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Experiment Proposal - opera - Infn

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Figure 151: Prototype scintillator strip modules at the assembly site.<br />

• location accuracy with a prototype scintillator strip tracker and a dummy brick target.<br />

The modules were stacked, with their planes perpendicular to the beam, on a remotely controlled<br />

platform which could be moved vertically (along the Y axis) and horizontally (along the X axis) across<br />

the beam. This allowed to scan the sensitive area of the modules and measure their response at different<br />

positions across and along the strips.<br />

The beam spot had a full width of about 3 × 5 cm 2 . The trigger telescope includes scintillator<br />

counters and four multi-wire beam profile chambers (BPCs). Only non-interacting beam particles with<br />

less than 2 mip deposit in each trigger counter are selected for the analysis. Additional cuts are imposed<br />

on the beam incidence angle and impact position, as measured by the BPCs.<br />

The module PMT’s are calibrated with the LED pulser tuned so as to measure the response of each<br />

pixel to a single photoelectron. Single photoelectron signals are clearly separated from the pedestals<br />

(Fig. 152). This allows us to express raw strip signal pulse-heights (PH) in photoelectrons, defined for<br />

each strip as the PH at the maximum of its single photoelectron peak. The effect of pixel-to-pixel gain<br />

variations is eliminated.<br />

Due to pixel-to-pixel crosstalk in a PMT, small signals (≤ 1 p.e.) appear in pixels adjacent to the one<br />

coupled to the hit strip. Therefore, we associate a hit in a mip event with the strip producing the largest<br />

pulse-height (PH max ). Fig. 153 (left) shows the average PH max as a function of the corresponding strip<br />

number in one module. The strip response fluctuates by 6% due to variations in scintillator strip and WLS<br />

fibre light yield, light attenuation in fibres, strip-fibre and fibre-PMT coupling, light trapping efficiency,<br />

etc., and also due to the photocathode disuniformity. Fig. 153 (right) shows the overall PH max distribution<br />

measured at the far end of one module (at 84 cm from the PMT). The mean value of this distribution is<br />

7.7 p.e. for events with PH max > 1 p.e. Asinglep.e. signal is still recognisable in the PH max distribution.<br />

208

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