Title: Presented by M G Pia (CERN, INFN)
1- Presented by M G Pia (CERN, INFN)
- Authors
- P Truscott F Lei
- (Defence Evaluation Research Agency, UK)
- C Ferguson R Gurriaran (University of
Southampton, UK) - P Nieminen E Daly
- (ESA /ESTEC)
- J Apostolakis, S Giani, M G Pia (CERN,
Switzerland) - L Urban (KFKI Hungary)
- M Maire (LAPP, France)
2Principal Sources of Radiation in theNear-Earth
Environment
Extra-Solar System ?-rays, X-rays
Galactic Cosmic Rays (protons heavier
nuclei) 1MeV/nuc - 100s GeV/nuc
Solar Protons Heavier Ions (up to 100
MeV/nuc) X-rays, ?-rays
Trapped Particles protons (1 MeV - 100s
MeV) electrons (1 keV - several MeV)
3- The Environment
- Spacecraft are required to operate in a severe,
energetic radiation environment comprising
cosmic-ray protons and heavier nuclei, trapped
protons and electrons that form the Van Allen
radiation belts, and solar particles emitted
during flare events and coronal mass ejections.
The interactions of these particles in spacecraft
materials not only attenuates the radiation, but
may also give rise to secondary particles (e.g.
protons, neutrons, bremsstrahlung) that may have
higher fluxes and/or greater effects than the
primaries. - The Effects
- The radiation environment can give rise to a
range of deleterious effects in spacecraft
microelectronics, solar arrays, sensors and
specialised (mission-specific) instruments such
as ?-ray detectors - Total ionising dose
- Atomic displacement (bulk) damage
- Single event effects (SEE), in which ionisation
by single particles can temporarily upset or
destroy integrated circuits - Induced radioactivity and enhanced background
rates in sensors
4- Applications for Radiation Transport Models
- Spacecraft instrument design/operation for
mitigation of effects Radiation transport
models may be used to predict the effects of the
environment on the systems making up the
spacecraft platform and payload, and to allow
designers to develop and optimise hardening
strategies. The planning of spacecraft
operations must take into consideration
variations in the environment during the mission
(such as solar particle events) and radiation
transport models help quantify the threat to
instruments and the effectiveness of possible
operational measures. - Trouble-shooting Such tools are also valuable
for trouble-shooting in-flight anomalies
experienced in spacecraft that have already been
launched, and for assessing possible mitigation
strategies. - Optimise detector/sensor designs Simulation of
radiation transport is necessary for optimising
the design of radiation detectors, such as those
used for ?-ray or X-ray missions. - Data interpretation The interpretation of data
from such instruments may also be critically
dependent upon model results, e.g. predictions of
induced X-ray yields from asteroids/moons are
required to derive composition from detected
X-ray fluxes.
5Spacecraft Missions and Radiation Effects
6- Geant4 Overview and Features (see CHEP 2000 Paper
140) - The result of a world-wide collaboration of 100
scientists and computer engineers from 40
institutes - Latest release is Geant4.1.0 issued 8th Dec 99
- Monte Carlo simulation for nuclei, hadrons,
leptons and bosons in 3D - Object Oriented design (implemented in C)
- Geant4 Adaptive GUI available
- Excellent facilities for visualisation (essential
for geometry debugging) - Comprehensive range of physical processes already
implemented as well as planned - Fast simulation mode - response of a volume may
be parameterised based on empirical or simulation
data - Facilities for event biasing
- Geometry can be constructed from solid simple
volumes or breps - Defined by user-written C
- STEP interpreter for geometry input from CAD
tools
7Applications of Geant4 Physical Processes
Hadron-nucleon or hadron-nuclear
Parameterised
Parton-string (gt5GeV)
Cosmic ray nuclei and secondaries
Kinetic (10MeV - 10GeV)
Trapped protons and secondaries
QMD models
Pre-compound (2-100 MeV)
Secondary neutrons, including atmospheric/planetar
y albedo neutrons
Low-energy neutron (thermal - 20 MeV)
Induced radioactive background calculations
Isotope production
Nuclearde-excitation
Evaporation (Agt16)
Treatment for seondaries from cosmic ray nuclei
and trapped protons, esp. important in
calculation of single event effects
(microdosimetry)
Fermi break-up (A?16)
Fission (A?65)
Multi-fragmentation
Photo-evaporation (ENSDF)
Induced and natural radioactive backgrounds
Radioactive decay (ENSDF)
8Applications of Geant4 Physical Processes
Electromagnetic
Ionisation
Important for treatment of SEE (microdosimetry
from nuclear recoil and evaporation prods)
Multiple scattering
?-ray production
Trapped electron effects
Bremsstrahlung
annihilation
Photo-electric effect
Compton scattering
Rayleigh scattering
Pair-production
Atomic relaxation
Induced and natural radioactive backgrounds
9Space Specific GEANT4 Modules
- Clearly Geant4 offers a very comprehensive
environment to specify a geometry, perform
particle tracking, and model a wide range of
physical interaction processes. Furthermore the
object-oriented design allows relatively
straightforward extension of the toolkit through
class inheritance. - The particular requirements of spacecraft
radiation effects studies have led the European
Space Agency to sponsor the development of a
number of space-specific components. These are
now discussed.
10- MGA for Geant4 STEP Interface
- The CAD STEP (Standard for Exchange of Product
Data - ISO 10303) interface provides an efficient
method of defining spacecraft system geometries
for Geant4, especially since the use of CAD tools
is widespread in the aerospace industry. In
addition, a number of commercial CAD tools
already have STEP interfaces. - However, the protocol (AP203) of STEP does not
allow the association of materials information
with each volume. The Materials and Geometry
Association (MGA) tool is a Java-based utility to
attribute material information and visualisation
properties with volumes in a STEP file. This can
be achieved manually by the user through the
Graphical User Interface, or automatically if the
CAD engineer uses pre-defind meta-data
information in the PRODUCT records for each
volume in the STEP file. The user can draw upon
a database of standard spacecraft materials, or
create her own materials by defining elemental
and nuclide composition. Once this association
is complete, both the STEP and MGA files are read
by Geant4 to obtain a complete description of the
geometry.
