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. 2022 Mar 15;82(3):226. doi: 10.1140/epjc/s10052-022-10161-y

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© The Author(s) 2022

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Fig. 12 — The weighting potential at $z = 0$ (i.e. events originating at the passivated surface) for the PONaMa-1 detector, calculated using mjd_fieldgen. Note that the electron contribution to the signal is small over most of the surface, and rises dramatically at small radii