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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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Nonstandard Neutrinos 261<br />

In three-dimensional flavor space one is free to choose any superposition<br />

of states <strong>as</strong> a b<strong>as</strong>is. It is convenient and common practice to use<br />

the m<strong>as</strong>s eigenstates (vacuum propagation eigenstates) <strong>for</strong> each column<br />

of Fig. 7.1. Thus by definition the electron is the charged lepton with<br />

the smallest m<strong>as</strong>s eigenvalue, the muon the second, and the tau the<br />

heaviest, and similarly <strong>for</strong> the quarks.<br />

All fermions interact by virtue of the weak <strong>for</strong>ce and thus couple to<br />

the W ± and Z ◦ gauge bosons, the quarks and charged leptons in addition<br />

couple to photons, while only the quarks interact by the strong<br />

<strong>for</strong>ce and thus couple to gluons. The W ± (charged current) interaction<br />

h<strong>as</strong> the important property of changing, <strong>for</strong> example, a charged<br />

lepton into a neutrino <strong>as</strong> in the reaction p + e − → n + ν e (Fig. 7.3). If<br />

the initial charged lepton w<strong>as</strong> an electron (the lightest charged lepton<br />

m<strong>as</strong>s eigenstate), the outgoing neutrino state is defined to be an “electron<br />

neutrino” or ν e which in general will be a certain superposition of<br />

neutrino m<strong>as</strong>s eigenstates.<br />

Fig. 7.3. Typical charged-current reaction.<br />

This phenomenon of Cabbibo mixing is well established among the<br />

quarks. For example, in the process of Fig. 7.3 the transition among the<br />

quarks is between u and cos θ C d + sin θ C s where cos θ C = 0.975 refers<br />

to the Cabbibo angle. Kinematics permitting, the final-state hadron<br />

will sometimes be uds which constitutes the Λ particle with a m<strong>as</strong>s of<br />

1.116 GeV compared with 0.934 GeV <strong>for</strong> the neutron (udd).<br />

The superposition of quark states into which u trans<strong>for</strong>ms by a<br />

charged-current interaction is commonly denoted by d ′ , charm couples<br />

to s ′ , and top to b ′ while the unprimed states refer to the first, second,<br />

and third m<strong>as</strong>s eigenstates in the d-column of Fig. 7.1. Ignoring the<br />

third family one h<strong>as</strong><br />

( d<br />

′<br />

s ′ )<br />

=<br />

( ) ( cos θC sin θ C d<br />

− sin θ C cos θ C s<br />

)<br />

. (7.5)<br />

It is only by convention that the mixing is applied to the d-column of<br />

the quarks rather than the u-column or both.

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