1 analysing samples with complex geometries particles inclusions bubbles lamellae & phase...
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Analysing samples with complex geometries
Particles Inclusions
BubblesLamellae & phase boundaries
Multilayers
etc…
Hartford 2014
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General-purpose Monte Carlo subroutine package for the simulation of
coupled electron-photon transport in arbitrary geometries (75 eV – 1
GeV)
Developed and maintained at the UB. Distributed by the OECD-NEA
Data Bank (Paris)
PENetration and Energy LOss of Positrons and Electrons (... and photons)
http://www.nea.fr/lists/penelope.html
PENEPMA: EPMA simulations made easy
Based on PENELOPE. Latest version v. 2014
You can define the energy, direction and position of the electron beam
The geometry of the sample (and its environment) is defined by using PENGEOM
Provides the x-ray spectrum at different photon detectors
Salvat et al. (1996 2014) The simulation code PENELOPE
Hartford 2014
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Running PENEPMA with PYPENELOPE (v. 2011)
Hartford 2014
Interface created by Philippe Pinard http://pypenelope.sourceforge.net
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Running PENEPMA with PYPENELOPE
Hartford 2014
Defining a new simulation
Starting a new simulation
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Running PENEPMA with PYPENELOPE
Hartford 2014
Simulation’s folder & title
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Running PENEPMA with PYPENELOPE
Hartford 2014
Incident electron beam characteristics
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Running PENEPMA with PYPENELOPE
Hartford 2014
Sample geometry: bulk, multilayer, inclusion, grain boundaries
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Running PENEPMA with PYPENELOPE
Hartford 2014
Material compounds can be defined by means of their chemical formula
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Running PENEPMA with PYPENELOPE
Hartford 2014
… or by clicking each element in the periodic table
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Running PENEPMA with PYPENELOPE
Hartford 2014
Simulation parameters related to the mixed simulation algorithm of PENELOPE: Eabs (electrons & photons), C1, C2, WCC, WCR
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Running PENEPMA with PYPENELOPE
Hartford 2014
Interaction forcing values for each interaction mechanism e.g. ionization & bremsstrahlung emission
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Running PENEPMA with PYPENELOPE
Hartford 2014
Different kind of photon detectors can be defined
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Running PENEPMA with PYPENELOPE
Hartford 2014
A simulation will stop if the number of showers, simulation time or uncertainty on a specific X-ray line is reached
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Running PENEPMA with PYPENELOPE
Hartford 2014
Running the defined simulation
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Running PENEPMA with PYPENELOPE
Hartford 2014
Characteristic X-ray intensities (primary, fluorescence characteristic, fluorescence bremss, total) and statistical uncertainties
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Running PENEPMA with PYPENELOPE
Hartford 2014
Results can be visualized on-line or exported to data files
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Running PENEPMA manually
Hartford 2014
Geometry definition file (PENGEOM)
The corresponding material-data files (by running the program
material)
The input file containing details on the electron beam, simulation
parameters, detectors, variance reduction, methods and spatial
distribution of x-ray events, simulation time or number of trajectories,
etc
To run PENEPMA manually we usually must prepare:
Advantages of running PENEPMA manually:
Parallel processing possible (v. 2014)
Any geometry can be defined (sample, microscope, etc..)
2D distributions of X-ray emission can be obtained
Scripts prepared to visualize output results using gnuplot
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Preparing the input file
Hartford 2014
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Preparing the input file
Hartford 2014
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Preparing the input file
Hartford 2014
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Example: Ca4Al4MgO11 inclusion on Fe
Hartford 2014
Fe
Ca4Al4MgO11
electron beam (y = 1mm, x = 0mm)
E = 15 keV
y
z
r = 2 mm
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Results: characteristic x-ray spectrum
Hartford 2014
Fe
Ca
Si
Mg
O
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Results: EPMA spectrum
Hartford 2014
Fe
CaSiMg
O
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Results: depth distribution of X-ray emission (Fe Ka)
Hartford 2014
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Fe Ka
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Fe Ka
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Fe Ka
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Fe Ka