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PENELOPE 2003 - OECD Nuclear Energy Agency

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6.3. Selecting the simulation parameters 203<br />

2 Ε− 5<br />

mixed (C 1<br />

=C 2<br />

=0.15)<br />

det a il ed (C 1<br />

=C 2<br />

=0)<br />

1 Ε− 5<br />

p ( E t<br />

) (1/eV)<br />

8 Ε− 6<br />

Al<br />

➤ ➤<br />

➤<br />

E t<br />

4 Ε− 6<br />

0Ε+0<br />

2E+5 3 E+5 4 E+5<br />

E t<br />

(eV)<br />

4 Ε− 7<br />

p ( E b<br />

) (1/eV)<br />

3 Ε− 7<br />

2 Ε− 7<br />

Al<br />

E b<br />

mixed (C 1<br />

=C 2<br />

=0.15)<br />

➤ ➤<br />

1 Ε− 7<br />

det a il ed (C 1<br />

=C 2<br />

=0)<br />

0Ε+0<br />

0E+0 1 E+5 2 E+5 3 E+5 4 E+5 5 E+5<br />

E b<br />

(eV)<br />

Figure 6.6: Results from PENSLAB for a 500 keV electron beam impinging normally on the<br />

surface of a 200-µm-thick aluminium slab (further details are given in the text). Top: energy<br />

distribution of transmitted electrons. Bottom: energy distribution of backscattered electrons.<br />

Secondary electrons are included in both cases.

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