Development of a Liquid Scintillator and of Data ... - Borexino - Infn
Development of a Liquid Scintillator and of Data ... - Borexino - Infn
Development of a Liquid Scintillator and of Data ... - Borexino - Infn
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2.3 Detector Design<br />
the CTF for radioactive impurities <strong>and</strong> for optical properties <strong>and</strong> then stored in three 120 m<br />
stainless steel storage vessels until filling <strong>of</strong> the BOREXINO detector. The raw material for the<br />
PC may come from different petroleum sources, which can cause variability in the C level.<br />
The CTF will be used to test the C level to assure that the scintillator is appropriate for BO-<br />
REXINO. The fluor PPO will be purified <strong>of</strong>f-line as concentrated solution in pseudocumene.<br />
The existing CTF purification plant will be modified to process the fluor solution, by a combination<br />
<strong>of</strong> water extraction <strong>and</strong> distillation. The concentrated fluor solution will be stored in<br />
two 4 m vessels until it is added to the solvent during the filling operation to a concentration<br />
<strong>of</strong> 1.5 g/l. The PC used for shielding will be delivered <strong>and</strong> purified on-line for direct filling <strong>of</strong><br />
the buffer. The DMP is added on-line to a concentration <strong>of</strong> 5 g/l .<br />
Water Purification System<br />
Water is a major shielding component for both BOREXINO <strong>and</strong> the CTF, attenuating<br />
the gamma ray flux from the rock surrounding hall C. The design purity goal is about<br />
Í in the CTF <strong>and</strong> about Í in BOREXINO (where additional shielding<br />
is provided by the PC buffer). The water purification system consists <strong>of</strong> a purification<br />
system for raw water from the rock, <strong>and</strong> a recirculation loop to maintain the purity <strong>of</strong> the water.<br />
The water is processed by reverse osmosis, a continuous deionization unit, ultra filtration,<br />
an ion exchanger <strong>and</strong> a final nitrogen stripping to remove Rn. For details see [Bal96].<br />
Nitrogen System<br />
Nitrogen gas is used in BOREXINO as a purge gas to remove gaseous contaminations ( Rn,<br />
Kr) from the scintillator <strong>and</strong> buffer fluids as well as a buffer gas against recontamination with<br />
atmospheric air. Two qualities <strong>of</strong> gaseous nitrogen with the following Rn-purity are provided<br />
by the nitrogen plant: regular nitrogen (RN , 1 mBq/m ) <strong>and</strong> high purity nitrogen (HPN ,<br />
10 ÕÑ ). The primary source <strong>of</strong> the nitrogen will be liquid nitrogen commercially delivered<br />
to the LNGS <strong>and</strong> stored in three 6 m tanks. The regular nitrogen is produced by direct<br />
evaporation <strong>of</strong> the liquid. The high purity nitrogen is obtained from two high purity charcoal<br />
traps operated at Æ in line with the liquid flow from the storage tanks to a special evaporator<br />
<strong>and</strong> heater. The high purity line is fabricated <strong>of</strong> electropolished stainless steel to maintain<br />
the Rn-purity level. For a detailed description <strong>of</strong> the system see [Rau99, Heu00].<br />
Electronics <strong>and</strong> <strong>Data</strong> Acquisition<br />
In order to get the information on time, position <strong>and</strong> energy <strong>of</strong> an event, the time <strong>and</strong> pulse<br />
height information <strong>of</strong> each PMT are needed. The basic block diagram <strong>of</strong> the electronics is<br />
shown in fig. 2.8. The PMTs will work mainly in the single photoelectron mode (events in<br />
the neutrino window have pulse heights between 50 <strong>and</strong> 300 photoelectrons), but can also<br />
give very large signals due to cosmic rays. The PMT signals arrive at the Front End Board,<br />
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