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Development of a Liquid Scintillator and of Data ... - Borexino - Infn

Development of a Liquid Scintillator and of Data ... - Borexino - Infn

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2.4 Background<br />

- Potassium is ubiquitous with a concentration <strong>of</strong> 2.4 % in the earth’s crust. Naturally<br />

occurring K has an isotopic abundance <strong>of</strong> ¢ with a half life <strong>of</strong> ¢ years;<br />

89 % <strong>of</strong> its decays proceed by beta emission with an endpoint <strong>of</strong> 1.3 MeV <strong>and</strong> 11 %<br />

decay by electron capture with the emission <strong>of</strong> a 1.46 MeV gamma. The tolerable limit<br />

for BOREXINO is 10 g/g (KÒØ) in the scintillator. The potassium content in the fluor<br />

PPO as delivered was measured by NAA to be ¡ g/g [Gol97]. By water extraction<br />

<strong>of</strong> a concentrated solution (100 g/l PPO in PC) this could be reduced several orders<br />

<strong>of</strong> magnitude, so that the final potassium concentration in the CTF scintillator (1.5 g/l<br />

PPO in PC) was below the sensitivity limit <strong>of</strong> both the CTF ( ¡ g/g) <strong>and</strong> NAA<br />

( ¡ g/g). The purity requirement is thus not directly confirmed, but it is expected<br />

to be met because <strong>of</strong> the high efficiency <strong>of</strong> the water extraction.<br />

- Be can be formed by proton <strong>and</strong> neutron reactions on C from cosmic radiation. It<br />

decays by electron capture with a half life <strong>of</strong> 53 days, with a 10 %-branch emitting a<br />

478 keV gamma. In equilibrium at the earth’s surface Be gammas are expected to give<br />

a count rate <strong>of</strong> 2700 per day <strong>and</strong> ton <strong>of</strong> scintillator [Vog96]. This rate can be reduced by<br />

bringing the scintillator underground directly after distillation, before the equilibrium<br />

rate <strong>of</strong> Be is reached (after one day <strong>of</strong> surface exposure the expected gamma rate is<br />

per day <strong>and</strong> ton), <strong>and</strong> storing the scintillator underground for a sufficient period <strong>of</strong><br />

time to allow the Be to decay, or by removing the Be through purification. At a small<br />

rate, Be will also be produced on site by cosmic ray muons (see paragraph 2.4.3).<br />

Though there is no clear signature for a single neutrino event, there are several methods to<br />

discriminate certain classes <strong>of</strong> background events:<br />

- correlated events: the method consists <strong>of</strong> tagging delayed coincidences in the U <strong>and</strong><br />

Th decay chains ( Bi- Po, ¬-« with t s; Bi- Po, ¬-« with t <br />

Isotope Abundance T [a] Concentration [g/g]<br />

Cd 12.2 % ¡<br />

In 95.8 % ¡<br />

K 0.01 % ¡<br />

<br />

<br />

¡<br />

¡<br />

¡<br />

La 0.09 % ¡ ¡<br />

Lu 2.59 % ¡ ¡<br />

Rb 27.8 % ¡ ¡<br />

Th 100 % ¡ ¡<br />

U 99.3 % ¡<br />

Table 2.2: Trace element concentrations at an equal amount <strong>of</strong> 1 event/(100t day) to the background<br />

rate in BOREXINO in the energy range from 250 - 800 keV, after application <strong>of</strong> all cuts<br />

(correlated events, «/¬ discrimination, statistical subtraction).<br />

<br />

¡<br />

<br />

<br />

<br />

<br />

<br />

<br />

31

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