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Experiment Proposal - opera - Infn

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1 Introduction<br />

In this document we propose an experiment (OPERA) for the direct observation of ν τ appearance from<br />

ν µ ↔ ν τ oscillations in the CNGS long baseline beam [1] from the CERN SPS to the Gran Sasso Laboratory.<br />

OPERA aims at high sensitivity in the parameter region indicated by the deficit of atmospheric<br />

muon neutrinos and by its zenith angle dependence as observed by the Super-Kamiokande experiment.<br />

The experiment exploits nuclear emulsions as very high resolution tracking devices for the direct detection<br />

of the decay of the τ produced in the charged current (CC) interaction of the ν τ with the target. Preliminary<br />

ideas and designs of the experiment can be found in [2–5] and in the Progress Report presented<br />

to the Scientific Committees in 1999 [6].<br />

The technique of nuclear emulsion has found a large scale application in the target of the CHORUS<br />

experiment [7] in which the automatic scanning of a large sample of events has first been applied. This<br />

technique can be further improved and lead to the much larger scale of the OPERA target. Its mass<br />

is made of lead plates, with emulsion films used as high precision trackers, unlike in CHORUS in which<br />

emulsions constitute the bulk of the target mass.<br />

The experiment design is based on the Emulsion Cloud Chamber (ECC) detector, a modular structure<br />

made of a sandwich of passive material plates interspaced with emulsion layers (Fig. 1). By assembling<br />

a large quantity of such modules, it is possible to conceive and realise a ∼ 2000 ton fine-grained vertex<br />

detector optimised for the study of ν τ appearance.<br />

Beam<br />

Emulsion Sheet (ES)<br />

Passive material plate<br />

Figure 1: Schematic structure of an Emulsion Cloud Chamber (ECC).<br />

This target is complemented by arrays of electronic trackers for the real time determination of the<br />

event position and by magnetised iron spectrometers for muon identification and for the reconstruction<br />

of their charge and momentum.<br />

5

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