361 (Spring 2010) Syllabus http://www.physics.smu.edu/~kehoe/7361_10s Instructor: Professor Bob Kehoe Office: Fondren Science 113 e-mail: kehoe@physics.smu.edu
More informationReconstruction of Neutron Cross-sections and Sampling
Reconstruction of Neutron Cross-sections and Sampling Harphool Kumawat Nuclear Physics Division, BARC 1 Outline Introduction Reconstruction of resonance cross-section Linearization of cross-section Unionization
More informationInteraction of Ionizing Radiation with Matter
Type of radiation charged particles photonen neutronen Uncharged particles Charged particles electrons (β - ) He 2+ (α), H + (p) D + (d) Recoil nuclides Fission fragments Interaction of ionizing radiation
More informationRadiation damage calculation in PHITS
Radiation Effects in Superconducting Magnet Materials (RESMM'12), 13 Feb. 15 Feb. 2012 Radiation damage calculation in PHITS Y. Iwamoto 1, K. Niita 2, T. Sawai 1, R.M. Ronningen 3, T. Baumann 3 1 JAEA,
More informationSilver Thin Film Characterization
Silver Thin Film Characterization.1 Introduction Thin films of Ag layered structures, typically less than a micron in thickness, are tailored to achieve desired functional properties. Typical characterization
More information3/29/2010. Structure of the Atom. Knowledge of atoms in 1900 CHAPTER 6. Evidence in 1900 indicated that the atom was not a fundamental unit:
3/9/010 CHAPTER 6 Rutherford Scattering 6.1 The Atomic Models of Thomson and Rutherford 6. Definition of Cross Section 6. Rutherford Scattering 6.3 Structure of the Nucleus The opposite of a correct statement
More informationHeavy charged particle passage through matter
Heavy charged particle passage through matter Peter H. Hansen University of Copenhagen Content Bohrs argument The Bethe-Bloch formula The Landau distribution Penetration range Biological effects Bohrs
More information