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Etude et impact du bruit de fond corrélé pour la mesure de l'angle ...

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Chapter 2<br />

Neutrino physics<br />

tel-00821629, version 1 - 11 May 2013<br />

In this chapter the physics re<strong>la</strong>ted to the neutrino is wi<strong>de</strong>ly discussed both<br />

from the theor<strong>et</strong>ical and experimental point of view, with a particu<strong>la</strong>r focus<br />

on neutrino oscil<strong>la</strong>tion. The current state of the art regarding the measurement<br />

of the oscil<strong>la</strong>tion param<strong>et</strong>ers is given with a <strong>de</strong>scription of the most<br />

important experiments in this field. The problem re<strong>la</strong>ted to the nature of the<br />

neutrino mass is also briefly <strong>de</strong>scribed. Finally, the open questions and the<br />

future e↵orts to be addressed by the neutrino community are also discussed.<br />

2.1 The standard mo<strong>de</strong>l of particle physics, an<br />

overview<br />

The Standard Mo<strong>de</strong>l of particle physics (SM) is the theory <strong>de</strong>scribing how<br />

the fundamental constituents of our universe interact.<br />

From the technical point of view the SM is a renormalisable gauge field theory,<br />

based on the symm<strong>et</strong>ry group SU(3) C ⌦SU(2) L ⌦U(1) Y which <strong>de</strong>scribe<br />

strong, weak and electromagn<strong>et</strong>ic interaction, via the exchange of spin-1<br />

gauge field: eight massless gluons for the strong interaction, one massless<br />

photon for the electromagn<strong>et</strong>ic interaction and three massive bosons, W ±<br />

and Z 0 for the weak interaction.<br />

The known elementary particles and antiparticles are fermions with spin-1/2<br />

and are organised in two families according on how they interact: quarks<br />

and leptons. Quarks interacts with all the three forces, while leptons interact<br />

only through the electromagn<strong>et</strong>ic and/or the weak force. Quarks<br />

and leptons exist in three generations or f<strong>la</strong>vours, with di↵erent masses and<br />

f<strong>la</strong>vour quantum numbers, but with i<strong>de</strong>ntical interactions, which make the<br />

SM symm<strong>et</strong>ric with respect to the f<strong>la</strong>vour. A summary of SM fermions<br />

and bosons is shown Fig. 2.1.<br />

The fermions are a representation of the symm<strong>et</strong>ry group and can be written<br />

17

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