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THE EGS5 CODE SYSTEM

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tranport step 1<br />

DEINITIAL1 DERESID1<br />

transport step 2<br />

DEINITIAL2<br />

DERESID2<br />

translation step,<br />

DERESID1 + DEINITIAL2<br />

A.) Escape prior to end<br />

of transport step<br />

previous energy hinge<br />

Boundary<br />

A.) Energy decremented at last hinge,<br />

but not yet deposited in translation<br />

A.) DENSTEP<br />

next energy hinge<br />

B.) Energy deposited in<br />

translation, but not yet<br />

decremented<br />

Energy deposition<br />

Boundary<br />

B.) DENSTEP<br />

B.) Escape after end of<br />

transport step<br />

Figure 2.14: Electron boundary crossing during translation steps. In the top schematic (case A),<br />

the electron crosses escapes the problem volume before traversing the full distance corresponding<br />

to the initial transport step (i.e., through both legs of the hinge), while in the bottom schematic<br />

(case B), the particle escapes the volume after the completion of initial transport step. In case A,<br />

the full transport step CSDA energy loss is decremented from the particle’s energy at the time it<br />

passes through the hinge point, but as the particle has not traveled the distance corresponding to<br />

that amount of energy loss, some kinetic energy must be added back to the particle. In case B,<br />

the particle crosses the boundary during the first leg of the second energy hinge step, thus it has<br />

deposited energy into the system even though its energy has not been updated, so some kinetic<br />

energy must be subtracted at that point. In either instance, the final energy of the electron can be<br />

shown to be E = E − DEINITIAL + DENSTEP.<br />

107

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