The Charged Anticounter for the Na62 Experiment at Cern

Abstract

The NA62 experiment at CERN aims at the very challenging task of measuring with 10% relative error the Branching Ratio of the ultra-rare decay K + → π + νν, which is expected to occur only in about 8 out of 10 11 kaon decays. This will be achieved by means of an intense hadron beam, an accurate kinematical reconstruction and a redundant veto system for identifying and suppressing all spurious events. In particular, beam induced background, caused by inelastic interactions of the hadron beam with the Si based detector which measures kaon momentum (the so called Gigatracker, GTK) can mimic the signal in case only one pion is detected downstream. To suppress this background we have designed the so called CHarged ANTIcounter (CHANTI) i.e. a series of six guard counters, to be operated in vacuum and covering a wide angular region downstream the last GTK station. CHANTI must have time resolution ∼1 ns, must be highly efficient in detecting charged particles and must cope with rates which in the inner part can be some kHz/cm 2 . We have adopted a solution based on triangularly shaped scintillator bars coupled with fast wavelength shifting fibers and individually read by means of Silicon Photomultipliers (SiPM). The full scale prototype of one counter has been built and tested using a prototype front end electronic board which allows fast amplification and individual channel fine bias setting with O(mV) resolution and 0.1% stability. We show first results on the response of the detector to minimum ionizing particles as well as on its time resolution, which are well in line with the specifications.

CHANTI: a fast and efficient charged particle veto detector for the NA62 experiment at CERN

“…It is sufficient here to stress that tests done in different conditions, using beams or cosmic rays, have all pointed towards a single hit time resolution of the CHANTI (after time walk and position corrections are applied) of order 1 ns (cfr. 1.03 ± 0.01 in [16]). Regarding the efficiency, the first laboratory measurement was carried out using a prototype made of 5 bars.…”

“…In order to apply the time-walk correction also to the signals which only cross the low threshold, the distribution in figure 9 has been fitted and the δt correction has been parametrized as a logarithmic function of the ToT . Details of the tests performed have been reported elsewhere [14], [15], [16]. It is sufficient here to stress that tests done in different conditions, using beams or cosmic rays, have all pointed towards a single hit time resolution of the CHANTI (after time walk and position corrections are applied) of order 1 ns (cfr.…”