11Evaluation of CAD Tools
- CAD Product Suitability for G4 based
- ProEngineer (Parametric) yes
- Euclid (Matra Datavision) yes (with translator)
- Catia (IBM Dassault) yes
- MicroStation (Bentley) translator released ?
- AutoCAD (AutoDesk) yes (R14.01 )
- I-deas (SDRC) yes
12MGA Data Entry Windows
Volume, material and Vis attribute association
Materials specification window
Creation of internal databases (materials and
colours)
13- Low-Energy Electromagnetic Interactions
- Previously, the minimum energies for accurate
?-ray and electron transport in Geant3 and in EGS
and ITS was 10 keV and 1 keV respectively. A key
requirement identified by ESA for a general space
radiation tool was that it treat X-ray
fluorescence from the surfaces of asteroids and
moons. This necessitates cut-offs of 250 eV. To
achieve this, new processes (for low-energy
Compton, Rayleigh, photo-electric effect,
Bremsstrahlung, ionisation and fluorescence) have
been introduced which utilise data
parameterisations to evaluated data from Lawrence
Livermore National Laboratory (EPDL97, EEDL and
EADL). - It is planned to also extend the low-energy EM
physics for positrons to below 1 keV, as well as
treat Auger electron production. - The physics for ionisation caused by low-energy
hadrons, ions has been extended using
parameterisations to particle range and stopping
power data from Ziegler and ICRU, permitting
accurate tracking down to 1 keV. Accurate
treatment of these physical processes is
essential for simulating single event effects in
microelectronics as a result of proton- or
neutron-nuclear interactions. A similar extension
is in progress for antiprotons.
14Low-Energy Electromagnetic Interactions
15- Radioactive Decay Module
- Long-term (gt1?s) radioactive decay induced by
spallation interactions can represent an
important contributor to background levels in
spaceborne ?-ray and X-ray instruments, as the
ionisation events that result often occur outside
the time-scales of any veto pulse. The
Radioactive Decay Module (RDM) treats the nuclear
de-excitation following prompt photo-evaporation
by simulating the production of ?, ?-, ?, ? and
anti-?, as well as the de-excitation ?-rays. The
model can follow all the descendants of the decay
chain, applying, if required, variance reduction
schemes to bias the decays to occur at
user-specified times of observation. The
branching ratio and decay scheme data are based
on the Evaluated Nuclear Structure Data File
(ENSDF), and the existing Geant4
photo-evaporation model is used to treat prompt
nuclear de-excitation following decay to an
excited level in the daughter nucleus. (Atomic
de-excitation following nuclear decay is treated
by the Geant4 EM physics processes.) - The RDM has applications in the study of induced
radioactive background in space-borne detectors
and the determination of solar system body
composition from radioactive ?- ray emission.
16- Sector Shielding Analysis Tool
- It is often possible to obtain a first-order
estimate of the radiation dose received within a
spacecraft as a function of location using shield
distribution data for that location in
conjunction with dose-versus-depth information.
The Sector Shielding Analysis Tool can provide
shield distribution data using particle tracking
facilities in Geant4. The so-called geantino
particle is used to determine the path-lengths
between material boundaries for rays emanating
from a user-defined point. The
user is able to define the limits of the solid
angle analysed (the direction window) based on an
arbitrary co-ordinate system, and then sub-divide
divisions in this solid angle. Geantino rays can
be sampled randomly within each sub-division so
that the shielding can be assessed as a function
of ? and ?. Analysis output can be provided as a
function of material in units of g/cm2, cm or
radiation lengths, or for overall thickness
irrespective of material type.
17- General Source Particle Module
- The space radiation environment is often quite
complex in energy and angular distribution, and
requires sophisticated sampling algorithms. The
General Source Particle Module (GSPM) allows the
user to define his source particle distribution
(without the need for coding) in terms of the
following - Spectrum linear, exponential, power-law,
black-body, or piece-wise linear (or logarithmic)
fit to data - Angular unidirectional, isotropic, cosine-law,
or arbitrary (user-defined) - Spatial sampling from simple 2D or 3D surfaces,
such as discs, spheres, boxes, cylinders - The GSPM also provides the option of biasing the
sampling distribution. This is advantageous, for
example, for sampling the area of a spacecraft
where greater sensitivity to radiation effects is
expected (e.g. where radiation detectors are
located) or increasing the number of high-energy
particles simulated, since these may produce
greater numbers of secondaries.
18Summary
- Geant4 is a new-generation toolkit for Monte
Carlo particle simulation - Unlike other codes Geant4 has been developed to
provide comprehensive particle simulation in a
single tool, but due to its OO design, it permits
easy extension of physics modelled . if required - The Geant4 Toolkit has wide applications
including not only HEP, but also space and
medicine - Geant4 fulfils the functions required for space
radiation effects studies and will be the basis
of ESAs next generation of spacecraft radiation
shielding tools
19Visit Our Web Sites
- ESA/DERA/UoS Spacecraft Radiation Shielding and
Effects - http//www.estec.esa.nl/wmwww/WMA/research/Shieldi
ng_tools.html http//www.space.dera.gov.uk/space_e
nv/geant_mn.html - Geant4 collaboration at CERN
- http//wwwinfo.cern.ch/asd/geant4/geant4.html