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1. Introduction<br />

Among the large number of topics relevant to the design of the n_TOF facility at CERN, a<br />

question of primary importance from the experimental point of view is the determination and<br />

definition of the characteristics of the installation. The time-of-flight (TOF) measurements require a<br />

geometrically well-defined neutron beam at the sample position and the absence of backgrounds.<br />

Moreover, the neutron beam has to be adapted to the size of the samples, which is limited by the<br />

available amounts of high purity materials, by the target construction procedure and also by their<br />

intrinsic radioactivity (in case of unstable isotopes). The neutron beam has to be compatible with the<br />

requirements coming from the various proposed experimental techniques. The experimental<br />

programme of the n_TOF project covers a wide range of measurements summarised as follows:<br />

• (n,γ) cross-section measurements with C 6 D 6 detectors (in a first phase) and with a total<br />

absorption 4π calorimeter (in the second phase).<br />

• (n,f) cross-section measurements with Parallel Plate Avalanche Chambers (PPAC).<br />

• (n,xn) cross-section measurements with Ge or Si detectors.<br />

Even though many sources of background can be highly suppressed through the time-of-flight<br />

tagging, those background events having a time correlation similar to the neutrons may not be rejected<br />

and may severely distort the measurements. Such background sources can be classified in two<br />

categories: i) neutron reactions at the sample without the proper time-energy relation and ii) signals in<br />

the detectors (produced by photons, neutron recoils or other particles) not originating from the reaction<br />

under study. In the first case, the background can be highly reduced by designing the optical and<br />

shielding elements (beam tube, collimators and walls) of the neutron beam line. The second<br />

background species are also reduced in this way, but in addition the number of secondary reactions (of<br />

neutrons and charged particles) has to be minimised also at the experimental area and its vicinity. The<br />

n_TOF collaboration has dedicated a big effort to the studies needed for the definition of the neutron<br />

beam design. Such studies covered a large spectrum of issues that can be summarised as follows:<br />

• Study of the neutronic properties of the spallation target. In particular, production rates, the<br />

energy, the time, the spatial and the angular distribution of the neutrons.<br />

• Study and design of the beam optics, i.e. beam tube and collimators.<br />

• Design of the necessary shielding elements, which guarantee clean experimental conditions.<br />

It should be emphasised that all these investigations were made under the scope of providing<br />

optimal conditions to the measurements, according to the following directives:<br />

• The neutron beam size should have a radius as small as 2 cm, given the availability of the<br />

samples, its intrinsic radioactivity, the overall detection efficiencies and the experimental<br />

requirements arising from the capture (both the C 6 D 6 detectors and the 4π calorimeter), the<br />

fission and the (n, xn) measurements. However, further developments are considered in order<br />

to adapt the beam characteristics to particular measurements by studying and designing<br />

variable size collimators.<br />

• Design the corresponding beam optics (beam tube and collimators) such as to achieve neutron<br />

and gamma backgrounds by order of magnitudes lower than the beam flux.<br />

• Define the shielding elements such, as to improve the background attenuation and respect at<br />

the same time the conditions imposed by the CERN safety rules, which impose the<br />

accessibility and emergency escape paths of the installation.<br />

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