Abstract
In recent years Siegmund et al.1,2have attempted to combine in one detector the position resolution of the multi-wire proportional counter (MWPC)3–5or the parallel-plate imaging proportional counter (PPIPC)6,7with the energy resolution of the gas-scintillation proportional counter (GSPC)8–11, using light from avalanches in a PPIPC. By counting the light flashes from individual primary electrons, Fano factor limited energy resolution was obtained but only for energies below 2 keV. The position resolution was ≈350 µm over an active diameter of 25mm. Sipila and coworkers12,13used Penning gas14,15mixtures to improve the energy resolution to 11% at 6 keV. However, this was achieved at gas gains of 105. The concept of two-stage avalanching was first reported by Charpak et al.16and used by Breskin et al.17. We have built and tested a laboratory version of such a detector (Fig. 1), which we call the Penning gas imager (PGI). A Penning gas and a two-stage parallel grid avalanche geometry are combined with a wedge and strip anode (WSA) position read-out system18. Preliminary experimental energy resolution is 12% FWHM at 6 keV (24% FWHM at 1.5 keV) and the position resolution is 100 µ m FWHM at 1.5 keV. This compares with ≈ 10% and ≈ 1 mm for the GSPC and ≈18% and a few hundred micrometres for the MWPC. The particle background can be reduced by an estimated 99% using an anticoincidence technique.
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