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. 2016 Feb 17;43(3):1285–1294. doi: 10.1118/1.4941309

FIG. 3.

FIG. 3.

Comparison of the electron current from a conventional and RF electron source at the beginning (source) and end (target) of the accelerator. Note that current is not a particularly well defined concept when dealing with electron bunches over short time scales, and this is the cause of the variability in the target current peaks.