Geant4 and the Vanderbilt Radiation Effects Simulation Strategy, RADSAFE

Size: px
Start display at page:

Download "Geant4 and the Vanderbilt Radiation Effects Simulation Strategy, RADSAFE"

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 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 information

Application of the RADSAFE Concept

Application 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 information

Impact of Ion Energy and Species on Single Event Effect Analysis

Impact 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 information

Virtual Irradiation: Single Event Rate Prediction for Advanced Technologies

Virtual 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 information

Single Event Latchup in 65 nm CMOS SRAMs

Single 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 information

New 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 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 information

Generalized SiGe HBT Event Rate Predictions Using MRED

Generalized 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 information

Final 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 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 information

Hans-Herbert Fischer and Klaus Thiel

Hans-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 information

Probabilistic Modeling for Solar Energetic Particle Events

Probabilistic 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 information

James Michael Trippe. Thesis. Submitted to the Faculty of the. Graduate School of Vanderbilt University. in partial fulfillment of the requirements

James 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 information

User Documentation and Examples (II) in GEANT p01

User 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 information

ON 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. 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 information

User Documents and Examples II

User 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 information

Atmospheric 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 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 information

Simulation 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 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 information

CHARGE 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. 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 information

Neutron Interactions Part I. Rebecca M. Howell, Ph.D. Radiation Physics Y2.5321

Neutron 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 information

Nonionizing Energy Loss (NIEL) for Protons

Nonionizing 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 information

Today, I will present the first of two lectures on neutron interactions.

Today, 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 information

Radiation Effect Modeling

Radiation 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 information

Chapter V: Interactions of neutrons with matter

Chapter 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 information

Interaction of ion beams with matter

Interaction 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 information

Atmospheric 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 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 information

Electron-induced Single-Event Upsets in integrated memory device

Electron-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 information

Radiation Effect Modeling

Radiation 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 information

Science Curriculum Matrix

Science 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 information

SENSITIVE 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 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 information

Outline. Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter. Photon interactions. Photoelectric effect

Outline. 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 information

Radiation Transport Tools for Space Applications: A Review

Radiation 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 information

Dario Barberis Evaluation of GEANT4 electromagnetic physics in ATLAS

Dario 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 information

qq k d Chapter 16 Electric and Magnetic Forces Electric charge Electric charges Negative (electron) Positive (proton)

qq 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 information

Simulation of Radiation Monitors for Future Space Missions

Simulation 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 information

The ALICE Inner Tracking System Off-line Software

The 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 information

O WILEY- MODERN NUCLEAR CHEMISTRY. WALTER D. LOVELAND Oregon State University. DAVID J. MORRISSEY Michigan State University

O 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 information

Development of Contactless Method of the DUT Heating during Single-Event Effect Tests

Development 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 information

An Interdigitated Pixel PIN Detector for Energetic Particle Spectroscopy in Space

An 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 information

Interaction of Particles and Matter

Interaction 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 information

Geant4 Simulation of Very Low Energy Electromagnetic Interactions

Geant4 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 information

III. Energy Deposition in the Detector and Spectrum Formation

III. 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 information

IAC-08-A MONTE CARLO SIMULATIONS OF ENERGY LOSSES BY SPACE PROTONS IN THE CRATER DETECTOR

IAC-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 information

Nuclear Physics and Astrophysics

Nuclear 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 information

CHARGED PARTICLE INTERACTIONS

CHARGED 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 information

The interaction of radiation with matter

The 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 information

Last Lecture 1) Silicon tracking detectors 2) Reconstructing track momenta

Last 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 information

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

The 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 information

Radiation Quantities and Units

Radiation 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 information

Estec final presentation days 2018

Estec 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 information

Usage of GEANT 4 versions: 6, 7 & 8 in BABAR

Usage 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 information

Probing the sub-disciplines: what do we know? what do we need to know? The physics The chemistry - Modelling

Probing 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 information

GEANT4 simulation of the testbeam set-up for the ALFA detector

GEANT4 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 information

Introduction. Neutron Effects NSEU. Neutron Testing Basics User Requirements Conclusions

Introduction. 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 information

IMPACT 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. 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 information

Tracking at the LAND/R B setup on 17

Tracking 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 information

Outline. Radiation Interactions. Spurs, Blobs and Short Tracks. Introduction. Radiation Interactions 1

Outline. 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 information

Laser-Induced Current Transients in Strained-Si Diodes

Laser-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 information

AISSCE 2016 EXPECTED (SURE SHORT) QUESTIONS WEIGHTAGE-WISE 2016

AISSCE 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 information

Radioactivity. Lecture 6 Detectors and Instrumentation

Radioactivity. 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 information

Total probability for reaction Yield

Total 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 information

AIM AIM. Study of Rare Interactions. Discovery of New High Mass Particles. Energy 500GeV High precision Lots of events (high luminosity) Requirements

AIM 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 information

Abstract: J. Urbar [1], J. Scheirich [2], J. Jakubek [3] MEDIPIX CR tracking device flown on ESA BEXUS-7 stratospheric balloon flight

Abstract: 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 information

Lecture 14 (11/1/06) Charged-Particle Interactions: Stopping Power, Collisions and Ionization

Lecture 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 information

Preliminary results from gamma-ray observations with the CALorimeteric Electron Telescope (CALET)

Preliminary 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 information

HEAVY 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. 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 information

Selected 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 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 information

Tracking. Witold Pokorski, Alberto Ribon CERN PH/SFT

Tracking. 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 information

Detekce a spektrometrie neutronů. neutron detection and spectroscopy

Detekce 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 information

Dario Barberis Evaluation of GEANT4 Electromagnetic and Hadronic Physics in ATLAS

Dario 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 information

Geant4 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 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 information

SIMULATION OF THE LIQUID TARGETS FOR MOLYBDENUM-99 PRODUCTION

SIMULATION 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 information

The 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 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 information

ENERGETIC 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. 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 information

Nuclear 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 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 information

Ion-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 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 information

Geant4 version 10.0.p01. Hadronic Physics I. Geant4 Tutorial: version 10.0.p01. Michael Kelsey, Wed 5 Mar 2014

Geant4 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 information

Physics of particles. H. Paganetti PhD Massachusetts General Hospital & Harvard Medical School

Physics 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 information

Displacement Damage Characterization of Electron Radiation in. Triple-Junction GaAs Solar Cells

Displacement 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 information

Physics of Radiotherapy. Lecture II: Interaction of Ionizing Radiation With Matter

Physics 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 information

Analysis distribution of galactic cosmic rays particle energy with polar orbit satellite for Geant4 application

Analysis 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 information

A 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 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 information

ENERGY 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. 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 information

Simulating Gamma-Ray Telescopes in Space Radiation Environments with Geant4: Detector Activation

Simulating 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 information

A detailed FLUKA-2005 Monte-Carlo simulation for the ATIC detector

A 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 information

Secondary beam production with fragment separators

Secondary 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 information

THE LHC, currently under construction at the European Organization

THE 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 information

Development of a Radiation Hard CMOS Monolithic Pixel Sensor

Development 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 information

Geant Hadronic Physics I. Geant4 Tutorial at Lund University. 6 September 2018 Dennis Wright

Geant 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 information

Emphasis on what happens to emitted particle (if no nuclear reaction and MEDIUM (i.e., atomic effects)

Emphasis 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 information

Concepts of Event Reconstruction

Concepts 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 information

USING 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. 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 information

External MC code : PHITS

External 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 information

EE 5211 Analog Integrated Circuit Design. Hua Tang Fall 2012

EE 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 information

Particle Interactions in Detectors

Particle 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 information

Experimental Methods of Particle Physics

Experimental 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 information

Reconstruction of Neutron Cross-sections and Sampling

Reconstruction 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 information

Interaction of Ionizing Radiation with Matter

Interaction 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 information

Radiation damage calculation in PHITS

Radiation 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 information

Silver Thin Film Characterization

Silver 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 information

3/29/2010. Structure of the Atom. Knowledge of atoms in 1900 CHAPTER 6. Evidence in 1900 indicated that the atom was not a fundamental unit:

3/29/2010. 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 information

Heavy charged particle passage through matter

Heavy 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